TWI817205B - Optical lens assembly, imaging apparatus and electronic device - Google Patents

Optical lens assembly, imaging apparatus and electronic device Download PDF

Info

Publication number
TWI817205B
TWI817205B TW110137381A TW110137381A TWI817205B TW I817205 B TWI817205 B TW I817205B TW 110137381 A TW110137381 A TW 110137381A TW 110137381 A TW110137381 A TW 110137381A TW I817205 B TWI817205 B TW I817205B
Authority
TW
Taiwan
Prior art keywords
optical lens
wavelength
optical
infrared filter
absorbing material
Prior art date
Application number
TW110137381A
Other languages
Chinese (zh)
Other versions
TW202235951A (en
Inventor
張沛頎
陳泓碩
鄧鈞鴻
Original Assignee
大立光電股份有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 大立光電股份有限公司 filed Critical 大立光電股份有限公司
Priority to CN202111402486.8A priority Critical patent/CN114545592A/en
Priority to BR102021023655-8A priority patent/BR102021023655A2/en
Priority to EP21210263.6A priority patent/EP4006595A1/en
Priority to US17/534,564 priority patent/US20220163710A1/en
Publication of TW202235951A publication Critical patent/TW202235951A/en
Application granted granted Critical
Publication of TWI817205B publication Critical patent/TWI817205B/en

Links

Images

Landscapes

  • Lenses (AREA)
  • Lens Barrels (AREA)
  • Studio Devices (AREA)
  • Camera Bodies And Camera Details Or Accessories (AREA)

Abstract

According to the present disclosure, an optical lens assembly includes at least three optical lens elements. At least one optical lens element of the optical lens elements includes an infrared filter coating. The optical lens element including the infrared filter coating is made of a plastic material. The infrared filter coating is disposed on a surface of an object-side surface or an image-side surface of the optical lens element. The surface of the optical lens element having the infrared filter coating is aspheric. The infrared filter coating includes at least two different refractive indices. At least one optical lens element of the optical lens elements includes a long wavelength absorbing material. The optical lens element including the long wavelength absorbing material is made of a plastic material. Therefore, the light leak problem of the conventional optical lens with the infrared filter coating can be solved, which can improve the miniaturization the optical lens assembly and reduce the manufacturing cost of the optical lens assembly.

Description

光學鏡頭、取像裝置及電子裝置Optical lenses, imaging devices and electronic devices

本揭示內容是有關於一種光學鏡頭及取像裝置,且特別是有關於一種應用於電子裝置中並可濾除紅外線的光學鏡頭及取像裝置。The present disclosure relates to an optical lens and an imaging device, and in particular, to an optical lens and an imaging device that are used in electronic devices and can filter out infrared rays.

光學鏡頭由鏡片群和影像感測元件所組成,其中,影像感測元件由於會感測可見光以外的紅外光,因此需要設置紅外線濾除元件。習知作法是在平板元件上鍍膜來濾除紅外線,以避免紅外線感應而導致色偏,但由於反射式的鍍膜技術是採用干涉原理,其在大角度入射光處會產生反射漏光,習知作法會再以吸收式藍玻璃來解決漏光問題。The optical lens is composed of a lens group and an image sensing element. Since the image sensing element can sense infrared light other than visible light, it needs to be equipped with an infrared filter element. The common practice is to coat flat components to filter out infrared rays to avoid color cast caused by infrared ray induction. However, since the reflective coating technology uses the interference principle, it will produce reflected light leakage at large angles of incident light. We will use absorptive blue glass to solve the light leakage problem.

因此更發展出直接在藍玻璃表面製作紅外線濾除鍍膜的技術,以達到減少元件之目標,然而,具有鍍膜的藍玻璃元件成本高、微型化困難且容易碎裂。雖紅外線濾除鍍膜也可製作在塑膠鏡片表面,卻未能有效解決大角度漏光的缺陷,光線通過塑膠鏡片表面的濾除鍍膜後,會在光線大角度入射處發生較光線垂直入射的中心處更為嚴重的反射現象,鏡片離軸處的大角度入射光線會造成穿透率的波段偏移,而產生漏光反射問題。光學系統內的反射光線漫射後,將使非預期的光線進入感測元件內成像,而造成干擾真實色彩的色偏問題,因此藍玻璃仍遲遲無法被取代。Therefore, the technology of making an infrared filtering coating directly on the surface of blue glass has been developed to achieve the goal of reducing components. However, coated blue glass components are costly, difficult to miniaturize, and prone to breakage. Although infrared filtering coatings can also be made on the surface of plastic lenses, they cannot effectively solve the problem of light leakage at large angles. After light passes through the filtering coating on the surface of plastic lenses, light will occur at the center where the light is incident at a large angle than at the center where the light is vertically incident. For more serious reflection phenomena, the large angle of incident light off the axis of the lens will cause the transmittance to shift in the band, resulting in light leakage and reflection problems. After the reflected light in the optical system is diffused, unintended light will enter the sensing element and form an image, causing a color cast that interferes with the true color. Therefore, blue glass still cannot be replaced.

再者,通常在離軸處且靠近最大有效徑範圍處的光線會導致帶通波段偏移的情況,進而造成影像色均勻度不佳之問題。當紅外線濾除鍍膜被製作在曲率半徑變化劇烈的鏡片表面時,會使光線穿透濾除鍍膜的反射角度的變化更難以控制。Furthermore, the light that is usually off-axis and close to the maximum effective diameter range will cause the bandpass band to shift, thereby causing the problem of poor image color uniformity. When the infrared filter coating is made on the surface of a lens whose radius of curvature changes drastically, it will be more difficult to control the change in the reflection angle of light penetrating the filter coating.

隨著成像品質要求提升,鏡片數量相應增加,以獲得較佳的成像品質與較佳的像差修正效果。為使鏡頭成像色彩更接近真實並獲得鏡頭尺寸微小化的優勢,需發展減少光學系統中元件數量的方式,在減除藍玻璃平板元件時勢必得研發替代技術,因此亟需可減少元件數量,並具有高影像品質的創新技術。As imaging quality requirements increase, the number of lenses increases accordingly to obtain better imaging quality and better aberration correction effects. In order to make the imaging color of the lens closer to reality and gain the advantage of miniaturizing the lens size, it is necessary to develop ways to reduce the number of components in the optical system. When removing blue glass flat components, it is necessary to develop alternative technologies. Therefore, there is an urgent need to reduce the number of components and Innovative technology with high image quality.

本揭示內容提供之光學鏡頭、取像裝置及電子裝置中,藉由控制光學鏡片表面的全視場範圍內的入射光角度之最佳設計,通過分析主光線在光學鏡片表面的入射角,在最佳的光學鏡片表面配置特定的波長濾除鍍膜,並在最佳的光學鏡片添加長波長吸收材料,有助於解決習知具有紅外線濾除鍍膜的光學鏡片的漏光問題。再者,更直接減除藍玻璃元件,促進光學鏡頭的微型化,不僅降低光學鏡頭的製造成本,更無玻璃元件碎裂、損壞等問題。本揭示內容透過決定最適合配置鍍膜的光學鏡片表面之技術,不僅可以獲得紅外線濾除鍍膜的最佳製作效果,在最均勻的光學鏡片表面的鍍膜條件下,發揮應有濾除效果與減少強光反射問題,有效提升整體光學鏡頭的影像品質。本揭示內容藉由控制光學鏡片表面面形的細微變化,有助於解決嚴重強光反射現象所導致的雜散光缺陷。本揭示內容進一步藉由分析各光學鏡片的最佳光程數據,得到最有利的吸收材料添加因子,有效解決大角度入射光的偏移漏光缺陷。In the optical lens, imaging device and electronic device provided by this disclosure, by controlling the optimal design of the incident light angle within the full field of view of the optical lens surface, and by analyzing the incident angle of the chief ray on the optical lens surface, Configuring a specific wavelength filtering coating on the surface of the best optical lenses, and adding long-wavelength absorbing materials to the best optical lenses, can help solve the light leakage problem of conventional optical lenses with infrared filtering coatings. Furthermore, it directly eliminates blue glass components and promotes the miniaturization of optical lenses, which not only reduces the manufacturing cost of optical lenses, but also eliminates problems such as glass component breakage and damage. This disclosure not only obtains the best production effect of infrared filter coating by determining the most suitable optical lens surface for coating, but also exerts the proper filtering effect and reduces intensity under the most uniform coating conditions on the optical lens surface. Light reflection problem effectively improves the image quality of the overall optical lens. This disclosure helps to solve stray light defects caused by severe strong light reflection by controlling subtle changes in the surface shape of optical lenses. This disclosure further analyzes the optimal optical path data of each optical lens to obtain the most favorable absorption material addition factor, effectively solving the offset light leakage defect of large-angle incident light.

依據本揭示內容提供的一種光學鏡頭,其包含至少三光學鏡片。所述至少三光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,紅外線濾除鍍膜具有至少二種不同的折射率。所述至少三光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值為AICmax,光學鏡頭於波長500 nm – 600 nm的平均穿透率為T5060,光學鏡頭於波長700 nm – 1000 nm的平均穿透率為T70100,其滿足下列條件:AICmax ≤ 40度;80% ≤ T5060;以及T70100 ≤ 10%。An optical lens provided according to the present disclosure includes at least three optical lenses. At least one of the at least three optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located on the object-side surface and the image-side surface of the optical lens. One of the surfaces, the optical lens surface including the infrared filter coating, is an aspherical surface, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the at least three optical lenses includes a long-wavelength absorbing material, and the optical lens including the long-wavelength absorbing material is made of a plastic material. The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating is AICmax. The average transmittance of the optical lens at a wavelength of 500 nm – 600 nm is T5060. The optical lens has a wavelength of 700 nm – 1000 nm. The average penetration rate is T70100, which meets the following conditions: AICmax ≤ 40 degrees; 80% ≤ T5060; and T70100 ≤ 10%.

依據本揭示內容提供的一種取像裝置,其包含如前段所述之光學鏡頭以及一電子感光元件,其中電子感光元件設置於光學鏡頭的一成像面。An imaging device provided according to the present disclosure includes the optical lens as described in the previous paragraph and an electronic photosensitive element, wherein the electronic photosensitive element is disposed on an imaging surface of the optical lens.

依據本揭示內容提供的一種電子裝置,其為一行動裝置,且電子裝置包含如前段所述的取像裝置。An electronic device is provided according to the present disclosure, which is a mobile device, and the electronic device includes the imaging device as described in the previous paragraph.

依據本揭示內容提供的一種電子裝置,其為一行動裝置,且電子裝置包含如前段所述的光學鏡頭,且所述光學鏡頭更包含一電子感光元件及一平板玻璃。電子感光元件設置於光學鏡頭的一成像面,且平板玻璃設置於電子感光元件的一表面。An electronic device is provided according to the present disclosure, which is a mobile device, and the electronic device includes the optical lens as described in the previous paragraph, and the optical lens further includes an electronic photosensitive element and a flat glass. The electronic photosensitive element is arranged on an imaging surface of the optical lens, and the flat glass is arranged on a surface of the electronic photosensitive element.

依據本揭示內容提供的一種電子裝置,其為一行動裝置,且電子裝置包含如前段所述的光學鏡頭。所述光學鏡頭中包含長波長吸收材料的光學鏡片在波長1050 nm的穿透率小於在波長500 nm的穿透率,且所述光學鏡頭更包含一電子感光元件,其設置於光學鏡頭的一成像面。An electronic device is provided according to the present disclosure, which is a mobile device, and the electronic device includes the optical lens as described in the previous paragraph. The transmittance of the optical lens containing long-wavelength absorbing material in the optical lens at a wavelength of 1050 nm is less than the transmittance at a wavelength of 500 nm, and the optical lens further includes an electronic photosensitive element that is disposed on a side of the optical lens. imaging surface.

依據本揭示內容提供的一種光學鏡頭,其包含至少一光學鏡片以及至少一光學元件。所述至少一光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,紅外線濾除鍍膜具有至少二種不同的折射率。所述光學元件位於光學鏡片的像側,所述至少一光學元件中至少一光學元件包含一長波長吸收材料。全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值為AICmax,光學鏡頭於波長500 nm – 600 nm的平均穿透率為T5060,光學鏡頭於波長700 nm – 1000 nm的平均穿透率為T70100,其滿足下列條件:AICmax ≤ 40度;80% ≤ T5060;以及T70100 ≤ 10%。An optical lens is provided according to the present disclosure, which includes at least one optical lens and at least one optical element. At least one of the at least one optical lens includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located on the object-side surface and the image-side surface of the optical lens. One of the surfaces, the optical lens surface including the infrared filter coating, is an aspherical surface, and the infrared filter coating has at least two different refractive indexes. The optical element is located on the image side of the optical lens, and at least one of the at least one optical element includes a long wavelength absorbing material. The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating is AICmax. The average transmittance of the optical lens at a wavelength of 500 nm – 600 nm is T5060. The optical lens has a wavelength of 700 nm – 1000 nm. The average penetration rate is T70100, which meets the following conditions: AICmax ≤ 40 degrees; 80% ≤ T5060; and T70100 ≤ 10%.

依據本揭示內容提供的一種電子裝置,其為一行動裝置,且電子裝置包含如前段所述的光學鏡頭。An electronic device is provided according to the present disclosure, which is a mobile device, and the electronic device includes the optical lens as described in the previous paragraph.

當AICmax滿足上述條件時,藉由控制全視場範圍內的光學鏡片表面的入射光角度,有助於解決習知具有紅外線濾除鍍膜的光學鏡片的漏光問題。When AICmax meets the above conditions, by controlling the incident light angle on the surface of the optical lens within the entire field of view, it helps to solve the light leakage problem of conventional optical lenses with infrared filter coatings.

當T5060滿足上述條件時,高穿透率可以使光學鏡頭具有良好影像品質。When T5060 meets the above conditions, high transmittance can make the optical lens have good image quality.

當T70100滿足上述條件時,可以避免近紅外線干擾成像而降低影像品質。When the T70100 meets the above conditions, it can avoid near-infrared rays interfering with imaging and reducing image quality.

本揭示內容一實施方式提供一種光學鏡頭,其包含至少三光學鏡片。所述至少三光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,紅外線濾除鍍膜具有至少二種不同的折射率。所述至少三光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。An embodiment of the present disclosure provides an optical lens, which includes at least three optical lenses. At least one of the at least three optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located on the object-side surface and the image-side surface of the optical lens. One of the surfaces, the optical lens surface including the infrared filter coating, is an aspherical surface, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the at least three optical lenses includes a long-wavelength absorbing material, and the optical lens including the long-wavelength absorbing material is made of a plastic material.

全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值為AICmax,光學鏡頭於波長500 nm – 600 nm的平均穿透率為T5060,光學鏡頭於波長700 nm – 1000 nm的平均穿透率為T70100,其滿足下列條件:AICmax ≤ 40度;80% ≤ T5060;以及T70100 ≤ 10%。The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating is AICmax. The average transmittance of the optical lens at a wavelength of 500 nm – 600 nm is T5060. The optical lens has a wavelength of 700 nm – 1000 nm. The average penetration rate is T70100, which meets the following conditions: AICmax ≤ 40 degrees; 80% ≤ T5060; and T70100 ≤ 10%.

本揭示內容藉由控制光學鏡片表面的全視場範圍內的入射光角度之最佳設計,在最佳的光學鏡片表面配置特定的波長濾除鍍膜,並在最佳的光學鏡片添加長波長吸收材料,有助於解決習知具有紅外線濾除鍍膜的光學鏡片的漏光問題。再者,更直接減除藍玻璃元件,促進光學鏡頭的微型化,不僅降低光學鏡頭的製造成本,更無玻璃元件碎裂、損壞等問題。This disclosure controls the optimal design of the incident light angle within the full field of view of the optical lens surface, configures a specific wavelength filter coating on the optimal optical lens surface, and adds long-wavelength absorption to the optimal optical lens The material helps to solve the light leakage problem of conventional optical lenses with infrared filter coating. Furthermore, it directly eliminates blue glass components and promotes the miniaturization of optical lenses, which not only reduces the manufacturing cost of optical lenses, but also eliminates problems such as glass component breakage and damage.

全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值為AICmax,其滿足下列條件:AICmax ≤ 40度。或者,其可以滿足下列條件:AICmax ≤ 45度;AICmax ≤ 35度;AICmax ≤ 30度;AICmax ≤ 25度;AICmax ≤ 20度;或AICmax ≤ 15度。The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating is AICmax, which meets the following conditions: AICmax ≤ 40 degrees. Alternatively, it may satisfy the following conditions: AICmax ≤ 45 degrees; AICmax ≤ 35 degrees; AICmax ≤ 30 degrees; AICmax ≤ 25 degrees; AICmax ≤ 20 degrees; or AICmax ≤ 15 degrees.

光學鏡頭於波長500 nm – 600 nm的平均穿透率為T5060,其滿足下列條件:80% ≤ T5060。或者,其可以滿足下列條件:75% ≤ T5060;85% ≤ T5060;或90% ≤ T5060 < 100%。如此,高穿透率可以使光學鏡頭具有良好影像品質。The average transmittance of the optical lens at wavelengths 500 nm – 600 nm is T5060, which meets the following conditions: 80% ≤ T5060. Alternatively, it can meet the following conditions: 75% ≤ T5060; 85% ≤ T5060; or 90% ≤ T5060 < 100%. In this way, high transmittance can make the optical lens have good image quality.

光學鏡頭於波長700 nm – 1000 nm的平均穿透率為T70100,其滿足下列條件:T70100 ≤ 10%。或者,其可以滿足下列條件:T70100 ≤ 5%;T70100 ≤ 4%;T70100 ≤ 3%;T70100 ≤ 2%;或0% < T70100 ≤ 1%。如此,可以避免近紅外線干擾成像而降低影像品質。The average transmittance of the optical lens at wavelengths 700 nm – 1000 nm is T70100, which meets the following conditions: T70100 ≤ 10%. Alternatively, it can satisfy the following conditions: T70100 ≤ 5%; T70100 ≤ 4%; T70100 ≤ 3%; T70100 ≤ 2%; or 0% < T70100 ≤ 1%. In this way, near-infrared rays can be prevented from interfering with imaging and degrading image quality.

各光學鏡片表面的鍍膜配置主因子為FC,各光學鏡片表面的鍍膜配置第一因子為Fc1,各光學鏡片表面的鍍膜配置第二因子為Fc2,FC = LOG(Fc1×Fc2),且包含紅外線濾除鍍膜的光學鏡片的至少一表面可以滿足條件:0.96 ≤ FC。如此,可以決定最適合配置鍍膜的光學鏡片表面之技術,不僅可以獲得紅外線濾除鍍膜的最佳製作效果,在最均勻的光學鏡片表面的鍍膜條件下,發揮應有濾除效果與減少強光反射問題,有效提升整體光學鏡頭的影像品質。再者,其可以滿足下列條件:0.3 ≤ FC;0.5 ≤ FC;0.7 ≤ FC;1 ≤ FC ≤ 100;2 ≤ FC ≤ 1000;或3 ≤ FC < ∞。The main factor of the coating configuration on the surface of each optical lens is FC, the first factor of the coating configuration on the surface of each optical lens is Fc1, and the second factor of the coating configuration on the surface of each optical lens is Fc2, FC = LOG(Fc1×Fc2), and includes infrared rays At least one surface of the filter-coated optical lens can meet the condition: 0.96 ≤ FC. In this way, the most suitable technology for configuring the optical lens surface with coating can be determined. Not only can the best production effect of infrared filtering coating be obtained, but under the most uniform coating conditions on the optical lens surface, the proper filtering effect and glare reduction can be exerted. Reflection problems effectively improve the image quality of the overall optical lens. Furthermore, it can satisfy the following conditions: 0.3 ≤ FC; 0.5 ≤ FC; 0.7 ≤ FC; 1 ≤ FC ≤ 100; 2 ≤ FC ≤ 1000; or 3 ≤ FC < ∞.

各光學鏡片表面的鍍膜配置第一因子為Fc1,各光學鏡片於光軸上的厚度為CT,各光學鏡片表面上與光軸交點間水平位移的最大值為SAGmax,Fc1 = CT/|SAGmax|,且包含紅外線濾除鍍膜的光學鏡片的至少一表面可以滿足條件:1.82 ≤ Fc1。如此,藉由控制光學鏡片厚度與光學鏡片表面的水平位移變化,可以獲得紅外線濾除鍍膜的最佳配置效果,有效發揮濾除效果與減少強光嚴重反射。再者,其可以滿足下列條件:2 ≤ Fc1;2.5 ≤ Fc1;5 ≤ Fc1;10 ≤ Fc1;15 ≤ Fc1 ≤ 1000;或20 ≤ Fc1 < ∞。The first factor of the coating configuration on the surface of each optical lens is Fc1, the thickness of each optical lens on the optical axis is CT, the maximum horizontal displacement between the intersection point on the surface of each optical lens and the optical axis is SAGmax, Fc1 = CT/|SAGmax| , and at least one surface of the optical lens containing the infrared filter coating can meet the condition: 1.82 ≤ Fc1. In this way, by controlling the thickness of the optical lens and the horizontal displacement of the optical lens surface, the optimal configuration of the infrared filter coating can be achieved, effectively exerting the filtering effect and reducing severe reflection of strong light. Furthermore, it can satisfy the following conditions: 2 ≤ Fc1; 2.5 ≤ Fc1; 5 ≤ Fc1; 10 ≤ Fc1; 15 ≤ Fc1 ≤ 1000; or 20 ≤ Fc1 < ∞.

各光學鏡片表面的鍍膜配置第二因子為Fc2,各光學鏡片表面於光學有效徑範圍內的切線斜率的平均值為SPavg,各光學鏡片表面於光學有效徑範圍內的切線斜率的最小值為SPmin,Fc2 = |SPavg|×|SPmin|,且包含紅外線濾除鍍膜的光學鏡片的至少一表面可以滿足條件:4.98 ≤ Fc2。如此,藉由控制光學鏡片表面面形的細微變化,有助於解決嚴重強光反射現象所導致的雜散光缺陷。再者,其可以滿足下列條件:1 ≤ Fc2;5 ≤ Fc2;10 ≤ Fc2;20 ≤ Fc2;25 ≤ Fc2 ≤ 10000;或45 ≤ Fc2 < ∞。The second factor of the coating configuration on the surface of each optical lens is Fc2, the average tangent slope of each optical lens surface within the optical effective diameter range is SPavg, and the minimum value of the tangent slope of each optical lens surface within the optical effective diameter range is SPmin , Fc2 = |SPavg|×|SPmin|, and at least one surface of the optical lens containing the infrared filter coating can meet the condition: 4.98 ≤ Fc2. In this way, by controlling subtle changes in the surface shape of optical lenses, it helps to solve stray light defects caused by severe strong light reflection. Furthermore, it can satisfy the following conditions: 1 ≤ Fc2; 5 ≤ Fc2; 10 ≤ Fc2; 20 ≤ Fc2; 25 ≤ Fc2 ≤ 10000; or 45 ≤ Fc2 < ∞.

包含紅外線濾除鍍膜的光學鏡片表面於離軸處可以無反曲點或臨界點。如此,藉由光學鏡片表面於離軸處無反曲點或無臨界點的設計,可以減少面形變化程度,以獲得均勻的濾除效果。Optical lens surfaces containing infrared filtering coatings may have no inflection points or critical points off-axis. In this way, through the design of the optical lens surface with no inflection point or critical point off-axis, the degree of surface shape change can be reduced to obtain a uniform filtering effect.

