CN116819728A - projection lens - Google Patents
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- CN116819728A CN116819728A CN202310803357.2A CN202310803357A CN116819728A CN 116819728 A CN116819728 A CN 116819728A CN 202310803357 A CN202310803357 A CN 202310803357A CN 116819728 A CN116819728 A CN 116819728A
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- 230000003287 optical effect Effects 0.000 claims abstract description 83
- 238000003384 imaging method Methods 0.000 claims abstract description 40
- 238000002834 transmittance Methods 0.000 claims description 13
- 238000000926 separation method Methods 0.000 claims description 4
- 230000009286 beneficial effect Effects 0.000 description 13
- 239000000463 material Substances 0.000 description 9
- 230000004075 alteration Effects 0.000 description 7
- 230000014509 gene expression Effects 0.000 description 7
- 230000035945 sensitivity Effects 0.000 description 6
- 238000004904 shortening Methods 0.000 description 5
- 230000002349 favourable effect Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000009826 distribution Methods 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000000007 visual effect Effects 0.000 description 2
- MKYBYDHXWVHEJW-UHFFFAOYSA-N N-[1-oxo-1-(2,4,6,7-tetrahydrotriazolo[4,5-c]pyridin-5-yl)propan-2-yl]-2-[[3-(trifluoromethoxy)phenyl]methylamino]pyrimidine-5-carboxamide Chemical compound O=C(C(C)NC(=O)C=1C=NC(=NC=1)NCC1=CC(=CC=C1)OC(F)(F)F)N1CC2=C(CC1)NN=N2 MKYBYDHXWVHEJW-UHFFFAOYSA-N 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000018109 developmental process Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
Classifications
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/14—Details
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
- G02B13/002—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
- G02B13/004—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having four lenses
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Abstract
The application discloses a projection lens, which sequentially comprises the following components from an image source side to an imaging side along an optical axis: a first lens having positive optical power, the image source side surface of which is convex; a second lens having negative optical power, the image source side surface and the image side surface of which are both concave; a third lens having positive or negative optical power; and a fourth lens having positive optical power, the imaging side surface of which is convex; the total effective focal length f of the projection lens and the effective focal length f4 of the fourth lens meet the conditions that f/f4 is smaller than 1.5 and smaller than 2.5.
Description
Filing and applying for separate cases
The application relates to a division application of Chinese application patent application with the name of 'projection lens' and the application number of 201711348942.9, which is submitted in 2017, 12 and 15 days.
Technical Field
The present application relates to a projection lens, and more particularly, to a projection lens including four lenses.
Background
In recent years, with the continuous progress of technology, interactive devices are gradually rising, and the application range of projection lenses is also wider and wider. Today, chip technology and intelligent algorithms are rapidly developed, and three-dimensional images with object position and depth information can be calculated by projecting images to space objects by using an optical projection lens and receiving the image signals. The specific method comprises the following steps: projecting light emitted by an infrared Laser Diode (LD) or a Vertical Cavity Surface Emitting Laser (VCSEL) towards a target object by using an optical projection lens; the projected beam after passing through an optical diffraction element (DOE) achieves a redistribution of the projected image on the target object; and receiving the image projected onto the object by using the imaging lens, and calculating a three-dimensional image containing the position and depth information of the projected object. The three-dimensional image with depth information can be further used for various depth application developments such as biological recognition.
In general, a conventional projection lens eliminates various aberrations and improves resolution by increasing the number of lenses. However, increasing the number of lenses results in an increase in the total optical length of the projection lens, which is disadvantageous in downsizing the lens. In addition, the general large-field angle projection lens has many problems of large distortion, poor imaging quality and the like, and cannot be matched with an optical diffraction element (DOE) to accurately realize the redistribution of the projection beam on the target object.
Disclosure of Invention
The present application provides a projection lens applicable to a portable electronic product, which at least solves or partially solves at least one of the above-mentioned drawbacks of the prior art.
The present application provides a projection lens, which may include, in order from an image source side to an image forming side along an optical axis: a first lens having positive optical power, the image source side surface of which is convex; a second lens having negative optical power, both of which may be concave on the image source side surface and the image side surface; a third lens having positive or negative optical power; a fourth lens having positive optical power, an imaging side surface of which may be convex; the number of the lenses with the focal power of the projection lens is four, and the total effective focal length f of the projection lens and the effective focal length f4 of the fourth lens can meet the conditions that 1.5 is smaller than f/f4 is smaller than 2.5.
In one embodiment, the total effective focal length f of the projection lens and the effective focal length f1 of the first lens may satisfy 2.0 < f/f1 < 3.5.