紅外線濾除鍍膜的總層數為tLs,其可以滿足條件:40 < tLs ≤ 80。如此,藉由將紅外線濾除鍍膜的總層數控制於最佳數量,可以在濾除效果與成本控制間取得平衡,進一步在高效率的狀態下濾除光線。再者,其可以滿足下列條件:30 ≤ tLs ≤ 90;35 ≤ tLs ≤ 80;38 ≤ tLs ≤ 70;40 ≤ tLs ≤ 65;或42 ≤ tLs ≤ 50。The total number of layers of infrared filter coating is tLs, which can meet the conditions: 40 < tLs ≤ 80. In this way, by controlling the total number of layers of infrared filtering coating to an optimal number, a balance between filtering effect and cost control can be achieved, and light can be further filtered with high efficiency. Furthermore, it can satisfy the following conditions: 30 ≤ tLs ≤ 90; 35 ≤ tLs ≤ 80; 38 ≤ tLs ≤ 70; 40 ≤ tLs ≤ 65; or 42 ≤ tLs ≤ 50.

紅外線濾除鍍膜的總膜厚為tTk,其可以滿足條件:4000 nm < tTk ≤ 10000 nm。如此,藉由適當的膜厚設計,可以獲得所需的濾除與通透效果,減少雜波產生與提升影像品質,進而有效維持紅外線濾除鍍膜的完整性,並避免光學鏡片變形。再者,其可以滿足下列條件:4500 nm ≤ tTk ≤ 10000 nm;4700 nm ≤ tTk ≤ 9000 nm;5100 nm ≤ tTk ≤ 8000 nm;5200 nm ≤ tTk ≤ 7000 nm;或5500 nm ≤ tTk ≤ 6000 nm。The total film thickness of the infrared filter coating is tTk, which can meet the conditions: 4000 nm < tTk ≤ 10000 nm. In this way, through appropriate film thickness design, the required filtering and transparency effects can be achieved, reducing clutter generation and improving image quality, thereby effectively maintaining the integrity of the infrared filtering coating and avoiding optical lens deformation. Furthermore, it can satisfy the following conditions: 4500 nm ≤ tTk ≤ 10000 nm; 4700 nm ≤ tTk ≤ 9000 nm; 5100 nm ≤ tTk ≤ 8000 nm; 5200 nm ≤ tTk ≤ 7000 nm; or 5500 nm ≤ tTk ≤ 6000 nm.

包含紅外線濾除鍍膜的光學鏡片可以為一種補正鏡片。如此,可以有效解決塑膠光學鏡片表面鍍膜時的溫度效應問題,有助於維持光學鏡片的鍍膜完整性與塑膠光學鏡片的高精度,達成高品質的成像鏡頭。Optical lenses containing infrared filtering coatings can be a type of corrective lens. In this way, the temperature effect problem when coating the surface of plastic optical lenses can be effectively solved, helping to maintain the coating integrity of the optical lenses and the high precision of the plastic optical lenses, and achieve high-quality imaging lenses.

光學鏡頭的全視角為FOV,其可以滿足條件:60度

Figure 110137381-A0305-02-0012-53
FOV
Figure 110137381-A0305-02-0012-78
200度。如此,藉由大視角之設計,有助於擴增影像擷取範圍,使光學鏡頭適用於各式高階行動裝置的主攝影鏡頭。再者,其可以滿足下列條件:40度
Figure 110137381-A0305-02-0012-54
FOV
Figure 110137381-A0305-02-0012-63
220度;70度
Figure 110137381-A0305-02-0012-60
FOV
Figure 110137381-A0305-02-0012-59
180度;80度
Figure 110137381-A0305-02-0012-58
FOV
Figure 110137381-A0305-02-0012-55
150度;75度
Figure 110137381-A0305-02-0012-62
FOV
Figure 110137381-A0305-02-0012-61
120度;或80度
Figure 110137381-A0305-02-0012-57
FOV
Figure 110137381-A0305-02-0012-56
100度。 The full viewing angle of the optical lens is FOV, which can meet the conditions: 60 degrees
Figure 110137381-A0305-02-0012-53
FOV
Figure 110137381-A0305-02-0012-78
200 degrees. In this way, the large viewing angle design helps to expand the image capture range, making the optical lens suitable for the main photography lens of various high-end mobile devices. Furthermore, it can meet the following conditions: 40 degrees
Figure 110137381-A0305-02-0012-54
FOV
Figure 110137381-A0305-02-0012-63
220 degrees; 70 degrees
Figure 110137381-A0305-02-0012-60
FOV
Figure 110137381-A0305-02-0012-59
180 degrees; 80 degrees
Figure 110137381-A0305-02-0012-58
FOV
Figure 110137381-A0305-02-0012-55
150 degrees; 75 degrees
Figure 110137381-A0305-02-0012-62
FOV
Figure 110137381-A0305-02-0012-61
120 degrees; or 80 degrees
Figure 110137381-A0305-02-0012-57
FOV
Figure 110137381-A0305-02-0012-56
100 degree.

各光學鏡片的吸收材料配置主因子為FA,各光學鏡片於全視場主光線光程比的平均值為CPavg,各光學鏡片於全視場主光線光程比的標準差為CPst,FA=LOG(1/(|(CPavg-1)×CPst|)),且包含長波長吸收材料的光學鏡片可以滿足條件:2.31

Figure 110137381-A0305-02-0012-64
FA。如此,藉由讓光學鏡片具有最佳光程設計,以添加長波長吸收材料和/或短波長吸收材料,可以有效使吸收材料均勻混合於光學鏡片中,使光學鏡片具有均勻的吸收效果,有助於在全視場範圍下完整解決大角度入射光的偏移漏光問題。再者,其可以滿足下列條件:0.5
Figure 110137381-A0305-02-0012-65
FA;1.0
Figure 110137381-A0305-02-0012-66
FA;1.5
Figure 110137381-A0305-02-0012-67
FA;1.7
Figure 110137381-A0305-02-0012-71
FA;2.0
Figure 110137381-A0305-02-0012-70
FA
Figure 110137381-A0305-02-0012-69
10;或2.5
Figure 110137381-A0305-02-0012-68
FA<∞。 The main factor of the absorption material configuration of each optical lens is FA, the average optical path length ratio of the chief ray of each optical lens in the full field of view is CPavg, and the standard deviation of the optical path ratio of the chief ray of each optical lens in the full field of view is CPst, FA= LOG(1/(|(CPavg-1)×CPst|)), and optical lenses containing long-wavelength absorbing materials can meet the conditions: 2.31
Figure 110137381-A0305-02-0012-64
FA. In this way, by allowing the optical lens to have an optimal optical path design and adding long-wavelength absorbing materials and/or short-wavelength absorbing materials, the absorbing materials can be effectively mixed evenly in the optical lens, so that the optical lens has a uniform absorption effect, and has Helps completely solve the problem of offset light leakage of incident light at large angles in the entire field of view. Furthermore, it can satisfy the following conditions: 0.5
Figure 110137381-A0305-02-0012-65
FA;1.0
Figure 110137381-A0305-02-0012-66
FA;1.5
Figure 110137381-A0305-02-0012-67
FA;1.7
Figure 110137381-A0305-02-0012-71
FA;2.0
Figure 110137381-A0305-02-0012-70
FA
Figure 110137381-A0305-02-0012-69
10; or 2.5
Figure 110137381-A0305-02-0012-68
FA<∞.

各光學鏡片於全視場主光線光程比的平均值為CPavg,且包含長波長吸收材料的光學鏡片可以滿足條件:0.9

Figure 110137381-A0305-02-0012-72
CPavg
Figure 110137381-A0305-02-0012-73
1.1。如此,可以使光學鏡片具有最佳光程設計,有效維持全視場區域內的吸收效果一致。再者,其可以滿足下列條件:0.95
Figure 110137381-A0305-02-0012-74
CPavg
Figure 110137381-A0305-02-0012-75
1.05;或0.96
Figure 110137381-A0305-02-0012-77
CPavg
Figure 110137381-A0305-02-0012-76
1.04。 The average optical path ratio of the chief ray of each optical lens in the full field of view is CPavg, and optical lenses containing long-wavelength absorbing materials can meet the condition: 0.9
Figure 110137381-A0305-02-0012-72
CPvg
Figure 110137381-A0305-02-0012-73
1.1. In this way, the optical lens can have an optimal optical path design and effectively maintain a consistent absorption effect in the entire field of view. Furthermore, it can satisfy the following conditions: 0.95
Figure 110137381-A0305-02-0012-74
CPvg
Figure 110137381-A0305-02-0012-75
1.05; or 0.96
Figure 110137381-A0305-02-0012-77
CPvg
Figure 110137381-A0305-02-0012-76
1.04.

長波長吸收材料於50%穿透率的波長可以小於紅外線濾除鍍膜於50%穿透率的波長,且長波長吸收材料於50%穿透率的波長與紅外線濾除鍍膜於50%穿透率的波長的差值可以為20 nm以上。如此,藉由長波長吸收材料和/或短波長吸收材料與紅外線濾除鍍膜的最佳配置設計,可以完整克服大角度入射光的漏光問題。The wavelength at which the long-wavelength absorbing material has a transmittance of 50% can be smaller than the wavelength at which the infrared filter coating has a transmittance of 50%, and the wavelength at which the long-wavelength absorbing material has a transmittance of 50% is less than the wavelength at which the infrared filter coating has a transmittance of 50%. The difference between the wavelengths of the rates can be more than 20 nm. In this way, through the optimal configuration design of long-wavelength absorbing materials and/or short-wavelength absorbing materials and infrared filter coatings, the light leakage problem of large-angle incident light can be completely overcome.

包含長波長吸收材料的光學鏡片可以較包含紅外線濾除鍍膜的光學鏡片表面靠近物側。如此,藉由包含長波長吸收材料和/或短波長吸收材料的光學鏡片較靠近物側之設計,使包含吸收材料的光學鏡片先吸收欲濾除波長之光線,在剩餘波長的光線到達紅外線濾除鍍膜時,即可減少大角度光學鏡片表面的反射光線強度,以克服漏光與提升影像品質。The surface of the optical lens containing the long-wavelength absorbing material can be closer to the object side than the surface of the optical lens containing the infrared filter coating. In this way, through the design of the optical lens containing the long-wavelength absorbing material and/or the short-wavelength absorbing material closer to the object side, the optical lens containing the absorbing material first absorbs the light of the wavelength to be filtered, and then the remaining wavelength of the light reaches the infrared filter. When removing the coating, the intensity of reflected light on the surface of large-angle optical lenses can be reduced to overcome light leakage and improve image quality.

光學鏡頭在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長為LWdT5,其可以滿足條件:600 nm ≤ LWdT5 ≤ 700 nm。如此,可以控制所需的穿透光線之波長範圍,避免近紅外線干擾成像,並藉由配置光學鏡頭的最佳穿透率,以提升整體影像品質。再者,其可以滿足下列條件:610 nm ≤ LWdT5 ≤ 660 nm;620 nm ≤ LWdT5 ≤ 650 nm;625 nm ≤ LWdT5 ≤ 645 nm;或630 nm ≤ LWdT5 ≤ 640 nm。The wavelength at which the optical lens reaches 50% transmittance in the long wavelength region and the trend of negative correlation between wavelength and transmittance is LWdT5, which can meet the conditions: 600 nm ≤ LWdT5 ≤ 700 nm. In this way, the required wavelength range of penetrating light can be controlled to avoid near-infrared interference with imaging, and the overall image quality can be improved by configuring the optimal transmittance of the optical lens. Furthermore, it can satisfy the following conditions: 610 nm ≤ LWdT5 ≤ 660 nm; 620 nm ≤ LWdT5 ≤ 650 nm; 625 nm ≤ LWdT5 ≤ 645 nm; or 630 nm ≤ LWdT5 ≤ 640 nm.

所述至少三光學鏡片中至少一光學鏡片可以包含一短波長吸收材料。如此,藉由消除具有高能量的短波長光線,可以延長光學鏡片的耐用性,並進一步減少紫邊等影像缺陷問題。At least one optical lens among the at least three optical lenses may include a short wavelength absorbing material. In this way, by eliminating high-energy short-wavelength light, the durability of optical lenses can be extended and image defects such as purple fringing can be further reduced.

光學鏡頭在短波長區域且波長與穿透率呈正相關的趨勢中達到50%穿透率的波長為SWuT5,其可以滿足下列條件:370 nm ≤ SWuT5 ≤ 450 nm;380 nm ≤ SWuT5 ≤ 440 nm;390 nm ≤ SWuT5 ≤ 430 nm;400 nm ≤ SWuT5 ≤ 430 nm;或415 nm ≤ SWuT5 ≤ 430 nm。如此,可以控制所需的穿透光線之波長範圍,使光學鏡頭具有良好影像品質與耐用性。The wavelength at which the optical lens reaches 50% transmittance in the short wavelength region and the trend of positive correlation between wavelength and transmittance is SWuT5, which can meet the following conditions: 370 nm ≤ SWuT5 ≤ 450 nm; 380 nm ≤ SWuT5 ≤ 440 nm; 390 nm ≤ SWuT5 ≤ 430 nm; 400 nm ≤ SWuT5 ≤ 430 nm; or 415 nm ≤ SWuT5 ≤ 430 nm. In this way, the required wavelength range of the transmitted light can be controlled, so that the optical lens has good image quality and durability.

光學鏡頭於波長350 nm – 400 nm的平均穿透率為T3540,其可以滿足下列條件:T3540 ≤ 30%;T3540 ≤ 25%;T3540 ≤ 20%;T3540 ≤ 15%;或0% < T3540 ≤ 10%。如此,可以使光學鏡頭具有良好耐用性。The average transmittance of the optical lens at wavelengths 350 nm – 400 nm is T3540, which can meet the following conditions: T3540 ≤ 30%; T3540 ≤ 25%; T3540 ≤ 20%; T3540 ≤ 15%; or 0% < T3540 ≤ 10 %. In this way, the optical lens can have good durability.

光學鏡頭於波長400 nm – 500 nm的平均穿透率為T4050,其可以滿足下列條件:50% ≤ T4050 ≤ 90%;60% ≤ T4050 ≤ 85%;或65% ≤ T4050 ≤ 80%。如此,較佳的穿透率使光學鏡頭具有良好影像品質與耐用性。The average transmittance of the optical lens at wavelengths 400 nm – 500 nm is T4050, which can meet the following conditions: 50% ≤ T4050 ≤ 90%; 60% ≤ T4050 ≤ 85%; or 65% ≤ T4050 ≤ 80%. In this way, better transmittance enables the optical lens to have good image quality and durability.

光學鏡頭於波長650 nm – 700 nm的平均穿透率為T6570,其可以滿足下列條件:T6570 ≤ 80%;T6570 ≤ 50%;T6570 ≤ 30%;5% ≤ T6570 ≤ 25%;或0% < T6570 ≤ 20%。如此,可以減少長波長紅光干擾,以獲得良好影像品質。The average transmittance of the optical lens at wavelengths 650 nm – 700 nm is T6570, which can meet the following conditions: T6570 ≤ 80%; T6570 ≤ 50%; T6570 ≤ 30%; 5% ≤ T6570 ≤ 25%; or 0% < T6570 ≤ 20%. In this way, long-wavelength red light interference can be reduced to obtain good image quality.

光學鏡頭於波長350 nm的穿透率為T35,其可以滿足下列條件:T35 ≤ 5%;T35 ≤ 4%;T35 ≤ 3%;T35 ≤ 2%;或0% < T35 ≤ 1%。The transmittance of the optical lens at a wavelength of 350 nm is T35, which can meet the following conditions: T35 ≤ 5%; T35 ≤ 4%; T35 ≤ 3%; T35 ≤ 2%; or 0% < T35 ≤ 1%.

光學鏡頭於波長400 nm的穿透率為T40,其可以滿足下列條件:0% < T40 ≤ 60%;10% ≤ T40 ≤ 50%;10% ≤ T40 ≤ 40%;或20% ≤ T40 ≤ 30%。The transmittance of the optical lens at a wavelength of 400 nm is T40, which can meet the following conditions: 0% < T40 ≤ 60%; 10% ≤ T40 ≤ 50%; 10% ≤ T40 ≤ 40%; or 20% ≤ T40 ≤ 30 %.

光學鏡頭於波長550 nm的穿透率為T55,其可以滿足下列條件:75% ≤ T55;80% ≤ T55;85% ≤ T55;或90% ≤ T55 < 100%。The transmittance of the optical lens at a wavelength of 550 nm is T55, which can meet the following conditions: 75% ≤ T55; 80% ≤ T55; 85% ≤ T55; or 90% ≤ T55 < 100%.

光學鏡頭於波長600 nm的穿透率為T60,其可以滿足下列條件:70% ≤ T60;75% ≤ T60;77% ≤ T60;或80% ≤ T60 < 100%。The transmittance of the optical lens at a wavelength of 600 nm is T60, which can meet the following conditions: 70% ≤ T60; 75% ≤ T60; 77% ≤ T60; or 80% ≤ T60 < 100%.

光學鏡頭於波長630 nm的穿透率為T63,其可以滿足下列條件:20% ≤ T63 ≤ 80%;30% ≤ T63 ≤ 70%;40% ≤ T63 ≤ 70%;或50% ≤ T63 ≤ 60%。The transmittance of the optical lens at a wavelength of 630 nm is T63, which can meet the following conditions: 20% ≤ T63 ≤ 80%; 30% ≤ T63 ≤ 70%; 40% ≤ T63 ≤ 70%; or 50% ≤ T63 ≤ 60 %.

光學鏡頭於波長640 nm的穿透率為T64,其可以滿足下列條件:20% ≤ T64 ≤ 80%;30% ≤ T64 ≤ 70%;40% ≤ T64 ≤ 60%;或40% ≤ T64 ≤ 50%。The transmittance of the optical lens at a wavelength of 640 nm is T64, which can meet the following conditions: 20% ≤ T64 ≤ 80%; 30% ≤ T64 ≤ 70%; 40% ≤ T64 ≤ 60%; or 40% ≤ T64 ≤ 50 %.

光學鏡頭於波長650 nm的穿透率為T65,其可以滿足下列條件:20% ≤ T65 ≤ 70%;25% ≤ T65 ≤ 60%;30% ≤ T65 ≤ 50%;或35% ≤ T65 ≤ 45%。The transmittance of the optical lens at a wavelength of 650 nm is T65, which can meet the following conditions: 20% ≤ T65 ≤ 70%; 25% ≤ T65 ≤ 60%; 30% ≤ T65 ≤ 50%; or 35% ≤ T65 ≤ 45 %.

光學鏡頭於波長700 nm的穿透率為T70,其可以滿足下列條件:T70 ≤ 5%;T70 ≤ 4%;T70 ≤ 3%;T70 ≤ 2%;或0% < T70 ≤ 1%。The transmittance of the optical lens at a wavelength of 700 nm is T70, which can meet the following conditions: T70 ≤ 5%; T70 ≤ 4%; T70 ≤ 3%; T70 ≤ 2%; or 0% < T70 ≤ 1%.

光學鏡頭於波長850 nm的穿透率為T85,其可以滿足下列條件:T85 ≤ 5%;T85 ≤ 4%;T85 ≤ 3%;T85 ≤ 2%;或0% < T85 ≤ 1%。The transmittance of the optical lens at a wavelength of 850 nm is T85, which can meet the following conditions: T85 ≤ 5%; T85 ≤ 4%; T85 ≤ 3%; T85 ≤ 2%; or 0% < T85 ≤ 1%.

本揭示內容在塑膠光學鏡片表面具有干涉型的高折射率膜層與低折射率膜層交替的紅外線濾除鍍膜,紅外線濾除鍍膜所使用的高折射率材料的折射率大於2.0,較佳選擇為TiO 2(NH = 2.6142),所使用的低折射率材料的折射率小於1.8,較佳選擇為SiO 2(NL = 1.4585)。 This disclosure includes an interference-type infrared filter coating with alternating high refractive index film layers and low refractive index film layers on the surface of a plastic optical lens. The refractive index of the high refractive index material used in the infrared filter coating is greater than 2.0, which is a better choice. For TiO 2 (NH = 2.6142), the refractive index of the low refractive index material used is less than 1.8, and the better choice is SiO 2 (NL = 1.4585).

靠近塑膠光學鏡片表面的第一層鍍膜材料可為TiO 2、AlN或Al 2O 3,可以強化材料與光學鏡片之間的附著性,以避免紅外線濾除鍍膜脫落,達到保護光學鏡片表面的效果,有效強化光學鏡片的環境耐候性。 The first layer of coating material close to the surface of the plastic optical lens can be TiO 2 , AlN or Al 2 O 3 , which can strengthen the adhesion between the material and the optical lens to prevent the infrared filter coating from falling off and achieve the effect of protecting the surface of the optical lens , effectively enhance the environmental weather resistance of optical lenses.

鍍膜材料(於波長587.6 nm時的折射率)可為SiO 2(1.4585)、Al 2O 3(1.7682)、Nb 2O 5(2.3403)、TiO 2(2.6142)、ZrO 2(2.1588)、HfO 2(1.8935)、ZnO(1.9269)、Sc 2O 3(1.9872)、Ta 2O 5(2.1306)、MgF 2(1.3777)、ZnS(2.2719)、Si 3N 4(2.0381)、AlN(2.0294)和/或TiN(3.1307)。 Coating materials (refractive index at wavelength 587.6 nm) can be SiO 2 (1.4585), Al 2 O 3 (1.7682), Nb 2 O 5 (2.3403), TiO 2 (2.6142), ZrO 2 (2.1588), HfO 2 (1.8935), ZnO (1.9269), Sc 2 O 3 (1.9872), Ta 2 O 5 (2.1306), MgF 2 (1.3777), ZnS (2.2719), Si 3 N 4 (2.0381), AlN (2.0294) and/ Or TiN (3.1307).

紅外線濾除鍍膜為干涉作用之濾除原理(反射式),紅外線濾除鍍膜是在塑膠光學鏡片表面上製鍍多層薄膜,可使用物理氣相沉積(PVD),如蒸發沉積或濺射沉積等,或使用化學氣相沉積法(CVD),如超高真空化學氣相沉積、微波電漿輔助化學氣相沉積、電漿增強化學氣相沉積法或原子層沉積法等。Infrared filter coating is based on the interference filtering principle (reflective type). Infrared filter coating is a multi-layer film coated on the surface of plastic optical lenses. Physical vapor deposition (PVD) can be used, such as evaporation deposition or sputtering deposition. Or use chemical vapor deposition (CVD), such as ultra-high vacuum chemical vapor deposition, microwave plasma-assisted chemical vapor deposition, plasma-enhanced chemical vapor deposition or atomic layer deposition, etc.

本揭示內容的包含長波長吸收材料之光學鏡片(Lens with LW Absorber)是採用吸收式原理。長波長吸收材料與塑膠光學鏡片的材料混合且均勻分布其中,長波長吸收材料須能承受射出成型過程的高溫且不會裂解,以維持應有的長波長吸收效果。The optical lens (Lens with LW Absorber) containing long-wavelength absorbing material in this disclosure adopts the absorption principle. The long-wavelength absorbing material is mixed with the material of the plastic optical lens and evenly distributed. The long-wavelength absorbing material must be able to withstand the high temperature of the injection molding process without cracking to maintain the proper long-wavelength absorption effect.

本揭示內容的光學鏡頭具有包含長波長吸收材料的光學鏡片,其具有消除反射漏光之效果,可以維持色均勻度比(R/G比及B/G比),使光學鏡頭具有優異成像品質。The optical lens disclosed in this disclosure has an optical lens containing a long-wavelength absorbing material, which has the effect of eliminating reflected light leakage and can maintain the color uniformity ratio (R/G ratio and B/G ratio), so that the optical lens has excellent imaging quality.

本揭示內容是在塑膠光學鏡片添加長波長吸收材料(LA1、LA2、LA3、LA4、LA5、LA6、LA7),上述材料各具有特定的50%穿透率的波長範圍,可配合紅外線濾除鍍膜的50%穿透率的波長範圍進行組合配置,以獲得最佳的濾除效果。This disclosure is about adding long-wavelength absorbing materials (LA1, LA2, LA3, LA4, LA5, LA6, LA7) to plastic optical lenses. Each of the above materials has a specific wavelength range of 50% transmittance and can be used with infrared filter coatings. The wavelength range of 50% transmittance can be combined and configured to obtain the best filtering effect.

長波長吸收材料在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長為LWdT5,其可以滿足下列表一之條件: 表一、長波長吸收材料 材料種類 LWdT5 (nm) LA1 575 – 585 LA2 595 – 605 LA3 625 – 635 LA4 630 – 640 LA5 635 – 645 LA6 665 – 675 LA7 680 – 690 The wavelength at which the long-wavelength absorbing material reaches 50% transmittance in the long-wavelength region and the trend of negative correlation between wavelength and transmittance is LWdT5, which can meet the conditions of Table 1 below: Table 1. Long wavelength absorbing materials Material type LWdT5 (nm) LA1 575 – 585 LA2 595 – 605 LA3 625 – 635 LA4 630 – 640 LA5 635 – 645 LA6 665 – 675 LA7 680 – 690

本揭示內容的包含短波長吸收材料之光學鏡片(Lens with SW Absorber)是採用吸收式原理。短波長吸收材料與塑膠光學鏡片的材料混合且均勻分布其中,短波長吸收材料須能承受射出成型過程的高溫且不會裂解,以維持應有的短波長吸收效果。The optical lens (Lens with SW Absorber) containing short-wavelength absorbing material in this disclosure adopts the absorption principle. The short-wavelength absorbing material is mixed with the plastic optical lens material and evenly distributed. The short-wavelength absorbing material must be able to withstand the high temperature of the injection molding process without cracking, in order to maintain the proper short-wavelength absorption effect.

本揭示內容的光學鏡頭具有包含短波長吸收材料的光學鏡片,其具有消除反射漏光之效果,可以維持色均勻度比(R/G比及B/G比)與提升光學鏡片的環境耐受性,使光學鏡頭具有優異成像品質。The optical lens disclosed in this disclosure has an optical lens containing a short-wavelength absorbing material, which has the effect of eliminating reflected light leakage, maintaining the color uniformity ratio (R/G ratio and B/G ratio) and improving the environmental tolerance of the optical lens , making the optical lens have excellent imaging quality.

本揭示內容是在塑膠光學鏡片添加短波長吸收材料(SA1、SA2、SA3、SA4、SA5、SA6、SA7),上述材料各具有特定的50%穿透率的波長範圍,可配合紅外線濾除鍍膜的50%穿透率的波長範圍進行組合配置,以獲得最佳的濾除效果。This disclosure is about adding short-wavelength absorbing materials (SA1, SA2, SA3, SA4, SA5, SA6, SA7) to plastic optical lenses. Each of the above materials has a specific wavelength range of 50% transmittance and can be used with infrared filtering coatings. The wavelength range of 50% transmittance can be combined and configured to obtain the best filtering effect.

短波長吸收材料在短波長區域且波長與穿透率呈正相關的趨勢中達到50%穿透率的波長為SWuT5,其可以滿足下列表二之條件: 表二、短波長吸收材料 材料種類 SWuT5 (nm) SA1 340 – 350 SA2 390 – 400 SA3 420 – 430 SA4 430 – 440 SA5 430 – 440 SA6 440 – 450 SA7 440 – 450 The wavelength at which the short-wavelength absorbing material reaches 50% transmittance in the short-wavelength region and the trend of positive correlation between wavelength and transmittance is SWuT5, which can meet the following conditions in Table 2: Table 2. Short wavelength absorbing materials Material type SWuT5 (nm) SA1 340 – 350 SA2 390 – 400 SA3 420 – 430 SA4 430 – 440 SA5 430 – 440 SA6 440 – 450 SA7 440 – 450

本揭示內容的全視場意指由中心視場(0 Field)至最大像高視場(1.0 Field)的範圍,全視場範圍涵蓋各光學鏡片表面的光學有效區域。The full field of view in this disclosure means the range from the center field of view (0 Field) to the maximum image height field of view (1.0 Field). The full field of view covers the optically effective area of the surface of each optical lens.

本揭示內容的全視場主光線光程比的平均值與標準差計算方式,是將中心視場(0F)至最大像高視場(1.0F)以每0.02切分,等同有51個視場的數據,再計算每一視場主光線通過光學鏡片之光程與光學鏡片中心厚度的比值,再將所述視場主光線光程比進行平均值計算與標準差計算。The calculation method of the average and standard deviation of the chief ray optical path ratio of the full field of view in this disclosure is to divide the central field of view (0F) to the maximum image height field of view (1.0F) into every 0.02, which is equivalent to 51 fields of view. Field data, and then calculate the ratio of the optical path of the chief ray of each field of view through the optical lens to the center thickness of the optical lens, and then calculate the average and standard deviation of the optical path ratio of the chief ray of the field of view.

光學鏡片表面的切線斜率是在光軸為水平方向的狀態下進行計算,切線斜率在近光軸處為無限大(Infinity、INF、∞)。The tangent slope of the optical lens surface is calculated when the optical axis is in the horizontal direction, and the tangent slope is infinite (Infinity, INF, ∞) at the near optical axis.

本揭示內容所定義之長波長範圍是500 nm以上之區域,短波長範圍是500 nm以下之區域。The long wavelength range defined in this disclosure is the area above 500 nm, and the short wavelength range is the area below 500 nm.

本揭示內容的LWdT5及SWuT5為包含穿透率50%之波長的區間範圍。LWdT5 and SWuT5 in this disclosure are the ranges of wavelengths containing 50% transmittance.

本揭示內容的穿透率數據可為單一光學鏡片的量測數據,亦可為光學鏡片組成光學鏡頭後的量測數據。如果包含吸收材料的光學鏡片與包含紅外線濾除鍍膜的光學鏡片為不同片光學鏡片時,則以光學鏡頭量測的穿透率數據為主。The transmittance data in this disclosure can be the measurement data of a single optical lens, or the measurement data of the optical lenses combined into an optical lens. If the optical lens containing the absorbing material and the optical lens containing the infrared filter coating are different pieces of optical lenses, the transmittance data measured by the optical lens shall be the main one.

本揭示內容的穿透率數據皆以0度入射角的穿透率數據作為比較基準。The transmittance data in this disclosure are based on the transmittance data at an incident angle of 0 degrees as a comparison basis.

塑膠光學鏡片因厚度與高溫導致面形變化誤差過大,當紅外線濾除鍍膜的膜層數越多,則溫度影響面形精度的狀況越明顯。藉由鏡片補正技術,能有效解決塑膠光學鏡片表面鍍膜時的溫度效應問題,有助於維持光學鏡片的鍍膜完整性與塑膠光學鏡片的高精度,為達成高品質成像鏡頭的關鍵技術。Plastic optical lenses have excessive surface shape changes due to thickness and high temperature. The more layers of infrared filtering coating there are, the more obvious the effect of temperature on surface shape accuracy will be. Lens correction technology can effectively solve the problem of temperature effects when coating the surface of plastic optical lenses, helping to maintain the coating integrity of optical lenses and the high precision of plastic optical lenses, which is a key technology for achieving high-quality imaging lenses.

鏡片補正技術可為應用模流(Moldflow)分析方法、曲線擬合函數方法或波前誤差方法等,但不以此為限。其中模流分析方法是藉由模流分析找出光學鏡片表面於Z軸收縮的立體輪廓節點,轉成非球面曲線後再與原始曲線比較差異,同時考慮材料收縮率與面形變形趨勢計算得到補正值。其中曲線擬合函數方法是藉由量測元件表面輪廓誤差,以函數進行曲線擬合後並配合最佳化演算法將擬合曲線逼近量測點得到補正值。函數可以是指數(Exponential)或多項式(Polynomial)等,演算法可以是高斯牛頓法(Gauss Newton)、單形演算法(Simplex Algorithm)或最大陡降法(Steepest Descent Method)等。其中波前誤差方法是藉由干涉儀量測光學系統波前誤差(成像誤差)數據,以原始設計值波前誤差綜合分析製造組裝所產生的波前誤差,再經光學軟體優化得到補正值。The lens correction technology can be the application of mold flow analysis method, curve fitting function method or wavefront error method, but is not limited to this. The mold flow analysis method is to find out the three-dimensional contour nodes where the surface of the optical lens shrinks in the Z-axis through mold flow analysis, convert it into an aspherical curve, and then compare the difference with the original curve, while taking into account the material shrinkage rate and surface deformation trend. Correction value. Among them, the curve fitting function method is to measure the surface profile error of the component, perform curve fitting with a function, and cooperate with the optimization algorithm to approximate the fitting curve to the measurement point to obtain the correction value. The function can be exponential (Exponential) or polynomial (Polynomial), etc., and the algorithm can be Gauss Newton method (Gauss Newton method), simplex algorithm (Simplex Algorithm) or maximum steep descent method (Steepest Descent Method), etc. Among them, the wavefront error method uses an interferometer to measure the wavefront error (imaging error) data of the optical system, comprehensively analyzes the wavefront error caused by manufacturing and assembly with the original design value wavefront error, and then optimizes the optical software to obtain the corrected value.

本揭示內容在塑膠光學鏡片表面具有干涉型的高折射率膜層與低折射率膜層交替的紅外線濾除鍍膜,其配置在具有最佳鍍膜配置主因子(FC)的光學鏡片表面,使光學鏡片具有優異的鍍膜均勻性、低雜光反射現象與均勻的濾除效果。The present disclosure has an interference-type infrared filter coating with alternating high refractive index film layers and low refractive index film layers on the surface of the plastic optical lens, which is configured on the surface of the optical lens with the optimal coating configuration principal factor (FC), making the optical lens The lens has excellent coating uniformity, low stray light reflection and uniform filtering effect.

本揭示內容藉由吸收材料配置主因子(FA)來決定最適合添加吸收材料的光學鏡片,使吸收材料均勻混合於光學鏡片中,且包含吸收材料的光學鏡片在全視場範圍內皆具有高均勻度的特定波段吸收效果。This disclosure determines the most suitable optical lens for adding absorbent materials through the main factor (FA) of absorbing material configuration, so that the absorbing materials are evenly mixed in the optical lenses, and the optical lenses containing the absorbing materials have high performance in the entire field of view. Specific band absorption effect of uniformity.

本揭示內容的光學鏡頭須藉由紅外線濾除鍍膜、長波長吸收材料與短波長吸收材料的組合配置,並以多項因子參數對光學鏡片進行評價,在鍍膜評價(Coating Evaluation by FC)與吸收評價(Absorbing Evaluation by FA)的雙因子共同評價下作出最佳設計。The optical lens disclosed in this disclosure must be configured through a combination of infrared filtering coating, long-wavelength absorbing material, and short-wavelength absorbing material, and the optical lens must be evaluated using multiple factor parameters. In the coating evaluation (Coating Evaluation by FC) and absorption evaluation The optimal design is made under the two-factor joint evaluation of (Absorbing Evaluation by FA).

本揭示內容另一實施方式提供一種取像裝置,其包含前述之光學鏡頭以及一電子感光元件,電子感光元件設置於光學鏡頭的一成像面。Another embodiment of the present disclosure provides an imaging device, which includes the aforementioned optical lens and an electronic photosensitive element. The electronic photosensitive element is disposed on an imaging surface of the optical lens.

本揭示內容的光學鏡頭更可包含一電子感光元件以及一平板玻璃,其中電子感光元件設置於光學鏡頭的一成像面,且平板玻璃設置於電子感光元件的一表面。The optical lens of the present disclosure may further include an electronic photosensitive element and a flat glass, wherein the electronic photosensitive element is arranged on an imaging surface of the optical lens, and the flat glass is arranged on a surface of the electronic photosensitive element.

由於傳統光線角度過大時,會導致光線無法順利入射電子感光元件,或造成畫素錯位響應而產生色偏並降低成像品質,本揭示內容藉由將平板玻璃設置在電子感光元件的表面,經平板玻璃折射後降低入射角而使光線順利入射於電子感光元件,提升大主光線角度光學系統的應用範圍,並具有降低主光線角度、減少後焦長、縮減光學鏡頭總長、縮小最大像高與簡化製程等效果。Because when the traditional light angle is too large, the light will not be able to smoothly enter the electronic photosensitive element, or the pixels will be misaligned to respond, resulting in color casts and reduced imaging quality. In this disclosure, flat glass is placed on the surface of the electronic photosensitive element. After refraction of the glass, the incident angle is reduced so that the light can smoothly enter the electronic photosensitive element, thereby increasing the application range of optical systems with large chief ray angles. It also has the advantages of lowering the chief ray angle, reducing the back focal length, reducing the total length of the optical lens, reducing the maximum image height and simplifying Process and other effects.

光學鏡頭於最大像高視場處的主光線入射平板玻璃的一表面的角度為CRAg,其可以滿足下列條件:40度 ≤ CRAg。藉此,本揭示內容之設計特別適合應用在CRAg角度大於40度的大主光線角的光學系統,可以克服光學系統主光線角度設計的應用上限。The angle at which the chief ray of the optical lens is incident on a surface of the flat glass at the maximum image height field of view is CRAg, which can meet the following conditions: 40 degrees ≤ CRAg. Therefore, the design disclosed in this disclosure is particularly suitable for applications in optical systems with large chief ray angles where the CRAg angle is greater than 40 degrees, and can overcome the application upper limit of chief ray angle design of optical systems.

平板玻璃的物側表面可以具有一長波長吸收材料,藉此,平板玻璃表面具有長波長吸收材料可強化吸收效果,並適合大主光線角度的光學系統應用。The object-side surface of the flat glass can be provided with a long-wavelength absorbing material, whereby the long-wavelength absorbing material on the surface of the flat glass can enhance the absorption effect and is suitable for optical system applications with large chief ray angles.

平板玻璃的至少一表面可以具有一抗反射膜層,抗反射膜層可以具有一次波長微結構,藉此,具有次波長微結構的抗反射膜層可以產生廣域波長範圍的抗反射效果,避免大角度光線的偏移漏光問題。At least one surface of the flat glass can have an anti-reflective coating layer, and the anti-reflective coating layer can have a primary wavelength microstructure. Therefore, the anti-reflective coating layer with sub-wavelength microstructure can produce an anti-reflective effect over a wide wavelength range, preventing The problem of offset light leakage of large-angle light.

平板玻璃的像側表面可以具有一長波長吸收材料,藉此,可以減少元件數量與降低製程複雜度。The image-side surface of the flat glass can have a long-wavelength absorbing material, thereby reducing the number of components and reducing the complexity of the process.

本揭示內容的光學鏡頭中包含長波長吸收材料的光學鏡片在波長1050 nm的穿透率可以小於在波長500 nm的穿透率,且光學鏡頭更可包含一電子感光元件,其設置於光學鏡頭的一成像面。In the optical lens of the present disclosure, the transmittance of the optical lens containing the long-wavelength absorbing material at the wavelength of 1050 nm may be less than the transmittance at the wavelength of 500 nm, and the optical lens may further include an electronic photosensitive element disposed on the optical lens An imaging plane.

本揭示內容藉由長波長吸收材料的光學鏡片設計,達到完整消除近紅外光的漏光問題干擾,有效避免色偏與提升整體成像品質。This disclosure uses the design of optical lenses made of long-wavelength absorbing materials to completely eliminate the light leakage problem of near-infrared light, effectively avoiding color casts and improving overall imaging quality.

本揭示內容又一實施方式提供一種光學鏡頭,其包含至少一光學鏡片以及至少一光學元件。所述至少一光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,紅外線濾除鍍膜具有至少二種不同的折射率。所述光學元件位於光學鏡片的像側,所述至少一光學元件中至少一光學元件包含一長波長吸收材料。全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值為AICmax,光學鏡頭於波長500 nm – 600 nm的平均穿透率為T5060,光學鏡頭於波長700 nm – 1000 nm的平均穿透率為T70100,其滿足下列條件:AICmax ≤ 40度;80% ≤ T5060;以及T70100 ≤ 10%。Yet another embodiment of the present disclosure provides an optical lens, which includes at least one optical lens and at least one optical element. At least one of the at least one optical lens includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located on the object-side surface and the image-side surface of the optical lens. One of the surfaces, the optical lens surface including the infrared filter coating, is an aspherical surface, and the infrared filter coating has at least two different refractive indexes. The optical element is located on the image side of the optical lens, and at least one of the at least one optical element includes a long wavelength absorbing material. The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating is AICmax. The average transmittance of the optical lens at a wavelength of 500 nm – 600 nm is T5060. The optical lens has a wavelength of 700 nm – 1000 nm. The average penetration rate is T70100, which meets the following conditions: AICmax ≤ 40 degrees; 80% ≤ T5060; and T70100 ≤ 10%.

本揭示內容的光學元件具有長波長吸收材料,進而可減少元件數量、增加長波長濾除效果與降低製程複雜度。The optical element of the present disclosure has long-wavelength absorbing materials, thereby reducing the number of components, increasing the long-wavelength filtering effect, and reducing process complexity.

包含長波長吸收材料的光學元件可為一微透鏡,且微透鏡的表面可具有長波長吸收材料。The optical element including the long-wavelength absorbing material may be a microlens, and the surface of the microlens may have the long-wavelength absorbing material.

包含長波長吸收材料的光學元件可為一彩色濾光片,且彩色濾光片可具有長波長吸收材料。The optical element including the long wavelength absorbing material can be a color filter, and the color filter can have the long wavelength absorbing material.

所述至少一光學鏡片可以具有長波長吸收材料。The at least one optical lens may have long wavelength absorbing material.

包含長波長吸收材料的光學元件可為一平板玻璃,且平板玻璃的至少一表面可具有長波長吸收材料。The optical element including the long wavelength absorbing material may be a flat glass, and at least one surface of the flat glass may have the long wavelength absorbing material.

本揭示內容再一實施方式提供一種電子裝置,其為一行動裝置且包含前述的光學鏡頭或取像裝置。本揭示內容的電子裝置亦可為車用裝置、航空裝置或監視裝置等,且不以此為限。Yet another embodiment of the present disclosure provides an electronic device, which is a mobile device and includes the aforementioned optical lens or imaging device. The electronic device in this disclosure may also be a vehicle device, an aviation device, a monitoring device, etc., and is not limited thereto.

根據上述說明,以下提出具體實施例予以詳細說明。Based on the above description, specific embodiments are provided below for detailed description.

<第一實施例><First Embodiment>

第一實施例的光學鏡頭包含五光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4及光學鏡片L5。所述五光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。所述五光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。第一實施例的光學鏡頭的全視角為FOV,其滿足下列條件:FOV = 80度。The optical lens of the first embodiment includes five optical lenses, from the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4 and optical lens L5. At least one of the five optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located between the object-side surface and the image-side surface of the optical lens. On one surface, the surface of the optical lens including the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes. At least one of the five optical lenses includes a long wavelength absorbing material, and the optical lens including the long wavelength absorbing material is made of a plastic material. The full viewing angle of the optical lens of the first embodiment is FOV, which satisfies the following conditions: FOV = 80 degrees.

光學鏡片L1的物側表面為R1,全視場主光線於光學鏡片L1的物側表面R1的入射角最大值為AICmax,其滿足下列條件:AICmax = 31.09度。光學鏡片L1的像側表面為R2,全視場主光線於光學鏡片L1的像側表面R2的入射角最大值為AICmax,其滿足下列條件:AICmax = 28.30度。The object-side surface of the optical lens L1 is R1, and the maximum incident angle of the full-field chief ray on the object-side surface R1 of the optical lens L1 is AICmax, which meets the following conditions: AICmax = 31.09 degrees. The image-side surface of the optical lens L1 is R2, and the maximum incident angle of the full-field chief ray on the image-side surface R2 of the optical lens L1 is AICmax, which meets the following conditions: AICmax = 28.30 degrees.

光學鏡片L1的物側表面R1的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 1.82。光學鏡片L1的物側表面R1的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 4.98。光學鏡片L1的物側表面R1的鍍膜配置主因子為FC,其滿足下列條件:FC = 0.96。The first factor of the coating configuration of the object-side surface R1 of the optical lens L1 is Fc1, which satisfies the following conditions: Fc1 = 1.82. The second factor of the coating configuration of the object-side surface R1 of the optical lens L1 is Fc2, which meets the following conditions: Fc2 = 4.98. The main factor of the coating configuration of the object-side surface R1 of the optical lens L1 is FC, which satisfies the following conditions: FC = 0.96.

光學鏡片L1的像側表面R2的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 41.66。光學鏡片L1的像側表面R2的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 309.60。光學鏡片L1的像側表面R2的鍍膜配置主因子為FC,其滿足下列條件:FC = 4.11。The first factor of the coating configuration of the image-side surface R2 of the optical lens L1 is Fc1, which satisfies the following conditions: Fc1 = 41.66. The second factor of the coating configuration of the image-side surface R2 of the optical lens L1 is Fc2, which meets the following conditions: Fc2 = 309.60. The main factor of the coating configuration of the image-side surface R2 of the optical lens L1 is FC, which satisfies the following conditions: FC = 4.11.

光學鏡片L1於全視場主光線光程比的平均值為CPavg,其滿足下列條件:CPavg = 1.04。光學鏡片L1的吸收材料配置主因子為FA,其滿足下列條件:FA = 2.92。The average optical path ratio of the chief ray of the optical lens L1 in the full field of view is CPavg, which meets the following conditions: CPavg = 1.04. The main factor of the absorption material configuration of optical lens L1 is FA, which meets the following conditions: FA = 2.92.

光學鏡片L2的物側表面為R1,全視場主光線於光學鏡片L2的物側表面R1的入射角最大值為AICmax,其滿足下列條件:AICmax = 45.11度。光學鏡片L2的像側表面為R2,全視場主光線於光學鏡片L2的像側表面R2的入射角最大值為AICmax,其滿足下列條件:AICmax = 28.20度。The object-side surface of the optical lens L2 is R1, and the maximum incident angle of the full-field chief ray on the object-side surface R1 of the optical lens L2 is AICmax, which meets the following conditions: AICmax = 45.11 degrees. The image-side surface of the optical lens L2 is R2, and the maximum incident angle of the full-field chief ray on the image-side surface R2 of the optical lens L2 is AICmax, which meets the following conditions: AICmax = 28.20 degrees.

光學鏡片L2的物側表面R1的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 8.48。光學鏡片L2的物側表面R1的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 95.24。光學鏡片L2的物側表面R1的鍍膜配置主因子為FC,其滿足下列條件:FC = 2.91。The first factor of the coating configuration of the object-side surface R1 of the optical lens L2 is Fc1, which satisfies the following conditions: Fc1 = 8.48. The second factor of the coating configuration of the object-side surface R1 of the optical lens L2 is Fc2, which meets the following conditions: Fc2 = 95.24. The main factor of the coating configuration of the object-side surface R1 of the optical lens L2 is FC, which satisfies the following conditions: FC = 2.91.

光學鏡片L2的像側表面R2的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 4.13。光學鏡片L2的像側表面R2的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 47.62。光學鏡片L2的像側表面R2的鍍膜配置主因子為FC,其滿足下列條件:FC = 2.29。The first factor of the coating configuration of the image-side surface R2 of the optical lens L2 is Fc1, which satisfies the following conditions: Fc1 = 4.13. The second factor of the coating configuration of the image-side surface R2 of the optical lens L2 is Fc2, which meets the following conditions: Fc2 = 47.62. The main factor of the coating configuration of the image-side surface R2 of the optical lens L2 is FC, which satisfies the following conditions: FC = 2.29.

光學鏡片L2於全視場主光線光程比的平均值為CPavg,其滿足下列條件:CPavg = 1.05。光學鏡片L2的吸收材料配置主因子為FA,其滿足下列條件:FA = 2.64。The average optical path ratio of the chief ray of the optical lens L2 in the full field of view is CPavg, which meets the following conditions: CPavg = 1.05. The main factor of the absorption material configuration of optical lens L2 is FA, which meets the following conditions: FA = 2.64.