In one embodiment, the total effective focal length f of the projection lens and the effective focal length f2 of the second lens can satisfy f/f 2. Ltoreq.4.0.
In one embodiment, the effective focal length f3 of the third lens and the total effective focal length f of the projection lens may satisfy 1.0 < f3/f < 5.5.
In one embodiment, the projection lens has a light transmittance of greater than 85% in the light wave band of 800nm to 1000 nm.
In one embodiment, the distance TTL between the image source surface of the projection lens and the imaging side surface of the fourth lens on the optical axis and the total effective focal length f of the projection lens can satisfy TTL/f < 1.0.
In one embodiment, the maximum effective half-caliber DT42 of the imaging side surface of the fourth lens and the maximum effective half-caliber DT41 of the image source side surface of the fourth lens may satisfy 1.0 < DT42/DT41 < 1.4.
In one embodiment, the separation distance T12 of the first lens and the second lens on the optical axis and the separation distance T23 of the second lens and the third lens on the optical axis can satisfy 0.8 < T12/T23 < 2.2.
In one embodiment, the center thickness CT4 of the fourth lens element on the optical axis and the center thickness CT2 of the second lens element on the optical axis may satisfy 1.5 < CT4/CT2 < 3.0.
In one embodiment, the radius of curvature R8 of the imaging side surface of the fourth lens and the radius of curvature R1 of the image source side surface of the first lens may satisfy-1.5.ltoreq.R8/R1.ltoreq.1.0.
In one embodiment, the radius of curvature R4 of the image side surface of the second lens and the radius of curvature R3 of the image source side surface of the second lens may satisfy-2.4 < R4/R3 < -0.8.
The application adopts a plurality of (for example, four) lenses, and the projection lens has at least one beneficial effects of large aperture, miniaturization, high imaging quality and the like by reasonably distributing the focal power, the surface type, the center thickness of each lens, the axial spacing between each lens and the like.
Drawings
Other features, objects and advantages of the present application will become more apparent from the following detailed description of non-limiting embodiments, taken in conjunction with the accompanying drawings. In the drawings:
fig. 1 shows a schematic configuration of a projection lens according to embodiment 1 of the present application;
fig. 2 shows a distortion curve of the projection lens of embodiment 1;
fig. 3 is a schematic view showing the structure of a projection lens according to embodiment 2 of the present application;
fig. 4 shows a distortion curve of the projection lens of embodiment 2;
fig. 5 shows a schematic structural view of a projection lens according to embodiment 3 of the present application;
fig. 6 shows a distortion curve of the projection lens of embodiment 3;
fig. 7 is a schematic view showing the structure of a projection lens according to embodiment 4 of the present application;
fig. 8 shows a distortion curve of the projection lens of embodiment 4;
fig. 9 is a schematic view showing the structure of a projection lens according to embodiment 5 of the present application;
fig. 10 shows a distortion curve of the projection lens of embodiment 5;
fig. 11 is a schematic view showing the structure of a projection lens according to embodiment 6 of the present application;
fig. 12 shows a distortion curve of the projection lens of example 6;
fig. 13 is a schematic view showing the structure of a projection lens according to embodiment 7 of the present application;
fig. 14 shows a distortion curve of the projection lens of embodiment 7;
fig. 15 shows a schematic structural view of a projection lens according to embodiment 8 of the present application;
fig. 16 shows a distortion curve of the projection lens of embodiment 8;
fig. 17 is a schematic view showing the structure of a projection lens according to embodiment 9 of the present application;
fig. 18 shows a distortion curve of the projection lens of embodiment 9.
Detailed Description
For a better understanding of the application, various aspects of the application will be described in more detail with reference to the accompanying drawings. It should be understood that the detailed description is merely illustrative of exemplary embodiments of the application and is not intended to limit the scope of the application in any way. Like reference numerals refer to like elements throughout the specification. The expression "and/or" includes any and all combinations of one or more of the associated listed items.
It should be noted that in this specification, the expressions first, second, etc. are only used to distinguish one feature from another feature, and do not represent any limitation of the feature. Accordingly, a first lens discussed below may also be referred to as a second lens, and a second lens may also be referred to as a first lens, without departing from the teachings of the present application.
In the drawings, the thickness, size, and shape of the lenses have been slightly exaggerated for convenience of explanation. In particular, the spherical or aspherical shape shown in the drawings is shown by way of example. That is, the shape of the spherical or aspherical surface is not limited to the shape of the spherical or aspherical surface shown in the drawings. The figures are merely examples and are not drawn to scale.
Herein, the paraxial region refers to a region near the optical axis. If the lens surface is convex and the convex position is not defined, then the lens surface is convex at least in the paraxial region; if the lens surface is concave and the concave position is not defined, it means that the lens surface is concave at least in the paraxial region. The surface of each lens closest to the image source side is referred to as an image source side surface, and the surface of each lens closest to the image side is referred to as an image side surface.