光學鏡片L3的物側表面為R1,全視場主光線於光學鏡片L3的物側表面R1的入射角最大值為AICmax,其滿足下列條件:AICmax = 35.90度。光學鏡片L3的像側表面為R2,全視場主光線於光學鏡片L3的像側表面R2的入射角最大值為AICmax,其滿足下列條件:AICmax = 20.07度。The object-side surface of the optical lens L3 is R1, and the maximum incident angle of the full-field chief ray on the object-side surface R1 of the optical lens L3 is AICmax, which meets the following conditions: AICmax = 35.90 degrees. The image-side surface of the optical lens L3 is R2, and the maximum incident angle of the full-field chief ray on the image-side surface R2 of the optical lens L3 is AICmax, which meets the following conditions: AICmax = 20.07 degrees.

光學鏡片L3的物側表面R1的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 1.51。光學鏡片L3的物側表面R1的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 6.48。光學鏡片L3的物側表面R1的鍍膜配置主因子為FC,其滿足下列條件:FC = 0.99。The first factor of the coating configuration of the object-side surface R1 of the optical lens L3 is Fc1, which satisfies the following conditions: Fc1 = 1.51. The second factor of the coating configuration of the object-side surface R1 of the optical lens L3 is Fc2, which satisfies the following conditions: Fc2 = 6.48. The main factor of the coating configuration of the object-side surface R1 of the optical lens L3 is FC, which satisfies the following conditions: FC = 0.99.

光學鏡片L3的像側表面R2的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 2.66。光學鏡片L3的像側表面R2的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 33.16。光學鏡片L3的像側表面R2的鍍膜配置主因子為FC,其滿足下列條件:FC = 1.95。The first factor of the coating configuration of the image-side surface R2 of the optical lens L3 is Fc1, which satisfies the following conditions: Fc1 = 2.66. The second factor of the coating configuration of the image-side surface R2 of the optical lens L3 is Fc2, which meets the following conditions: Fc2 = 33.16. The main factor of the coating configuration of the image-side surface R2 of the optical lens L3 is FC, which satisfies the following conditions: FC = 1.95.

光學鏡片L3於全視場主光線光程比的平均值為CPavg,其滿足下列條件:CPavg = 1.06。光學鏡片L3的吸收材料配置主因子為FA,其滿足下列條件:FA = 2.60。The average optical path ratio of the chief ray of the optical lens L3 in the full field of view is CPavg, which meets the following conditions: CPavg = 1.06. The main factor of the absorption material configuration of optical lens L3 is FA, which meets the following conditions: FA = 2.60.

光學鏡片L4的物側表面為R1,全視場主光線於光學鏡片L4的物側表面R1的入射角最大值為AICmax,其滿足下列條件:AICmax = 28.55度。光學鏡片L4的像側表面為R2,全視場主光線於光學鏡片L4的像側表面R2的入射角最大值為AICmax,其滿足下列條件:AICmax = 22.46度。The object-side surface of the optical lens L4 is R1, and the maximum incident angle of the full-field chief ray on the object-side surface R1 of the optical lens L4 is AICmax, which meets the following conditions: AICmax = 28.55 degrees. The image-side surface of the optical lens L4 is R2, and the maximum incident angle of the full-field chief ray on the image-side surface R2 of the optical lens L4 is AICmax, which meets the following conditions: AICmax = 22.46 degrees.

光學鏡片L4的物側表面R1的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 1.92。光學鏡片L4的物側表面R1的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 7.93。光學鏡片L4的物側表面R1的鍍膜配置主因子為FC,其滿足下列條件:FC = 1.18。The first factor of the coating configuration of the object-side surface R1 of the optical lens L4 is Fc1, which satisfies the following conditions: Fc1 = 1.92. The second factor of the coating configuration of the object-side surface R1 of the optical lens L4 is Fc2, which satisfies the following conditions: Fc2 = 7.93. The main factor of the coating configuration of the object-side surface R1 of the optical lens L4 is FC, which satisfies the following conditions: FC = 1.18.

光學鏡片L4的像側表面R2的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1 = 0.98。光學鏡片L4的像側表面R2的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2 = 3.53。光學鏡片L4的像側表面R2的鍍膜配置主因子為FC,其滿足下列條件:FC = 0.54。The first factor of the coating configuration of the image-side surface R2 of the optical lens L4 is Fc1, which satisfies the following conditions: Fc1 = 0.98. The second factor of the coating configuration of the image-side surface R2 of the optical lens L4 is Fc2, which satisfies the following conditions: Fc2 = 3.53. The main factor of the coating configuration of the image side surface R2 of the optical lens L4 is FC, which satisfies the following conditions: FC = 0.54.

光學鏡片L4於全視場主光線光程比的平均值為CPavg,其滿足下列條件:CPavg = 0.78。光學鏡片L4的吸收材料配置主因子為FA,其滿足下列條件:FA = 1.51。The average optical path ratio of the chief ray of the optical lens L4 in the full field of view is CPavg, which meets the following conditions: CPavg = 0.78. The main factor of the absorption material configuration of optical lens L4 is FA, which meets the following conditions: FA = 1.51.

光學鏡片L5的物側表面為R1,全視場主光線於光學鏡片L5的物側表面R1的入射角最大值為AICmax,其滿足下列條件:AICmax=48.49度。光學鏡片L5的像側表面為R2,全視場主光線於光學鏡片L5的像側表面R2的入射角最大值為AICmax,其滿足下列條件:AICmax=20.40度。 The object-side surface of the optical lens L5 is R1, and the maximum incident angle of the full-field chief ray on the object-side surface R1 of the optical lens L5 is AICmax, which meets the following conditions: AICmax=48.49 degrees. The image-side surface of the optical lens L5 is R2, and the maximum incident angle of the full-field chief ray on the image-side surface R2 of the optical lens L5 is AICmax, which meets the following conditions: AICmax=20.40 degrees.

光學鏡片L5的物側表面R1的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1=0.63。光學鏡片L5的物側表面R1的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2=8.03。光學鏡片L5的物側表面R1的鍍膜配置主因子為FC,其滿足下列條件:FC=0.70。 The first factor of the coating configuration of the object-side surface R1 of the optical lens L5 is Fc1, which satisfies the following conditions: Fc1=0.63. The second factor of the coating configuration of the object-side surface R1 of the optical lens L5 is Fc2, which satisfies the following conditions: Fc2=8.03. The main factor of the coating configuration of the object-side surface R1 of the optical lens L5 is FC, which satisfies the following conditions: FC=0.70.

光學鏡片L5的像側表面R2的鍍膜配置第一因子為Fc1,其滿足下列條件:Fc1=0.76。光學鏡片L5的像側表面R2的鍍膜配置第二因子為Fc2,其滿足下列條件:Fc2=4.11。光學鏡片L5的像側表面R2的鍍膜配置主因子為FC,其滿足下列條件:FC=0.49。 The first factor of the coating configuration of the image-side surface R2 of the optical lens L5 is Fc1, which satisfies the following conditions: Fc1=0.76. The second factor of the coating configuration of the image-side surface R2 of the optical lens L5 is Fc2, which satisfies the following conditions: Fc2=4.11. The main factor of the coating configuration of the image-side surface R2 of the optical lens L5 is FC, which satisfies the following conditions: FC=0.49.

光學鏡片L5於全視場主光線光程比的平均值為CPavg,其滿足下列條件:CPavg=1.79。光學鏡片L5的吸收材料配置主因子為FA,其滿足下列條件:FA=0.38。 The average optical path ratio of the chief ray of the optical lens L5 in the full field of view is CPavg, which meets the following conditions: CPavg=1.79. The main factor of the absorption material configuration of optical lens L5 is FA, which meets the following conditions: FA=0.38.

第一實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表三、表四及表五。 The detailed parameters and sizes of each optical lens included in the optical lens of the first embodiment are listed in Table 3, Table 4 and Table 5 below.

Figure 110137381-A0305-02-0028-1
Figure 110137381-A0305-02-0028-1
Figure 110137381-A0305-02-0029-2
Figure 110137381-A0305-02-0029-2
Figure 110137381-A0305-02-0030-3
Figure 110137381-A0305-02-0030-3
Figure 110137381-A0305-02-0031-4
Figure 110137381-A0305-02-0031-4

Figure 110137381-A0305-02-0031-5
Figure 110137381-A0305-02-0031-5
Figure 110137381-A0305-02-0032-6
Figure 110137381-A0305-02-0032-6

Figure 110137381-A0305-02-0032-7
Figure 110137381-A0305-02-0032-7

其中,各光學鏡片於光軸上的厚度為CT,各光學鏡片表面上與光軸交點間水平位移的最大值為SAGmax,各光學鏡片表面於光學有效徑範圍內的切線斜率的平均值為SPavg,各光學鏡片表面於光學有效徑範圍內的切線斜率的最小值為SPmin,各光學鏡片於全視場主光線光程比的標準差為CPst。 Among them, the thickness of each optical lens on the optical axis is CT, the maximum value of the horizontal displacement between the intersection point of each optical lens surface and the optical axis is SAGmax, and the average value of the tangent slope of each optical lens surface within the optical effective diameter range is SPavg , the minimum value of the tangent slope of each optical lens surface within the optical effective diameter range is SPmin, and the standard deviation of the optical path ratio of the chief ray of each optical lens in the full field of view is CPst.

<第二實施例> <Second Embodiment>

第二實施例的光學鏡頭包含六光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4、光學鏡片L5及光學鏡片L6。所述六光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包 含紅外線濾除鍍膜的光學鏡片表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。所述六光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。 The optical lens of the second embodiment includes six optical lenses, from the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4, optical lens L5 and optical lens L6. At least one of the six optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located between the object-side surface and the image-side surface of the optical lens. One surface, package The surface of the optical lens containing the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the six optical lenses includes a long-wavelength absorbing material, and the optical lens including the long-wavelength absorbing material is made of a plastic material.

第二實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表六、表七及表八。各表的參數定義皆與第一實施例相同,於此不再贅述。 The detailed parameters and sizes of each optical lens included in the optical lens of the second embodiment are listed in Table 6, Table 7 and Table 8 below. The parameter definitions of each table are the same as those in the first embodiment and will not be repeated here.

Figure 110137381-A0305-02-0033-8
Figure 110137381-A0305-02-0033-8
Figure 110137381-A0305-02-0034-9
Figure 110137381-A0305-02-0034-9
Figure 110137381-A0305-02-0035-10
Figure 110137381-A0305-02-0035-10

Figure 110137381-A0305-02-0035-11
Figure 110137381-A0305-02-0035-11
Figure 110137381-A0305-02-0036-12
Figure 110137381-A0305-02-0036-12
Figure 110137381-A0305-02-0037-13
Figure 110137381-A0305-02-0037-13

Figure 110137381-A0305-02-0037-14
Figure 110137381-A0305-02-0037-14
Figure 110137381-A0305-02-0038-15
Figure 110137381-A0305-02-0038-15

<第三實施例> <Third Embodiment>

第三實施例的光學鏡頭包含六光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4、光學鏡片L5及光學鏡片L6。其中,光學鏡片L1包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片L1由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片L1的像側表面R2,包含紅外線濾除鍍膜的光學鏡片L1表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。其中,光學鏡片L1包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片L1由一塑膠材料所製成。 The optical lens of the third embodiment includes six optical lenses, from the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4, optical lens L5 and optical lens L6. Among them, the optical lens L1 includes an infrared filter coating. The optical lens L1 including the infrared filter coating is made of a plastic material. The infrared filter coating is located on the image side surface R2 of the optical lens L1. The optical lens L1 including the infrared filter coating is The surface of the lens L1 is aspherical, and the infrared filtering coating has at least two different refractive indexes. The optical lens L1 includes a long-wavelength absorbing material, and the optical lens L1 including the long-wavelength absorbing material is made of a plastic material.

第三實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表九、表十及表十一。各表的參數定義皆與第一實施例相同,於此不再贅述。 The detailed parameters and sizes of each optical lens included in the optical lens of the third embodiment are listed in Table 9, Table 10 and Table 11 below. The parameter definitions of each table are the same as those in the first embodiment and will not be repeated here.

Figure 110137381-A0305-02-0038-16
Figure 110137381-A0305-02-0038-16
Figure 110137381-A0305-02-0039-17
Figure 110137381-A0305-02-0039-17
Figure 110137381-A0305-02-0040-18
Figure 110137381-A0305-02-0040-18

Figure 110137381-A0305-02-0040-20
Figure 110137381-A0305-02-0040-20
Figure 110137381-A0305-02-0041-21
Figure 110137381-A0305-02-0041-21
Figure 110137381-A0305-02-0042-22
Figure 110137381-A0305-02-0042-22

Figure 110137381-A0305-02-0042-23
Figure 110137381-A0305-02-0042-23
Figure 110137381-A0305-02-0043-24
Figure 110137381-A0305-02-0043-24

請一併參照第1圖及下表十二,第1圖為第三實施例的光學鏡片L1的穿透率與波長的關係圖,其中入射至光學鏡片L1的光線入射角角度分別為0度及30度,且不同波長的光線的穿透率已列於表十二。其中,光學鏡片L1在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長為LWdT5,其滿足下列條件:600nm

Figure 110137381-A0305-02-0043-79
LWdT5
Figure 110137381-A0305-02-0043-80
700nm,光學鏡片L1在短波長區域且波長與穿透率呈正相關的趨勢中達到50%穿透率的波長為SWuT5,其可以滿足下列條件:370nm
Figure 110137381-A0305-02-0043-81
SWuT5
Figure 110137381-A0305-02-0043-82
450nm。 Please refer to Figure 1 and Table 12 below. Figure 1 is a graph showing the relationship between the transmittance and wavelength of the optical lens L1 of the third embodiment. The incident angle of the light incident on the optical lens L1 is 0 degrees. and 30 degrees, and the transmittance of light of different wavelengths is listed in Table 12. Among them, the wavelength at which the optical lens L1 reaches 50% transmittance in the long wavelength region and the trend that wavelength and transmittance are negatively correlated is LWdT5, which meets the following conditions: 600nm
Figure 110137381-A0305-02-0043-79
wx5
Figure 110137381-A0305-02-0043-80
700nm, the wavelength at which optical lens L1 reaches 50% transmittance in the short wavelength region and the trend of positive correlation between wavelength and transmittance is SWuT5, which can meet the following conditions: 370nm
Figure 110137381-A0305-02-0043-81
SWuT5
Figure 110137381-A0305-02-0043-82
450nm.

Figure 110137381-A0305-02-0043-25
Figure 110137381-A0305-02-0043-25
Figure 110137381-A0305-02-0044-1
Figure 110137381-A0305-02-0044-1

請一併參照第2圖及下表十三,第2圖為第三實施例的光學鏡頭的穿透率與波長的關係圖,其中入射至光學鏡頭的光線入射角角度分別為0度及30度,且不同波長的光線的穿透率已列於表十三。其中,光學鏡頭在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長為LWdT5,其滿足下列條件:600 nm ≤ LWdT5 ≤ 700 nm,光學鏡頭在短波長區域且波長與穿透率呈正相關的趨勢中達到50%穿透率的波長為SWuT5,其可以滿足下列條件:370 nm ≤ SWuT5 ≤ 450 nm。 表十三、第三實施例的光學鏡頭的穿透率 T (%) 0度 T (%) 30度 LWdT5 (nm) 635 – 640 LWdT5 (nm) 630 – 635 SWuT5 (nm) 420 – 425 SWuT5 (nm) 420 – 425 T (%) 0度 T (%) 30度 T3540 (%) 4.39 T3540 (%) 6.31 T4050 (%) 69.66 T4050 (%) 65.85 T5060 (%) 90.31 T5060 (%) 87.87 T6570 (%) 17.74 T6570 (%) 8.26 T70100 (%) 0.06 T70100 (%) 0.04 T35 (%) 0.00 T35 (%) 0.00 T40 (%) 24.85 T40 (%) 21.34 T55 (%) 93.04 T55 (%) 86.63 T60 (%) 82.07 T60 (%) 79.52 T63 (%) 57.65 T63 (%) 55.97 T64 (%) 46.65 T64 (%) 42.59 T65 (%) 40.64 T65 (%) 36.50 T70 (%) 0.10 T70 (%) 0.01 T85 (%) 0.00 T85 (%) 0.00 Please refer to Figure 2 and Table 13 below. Figure 2 is a graph showing the relationship between transmittance and wavelength of the optical lens of the third embodiment. The incident angles of the light incident on the optical lens are 0 degrees and 30 degrees respectively. degree, and the transmittance of light of different wavelengths is listed in Table 13. Among them, the wavelength at which the optical lens achieves 50% transmittance in the long wavelength region and the trend of negative correlation between wavelength and transmittance is LWdT5, which meets the following conditions: 600 nm ≤ LWdT5 ≤ 700 nm, and the optical lens in the short wavelength region And in the trend of positive correlation between wavelength and transmittance, the wavelength that reaches 50% transmittance is SWuT5, which can meet the following conditions: 370 nm ≤ SWuT5 ≤ 450 nm. Table 13. Transmittance of the optical lens of the third embodiment T(%) 0 degree T(%) 30 degrees LWdT5 (nm) 635 – 640 LWdT5 (nm) 630 – 635 SWuT5 (nm) 420 – 425 SWuT5 (nm) 420 – 425 T(%) 0 degree T(%) 30 degrees T3540 (%) 4.39 T3540 (%) 6.31 T4050 (%) 69.66 T4050 (%) 65.85 T5060 (%) 90.31 T5060 (%) 87.87 T6570 (%) 17.74 T6570 (%) 8.26 T70100 (%) 0.06 T70100 (%) 0.04 T35 (%) 0.00 T35 (%) 0.00 T40 (%) 24.85 T40 (%) 21.34 T55 (%) 93.04 T55 (%) 86.63 T60 (%) 82.07 T60 (%) 79.52 T63 (%) 57.65 T63 (%) 55.97 T64 (%) 46.65 T64 (%) 42.59 T65 (%) 40.64 T65 (%) 36.50 T70 (%) 0.10 T70 (%) 0.01 T85 (%) 0.00 T85 (%) 0.00

第三實施例的光學鏡片L1的鍍膜設計已列於下表十四。其中,紅外線濾除鍍膜的總層數為tLs,其滿足下列條件:40 < tLs ≤ 80,紅外線濾除鍍膜的總膜厚為tTk,其滿足下列條件:4000 nm < tTk ≤ 10000 nm。 表十四、第三實施例的鍍膜設計 tLs 46 tTk (nm) 5527 材料折射率 厚度 (nm) 12 36 113 173 109 174 104 158 96 168 108 178 107 163 91 161 106 178 109 166 91 155 104 176 109 167 92 143 88 140 84 141 84 143 82 143 82 143 84 143 87 140 89 150 84 73 The coating design of the optical lens L1 of the third embodiment is listed in Table 14 below. Among them, the total number of layers of infrared filtering coating is tLs, which meets the following conditions: 40 < tLs ≤ 80. The total film thickness of infrared filtering coating is tTk, which meets the following conditions: 4000 nm < tTk ≤ 10000 nm. Table 14. Coating design of the third embodiment tL 46 tTk (nm) 5527 Material refractive index Thickness(nm) high 12 Low 36 high 113 Low 173 high 109 Low 174 high 104 Low 158 high 96 Low 168 high 108 Low 178 high 107 Low 163 high 91 Low 161 high 106 Low 178 high 109 Low 166 high 91 Low 155 high 104 Low 176 high 109 Low 167 high 92 Low 143 high 88 Low 140 high 84 Low 141 high 84 Low 143 high 82 Low 143 high 82 Low 143 high 84 Low 143 high 87 Low 140 high 89 Low 150 high 84 Low 73

再者,請參照第3A圖及第3B圖,第3A圖為第三實施例的光學鏡頭的成像品質圖,第3B圖為比較例的光學鏡頭的成像品質圖,其中,第三實施例的光學鏡頭不包含紅外線濾除藍玻璃,而比較例的光學鏡頭包含紅外線濾除藍玻璃。由第3A圖及第3B圖的右上角可以看出,比較例的光學鏡頭產生明顯的雜光斑點,而第三實施例的光學鏡頭則無,代表本揭示內容的光學鏡頭可以有效解決嚴重強光反射現象所導致的雜散光缺陷。Furthermore, please refer to Figures 3A and 3B. Figure 3A is an imaging quality diagram of the optical lens of the third embodiment. Figure 3B is an imaging quality diagram of the optical lens of the comparative example. Among them, the The optical lens does not include infrared filtering blue glass, while the optical lens of the comparative example includes infrared filtering blue glass. As can be seen from the upper right corners of Figures 3A and 3B, the optical lens of the comparative example produces obvious stray light spots, while the optical lens of the third embodiment does not. It represents that the optical lens of the present disclosure can effectively solve the problem of severe glare. Stray light defects caused by light reflection phenomena.

此外,第三實施例的光學鏡頭於最大像高(IMGH)處的平均R/G比為0.98,第三實施例的光學鏡頭於最大像高處的平均B/G比為1.03,比較例的光學鏡頭於最大像高處的平均R/G比為0.97,比較例的光學鏡頭於最大像高處的平均B/G比為1.02。In addition, the average R/G ratio of the optical lens of the third embodiment at the maximum image height (IMGH) is 0.98, the average B/G ratio of the optical lens of the third embodiment at the maximum image height is 1.03, and the average B/G ratio of the optical lens of the third embodiment at the maximum image height is 1.03. The average R/G ratio of the optical lens at the maximum image height is 0.97, and the average B/G ratio of the optical lens in the comparative example at the maximum image height is 1.02.

<第四實施例><Fourth Embodiment>

第四實施例的光學鏡頭包含七光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4、光學鏡片L5、光學鏡片L6及光學鏡片L7。所述七光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。所述七光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。 The optical lens of the fourth embodiment includes seven optical lenses, from the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4, optical lens L5, optical lens L6 and optical lens L7. At least one of the seven optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located between the object-side surface and the image-side surface of the optical lens. On one surface, the surface of the optical lens including the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the seven optical lenses includes a long wavelength absorbing material, and the optical lens including the long wavelength absorbing material is made of a plastic material.

第四實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表十五、表十六及表十七。各表的參數定義皆與第一實施例相同,於此不再贅述。 The detailed parameters and sizes of each optical lens included in the optical lens of the fourth embodiment are listed in Table 15, Table 16 and Table 17 below. The parameter definitions of each table are the same as those in the first embodiment and will not be repeated here.

Figure 110137381-A0305-02-0049-26
Figure 110137381-A0305-02-0049-26
Figure 110137381-A0305-02-0050-27
Figure 110137381-A0305-02-0050-27
Figure 110137381-A0305-02-0051-28
Figure 110137381-A0305-02-0051-28
Figure 110137381-A0305-02-0052-29
Figure 110137381-A0305-02-0052-29

Figure 110137381-A0305-02-0052-30
Figure 110137381-A0305-02-0052-30
Figure 110137381-A0305-02-0053-31
Figure 110137381-A0305-02-0053-31
Figure 110137381-A0305-02-0054-32
Figure 110137381-A0305-02-0054-32

Figure 110137381-A0305-02-0054-33
Figure 110137381-A0305-02-0054-33
Figure 110137381-A0305-02-0055-34
Figure 110137381-A0305-02-0055-34

<第五實施例> <Fifth Embodiment>

第五實施例的光學鏡頭包含八光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4、光學鏡片L5、光學鏡片L6、光學鏡片L7及光學鏡片L8。所述八光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。所述八光學鏡片中至少一光學鏡片包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。 The optical lens of the fifth embodiment includes eight optical lenses. From the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4, optical lens L5, optical lens L6, optical lens L7 and optical lens L7. L8. At least one of the eight optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located between the object-side surface and the image-side surface of the optical lens. On one surface, the surface of the optical lens including the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the eight optical lenses includes a long-wavelength absorbing material, and the optical lens including the long-wavelength absorbing material is made of a plastic material.

第五實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表十八、表十九及表二十。各表的參數定義皆與第一實施例相同,於此不再贅述。 The detailed parameters and sizes of each optical lens included in the optical lens of the fifth embodiment are listed in Table 18, Table 19 and Table 20 below. The parameter definitions of each table are the same as those in the first embodiment and will not be repeated here.

Figure 110137381-A0305-02-0055-35
Figure 110137381-A0305-02-0055-35
Figure 110137381-A0305-02-0056-36
Figure 110137381-A0305-02-0056-36
Figure 110137381-A0305-02-0057-37
Figure 110137381-A0305-02-0057-37
Figure 110137381-A0305-02-0058-38
Figure 110137381-A0305-02-0058-38

Figure 110137381-A0305-02-0059-39
Figure 110137381-A0305-02-0059-39
Figure 110137381-A0305-02-0060-40
Figure 110137381-A0305-02-0060-40

Figure 110137381-A0305-02-0061-41
Figure 110137381-A0305-02-0061-41

<第六實施例> <Sixth Embodiment>

第六實施例的光學鏡頭包含九光學鏡片,由物側至像側分別為光學鏡片L1、光學鏡片L2、光學鏡片L3、光學鏡片L4、光學鏡片L5、光學鏡片L6、光學鏡片L7、光學鏡片L8及光學鏡片L9。所述九光學鏡片中至少一光學鏡片包含一紅外線濾除鍍膜,包含紅外線濾除鍍膜的光學鏡片由一塑膠材料所製成,紅外線濾除鍍膜位於光學鏡片的物側表面及像側表面的其中一表面,包含紅外線濾除鍍膜的光學鏡片表面為非球面,且紅外線濾除鍍膜具有至少二種不同的折射率。所述九光學鏡片中至少一光學鏡片 包含一長波長吸收材料,且包含長波長吸收材料的光學鏡片由一塑膠材料所製成。 The optical lens of the sixth embodiment includes nine optical lenses, from the object side to the image side, they are optical lens L1, optical lens L2, optical lens L3, optical lens L4, optical lens L5, optical lens L6, optical lens L7, optical lens L8 and optical lens L9. At least one of the nine optical lenses includes an infrared filter coating. The optical lens including the infrared filter coating is made of a plastic material. The infrared filter coating is located between the object-side surface and the image-side surface of the optical lens. On one surface, the surface of the optical lens including the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes. At least one optical lens among the nine optical lenses The optical lens includes a long wavelength absorbing material, and the optical lens including the long wavelength absorbing material is made of a plastic material.

第六實施例的光學鏡頭所包含的各光學鏡片的詳細參數大小已列於下表二十一、表二十二及表二十三。各表的參數定義皆與第一實施例相同,於此不再贅述。 The detailed parameters and sizes of each optical lens included in the optical lens of the sixth embodiment are listed in Table 21, Table 22 and Table 23 below. The parameter definitions of each table are the same as those in the first embodiment and will not be repeated here.

Figure 110137381-A0305-02-0062-42
Figure 110137381-A0305-02-0062-42
Figure 110137381-A0305-02-0063-43
Figure 110137381-A0305-02-0063-43
Figure 110137381-A0305-02-0064-44
Figure 110137381-A0305-02-0064-44
Figure 110137381-A0305-02-0065-45
Figure 110137381-A0305-02-0065-45

Figure 110137381-A0305-02-0065-46
Figure 110137381-A0305-02-0065-46
Figure 110137381-A0305-02-0066-47
Figure 110137381-A0305-02-0066-47
Figure 110137381-A0305-02-0067-48
Figure 110137381-A0305-02-0067-48

Figure 110137381-A0305-02-0067-49
Figure 110137381-A0305-02-0067-49
Figure 110137381-A0305-02-0068-50
Figure 110137381-A0305-02-0068-50

本揭示內容的光學鏡頭所述主光線定義為通過光學系統光圈(Aperture stop)中心之光線。 The chief ray of the optical lens of this disclosure is defined as the ray passing through the center of the aperture stop of the optical system.

本揭示內容僅以第三實施例進行完整示範,相同或再優化的鍍膜設計、膜層配置、膜厚配置和/或吸收材料配置皆可比照應用在其他實施例,以達到同等優異的結果,例如達到同等優異的穿透率、影像品質與色均勻度等。 This disclosure only uses the third embodiment for complete demonstration. The same or re-optimized coating design, film layer configuration, film thickness configuration and/or absorbing material configuration can be applied to other embodiments to achieve equally excellent results. For example, it can achieve equally excellent transmittance, image quality and color uniformity.

<第七實施例至第二十實施例> <Seventh Embodiment to Twentieth Embodiment>

第七實施例至第十一實施例的光學鏡頭各自包含七光學鏡片,分別為第一光學鏡片L1、第二光學鏡片L2、第三光學鏡片L3、第四光學鏡片L4、第五光學鏡片L5、第六光學鏡片L6及第七光學鏡片L7,且各光學鏡片分別具有一物側表面R1及一像側表面R2。 The optical lenses of the seventh to eleventh embodiments each include seven optical lenses, which are a first optical lens L1, a second optical lens L2, a third optical lens L3, a fourth optical lens L4, and a fifth optical lens L5. , the sixth optical lens L6 and the seventh optical lens L7, and each optical lens has an object-side surface R1 and an image-side surface R2 respectively.

第七實施例至第十一實施例的光學鏡頭的配置方式已列於下表二十四,其中光學鏡頭於最大像高視場處的主光線入射電子感光元件表面(成像面)的角度為CRA,且符號「*」代表所列之光學鏡片或光學鏡片表面具有長波長吸收材料或紅外線濾除鍍膜。 The configurations of the optical lenses of the seventh to eleventh embodiments are listed in Table 24 below. The angle at which the chief ray of the optical lens at the maximum image height field of view is incident on the surface (imaging plane) of the electronic photosensitive element is: CRA, and the symbol "*" indicates that the listed optical lenses or optical lens surfaces have long-wavelength absorbing materials or infrared filtering coatings.

Figure 110137381-A0305-02-0068-52
Figure 110137381-A0305-02-0068-52
Figure 110137381-A0305-02-0069-2
Figure 110137381-A0305-02-0069-2
Figure 110137381-A0305-02-0070-3
Figure 110137381-A0305-02-0070-3

第七實施例的光學鏡頭於最大像高視場處的主光線入射平板玻璃表面的角度為43度,第七實施例的光學鏡頭為七光學鏡片的光學系統,長波長吸收材料混入聚合物(Polymer)後,依需求設置於光學鏡頭像側端的光學元件表面或混製,如平板玻璃表面的聚合物層、複數平板玻璃間的聚合物層、微透鏡表面的聚合物層、微透鏡與彩色濾光片間的聚合物層或混製於彩色濾光片內。依本揭示內容的因子分析評估結果,紅外線濾除鍍膜可選擇設置於第一光學鏡片L1的像側表面R2、第二光學鏡片L2的物側表面R1或第三光學鏡片L3的物側表面R1以及其組合。The angle at which the chief ray of the optical lens of the seventh embodiment is incident on the surface of the flat glass at the maximum image height field of view is 43 degrees. The optical lens of the seventh embodiment is an optical system with seven optical lenses, and the long-wavelength absorbing material is mixed with a polymer ( After the Polymer), it is placed on the surface of the optical element at the image side of the optical lens or mixed according to the needs, such as a polymer layer on the surface of flat glass, a polymer layer between multiple flat glasses, a polymer layer on the surface of microlenses, microlenses and color The polymer layer between the filters may be mixed into the color filter. According to the factor analysis and evaluation results of this disclosure, the infrared filter coating can be selectively disposed on the image-side surface R2 of the first optical lens L1, the object-side surface R1 of the second optical lens L2, or the object-side surface R1 of the third optical lens L3. and combinations thereof.

第九實施例的光學鏡頭於最大像高視場處的主光線入射平板玻璃表面的角度為41度,第九實施例的光學鏡頭為七光學鏡片的光學系統,依本揭示內容的因子分析評估結果,長波長吸收材料可選擇添加於第一光學鏡片L1、第三光學鏡片L3、第四光學鏡片L4、第五光學鏡片L5或第七光學鏡片L7以及其組合。依本揭示內容的因子分析評估結果,紅外線濾除鍍膜可選擇設置於第一光學鏡片L1的物側表面R1、第一光學鏡片L1的像側表面R2、第二光學鏡片L2的物側表面R1、第三光學鏡片L3的像側表面R2、第四光學鏡片L4的物側表面R1或第四光學鏡片L4的像側表面R2以及其組合。The angle at which the chief ray of the optical lens of the ninth embodiment is incident on the surface of the flat glass at the maximum image height field of view is 41 degrees. The optical lens of the ninth embodiment is an optical system with seven optical lenses. According to the factor analysis and evaluation of this disclosure, As a result, the long wavelength absorbing material can be optionally added to the first optical lens L1, the third optical lens L3, the fourth optical lens L4, the fifth optical lens L5 or the seventh optical lens L7, and combinations thereof. According to the factor analysis and evaluation results of this disclosure, the infrared filter coating can be selectively disposed on the object-side surface R1 of the first optical lens L1, the image-side surface R2 of the first optical lens L1, and the object-side surface R1 of the second optical lens L2. , the image side surface R2 of the third optical lens L3, the object side surface R1 of the fourth optical lens L4, or the image side surface R2 of the fourth optical lens L4, and combinations thereof.

第十二實施例至第十八實施例的光學鏡頭各自包含八光學鏡片,分別為第一光學鏡片L1、第二光學鏡片L2、第三光學鏡片L3、第四光學鏡片L4、第五光學鏡片L5、第六光學鏡片L6、第七光學鏡片L7及第八光學鏡片L8,且各光學鏡片分別具有一物側表面R1及一像側表面R2。The optical lenses of the twelfth embodiment to the eighteenth embodiment each include eight optical lenses, which are a first optical lens L1, a second optical lens L2, a third optical lens L3, a fourth optical lens L4, and a fifth optical lens. L5, the sixth optical lens L6, the seventh optical lens L7 and the eighth optical lens L8, and each optical lens has an object-side surface R1 and an image-side surface R2 respectively.

第十二實施例至第十八實施例的光學鏡頭的配置方式已列於下表二十五,且表二十五的參數定義皆與第七實施例至第十一實施例相同,於此不再贅述。 表二十五 實施例 十二 十三 十四 十五 十六 十七 十八 光學鏡片 數量 8 8 8 8 8 8 8 CRA (度) 42 43 42 40 42 46 41   長波長吸收材料分析評估 L1   * * * * *   L2             * L3     *   * *   L4   * * * *     L5   * * *   * * L6               L7   * * * * * * L8           *   像側 光學元件 *     *         紅外線濾除鍍膜分析評估 L1 R1             * R2           * * L2 R1       * * *   R2       * * * * L3 R1 * * * * * *   R2 * * * * * *   L4 R1 * * * * * *   R2   * * *   *   L5 R1   *   *       R2 * *   *       L6 R1       *       R2               L7 R1               R2               L8 R1               R2               The configurations of the optical lenses of the twelfth to eighteenth embodiments are listed in Table 25 below, and the parameter definitions in Table 25 are the same as those of the seventh to eleventh embodiments. Here No more details. Table 25 Example twelve Thirteen fourteen fifteen sixteen seventeen eighteen Number of optical lenses 8 8 8 8 8 8 8 CRA (degree) 42 43 42 40 42 46 41 Analysis and Evaluation of Long Wavelength Absorbing Materials L1 * * * * * L2 * L3 * * * L4 * * * * L5 * * * * * L6 L7 * * * * * * L8 * Image side optical components * * Infrared filter coating analysis and evaluation L1 R1 * R2 * * L2 R1 * * * R2 * * * * L3 R1 * * * * * * R2 * * * * * * L4 R1 * * * * * * R2 * * * * L5 R1 * * R2 * * * L6 R1 * R2 L7 R1 R2 L8 R1 R2

第十九實施例及第二十實施例的光學鏡頭各自包含九光學鏡片,分別為第一光學鏡片L1、第二光學鏡片L2、第三光學鏡片L3、第四光學鏡片L4、第五光學鏡片L5、第六光學鏡片L6、第七光學鏡片L7、第八光學鏡片L8及第九光學鏡片L9,且各光學鏡片分別具有一物側表面R1及一像側表面R2。The optical lenses of the nineteenth embodiment and the twentieth embodiment each include nine optical lenses, which are respectively a first optical lens L1, a second optical lens L2, a third optical lens L3, a fourth optical lens L4, and a fifth optical lens. L5, the sixth optical lens L6, the seventh optical lens L7, the eighth optical lens L8 and the ninth optical lens L9, and each optical lens has an object-side surface R1 and an image-side surface R2 respectively.

第十九實施例及第二十實施例的光學鏡頭的配置方式已列於下表二十六,且表二十六的參數定義皆與第七實施例至第十一實施例相同,於此不再贅述。 表二十六 實施例 十九 二十 光學鏡片 數量 9 9 CRA (度) 41 41   長波長吸收材料分析評估 L1     L2     L3     L4   * L5   * L6     L7     L8   * L9   * 像側 光學元件 *     紅外線濾除鍍膜分析評估 L1 R1     R2 * * L2 R1 * * R2 * * L3 R1 * * R2 * * L4 R1 * * R2 * * L5 R1 * * R2   * L6 R1   * R2   * L7 R1     R2     L8 R1     R2     L9 R1     R2     The configuration of the optical lenses of the nineteenth and twentieth embodiments is listed in Table 26 below, and the parameter definitions in Table 26 are the same as those in the seventh to eleventh embodiments. Here No more details. Table 26 Example nineteen twenty Number of optical lenses 9 9 CRA (degree) 41 41 Analysis and Evaluation of Long Wavelength Absorbing Materials L1 L2 L3 L4 * L5 * L6 L7 L8 * L9 * Image side optical components * Infrared filter coating analysis and evaluation L1 R1 R2 * * L2 R1 * * R2 * * L3 R1 * * R2 * * L4 R1 * * R2 * * L5 R1 * * R2 * L6 R1 * R2 * L7 R1 R2 L8 R1 R2 L9 R1 R2

第十九實施例的光學鏡頭於最大像高視場處的主光線入射平板玻璃表面的角度為41度,第十九實施例的光學鏡頭為九光學鏡片的光學系統,長波長吸收材料混入聚合物(Polymer)後,依需求設置於光學鏡頭像側端的光學元件表面或混製,如平板玻璃表面的聚合物層、複數平板玻璃間的聚合物層、微透鏡表面的聚合物層、微透鏡與彩色濾光片間的聚合物層或混製於彩色濾光片內。依本揭示內容的因子分析評估結果,紅外線濾除鍍膜可選擇設置於第一光學鏡片L1的像側表面R2、第二光學鏡片L2的物側表面R1、第二光學鏡片L2的像側表面R2、第三光學鏡片L3的物側表面R1、第三光學鏡片L3的像側表面R2、第四光學鏡片L4的物側表面R1、第四光學鏡片L4的像側表面R2或第五光學鏡片L5的物側表面R1以及其組合。The angle at which the chief ray of the optical lens of the nineteenth embodiment is incident on the surface of the flat glass at the maximum image height field of view is 41 degrees. The optical lens of the nineteenth embodiment is an optical system with nine optical lenses. The long-wavelength absorbing material is mixed into the polymer After the object (Polymer), it is placed on the surface of the optical element at the image side of the optical lens or mixed as required, such as a polymer layer on the surface of flat glass, a polymer layer between multiple flat glasses, a polymer layer on the surface of microlenses, microlenses The polymer layer between the color filter and the color filter may be mixed in the color filter. According to the factor analysis and evaluation results of this disclosure, the infrared filter coating can be selectively disposed on the image-side surface R2 of the first optical lens L1, the object-side surface R1 of the second optical lens L2, and the image-side surface R2 of the second optical lens L2. , the object-side surface R1 of the third optical lens L3, the image-side surface R2 of the third optical lens L3, the object-side surface R1 of the fourth optical lens L4, the image-side surface R2 of the fourth optical lens L4, or the fifth optical lens L5 The object-side surface R1 and combinations thereof.

請參照第4圖,第4圖為傳統光學鏡頭與本揭示內容的光學鏡頭的結構示意圖,且第4圖上半部為本揭示內容的光學鏡頭的結構示意圖,第4圖下半部為傳統光學鏡頭的結構示意圖。Please refer to Figure 4. Figure 4 is a schematic structural diagram of a traditional optical lens and the optical lens disclosed herein. The upper half of Figure 4 is a schematic structural diagram of the optical lens disclosed herein. The lower half of Figure 4 is a schematic structural diagram of a traditional optical lens. Schematic diagram of the structure of an optical lens.

傳統光學鏡頭由物側至像側依序包含一光學系統110、一平板玻璃130b及一電子感光元件150b,平板玻璃130b的物側表面具有一抗反射膜層120b。詳言之,傳統光學鏡頭的平板玻璃130b設置方式為平板玻璃130b與電子感光元件150b的一表面140b(成像面)間有一空氣間距,最大像高視場處的主光線入射平板玻璃130b的表面的角度為α(即CRAg),當主光線經平板玻璃130b折射後會變成角度較小的β,而主光線出射於平板玻璃130b再經空氣折射後會變回原有角度α(即CRA),當主光線角過大時會導致光線無法順利入射電子感光元件150b,或造成畫素錯位響應而產生色偏而降低成像品質。A traditional optical lens includes an optical system 110, a flat glass 130b and an electronic photosensitive element 150b in order from the object side to the image side. The object side surface of the flat glass 130b has an anti-reflective film layer 120b. In detail, the flat glass 130b of the traditional optical lens is arranged in such a way that there is an air gap between the flat glass 130b and a surface 140b (imaging surface) of the electronic photosensitive element 150b, and the chief ray at the maximum image high field of view is incident on the surface of the flat glass 130b. The angle is α (that is, CRAg). When the chief ray is refracted by the flat glass 130b, it will change to a smaller angle β, and the chief ray emerges from the flat glass 130b and will change back to the original angle α (that is, CRA) after being refracted by the air. , when the chief ray angle is too large, the light will not be smoothly incident on the electronic photosensitive element 150b, or the pixels will be misaligned in response, resulting in color shift and reduced imaging quality.

本揭示內容的光學鏡頭由物側至像側可以依序包含一光學系統110、一平板玻璃130a及一電子感光元件150a,平板玻璃130a的物側表面具有一抗反射膜層120a。詳言之,本揭示內容的光學鏡頭的平板玻璃130a設置方式為平板玻璃130a直接設置於電子感光元件150a的一表面140a,最大像高視場處的主光線入射平板玻璃130a的表面的角度為α(即CRAg),當主光線經平板玻璃130a折射後會變成角度β,因平板玻璃130a與電子感光元件150a表面140a間無空氣間距,主光線得以用較小的角度β(即CRA)直接入射於電子感光元件150a,本揭示內容的光學鏡頭設計可有效避免傳統大角度光線無法成像與色偏的問題,並具有降低主光線角度、減少後焦長、縮減光學鏡頭總長度、縮小最大像高與製程簡化等優勢。The optical lens of the present disclosure may include an optical system 110, a flat glass 130a and an electronic photosensitive element 150a in sequence from the object side to the image side. The object side surface of the flat glass 130a has an anti-reflective film layer 120a. In detail, the flat glass 130a of the optical lens of the present disclosure is arranged in such a manner that the flat glass 130a is directly arranged on a surface 140a of the electronic photosensitive element 150a. The angle at which the chief ray at the maximum image high field of view enters the surface of the flat glass 130a is α (i.e. CRAg), when the chief ray is refracted by the flat glass 130a, it will become an angle β. Since there is no air gap between the flat glass 130a and the surface 140a of the electronic photosensitive element 150a, the main ray can be directed at a smaller angle β (i.e. CRA) Incident to the electronic photosensitive element 150a, the optical lens design disclosed in this disclosure can effectively avoid the problems of traditional large-angle light being unable to image and color cast, and has the advantages of lowering the main ray angle, reducing the back focal length, reducing the total length of the optical lens, and reducing the maximum image. High efficiency and process simplification.

<第二十一實施例至第二十四實施例><Twenty-first to Twenty-fourth Embodiment>

本揭示內容光學鏡頭中的光學鏡片或光學元件可另添加具有850 nm – 1200 nm波長範圍的長波長吸收材料(LA8),其吸收波峰約為1050 nm,以提升紅外線的完整濾除效果,且此長波長吸收材料在穿透率為50%(T50)的波長可介於900 nm至1000 nm間。本揭示內容中長波長吸收材料的使用濃度可介於0%~1.0%、0%~0.5%、0%~0.25%、0%~0.10%、0%~0.05%、0%~0.025%或0%~0.01%。The optical lenses or optical elements in the optical lens of this disclosure can be additionally added with a long wavelength absorbing material (LA8) with a wavelength range of 850 nm – 1200 nm, and its absorption peak is approximately 1050 nm to improve the complete filtering effect of infrared rays, and This long-wavelength absorbing material can range from 900 nm to 1000 nm at a wavelength with a transmission rate of 50% (T50). The concentration of the long wavelength absorbing material in this disclosure may be between 0% and 1.0%, 0% and 0.5%, 0% and 0.25%, 0% and 0.10%, 0% and 0.05%, and 0% and 0.025% respectively. 0%~0.01%.