It will be further understood that the terms "comprises," "comprising," "includes," "including," "having," "containing," and/or "including," when used in this specification, specify the presence of stated features, elements, and/or components, but do not preclude the presence or addition of one or more other features, elements, components, and/or groups thereof. Furthermore, when a statement such as "at least one of the following" appears after a list of features that are listed, the entire listed feature is modified instead of modifying a separate element in the list. Furthermore, when describing embodiments of the application, use of "may" means "one or more embodiments of the application. Also, the term "exemplary" is intended to refer to an example or illustration.
Unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the relevant art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
It should be noted that, without conflict, the embodiments of the present application and features of the embodiments may be combined with each other. The application will be described in detail below with reference to the drawings in connection with embodiments.
The features, principles, and other aspects of the present application are described in detail below.
The projection lens according to the exemplary embodiment of the present application may include, for example, four lenses having optical power, i.e., a first lens, a second lens, a third lens, and a fourth lens. The four lenses are arranged in sequence along the optical axis from the image source side to the image side.
In an exemplary embodiment, the first lens may have positive optical power; the second lens may have negative power, an image source side surface thereof may be concave, and an image forming side surface thereof may be concave; the third lens has positive optical power or negative optical power; the fourth lens may have positive optical power, and an imaging side surface thereof may be convex. The first lens with positive focal power is beneficial to realizing telecentricity of an image source side of a projection system, improving the light incoming quantity of an off-axis vision field of the projection system and increasing the resolution, brightness and uniformity of a projection image; the second lens with negative focal power has a concave image source side surface and a concave image side surface, which is beneficial to the main surface of the image source side to be far away from the image source, thereby shortening the total optical length TTL of the projection system and realizing the miniaturization of the lens; the third lens with focal power can effectively adjust the incident angle of off-axis visual field rays and correct off-axis visual field aberration; the fourth lens with positive focal power is beneficial to shortening the total optical length TTL of the projection system, and the convex surface of the imaging side of the fourth lens is beneficial to reducing the spherical aberration of the projection system and improving the imaging quality of the projection system.
In an exemplary embodiment, the image source side surface of the first lens may be convex.
In an exemplary embodiment, the third lens may have positive power, an image source side surface thereof may be concave, and an image forming side surface thereof may be convex.
In an exemplary embodiment, the image source side surface of the fourth lens may be concave.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression f/f2+.4.0, where f is the total effective focal length of the projection lens and f2 is the effective focal length of the second lens. More specifically, f and f2 may further satisfy-10.0.ltoreq.fF2.ltoreq.4.0, for example, -9.80.ltoreq.f2.ltoreq.5.41. Satisfying the condition f/f2 is less than or equal to-4.0, which is beneficial to achieving better balance between improving the imaging quality of the projection system and realizing the miniaturization of the projection system.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression 2.0 < f/f1 < 3.5, where f is the total effective focal length of the projection lens and f1 is the effective focal length of the first lens. More specifically, f and f1 may further satisfy 2.30 < f/f1 < 3.40, for example, 2.41. Ltoreq.f/f 1. Ltoreq.3.33. The condition that f/f1 is less than 2.0 and less than 3.5 is satisfied, the telecentricity of the image source side of the projection system is facilitated, the total optical length TTL of the projection system is shortened, and better balance is achieved between shortening the total optical length TTL of the projection system and improving the imaging quality of the projection system.
In an exemplary embodiment, the projection lens of the present application has a light transmittance of greater than 85% in the light wavelength band of about 800nm to about 1000 nm. Such an arrangement is advantageous in improving the transmittance of near infrared light through the projection lens to obtain a near infrared projection image with higher brightness.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression 1.0 < f3/f < 5.5, where f3 is an effective focal length of the third lens and f is a total effective focal length of the projection lens. More specifically, f3 and f may further satisfy 1.32.ltoreq.f3/f.ltoreq.5.39. Satisfying the condition 1.0 < f3/f < 5.5, being beneficial to adjusting the optical power distribution and avoiding the increase of tolerance sensitivity of the projection system caused by excessive concentration of optical power; meanwhile, when one or all of the second lens and the fourth lens is a glass lens, satisfying the condition that f3/f is smaller than 1.0 and smaller than 5.5 is beneficial to keeping the stability of the image plane under the condition that the temperature is changed, thereby being beneficial to improving the temperature characteristic of the projection system.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression-1.5R 8/R1, where R8 is a radius of curvature of an imaging side surface of the fourth lens and R1 is a radius of curvature of an image source side surface of the first lens. More specifically, R8 and R1 may further satisfy-1.35.ltoreq.R8/R1.ltoreq.1.00. Satisfying the condition-1.5 is less than or equal to R8/R1 is less than or equal to-1.0, which is beneficial to eliminating distortion and aberration of the projection system.