請一併參照第5圖,第5圖為第二十一實施例至第二十四實施例的光學鏡片的穿透率與波長的關係圖。第二十一實施例至第二十四實施例為具有長波長吸收材料LA8的光學鏡片,其於不同波長下的穿透率數據已列於下表二十七。 表二十七 實施例 二十一 二十二 二十三 二十四 LA8濃度 (%) 0 - 0.05 0 - 0.10 0 - 0. 25 0 - 1.0   光學鏡片穿透率 (%,0度) T4070 80.34 72.22 68.44 39.58 T5060 82.22 74.46 69.58 39.71 T7080 84.88 79.73 71.99 44.62 T90120 54.03 36.57 22.68 6.00 T95110 33.09 11.94 5.35 0.21 T100110 24.15 6.06 0.65 0 T40 63.59 48.01 48.58 16.54 T45 77.28 67.88 67.52 40.79 T50 78.87 67.94 63.78 29.89 T55 82.25 74.86 69.86 39.87 T60 84.52 78.71 73.73 47.56 T65 84.01 78.22 72.94 46.21 T70 83.36 78.04 71.93 44.46 T80 85.37 80.40 74.20 49.29 T85 82.40 72.58 67.64 34.98 T90 74.46 56.44 50.28 13.46 T95 65.87 40.90 28.68 2.44 T100 30.16 6.12 2.46 0.03 T105 8.89 0.46 0 0 T110 58.36 30.13 3.30 0.10 T115 82.89 75.19 40.02 6.80 T120 78.21 76.08 71.36 43.74 Please refer to Figure 5 as well. Figure 5 is a graph showing the relationship between transmittance and wavelength of the optical lenses of the twenty-first to twenty-fourth embodiments. The twenty-first to twenty-fourth embodiments are optical lenses with long wavelength absorbing material LA8, and their transmittance data at different wavelengths are listed in Table 27 below. Table 27 Example twenty one twenty two twenty-three twenty four LA8 concentration (%) 0-0.05 0-0.10 0 - 0.25 0-1.0 Optical lens transmittance (%, 0 degrees) T4070 80.34 72.22 68.44 39.58 T5060 82.22 74.46 69.58 39.71 T7080 84.88 79.73 71.99 44.62 T90120 54.03 36.57 22.68 6.00 T95110 33.09 11.94 5.35 0.21 T100110 24.15 6.06 0.65 0 T40 63.59 48.01 48.58 16.54 T45 77.28 67.88 67.52 40.79 T50 78.87 67.94 63.78 29.89 T55 82.25 74.86 69.86 39.87 T60 84.52 78.71 73.73 47.56 T65 84.01 78.22 72.94 46.21 T70 83.36 78.04 71.93 44.46 T80 85.37 80.40 74.20 49.29 T85 82.40 72.58 67.64 34.98 T90 74.46 56.44 50.28 13.46 T95 65.87 40.90 28.68 2.44 T100 30.16 6.12 2.46 0.03 T105 8.89 0.46 0 0 T110 58.36 30.13 3.30 0.10 T115 82.89 75.19 40.02 6.80 T120 78.21 76.08 71.36 43.74

本揭示內容第二十一實施例的光學鏡片在850 nm的穿透率小於在600 nm的穿透率、在850 nm的穿透率小於在650 nm的穿透率、在850 nm的穿透率小於在700 nm的穿透率;在900 nm的穿透率小於在450 nm的穿透率、在900 nm的穿透率小於在500 nm的穿透率、在900 nm的穿透率小於在550 nm的穿透率、在900 nm的穿透率小於在600 nm的穿透率、在900 nm的穿透率小於在650 nm的穿透率、在900 nm的穿透率小於在700 nm的穿透率;在950 nm的穿透率小於在450 nm的穿透率、在950 nm的穿透率小於在500 nm的穿透率、在950 nm的穿透率小於在550 nm的穿透率、在950 nm的穿透率小於在600 nm的穿透率、在950 nm的穿透率小於在650 nm的穿透率、在950 nm的穿透率小於在700 nm的穿透率;在1000 nm的穿透率小於在400 nm的穿透率、在1000 nm的穿透率小於在450 nm的穿透率、在1000 nm的穿透率小於在500 nm的穿透率、在1000 nm的穿透率小於在550 nm的穿透率、在1000 nm的穿透率小於在600 nm的穿透率、在1000 nm的穿透率小於在650 nm的穿透率、在1000 nm的穿透率小於在700 nm的穿透率;在1050 nm的穿透率小於在400 nm的穿透率、在1050 nm的穿透率小於在450 nm的穿透率、在1050 nm的穿透率小於在500 nm的穿透率、在1050 nm的穿透率小於在550 nm的穿透率、在1050 nm的穿透率小於在600 nm的穿透率、在1050 nm的穿透率小於在650 nm的穿透率、在1050 nm的穿透率小於在700 nm的穿透率;在1100 nm的穿透率小於在400 nm的穿透率、在1100 nm的穿透率小於在450 nm的穿透率、在1100 nm的穿透率小於在500 nm的穿透率、在1100 nm的穿透率小於在550 nm的穿透率、在1100 nm的穿透率小於在600 nm的穿透率、在1100 nm的穿透率小於在650 nm的穿透率、在1100 nm的穿透率小於在700 nm的穿透率。在1150 nm的穿透率小於在600 nm的穿透率、在1150 nm的穿透率小於在650 nm的穿透率、在1150 nm的穿透率小於在700 nm的穿透率。在1200 nm的穿透率小於在500 nm的穿透率、在1200 nm的穿透率小於在550 nm的穿透率、在1200 nm的穿透率小於在600 nm的穿透率、在1200 nm的穿透率小於在650 nm的穿透率、在1200 nm的穿透率小於在700 nm的穿透率。The optical lens according to the twenty-first embodiment of the disclosure has a transmittance at 850 nm that is less than the transmittance at 600 nm, a transmittance at 850 nm that is less than the transmittance at 650 nm, and a transmittance at 850 nm. The penetration rate is less than the penetration rate at 700 nm; the penetration rate at 900 nm is less than the penetration rate at 450 nm, the penetration rate at 900 nm is less than the penetration rate at 500 nm, the penetration rate at 900 nm is less than The penetration rate at 550 nm, the penetration rate at 900 nm is less than the penetration rate at 600 nm, the penetration rate at 900 nm is less than the penetration rate at 650 nm, the penetration rate at 900 nm is less than the penetration rate at 700 nm nm penetration rate; the penetration rate at 950 nm is less than the penetration rate at 450 nm, the penetration rate at 950 nm is less than the penetration rate at 500 nm, the penetration rate at 950 nm is less than the penetration rate at 550 nm The penetration rate at 950 nm is less than the penetration rate at 600 nm, the penetration rate at 950 nm is less than the penetration rate at 650 nm, the penetration rate at 950 nm is less than the penetration rate at 700 nm rate; the penetration rate at 1000 nm is less than the penetration rate at 400 nm, the penetration rate at 1000 nm is less than the penetration rate at 450 nm, the penetration rate at 1000 nm is less than the penetration rate at 500 nm, The penetration rate at 1000 nm is less than the penetration rate at 550 nm, the penetration rate at 1000 nm is less than the penetration rate at 600 nm, the penetration rate at 1000 nm is less than the penetration rate at 650 nm, the penetration rate at 1000 nm The penetration rate at 1050 nm is less than the penetration rate at 700 nm; the penetration rate at 1050 nm is less than the penetration rate at 400 nm, the penetration rate at 1050 nm is less than the penetration rate at 450 nm, the penetration rate at 1050 nm The penetration rate is less than the penetration rate at 500 nm, the penetration rate at 1050 nm is less than the penetration rate at 550 nm, the penetration rate at 1050 nm is less than the penetration rate at 600 nm, the penetration rate at 1050 nm The penetration rate is less than the penetration rate at 650 nm, the penetration rate at 1050 nm is less than the penetration rate at 700 nm; the penetration rate at 1100 nm is less than the penetration rate at 400 nm, the penetration rate at 1100 nm is less than The penetration rate at 450 nm, the penetration rate at 1100 nm is less than the penetration rate at 500 nm, the penetration rate at 1100 nm is less than the penetration rate at 550 nm, the penetration rate at 1100 nm is less than the penetration rate at 600 nm The penetration rate at 1100 nm is less than the penetration rate at 650 nm, and the penetration rate at 1100 nm is less than the penetration rate at 700 nm. The penetration rate at 1150 nm is less than the penetration rate at 600 nm, the penetration rate at 1150 nm is less than the penetration rate at 650 nm, and the penetration rate at 1150 nm is less than the penetration rate at 700 nm. The penetration rate at 1200 nm is less than the penetration rate at 500 nm, the penetration rate at 1200 nm is less than the penetration rate at 550 nm, the penetration rate at 1200 nm is less than the penetration rate at 600 nm, the penetration rate at 1200 nm The penetration rate at nm is less than the penetration rate at 650 nm, and the penetration rate at 1200 nm is less than the penetration rate at 700 nm.

光學鏡片於波長400 nm – 700 nm的平均穿透率為T4070,其可以滿足下列條件:35% ≤ T4070;60% ≤ T4070 < 100%;70% ≤ T4070 ≤ 99%;75% ≤ T4070 ≤ 99%;或80% ≤ T4070 ≤ 95%。The average transmittance of optical lenses at wavelengths 400 nm – 700 nm is T4070, which can meet the following conditions: 35% ≤ T4070; 60% ≤ T4070 < 100%; 70% ≤ T4070 ≤ 99%; 75% ≤ T4070 ≤ 99 %; or 80% ≤ T4070 ≤ 95%.

光學鏡片於波長500 nm – 600 nm的平均穿透率為T5060,其可以滿足下列條件:35% ≤ T5060;60% ≤ T5060 < 100%;70% ≤ T5060 ≤ 99%;75% ≤ T5060 ≤ 99%;或80% ≤ T5060 ≤ 95%。The average transmittance of optical lenses at wavelengths 500 nm – 600 nm is T5060, which can meet the following conditions: 35% ≤ T5060; 60% ≤ T5060 < 100%; 70% ≤ T5060 ≤ 99%; 75% ≤ T5060 ≤ 99 %; or 80% ≤ T5060 ≤ 95%.

光學鏡片於波長700 nm – 800 nm的平均穿透率為T7080,其可以滿足下列條件:35% ≤ T7080;60% ≤ T7080 < 100%;70% ≤ T7080 ≤ 99%;75% ≤ T7080 ≤ 99%;或80% ≤ T7080 ≤ 95%。The average transmittance of optical lenses at wavelengths 700 nm – 800 nm is T7080, which can meet the following conditions: 35% ≤ T7080; 60% ≤ T7080 < 100%; 70% ≤ T7080 ≤ 99%; 75% ≤ T7080 ≤ 99 %; or 80% ≤ T7080 ≤ 95%.

光學鏡片於波長900 nm – 1200 nm的平均穿透率為T90120,其可以滿足下列條件:0% ≤ T90120 < 100%;0% ≤ T90120 ≤ 95%;或5% ≤ T90120 ≤ 90%。The average transmittance of optical lenses at wavelengths 900 nm – 1200 nm is T90120, which can meet the following conditions: 0% ≤ T90120 < 100%; 0% ≤ T90120 ≤ 95%; or 5% ≤ T90120 ≤ 90%.

光學鏡片於波長950 nm – 1100 nm的平均穿透率為T95110,其可以滿足下列條件:0% ≤ T95110 < 100%;0% ≤ T95110 ≤ 95%;或5% ≤ T95110 ≤ 90%。The average transmittance of optical lenses at wavelengths 950 nm – 1100 nm is T95110, which can meet the following conditions: 0% ≤ T95110 < 100%; 0% ≤ T95110 ≤ 95%; or 5% ≤ T95110 ≤ 90%.

光學鏡片於波長1000 nm – 1100 nm的平均穿透率為T100110,其可以滿足下列條件:0% ≤ T100110 < 100%;0% ≤ T100110 ≤ 95%;或5% ≤ T100110 ≤ 90%。The average transmittance of optical lenses at wavelengths 1000 nm – 1100 nm is T100110, which can meet the following conditions: 0% ≤ T100110 < 100%; 0% ≤ T100110 ≤ 95%; or 5% ≤ T100110 ≤ 90%.

光學鏡片於波長400 nm的穿透率為T40,其可以滿足下列條件:10% ≤ T40 < 100%;70% ≤ T40 ≤ 99%;75% ≤ T40 ≤ 99%;或80% ≤ T40 ≤ 95%。The transmittance of the optical lens at a wavelength of 400 nm is T40, which can meet the following conditions: 10% ≤ T40 < 100%; 70% ≤ T40 ≤ 99%; 75% ≤ T40 ≤ 99%; or 80% ≤ T40 ≤ 95 %.

光學鏡片於波長450 nm的穿透率為T45,其可以滿足下列條件:40% ≤ T45 < 100%;70% ≤ T45 ≤ 99%;75% ≤ T45 ≤ 99%;或80% ≤ T45 ≤ 95%。The transmittance of the optical lens at a wavelength of 450 nm is T45, which can meet the following conditions: 40% ≤ T45 < 100%; 70% ≤ T45 ≤ 99%; 75% ≤ T45 ≤ 99%; or 80% ≤ T45 ≤ 95 %.

光學鏡片於波長500 nm的穿透率為T50,其可以滿足下列條件:20% ≤ T50 < 100%;70% ≤ T50 ≤ 99%;75% ≤ T50 ≤ 99%;或80% ≤ T50 ≤ 95%。The transmittance of optical lenses at a wavelength of 500 nm is T50, which can meet the following conditions: 20% ≤ T50 < 100%; 70% ≤ T50 ≤ 99%; 75% ≤ T50 ≤ 99%; or 80% ≤ T50 ≤ 95 %.

光學鏡片於波長550 nm的穿透率為T55,其可以滿足下列條件:30% ≤ T55 < 100%;70% ≤ T55 ≤ 99%;75% ≤ T55 ≤ 99%;或80% ≤ T55 ≤ 95%。The transmittance of the optical lens at a wavelength of 550 nm is T55, which can meet the following conditions: 30% ≤ T55 < 100%; 70% ≤ T55 ≤ 99%; 75% ≤ T55 ≤ 99%; or 80% ≤ T55 ≤ 95 %.

光學鏡片於波長600 nm的穿透率為T60,其可以滿足下列條件:40% ≤ T60 < 100%;70% ≤ T60 ≤ 99%;75% ≤ T60 ≤ 99%;或80% ≤ T60 ≤ 95%。The transmittance of the optical lens at a wavelength of 600 nm is T60, which can meet the following conditions: 40% ≤ T60 < 100%; 70% ≤ T60 ≤ 99%; 75% ≤ T60 ≤ 99%; or 80% ≤ T60 ≤ 95 %.

光學鏡片於波長650 nm的穿透率為T65,其可以滿足下列條件:40% ≤ T65 < 100%;70% ≤ T65 ≤ 99%;75% ≤ T65 ≤ 99%;或80% ≤ T65 ≤ 95%。The transmittance of the optical lens at a wavelength of 650 nm is T65, which can meet the following conditions: 40% ≤ T65 < 100%; 70% ≤ T65 ≤ 99%; 75% ≤ T65 ≤ 99%; or 80% ≤ T65 ≤ 95 %.

光學鏡片於波長700 nm的穿透率為T70,其可以滿足下列條件:40% ≤ T70 < 100%;70% ≤ T70 ≤ 99%;75% ≤ T70 ≤ 99%;或80% ≤ T70 ≤ 95%。The transmittance of the optical lens at a wavelength of 700 nm is T70, which can meet the following conditions: 40% ≤ T70 < 100%; 70% ≤ T70 ≤ 99%; 75% ≤ T70 ≤ 99%; or 80% ≤ T70 ≤ 95 %.

光學鏡片於波長800 nm的穿透率為T80,其可以滿足下列條件:0% ≤ T80 < 100%;0% ≤ T80 ≤ 95%;或5% ≤ T80 ≤ 90%。The transmittance of optical lenses at a wavelength of 800 nm is T80, which can meet the following conditions: 0% ≤ T80 < 100%; 0% ≤ T80 ≤ 95%; or 5% ≤ T80 ≤ 90%.

光學鏡片於波長850 nm的穿透率為T85,其可以滿足下列條件:0% ≤ T85 < 100%;0% ≤ T85 ≤ 95%;或5% ≤ T85 ≤ 90%。The transmittance of the optical lens at a wavelength of 850 nm is T85, which can meet the following conditions: 0% ≤ T85 < 100%; 0% ≤ T85 ≤ 95%; or 5% ≤ T85 ≤ 90%.

光學鏡片於波長900 nm的穿透率為T90,其可以滿足下列條件:0% ≤ T90 < 100%;0% ≤ T90 ≤ 95%;或5% ≤ T90 ≤ 90%。The transmittance of optical lenses at a wavelength of 900 nm is T90, which can meet the following conditions: 0% ≤ T90 < 100%; 0% ≤ T90 ≤ 95%; or 5% ≤ T90 ≤ 90%.

光學鏡片於波長950 nm的穿透率為T95,其可以滿足下列條件:0% ≤ T95 < 100%;0% ≤ T95 ≤ 95%;或5% ≤ T95 ≤ 90%。The transmittance of optical lenses at a wavelength of 950 nm is T95, which can meet the following conditions: 0% ≤ T95 < 100%; 0% ≤ T95 ≤ 95%; or 5% ≤ T95 ≤ 90%.

光學鏡片於波長1000 nm的穿透率為T100,其可以滿足下列條件:0% ≤ T100 < 100%;0% ≤ T100 ≤ 95%;或5% ≤ T100 ≤ 90%。The transmittance of optical lenses at a wavelength of 1000 nm is T100, which can meet the following conditions: 0% ≤ T100 < 100%; 0% ≤ T100 ≤ 95%; or 5% ≤ T100 ≤ 90%.

光學鏡片於波長1050 nm的穿透率為T105,其可以滿足下列條件:0% ≤ T105 < 100%;0% ≤ T105 ≤ 95%;或5% ≤ T105 ≤ 90%。The transmittance of the optical lens at a wavelength of 1050 nm is T105, which can meet the following conditions: 0% ≤ T105 < 100%; 0% ≤ T105 ≤ 95%; or 5% ≤ T105 ≤ 90%.

光學鏡片於波長1100 nm的穿透率為T110,其可以滿足下列條件:0% ≤ T110 < 100%;0% ≤ T110 ≤ 95%;或5% ≤ T110 ≤ 90%。The transmittance of the optical lens at a wavelength of 1100 nm is T110, which can meet the following conditions: 0% ≤ T110 < 100%; 0% ≤ T110 ≤ 95%; or 5% ≤ T110 ≤ 90%.

光學鏡片於波長1150 nm的穿透率為T115,其可以滿足下列條件:0% ≤ T115 < 100%;0% ≤ T115 ≤ 95%;或5% ≤ T115 ≤ 90%。The transmittance of the optical lens at a wavelength of 1150 nm is T115, which can meet the following conditions: 0% ≤ T115 < 100%; 0% ≤ T115 ≤ 95%; or 5% ≤ T115 ≤ 90%.

光學鏡片於波長1200 nm的穿透率為T120,其可以滿足下列條件:0% ≤ T120 < 100%;0% ≤ T120 ≤ 95%;或5% ≤ T120 ≤ 90%。The transmittance of the optical lens at a wavelength of 1200 nm is T120, which can meet the following conditions: 0% ≤ T120 < 100%; 0% ≤ T120 ≤ 95%; or 5% ≤ T120 ≤ 90%.

下表二十八為包含紅外線濾除鍍膜的光學鏡片以及具有包含紅外線濾除鍍膜的光學鏡片與包含長波長吸收材料的光學鏡片的光學鏡頭於波長600 nm~1200 nm的穿透率量測數據。 表二十八   包含紅外線濾除鍍膜的光學鏡片 包含紅外線濾除鍍膜的光學鏡片與包含長波長吸收材料的光學鏡片的光學鏡頭 波長 (nm) 穿透率 (%,0度) 穿透率 (%,30度) 穿透率 (%,0度) 穿透率 (%,30度) 600 84.52 78.71 73.73 47.56 605 84.62 78.92 74.33 48.53 610 84.70 79.48 74.71 49.67 615 84.87 79.88 75.22 50.90 620 85.01 80.10 75.56 51.72 625 84.94 80.29 75.61 52.41 630 84.98 80.18 75.54 52.01 635 84.96 79.94 75.02 51.12 640 84.77 79.53 74.76 49.73 645 84.50 79.16 73.86 48.22 650 84.01 78.22 72.94 46.21 655 83.63 77.69 72.34 45.10 660 83.59 77.27 71.64 43.48 665 83.34 76.74 71.15 42.74 670 83.25 76.60 71.08 42.12 675 83.05 76.87 71.01 42.28 680 83.44 77.28 70.99 42.83 685 83.43 77.67 71.55 43.50 690 83.47 78.00 71.70 44.22 695 83.41 77.99 71.91 44.44 700 83.36 78.04 71.93 44.46 705 83.36 78.06 71.84 44.18 710 83.59 78.28 71.51 43.50 715 83.84 78.56 71.43 43.38 720 84.13 78.93 71.18 42.95 725 84.40 79.11 71.03 42.53 730 84.65 79.19 70.99 42.70 735 84.71 79.36 70.96 42.19 740 84.81 79.62 71.08 42.19 745 85.01 79.83 70.99 42.39 750 85.15 80.08 71.12 42.30 755 85.41 80.11 71.31 43.37 760 85.41 80.24 71.65 43.57 765 85.51 80.44 71.91 44.88 770 85.61 80.61 72.33 45.17 775 85.76 80.63 72.72 45.80 780 85.70 80.75 73.02 47.17 785 85.72 80.77 73.39 47.77 790 85.55 80.70 73.52 48.13 795 85.48 80.58 73.77 49.11 800 85.37 80.40 74.20 49.29 805 84.99 79.94 73.97 48.53 810 84.94 79.83 73.84 48.57 815 84.64 79.22 74.00 48.26 820 84.34 78.68 73.60 46.80 825 84.06 77.87 72.64 46.62 830 83.89 77.02 72.16 44.56 835 83.38 76.10 71.60 43.12 840 83.15 74.93 71.15 41.97 845 82.67 73.72 69.88 40.05 850 82.40 72.58 67.64 34.98 855 81.67 70.94 64.62 31.03 860 81.20 69.65 63.90 29.17 865 80.47 68.14 61.80 27.13 870 79.68 66.49 60.56 24.60 875 78.91 64.67 59.10 22.47 880 78.01 63.00 57.44 20.84 885 77.19 61.37 55.46 18.51 890 76.15 59.64 54.26 16.98 895 75.25 57.95 51.83 14.94 900 74.46 56.44 50.28 13.46 905 73.75 55.13 48.21 11.60 910 73.02 53.80 46.28 10.68 915 72.49 52.67 44.30 9.07 920 71.85 51.64 42.41 7.81 925 71.36 50.56 40.72 6.71 930 70.79 49.34 38.87 5.74 935 69.90 47.85 36.32 4.77 940 68.94 46.00 33.94 3.71 945 67.54 43.66 31.36 2.87 950 65.87 40.90 28.68 2.44 955 63.62 37.49 25.30 1.69 960 61.04 33.80 22.23 1.12 965 58.10 29.97 19.02 0.79 970 54.91 26.06 16.11 0.50 975 51.16 21.96 13.07 0.30 980 47.31 18.13 10.16 0.16 985 43.26 14.65 7.74 0 990 38.91 11.40 5.78 0.05 995 34.35 8.45 4.15 0.01 1000 30.16 6.12 2.46 0.03 1005 26.52 4.39 1.66 0 1010 23.28 3.17 1.04 0 1015 20.35 2.29 0.71 0 1020 17.78 1.70 0.48 0 1025 15.36 1.25 0.28 0 1030 13.01 0.87 0.14 0.17 1035 10.88 0.63 0.05 0.03 1040 9.34 0.53 0.22 0 1045 8.67 0.41 0 0 1050 8.89 0.46 0 0 1055 10.35 0.59 0.07 0.29 1060 13.08 1.00 0 0 1065 16.89 1.83 0 0 1070 21.82 3.23 0.04 0.03 1075 27.80 5.50 0 0 1080 34.20 8.68 0.26 0.19 1085 40.56 12.82 0.85 0 1090 46.85 17.80 1.10 0 1095 53.00 23.80 1.77 0.14 1100 58.36 30.13 3.30 0.10 1105 63.12 36.38 4.74 0.22 1110 67.42 42.93 6.99 0 1115 71.36 49.34 10.17 0.44 1120 74.55 55.11 13.14 0.44 1125 77.11 60.08 16.73 0.79 1130 79.02 64.44 21.21 1.21 1135 80.61 68.12 25.71 1.75 1140 81.63 71.06 30.36 3.36 1145 82.34 73.26 35.21 4.72 1150 82.89 75.19 40.02 6.80 1155 83.16 76.58 45.03 9.60 1160 83.08 77.39 49.12 12.69 1165 82.36 77.46 52.84 16.03 1170 81.10 76.79 56.54 19.96 1175 79.31 75.70 59.83 24.20 1180 77.79 74.59 62.76 28.39 1185 76.85 74.06 65.09 32.42 1190 76.81 74.19 67.81 36.21 1195 77.38 75.03 69.98 40.34 1200 78.21 76.08 71.36 43.74 Table 28 below shows the transmittance measurement data at wavelengths 600 nm to 1200 nm for optical lenses containing infrared filtering coatings and optical lenses containing optical lenses containing infrared filtering coatings and optical lenses containing long wavelength absorbing materials. . Table 28 Optical lenses containing infrared filter coating Optical lenses containing infrared filter coatings and optical lenses containing long wavelength absorbing materials Wavelength(nm) Penetration rate (%, 0 degrees) Penetration rate (%, 30 degrees) Penetration rate (%, 0 degrees) Penetration rate (%, 30 degrees) 600 84.52 78.71 73.73 47.56 605 84.62 78.92 74.33 48.53 610 84.70 79.48 74.71 49.67 615 84.87 79.88 75.22 50.90 620 85.01 80.10 75.56 51.72 625 84.94 80.29 75.61 52.41 630 84.98 80.18 75.54 52.01 635 84.96 79.94 75.02 51.12 640 84.77 79.53 74.76 49.73 645 84.50 79.16 73.86 48.22 650 84.01 78.22 72.94 46.21 655 83.63 77.69 72.34 45.10 660 83.59 77.27 71.64 43.48 665 83.34 76.74 71.15 42.74 670 83.25 76.60 71.08 42.12 675 83.05 76.87 71.01 42.28 680 83.44 77.28 70.99 42.83 685 83.43 77.67 71.55 43.50 690 83.47 78.00 71.70 44.22 695 83.41 77.99 71.91 44.44 700 83.36 78.04 71.93 44.46 705 83.36 78.06 71.84 44.18 710 83.59 78.28 71.51 43.50 715 83.84 78.56 71.43 43.38 720 84.13 78.93 71.18 42.95 725 84.40 79.11 71.03 42.53 730 84.65 79.19 70.99 42.70 735 84.71 79.36 70.96 42.19 740 84.81 79.62 71.08 42.19 745 85.01 79.83 70.99 42.39 750 85.15 80.08 71.12 42.30 755 85.41 80.11 71.31 43.37 760 85.41 80.24 71.65 43.57 765 85.51 80.44 71.91 44.88 770 85.61 80.61 72.33 45.17 775 85.76 80.63 72.72 45.80 780 85.70 80.75 73.02 47.17 785 85.72 80.77 73.39 47.77 790 85.55 80.70 73.52 48.13 795 85.48 80.58 73.77 49.11 800 85.37 80.40 74.20 49.29 805 84.99 79.94 73.97 48.53 810 84.94 79.83 73.84 48.57 815 84.64 79.22 74.00 48.26 820 84.34 78.68 73.60 46.80 825 84.06 77.87 72.64 46.62 830 83.89 77.02 72.16 44.56 835 83.38 76.10 71.60 43.12 840 83.15 74.93 71.15 41.97 845 82.67 73.72 69.88 40.05 850 82.40 72.58 67.64 34.98 855 81.67 70.94 64.62 31.03 860 81.20 69.65 63.90 29.17 865 80.47 68.14 61.80 27.13 870 79.68 66.49 60.56 24.60 875 78.91 64.67 59.10 22.47 880 78.01 63.00 57.44 20.84 885 77.19 61.37 55.46 18.51 890 76.15 59.64 54.26 16.98 895 75.25 57.95 51.83 14.94 900 74.46 56.44 50.28 13.46 905 73.75 55.13 48.21 11.60 910 73.02 53.80 46.28 10.68 915 72.49 52.67 44.30 9.07 920 71.85 51.64 42.41 7.81 925 71.36 50.56 40.72 6.71 930 70.79 49.34 38.87 5.74 935 69.90 47.85 36.32 4.77 940 68.94 46.00 33.94 3.71 945 67.54 43.66 31.36 2.87 950 65.87 40.90 28.68 2.44 955 63.62 37.49 25.30 1.69 960 61.04 33.80 22.23 1.12 965 58.10 29.97 19.02 0.79 970 54.91 26.06 16.11 0.50 975 51.16 21.96 13.07 0.30 980 47.31 18.13 10.16 0.16 985 43.26 14.65 7.74 0 990 38.91 11.40 5.78 0.05 995 34.35 8.45 4.15 0.01 1000 30.16 6.12 2.46 0.03 1005 26.52 4.39 1.66 0 1010 23.28 3.17 1.04 0 1015 20.35 2.29 0.71 0 1020 17.78 1.70 0.48 0 1025 15.36 1.25 0.28 0 1030 13.01 0.87 0.14 0.17 1035 10.88 0.63 0.05 0.03 1040 9.34 0.53 0.22 0 1045 8.67 0.41 0 0 1050 8.89 0.46 0 0 1055 10.35 0.59 0.07 0.29 1060 13.08 1.00 0 0 1065 16.89 1.83 0 0 1070 21.82 3.23 0.04 0.03 1075 27.80 5.50 0 0 1080 34.20 8.68 0.26 0.19 1085 40.56 12.82 0.85 0 1090 46.85 17.80 1.10 0 1095 53.00 23.80 1.77 0.14 1100 58.36 30.13 3.30 0.10 1105 63.12 36.38 4.74 0.22 1110 67.42 42.93 6.99 0 1115 71.36 49.34 10.17 0.44 1120 74.55 55.11 13.14 0.44 1125 77.11 60.08 16.73 0.79 1130 79.02 64.44 21.21 1.21 1135 80.61 68.12 25.71 1.75 1140 81.63 71.06 30.36 3.36 1145 82.34 73.26 35.21 4.72 1150 82.89 75.19 40.02 6.80 1155 83.16 76.58 45.03 9.60 1160 83.08 77.39 49.12 12.69 1165 82.36 77.46 52.84 16.03 1170 81.10 76.79 56.54 19.96 1175 79.31 75.70 59.83 24.20 1180 77.79 74.59 62.76 28.39 1185 76.85 74.06 65.09 32.42 1190 76.81 74.19 67.81 36.21 1195 77.38 75.03 69.98 40.34 1200 78.21 76.08 71.36 43.74

本揭示內容所述穿透率為量測光學鏡片群組的穿透率,或進一步包含光學元件的穿透率,光學鏡片的表面可進一步設置抗反射鍍膜,如高低折射率膜層或次波長微結構膜層或及其組合。The transmittance described in this disclosure measures the transmittance of the optical lens group, or further includes the transmittance of the optical element. The surface of the optical lens can be further provided with an anti-reflective coating, such as a high and low refractive index coating or a sub-wavelength coating. Microstructured film layer or combination thereof.

本揭示內容藉由控制光學鏡片表面的全視場範圍內的入射光角度之最佳設計,通過分析主光線在光學鏡片表面的入射角,在最佳的光學鏡片表面配置特定的波長濾除鍍膜,並在最佳的光學鏡片添加長波長吸收材料,有助於解決習知具有紅外線濾除鍍膜的光學鏡片的漏光問題。再者,更直接減除藍玻璃元件,促進光學鏡頭的微型化,不僅降低光學鏡頭的製造成本,更無玻璃元件碎裂、損壞等問題。本揭示內容透過決定最適合配置鍍膜的光學鏡片表面之技術,不僅可以獲得紅外線濾除鍍膜的最佳製作效果,在最均勻的光學鏡片表面的鍍膜條件下,發揮應有濾除效果與減少強光反射問題,有效提升整體光學鏡頭的影像品質。本揭示內容藉由控制光學鏡片表面面形的細微變化,有助於解決嚴重強光反射現象所導致的雜散光缺陷。本揭示內容進一步藉由分析各光學鏡片的最佳光程數據,得到最有利的吸收材料添加因子,有效解決大角度入射光的偏移漏光缺陷。This disclosure controls the optimal design of the incident light angle within the full field of view of the optical lens surface, and configures a specific wavelength filtering coating on the optimal optical lens surface by analyzing the incident angle of the chief ray on the optical lens surface. , and adding long-wavelength absorbing materials to the best optical lenses can help solve the light leakage problem of conventional optical lenses with infrared filter coatings. Furthermore, it directly eliminates blue glass components and promotes the miniaturization of optical lenses, which not only reduces the manufacturing cost of optical lenses, but also eliminates problems such as glass component breakage and damage. This disclosure not only obtains the best production effect of infrared filter coating by determining the most suitable optical lens surface for coating, but also exerts the proper filtering effect and reduces intensity under the most uniform coating conditions on the optical lens surface. Light reflection problem effectively improves the image quality of the overall optical lens. This disclosure helps to solve stray light defects caused by severe strong light reflection by controlling subtle changes in the surface shape of optical lenses. This disclosure further analyzes the optimal optical path data of each optical lens to obtain the most favorable absorption material addition factor, effectively solving the offset light leakage defect of large-angle incident light.

本揭示內容的濾除鍍膜亦可額外製作在其他元件表面上,如平板玻璃、保護玻璃、塑膠平板、玻璃平板或反射元件等,其他元件表面上的濾除鍍膜具補強不足波段的完整濾除效果,因此光學鏡片表面製作的鍍膜可負責濾除特定波長區域,以減少膜層數量與厚度,在配置具吸收材料的光學鏡片後,藉由組合多元件的各自濾除效果以達成完整所需的濾除效果。The filter coating disclosed in this disclosure can also be additionally made on the surface of other components, such as flat glass, protective glass, plastic plate, glass plate or reflective components, etc. The filter coating on the surface of other components can enhance the complete filtering of insufficient wavebands. Therefore, the coating produced on the surface of the optical lens can be responsible for filtering out specific wavelength areas to reduce the number and thickness of the film layers. After configuring the optical lens with absorbing materials, the complete required filtering effects can be achieved by combining the respective filtering effects of multiple elements. filtering effect.

本揭示內容的光學鏡頭可藉由設計平板玻璃設置於電子感光元件的表面(光學鏡頭的成像面),結合光學鏡片中具有長波長吸收材料與紅外線濾除鍍膜製作於光學鏡片表面的組合方式,有助於光學鏡頭降低最大像高視場處的主光線入射於電子感光元件的角度,達到縮減後焦長與總長效果;為達到平板玻璃與電子感光元件表面的折射率接近或相同,可在電子感光元件與平板玻璃間設置高分子聚合物,使其折射率與平板玻璃折射率接近或相同,因此可讓光線未經折射而直接穿過平板玻璃與電子感光元件間的界面,避免再次折射而導致入射角度變大。The optical lens disclosed in this disclosure can be made by designing flat glass on the surface of the electronic photosensitive element (the imaging surface of the optical lens), and combining the long wavelength absorbing material in the optical lens with the infrared filter coating on the surface of the optical lens. It helps the optical lens to reduce the angle at which the chief ray at the maximum image height field of view is incident on the electronic photosensitive element, thereby reducing the back focal length and total length; in order to achieve that the refractive index of the flat glass and the surface of the electronic photosensitive element is close to or the same, it can be A polymer is placed between the electronic photosensitive element and the flat glass so that its refractive index is close to or the same as the refractive index of the flat glass. This allows light to pass directly through the interface between the flat glass and the electronic photosensitive element without refraction, avoiding re-refraction. This causes the angle of incidence to become larger.

本揭示內容的光學鏡頭的平板玻璃與電子感光元件間可具有空氣層或不具有空氣層,當本揭示內容的光學鏡頭為平板玻璃與電子感光元件間具有空氣層的光學系統設計,平板玻璃的物側表面與像側表面中至少一表面或兩表面皆可製作抗反射膜層;當本揭示內容的光學鏡頭為平板玻璃與電子感光元件間不具有空氣層的光學系統設計,可在平板玻璃的物側表面製作抗反射膜層。The optical lens of the present disclosure may or may not have an air layer between the flat glass and the electronic photosensitive element. When the optical lens of the present disclosure is an optical system design with an air layer between the flat glass and the electronic photosensitive element, the flat glass At least one or both surfaces of the object-side surface and the image-side surface can be made with anti-reflective coatings; when the optical lens disclosed in this disclosure is an optical system design that does not have an air layer between the flat glass and the electronic photosensitive element, the flat glass can be An anti-reflective coating is made on the object-side surface.

本揭示內容的光學鏡頭中的光學鏡片或光學元件,所述光學元件如平板玻璃(Cover glass)、微透鏡(Micro lens)、藍玻璃(Blue glass)與濾光元件(Filter,Color filter)等具有可見光穿透特性,在光學元件的物側表面或像側表面可具有抗反射膜層,抗反射膜層包含至少一膜層,如高折射率膜層與低折射率膜層交替組成,或由次波長微結構組成,或由高折射率膜層與次波長微結構共同組成,或由低折射率膜層與次波長微結構共同組成,或由高折射率膜層、低折射率膜層與次波長微結構共同組成。Optical lenses or optical elements in the optical lens of the present disclosure, such as cover glass, micro lens, blue glass, filter, color filter, etc. With visible light transmission properties, the optical element can have an anti-reflective film layer on the object-side surface or the image-side surface. The anti-reflective film layer includes at least one film layer, such as a high refractive index film layer and a low refractive index film layer alternately, or It consists of a sub-wavelength microstructure, or a high refractive index film layer and a sub-wavelength microstructure, or a low refractive index film layer and a sub-wavelength microstructure, or a high refractive index film layer and a low refractive index film layer. Together with sub-wavelength microstructures.

本揭示內容的光學鏡頭中的抗反射膜層於外側(鄰近空氣)可具有次波長微結構,且材質可為金屬氧化物如氧化鋁(Al 2O 3),抗反射膜層的次波長微結構包含複數個孔洞,且鄰近抗反射鍍膜外側的孔洞之尺寸大於鄰近抗反射鍍膜內側的孔洞之尺寸。本揭示內容的光學鏡頭中的抗反射膜層於內側(鄰近基材)可具有其他膜層,如高折射率膜層與低折射率膜層。 The anti-reflective coating layer in the optical lens of the present disclosure can have a sub-wavelength microstructure on the outside (near the air), and the material can be a metal oxide such as aluminum oxide (Al 2 O 3 ). The sub-wavelength micro-structure of the anti-reflective coating layer The structure includes a plurality of holes, and the size of the holes adjacent to the outside of the anti-reflective coating is larger than the size of the holes adjacent to the inside of the anti-reflective coating. The anti-reflective coating layer in the optical lens of the present disclosure may have other coating layers on the inner side (near the substrate), such as a high refractive index coating layer and a low refractive index coating layer.

本揭示內容的光學鏡頭中的光學鏡片或光學元件,如平板玻璃、微透鏡、藍玻璃與濾光元件的物側表面或像側表面可具有紅外線濾除鍍膜,紅外線濾除鍍膜包含至少一膜層,如高折射率膜層與低折射率膜層交替組成。The optical lenses or optical elements in the optical lens of the present disclosure, such as plate glass, microlenses, blue glass, and the object-side surface or image-side surface of the filter element can have an infrared filter coating, and the infrared filter coating includes at least one film Layers, such as high refractive index film layers and low refractive index film layers alternately form.

本揭示內容的光學鏡頭的高折射率膜層與低折射率膜層,高折射率膜層的材料折射率可大於1.80,低折射率膜層的材料折射率可小於1.80,如抗反射膜層材料(於波長587.6 nm時的折射率)可為:MgF 2(1.37)、SiO 2(1.45)、Al 2O 3(1.76)、HfO 2(1.89)、ZnO(1.92)、Sc 2O 3(1.98)、AlN(2.02)、Si 3N 4(2.03)、Ta 2O 5(2.13)、ZrO 2(2.15)、ZnS(2.27)、Nb 2O 5(2.34)、TiO 2(2.61)或TiN(3.13)。 In the high refractive index film layer and the low refractive index film layer of the optical lens disclosed in this disclosure, the refractive index of the material of the high refractive index film layer can be greater than 1.80, and the refractive index of the material of the low refractive index film layer can be less than 1.80, such as the anti-reflective film layer. Materials (refractive index at wavelength 587.6 nm) can be: MgF 2 (1.37), SiO 2 (1.45), Al 2 O 3 (1.76), HfO 2 (1.89), ZnO (1.92), Sc 2 O 3 ( 1.98), AlN (2.02), Si 3 N 4 (2.03), Ta 2 O 5 (2.13), ZrO 2 (2.15), ZnS (2.27), Nb 2 O 5 (2.34), TiO 2 (2.61) or TiN (3.13).

本揭示內容的光學鏡頭中的光學鏡片可具有長波長吸收材料,光學鏡片的物側表面與像側表面中至少一表面或兩表面皆可製作紅外線濾除鍍膜。The optical lens in the optical lens of the present disclosure may have long-wavelength absorbing materials, and at least one or both surfaces of the object-side surface and the image-side surface of the optical lens may be made of infrared filtering coatings.

本揭示內容的光學鏡頭中的光學鏡片可具有長波長吸收材料,光學鏡片的物側表面與像側表面中至少一表面或兩表面皆可製作紅外線濾除鍍膜,進一步可設計電子感光元件的物側具有藍玻璃。The optical lens in the optical lens of the present disclosure can have long-wavelength absorbing materials. At least one or both surfaces of the object-side surface and the image-side surface of the optical lens can be made of infrared filter coatings. Further, the electronic photosensitive element can be designed. Sides have blue glass.

本揭示內容的光學鏡頭中的光學鏡片可具有長波長吸收材料,光學鏡片的物側表面與像側表面中至少一表面或兩表面皆可製作紅外線濾除鍍膜,進一步可設計電子感光元件的物側具有平板玻璃,平板玻璃的物側表面與像側表面中至少一表面或兩表面皆可製作抗反射膜層。The optical lens in the optical lens of the present disclosure can have long-wavelength absorbing materials. At least one or both surfaces of the object-side surface and the image-side surface of the optical lens can be made of infrared filter coatings. Further, the electronic photosensitive element can be designed. There is flat glass on the side, and at least one or both surfaces of the object-side surface and the image-side surface of the flat glass can be made with anti-reflective coatings.

本揭示內容的光學鏡頭中,平板玻璃的物側表面與像側表面中至少一表面或兩表面皆可具有長波長吸收材料,藉由長波長吸收材料混入高分子聚合物,將聚合物設置在平板玻璃的表面,光學鏡片的物側表面與像側表面中至少一表面或兩表面皆可製作紅外線濾除鍍膜,進一步可設計複數平板玻璃間具有長波長吸收材料,再進一步可設計平板玻璃表面具有抗反射膜層。平板玻璃與電子感光元件間可具有空氣層或不具有空氣層,當本揭示內容的光學鏡頭為平板玻璃與電子感光元件間具有空氣層的光學系統設計,平板玻璃的物側表面與像側表面中至少一表面或兩表面皆可設計長波長吸收材料膜層,進一步可設計平板玻璃表面具有抗反射膜層。當本揭示內容的光學鏡頭為平板玻璃與電子感光元件間不具有空氣層的光學系統設計,平板玻璃的物側表面設計長波長吸收材料膜層,進一步可設計平板玻璃表面具有抗反射膜層。In the optical lens of the present disclosure, at least one or both surfaces of the object-side surface and the image-side surface of the flat glass can have a long-wavelength absorbing material. The long-wavelength absorbing material is mixed with a polymer to set the polymer on The surface of the flat glass, at least one or both surfaces of the object-side surface and the image-side surface of the optical lens can be made with infrared filter coating. Furthermore, long-wavelength absorbing materials can be designed between multiple flat glasses, and the surface of the flat glass can be further designed. With anti-reflective coating. There may or may not be an air layer between the flat glass and the electronic photosensitive element. When the optical lens of this disclosure is an optical system design with an air layer between the flat glass and the electronic photosensitive element, the object-side surface and the image-side surface of the flat glass At least one surface or both surfaces can be designed with a long-wavelength absorbing material film layer, and further, the surface of the flat glass can be designed with an anti-reflective film layer. When the optical lens disclosed in this disclosure is an optical system design that does not have an air layer between the flat glass and the electronic photosensitive element, the object-side surface of the flat glass is designed with a long-wavelength absorbing material film layer, and the surface of the flat glass can further be designed with an anti-reflective film layer.

本揭示內容的光學鏡頭中微透鏡的表面可具有長波長吸收材料,如長波長吸收材料混入高分子聚合物,並將聚合物設置在微透鏡的表面,光學鏡片的物側表面與像側表面中至少一表面或兩表面皆可製作紅外線濾除鍍膜,進一步可設計電子感光元件的表面具有平板玻璃,以有效保護電子感光元件。The surface of the microlens in the optical lens of the present disclosure may have a long-wavelength absorbing material. For example, the long-wavelength absorbing material is mixed with a polymer, and the polymer is disposed on the surface of the microlens. The object-side surface and the image-side surface of the optical lens Infrared filtering coating can be made on at least one surface or both surfaces, and the surface of the electronic photosensitive element can be designed to have flat glass to effectively protect the electronic photosensitive element.

本揭示內容的光學鏡頭中微透鏡的物側可具有長波長吸收材料,藉由長波長吸收材料混入高分子聚合物,將聚合物設置在微透鏡與彩色濾光片間做為連結層,或將長波長吸收材料混合設置在彩色濾光片中,進一步可選擇皆設置在紅色、綠色與藍色濾光片部分,或亦可僅選擇設置在紅色濾光片部分。In the optical lens of the present disclosure, the object side of the microlens can have a long-wavelength absorbing material. The long-wavelength absorbing material is mixed with a polymer, and the polymer is placed between the microlens and the color filter as a connecting layer, or The long-wavelength absorbing material is mixed and arranged in the color filter, and further can be selected to be arranged in the red, green and blue filter parts, or only in the red filter part.

本揭示內容所述濾光元件為可濾除特定波長範圍光線的光學元件,如組成電子感光元件一部份的彩色濾光片、紅外線濾除元件、藍玻璃、窄波長濾除元件、短波長濾除元件或長波長濾除元件等。The filter elements described in this disclosure are optical elements that can filter out light in a specific wavelength range, such as color filters, infrared filter elements, blue glass, narrow wavelength filter elements, short wavelength filters that form part of electronic photosensitive elements. Filter elements or long wavelength filter elements, etc.

雖然本揭示內容已以實施例揭露如上,然其並非用以限定本揭示內容,任何熟習此技藝者,在不脫離本揭示內容之精神和範圍內,當可作各種之組合、排列、更動與潤飾,因此本揭示內容之保護範圍當視後附之申請專利範圍所界定者為準。Although the present disclosure has been disclosed as above in the form of embodiments, it is not intended to limit the disclosure. Anyone skilled in the art can make various combinations, arrangements, modifications and changes without departing from the spirit and scope of the disclosure. Therefore, the scope of protection of this disclosure shall be subject to the scope of the appended patent application.

110:光學系統 120a,120b:抗反射膜層 130a,130b:平板玻璃 140a,140b:表面 150a,150b:電子感光元件 L1,L2,L3,L4,L5,L6,L7,L8,L9:光學鏡片 R1:物側表面 R2:像側表面 AICmax:全視場主光線於包含紅外線濾除鍍膜的光學鏡片表面的入射角最大值 T3540:光學鏡頭於波長350 nm – 400 nm的平均穿透率 T4050:光學鏡頭於波長400 nm – 500 nm的平均穿透率 T5060:光學鏡頭於波長500 nm – 600 nm的平均穿透率 T6570:光學鏡頭於波長650 nm – 700 nm的平均穿透率 T70100:光學鏡頭於波長700 nm – 1000 nm的平均穿透率 T35:光學鏡頭於波長350 nm的穿透率 T40:光學鏡頭於波長400 nm的穿透率 T55:光學鏡頭於波長550 nm的穿透率 T60:光學鏡頭於波長600 nm的穿透率 T63:光學鏡頭於波長630 nm的穿透率 T64:光學鏡頭於波長640 nm的穿透率 T65:光學鏡頭於波長650 nm的穿透率 T70:光學鏡頭於波長700 nm的穿透率 T85:光學鏡頭於波長850 nm的穿透率 FA:各光學鏡片的吸收材料配置主因子 FC:各光學鏡片表面的鍍膜配置主因子 Fc1:各光學鏡片表面的鍍膜配置第一因子 Fc2:各光學鏡片表面的鍍膜配置第二因子 FOV:光學鏡頭的全視角 CT:各光學鏡片於光軸上的厚度 CPavg:各光學鏡片於全視場主光線光程比的平均值 CPst:各光學鏡片於全視場主光線光程比的標準差 SAGmax:各光學鏡片表面上與光軸交點間水平位移的最大值 SPavg:各光學鏡片表面於光學有效徑範圍內的切線斜率的平均值 SPmin:各光學鏡片表面於光學有效徑範圍內的切線斜率的最小值 tLs:紅外線濾除鍍膜的總層數 tTk:紅外線濾除鍍膜的總膜厚 LWdT5:光學鏡頭在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長 SWuT5:光學鏡頭在短波長區域且波長與穿透率呈正相關的趨勢中達到50%穿透率的波長 CRAg:光學鏡頭於最大像高視場處的主光線入射平板玻璃的一表面的角度 CRA:光學鏡頭於最大像高視場處的主光線入射電子感光元件表面的角度 α,β:角度 110:Optical system 120a, 120b: anti-reflective coating 130a,130b: Flat glass 140a,140b: Surface 150a, 150b: Electronic photosensitive element L1,L2,L3,L4,L5,L6,L7,L8,L9: Optical lenses R1: object side surface R2: Image side surface AICmax: The maximum incident angle of the full-field chief ray on the surface of an optical lens containing an infrared filter coating T3540: Average transmittance of optical lens at wavelength 350 nm – 400 nm T4050: Average transmittance of optical lens at wavelength 400 nm – 500 nm T5060: Average transmittance of optical lens at wavelength 500 nm – 600 nm T6570: Average transmittance of optical lens at wavelength 650 nm – 700 nm T70100: Average transmittance of optical lens at wavelength 700 nm – 1000 nm T35: transmittance of optical lens at wavelength 350 nm T40: transmittance of optical lens at wavelength 400 nm T55: Transmittance of optical lens at wavelength 550 nm T60: transmittance of optical lens at wavelength 600 nm T63: Transmittance of optical lens at wavelength 630 nm T64: Transmittance of optical lens at wavelength 640 nm T65: transmittance of optical lens at wavelength 650 nm T70: transmittance of optical lens at wavelength 700 nm T85: Transmittance of optical lens at wavelength 850 nm FA: main factor of absorbing material configuration of each optical lens FC: Main factor of coating configuration on the surface of each optical lens Fc1: The first factor of coating configuration on the surface of each optical lens Fc2: The second factor of coating configuration on the surface of each optical lens FOV: Full viewing angle of the optical lens CT: Thickness of each optical lens on the optical axis CPavg: the average optical path ratio of the chief ray of each optical lens in the full field of view CPst: the standard deviation of the optical path ratio of the chief ray of each optical lens in the full field of view SAGmax: the maximum horizontal displacement between the intersection point of each optical lens surface and the optical axis SPavg: the average tangent slope of each optical lens surface within the optical effective diameter range SPmin: The minimum value of the tangent slope of each optical lens surface within the optical effective diameter range tLs: total number of layers of infrared filter coating tTk: total film thickness of infrared filter coating LWdT5: The wavelength at which the optical lens reaches 50% transmittance in the long wavelength region and the trend of wavelength and transmittance being negatively correlated SWuT5: The wavelength at which the optical lens reaches 50% transmittance in the short wavelength region and the wavelength and transmittance are positively correlated. CRAg: The angle at which the chief ray of an optical lens is incident on a surface of flat glass at the maximum image height field of view CRA: The angle at which the chief ray of the optical lens at the maximum image height field of view is incident on the surface of the electronic photosensitive element. α,β: angle

為讓本揭示內容之上述和其他目的、特徵、優點與實施例能更明顯易懂,所附圖式之說明如下: 第1圖為第三實施例的光學鏡片的穿透率與波長的關係圖; 第2圖為第三實施例的光學鏡頭的穿透率與波長的關係圖; 第3A圖為第三實施例的光學鏡頭的成像品質圖; 第3B圖為比較例的光學鏡頭的成像品質圖; 第4圖為傳統光學鏡頭與本揭示內容的光學鏡頭的結構示意圖;以及 第5圖為第二十一實施例至第二十四實施例的光學鏡片的穿透率與波長的關係圖。 In order to make the above and other objects, features, advantages and embodiments of the present disclosure more obvious and understandable, the accompanying drawings are described as follows: Figure 1 is a graph showing the relationship between transmittance and wavelength of the optical lens of the third embodiment; Figure 2 is a graph showing the relationship between transmittance and wavelength of the optical lens of the third embodiment; Figure 3A is an image quality diagram of the optical lens of the third embodiment; Figure 3B is a picture of the imaging quality of the optical lens of the comparative example; Figure 4 is a schematic structural diagram of a traditional optical lens and the optical lens disclosed in this disclosure; and Figure 5 is a graph showing the relationship between transmittance and wavelength of the optical lenses of the twenty-first to twenty-fourth embodiments.

Claims (31)

一種光學鏡頭,包含:至少三光學鏡片;其中,至少一該光學鏡片包含一紅外線濾除鍍膜,包含該紅外線濾除鍍膜的該光學鏡片由一塑膠材料所製成,該紅外線濾除鍍膜位於該光學鏡片的物側表面及像側表面的其中一表面,包含該紅外線濾除鍍膜的該光學鏡片表面為非球面,該紅外線濾除鍍膜具有至少二種不同的折射率;其中,至少一該光學鏡片包含一長波長吸收材料,且包含該長波長吸收材料的該光學鏡片由一塑膠材料所製成;其中,全視場主光線於包含該紅外線濾除鍍膜的該光學鏡片表面的入射角最大值為AICmax,該光學鏡頭於波長500nm-600nm的平均穿透率為T5060,該光學鏡頭於波長700nm-1000nm的平均穿透率為T70100,該紅外線濾除鍍膜的總膜厚為tTk,其滿足下列條件:AICmax
Figure 110137381-A0305-02-0096-83
40度;80%
Figure 110137381-A0305-02-0096-84
T5060;T70100
Figure 110137381-A0305-02-0096-85
10%;以及4000nm<tTk。
An optical lens, including: at least three optical lenses; wherein, at least one of the optical lenses includes an infrared filter coating, the optical lens including the infrared filter coating is made of a plastic material, and the infrared filter coating is located on the One of the object-side surface and the image-side surface of the optical lens, the surface of the optical lens including the infrared filter coating is an aspherical surface, and the infrared filter coating has at least two different refractive indexes; wherein, at least one of the optical lenses The lens includes a long-wavelength absorbing material, and the optical lens including the long-wavelength absorbing material is made of a plastic material; wherein, the incident angle of the full-field chief ray on the surface of the optical lens including the infrared filter coating is the largest The value is AICmax. The average transmittance of the optical lens at the wavelength of 500nm-600nm is T5060. The average transmittance of the optical lens at the wavelength of 700nm-1000nm is T70100. The total film thickness of the infrared filter coating is tTk, which satisfies The following conditions: AICmax
Figure 110137381-A0305-02-0096-83
40 degrees; 80%
Figure 110137381-A0305-02-0096-84
T5060; T70100
Figure 110137381-A0305-02-0096-85
10%; and 4000nm<tTk.
如請求項1所述之光學鏡頭,其中各該光學鏡片表面的鍍膜配置主因子為FC,且包含該紅外線濾除鍍膜的該光學鏡片的至少一表面滿足下列條件: 0.96
Figure 110137381-A0305-02-0097-96
FC。
The optical lens as described in claim 1, wherein the main factor of coating configuration on each optical lens surface is FC, and at least one surface of the optical lens including the infrared filter coating meets the following conditions: 0.96
Figure 110137381-A0305-02-0097-96
FC.
如請求項2所述之光學鏡頭,其中各該光學鏡片表面的鍍膜配置第一因子為Fc1,且包含該紅外線濾除鍍膜的該光學鏡片的至少一表面滿足下列條件:1.82
Figure 110137381-A0305-02-0097-97
Fc1。
The optical lens as described in claim 2, wherein the first factor of the coating configuration on each optical lens surface is Fc1, and at least one surface of the optical lens including the infrared filter coating meets the following conditions: 1.82
Figure 110137381-A0305-02-0097-97
Fc1.
如請求項3所述之光學鏡頭,其中各該光學鏡片表面的鍍膜配置第二因子為Fc2,且包含該紅外線濾除鍍膜的該光學鏡片的至少一表面滿足下列條件:4.98
Figure 110137381-A0305-02-0097-98
Fc2。
The optical lens as described in claim 3, wherein the second factor of the coating configuration on each optical lens surface is Fc2, and at least one surface of the optical lens including the infrared filter coating meets the following conditions: 4.98
Figure 110137381-A0305-02-0097-98
Fc2.
如請求項2所述之光學鏡頭,其中包含該紅外線濾除鍍膜的該光學鏡片表面於離軸處無反曲點或臨界點。 The optical lens according to claim 2, wherein the surface of the optical lens including the infrared filter coating has no inflection point or critical point off-axis. 如請求項2所述之光學鏡頭,其中該紅外線濾除鍍膜的總層數為tLs,其滿足下列條件:40<tLs
Figure 110137381-A0305-02-0097-99
80。
The optical lens as described in claim 2, wherein the total number of layers of the infrared filtering coating is tLs, which satisfies the following conditions: 40<tLs
Figure 110137381-A0305-02-0097-99
80.
如請求項2所述之光學鏡頭,其中該紅外線濾除鍍膜的總膜厚為tTk,其滿足下列條件:4500nm
Figure 110137381-A0305-02-0097-100
tTk。
The optical lens as described in claim 2, wherein the total film thickness of the infrared filtering coating is tTk, which meets the following conditions: 4500nm
Figure 110137381-A0305-02-0097-100
tTk.
如請求項2所述之光學鏡頭,其中包含該紅外線濾除鍍膜的該光學鏡片為一種補正鏡片。 The optical lens according to claim 2, wherein the optical lens including the infrared filter coating is a correction lens. 如請求項2所述之光學鏡頭,其中該光學鏡頭的全視角為FOV,其滿足下列條件:60度
Figure 110137381-A0305-02-0098-87
FOV
Figure 110137381-A0305-02-0098-88
200度。
The optical lens as described in claim 2, wherein the full viewing angle of the optical lens is FOV, which meets the following conditions: 60 degrees
Figure 110137381-A0305-02-0098-87
FOV
Figure 110137381-A0305-02-0098-88
200 degrees.
如請求項1所述之光學鏡頭,其中各該光學鏡片的吸收材料配置主因子為FA,且包含該長波長吸收材料的該光學鏡片滿足下列條件:2.31
Figure 110137381-A0305-02-0098-86
FA。
The optical lens as described in claim 1, wherein the main factor of the absorbing material configuration of each optical lens is FA, and the optical lens containing the long-wavelength absorbing material satisfies the following conditions: 2.31
Figure 110137381-A0305-02-0098-86
FA.
如請求項10所述之光學鏡頭,其中各該光學鏡片於全視場主光線光程比的平均值為CPavg,且包含該長波長吸收材料的該光學鏡片滿足下列條件:0.9
Figure 110137381-A0305-02-0098-89
CPavg
Figure 110137381-A0305-02-0098-90
1.1。
The optical lens as described in claim 10, wherein the average optical path ratio of the chief ray of each optical lens in the full field of view is CPavg, and the optical lens containing the long-wavelength absorbing material meets the following conditions: 0.9
Figure 110137381-A0305-02-0098-89
CPvg
Figure 110137381-A0305-02-0098-90
1.1.
如請求項10所述之光學鏡頭,其中該長波長吸收材料於50%穿透率的波長小於該紅外線濾除鍍膜於50%穿透率的波長,且該長波長吸收材料於50%穿透率的波長與該紅外線濾除鍍膜於50%穿透率的波長的差值為20nm以上。 The optical lens as described in claim 10, wherein the wavelength of the long-wavelength absorbing material at 50% transmittance is smaller than the wavelength of the infrared filter coating at 50% transmittance, and the long-wavelength absorbing material has a wavelength of 50% transmittance. The difference between the wavelength of high transmittance and the wavelength of 50% transmittance of the infrared filter coating is more than 20nm. 如請求項10所述之光學鏡頭,其中包含該 長波長吸收材料的該光學鏡片較包含該紅外線濾除鍍膜的該光學鏡片表面靠近物側。 The optical lens as described in claim 10, which includes the The optical lens made of long wavelength absorbing material is closer to the object side than the surface of the optical lens including the infrared filter coating. 如請求項10所述之光學鏡頭,其中該光學鏡頭在長波長區域且波長與穿透率呈負相關的趨勢中達到50%穿透率的波長為LWdT5,其滿足下列條件:600nm
Figure 110137381-A0305-02-0099-101
LWdT5
Figure 110137381-A0305-02-0099-102
700nm。
The optical lens as described in claim 10, wherein the wavelength at which the optical lens reaches 50% transmittance in the long wavelength region and the trend that wavelength and transmittance are negatively correlated is LWdT5, which meets the following conditions: 600nm
Figure 110137381-A0305-02-0099-101
wx5
Figure 110137381-A0305-02-0099-102
700nm.
如請求項10所述之光學鏡頭,其中至少一該光學鏡片包含一短波長吸收材料。 The optical lens of claim 10, wherein at least one of the optical lenses includes a short wavelength absorbing material. 一種取像裝置,包含:如請求項1所述之光學鏡頭;以及一電子感光元件,其設置於該光學鏡頭的一成像面。 An imaging device includes: the optical lens as described in claim 1; and an electronic photosensitive element, which is disposed on an imaging surface of the optical lens. 一種電子裝置,係為一行動裝置,該電子裝置包含:如請求項16所述之取像裝置。 An electronic device is a mobile device, and the electronic device includes: the imaging device described in claim 16. 如請求項1所述之光學鏡頭,更包含:一電子感光元件,其設置於該光學鏡頭的一成像面;以及一平板玻璃,其設置於該電子感光元件的一表面。 The optical lens according to claim 1 further includes: an electronic photosensitive element, which is arranged on an imaging surface of the optical lens; and a flat glass, which is arranged on a surface of the electronic photosensitive element. 如請求項18所述之光學鏡頭,其中該光學鏡頭於最大像高視場處的主光線入射該平板玻璃的一表面的角度為CRAg,其滿足下列條件:40度
Figure 110137381-A0305-02-0100-92
CRAg。
The optical lens as described in claim 18, wherein the angle at which the chief ray of the optical lens at the maximum image height field of view is incident on a surface of the flat glass is CRAg, which satisfies the following conditions: 40 degrees
Figure 110137381-A0305-02-0100-92
CRAgs.
如請求項18所述之光學鏡頭,其中該平板玻璃的物側表面具有一長波長吸收材料。 The optical lens according to claim 18, wherein the object-side surface of the flat glass has a long wavelength absorbing material. 如請求項18所述之光學鏡頭,其中該平板玻璃的至少一表面具有一抗反射膜層,該抗反射膜層具有一次波長微結構。 The optical lens of claim 18, wherein at least one surface of the flat glass has an anti-reflective film layer, and the anti-reflective film layer has a primary wavelength microstructure. 如請求項18所述之光學鏡頭,其中該平板玻璃的像側表面具有一長波長吸收材料。 The optical lens according to claim 18, wherein the image side surface of the flat glass has a long wavelength absorbing material. 一種電子裝置,係為一行動裝置,該電子裝置包含:如請求項18所述之光學鏡頭。 An electronic device is a mobile device, and the electronic device includes: an optical lens as described in claim 18. 如請求項1所述之光學鏡頭,其中該光學鏡頭中包含該長波長吸收材料的該光學鏡片在波長1050nm的穿透率小於在波長500nm的穿透率,且該光學鏡頭更包含:一電子感光元件,其設置於該光學鏡頭的一成像面。 The optical lens as described in claim 1, wherein the transmittance of the optical lens including the long-wavelength absorbing material at a wavelength of 1050 nm is less than the transmittance at a wavelength of 500 nm, and the optical lens further includes: an electron A photosensitive element is arranged on an imaging plane of the optical lens. 一種電子裝置,係為一行動裝置,該電子裝置包含:如請求項24所述之光學鏡頭。 An electronic device is a mobile device, and the electronic device includes: an optical lens as described in claim 24. 一種光學鏡頭,包含:至少一光學鏡片;以及至少一光學元件;其中,至少一該光學鏡片包含一紅外線濾除鍍膜,包含該紅外線濾除鍍膜的該光學鏡片由一塑膠材料所製成,該紅外線濾除鍍膜位於該光學鏡片的物側表面及像側表面的其中一表面,包含該紅外線濾除鍍膜的該光學鏡片表面為非球面,該紅外線濾除鍍膜具有至少二種不同的折射率;其中,該光學元件位於該光學鏡片的像側,至少一該光學元件包含一長波長吸收材料;其中,全視場主光線於包含該紅外線濾除鍍膜的該光學鏡片表面的入射角最大值為AICmax,該光學鏡頭於波長500nm-600nm的平均穿透率為T5060,該光學鏡頭於波長700nm-1000nm的平均穿透率為T70100,該紅外線濾除鍍膜的總膜厚為tTk,其滿足下列條件:AICmax
Figure 110137381-A0305-02-0101-93
40度;80%
Figure 110137381-A0305-02-0101-95
T5060;T70100
Figure 110137381-A0305-02-0101-94
10%;以及4000nm<tTk。
An optical lens, including: at least one optical lens; and at least one optical element; wherein, at least one of the optical lenses includes an infrared filter coating, and the optical lens including the infrared filter coating is made of a plastic material, and the The infrared filter coating is located on one of the object-side surface and the image-side surface of the optical lens, the surface of the optical lens including the infrared filter coating is aspherical, and the infrared filter coating has at least two different refractive indexes; Wherein, the optical element is located on the image side of the optical lens, and at least one of the optical elements includes a long-wavelength absorbing material; wherein the maximum incident angle of the full-field chief ray on the surface of the optical lens including the infrared filter coating is AICmax, the average transmittance of the optical lens at the wavelength of 500nm-600nm is T5060, the average transmittance of the optical lens at the wavelength of 700nm-1000nm is T70100, the total film thickness of the infrared filter coating is tTk, which meets the following conditions :AICmax
Figure 110137381-A0305-02-0101-93
40 degrees; 80%
Figure 110137381-A0305-02-0101-95
T5060; T70100
Figure 110137381-A0305-02-0101-94
10%; and 4000nm<tTk.
如請求項26所述之光學鏡頭,其中包含該長波長吸收材料的該光學元件為一微透鏡,且該微透鏡的表面具有該長波長吸收材料。 The optical lens of claim 26, wherein the optical element including the long-wavelength absorbing material is a microlens, and the surface of the microlens has the long-wavelength absorbing material. 如請求項26所述之光學鏡頭,其中包含該長波長吸收材料的該光學元件為一彩色濾光片,且該彩色濾光片具有該長波長吸收材料。 The optical lens of claim 26, wherein the optical element including the long-wavelength absorbing material is a color filter, and the color filter has the long-wavelength absorbing material. 如請求項26所述之光學鏡頭,其中至少一該光學鏡片具有該長波長吸收材料。 The optical lens according to claim 26, wherein at least one of the optical lenses has the long wavelength absorbing material. 如請求項26所述之光學鏡頭,其中包含該長波長吸收材料的該光學元件為一平板玻璃,且該平板玻璃的至少一表面具有該長波長吸收材料。 The optical lens of claim 26, wherein the optical element containing the long-wavelength absorbing material is a flat glass, and at least one surface of the flat glass has the long-wavelength absorbing material. 一種電子裝置,係為一行動裝置,該電子裝置包含:如請求項26所述之光學鏡頭。 An electronic device is a mobile device, and the electronic device includes: an optical lens as described in claim 26.
TW110137381A 2020-11-25 2021-10-07 Optical lens assembly, imaging apparatus and electronic device TWI817205B (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
CN202111402486.8A CN114545592A (en) 2020-11-25 2021-11-24 Optical lens, image capturing device and electronic device
BR102021023655-8A BR102021023655A2 (en) 2020-11-25 2021-11-24 SET OF OPTICAL LENSES, IMAGE FORMATION DEVICE AND ELECTRONIC DEVICE
EP21210263.6A EP4006595A1 (en) 2020-11-25 2021-11-24 Optical lens assembly, imaging apparatus and electronic device
US17/534,564 US20220163710A1 (en) 2020-11-25 2021-11-24 Optical lens assembly, imaging apparatus and electronic device

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US202063118030P 2020-11-25 2020-11-25
US63/118,030 2020-11-25

Publications (2)

Publication Number Publication Date
TW202235951A TW202235951A (en) 2022-09-16
TWI817205B true TWI817205B (en) 2023-10-01

Family

ID=84957184

Family Applications (2)

Application Number Title Priority Date Filing Date
TW112133708A TW202405503A (en) 2020-11-25 2021-10-07 Optical lens assembly, imaging apparatus and electronic device
TW110137381A TWI817205B (en) 2020-11-25 2021-10-07 Optical lens assembly, imaging apparatus and electronic device

Family Applications Before (1)

Application Number Title Priority Date Filing Date
TW112133708A TW202405503A (en) 2020-11-25 2021-10-07 Optical lens assembly, imaging apparatus and electronic device

Country Status (1)

Country Link
TW (2) TW202405503A (en)

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2010143458A1 (en) * 2009-06-10 2010-12-16 コニカミノルタオプト株式会社 Image pickup lens and image pickup device
CN108490585A (en) * 2018-05-22 2018-09-04 江西联创电子有限公司 Glass moulds hybrid lens
JP6414083B2 (en) * 2014-01-24 2018-10-31 コニカミノルタ株式会社 Imaging optical system, imaging optical device, and digital device
TW201944116A (en) * 2018-04-11 2019-11-16 大立光電股份有限公司 Optical image lens assembly, imaging apparatus and electronic device
WO2020095513A1 (en) * 2018-11-06 2020-05-14 富士フイルム株式会社 Imaging lens and imaging device
TW202022414A (en) * 2018-09-12 2020-06-16 日商Jsr股份有限公司 Optical filter and use thereof
CN111812762A (en) * 2020-07-16 2020-10-23 杭州美迪凯光电科技股份有限公司 Infrared cut-off filter for improving glare ghost phenomenon and preparation method thereof

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2010143458A1 (en) * 2009-06-10 2010-12-16 コニカミノルタオプト株式会社 Image pickup lens and image pickup device
JP6414083B2 (en) * 2014-01-24 2018-10-31 コニカミノルタ株式会社 Imaging optical system, imaging optical device, and digital device
TW201944116A (en) * 2018-04-11 2019-11-16 大立光電股份有限公司 Optical image lens assembly, imaging apparatus and electronic device
CN108490585A (en) * 2018-05-22 2018-09-04 江西联创电子有限公司 Glass moulds hybrid lens
TW202022414A (en) * 2018-09-12 2020-06-16 日商Jsr股份有限公司 Optical filter and use thereof
WO2020095513A1 (en) * 2018-11-06 2020-05-14 富士フイルム株式会社 Imaging lens and imaging device
CN111812762A (en) * 2020-07-16 2020-10-23 杭州美迪凯光电科技股份有限公司 Infrared cut-off filter for improving glare ghost phenomenon and preparation method thereof

Also Published As

Publication number Publication date
TW202405503A (en) 2024-02-01
TW202235951A (en) 2022-09-16

Similar Documents

Publication Publication Date Title
TWI614518B (en) Imaging lens assembly and electronic device
KR20160130987A (en) Near-infrared cut filter and solid-state imaging device
CN104204873A (en) Near infrared cut-off filter
CN110361831B (en) Optical image lens, image capturing device and electronic device
TWI598620B (en) Optical lens
US20240061150A1 (en) Optical lens assembly, imaging apparatus and electronic device
US9851531B2 (en) Optical lens assembly and imaging lens with infrared ray filtering
TWI817205B (en) Optical lens assembly, imaging apparatus and electronic device
CN112764135A (en) Narrow-band antireflection film with extremely low residual reflection
TWI782704B (en) Optical lens assembly, imaging apparatus and electronic device
CN216526487U (en) Optical lens, image capturing device and electronic device
TW201812382A (en) Imaging lens assembly and electronic device
TWI769862B (en) Optical lens assembly, imaging apparatus and electronic device
KR20010003000A (en) Image sensing module
KR20160123671A (en) Multi-layered lens and method for manufacturing the same
US20220163710A1 (en) Optical lens assembly, imaging apparatus and electronic device
US20220035128A1 (en) Optical lens assembly, imaging apparatus and electronic device
US11703660B2 (en) Optical imaging lens
US20220196881A1 (en) Optical lens assembly, imaging apparatus and electronic device
TWI843222B (en) Optical lens assembly, imaging apparatus and electronic device