In an exemplary embodiment, the projection lens of the present application may satisfy the condition of 1.5 < f/f4 < 2.5, where f is the total effective focal length of the projection lens and f4 is the effective focal length of the fourth lens. More specifically, f and f4 may further satisfy 1.63.ltoreq.f4.ltoreq.2.39. The condition that f/f4 is less than 2.5 and 1.5 is satisfied, so that the tolerance sensitivity of the fourth lens is reduced; meanwhile, when the fourth lens is a glass lens, the temperature sensitivity of the projection system is reduced, so that higher projection quality can be realized in a larger temperature range.
In an exemplary embodiment, the projection lens of the present application may satisfy the condition-2.4 < R4/R3 < -0.8, where R4 is a radius of curvature of an imaging side surface of the second lens and R3 is a radius of curvature of an image source side surface of the second lens. More specifically, R4 and R3 may further satisfy-2.25 < R4/R3 < -0.85, for example, -2.19.ltoreq.R 4/R3.ltoreq.0.96. Satisfies the condition that R4/R3 is less than-2.4 and less than-0.8, is favorable for reducing the incidence angle and the emergent angle of each view field at the second lens so as to reduce the tolerance sensitivity of the second lens and further improve the production yield of the projection lens.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression 0.8 < T12/T23 < 2.2, where T12 is a distance between the first lens and the second lens on the optical axis, and T23 is a distance between the second lens and the third lens on the optical axis. More specifically, T12 and T23 may further satisfy 0.88.ltoreq.T12/T23.ltoreq.2.11. The method meets the condition that T12/T23 is smaller than 2.2 and is favorable for reasonably distributing the interval distance between the lenses and adjusting the light path distribution, thereby reducing the tolerance sensitivity of the projection system; meanwhile, the lens assembly is facilitated, and the production yield of the projection system is improved.
In an exemplary embodiment, the projection lens of the present application may satisfy the condition of 1.5 < CT4/CT2 < 3.0, wherein CT4 is a center thickness of the fourth lens element on the optical axis, and CT2 is a center thickness of the second lens element on the optical axis. More specifically, CT4 and CT2 may further satisfy 1.59.ltoreq.CT4/CT 2.ltoreq.2.82. The condition that CT4/CT2 is smaller than 3.0 and 1.5 is satisfied is favorable for obtaining better balance between shortening the total optical length TTL of the projection system and improving the processing and manufacturing manufacturability of the second lens and the fourth lens.
In an exemplary embodiment, the projection lens of the present application may satisfy the conditional expression 1.0 < DT42/DT41 < 1.4, wherein DT42 is the maximum effective half-caliber of the image side surface of the fourth lens, and DT41 is the maximum effective half-caliber of the image source side surface of the fourth lens. More specifically, DT42 and DT41 may further satisfy 1.05 < DT42/DT41 < 1.25, e.g., 1.13. Ltoreq.DT 42/DT 41. Ltoreq.1.19. Satisfies the condition that DT42/DT41 is smaller than 1.4 and is beneficial to shortening the total optical length TTL of the projection system to realize miniaturization; at the same time, it is advantageous to better balance the tolerance sensitivity of the projection system.
In an exemplary embodiment, the projection lens of the present application may satisfy the condition that TTL/f < 1.0, where TTL is an on-axis distance from an image source surface to an imaging side surface of the fourth lens, and f is a total effective focal length of the projection lens. More specifically, TTL and f can further satisfy 0.60 < TTL/f < 0.90, e.g., 0.67. Ltoreq.TTL/f. Ltoreq.0.82. The ratio of TTL to f is reasonably controlled, which is beneficial to keeping the miniaturization of the projection lens.
In an exemplary embodiment, the projection lens may further include at least one diaphragm to improve the imaging quality of the lens. For example, a diaphragm may be provided between the fourth lens and the imaging side as needed.
Alternatively, the projection lens may further include other well-known optical projection elements, such as a prism, a field lens, and the like. Alternatively, the projection lens described above can be used in conjunction with a diffractive element (DOE).
The projection lens according to the above embodiment of the present application may employ, for example, four lenses, and may have the beneficial effects of large aperture, miniaturization, high imaging quality, etc. by reasonably distributing the focal power of each lens, the surface, the center thickness of each lens, the on-axis spacing between each lens, etc.
In an embodiment of the present application, at least one of the mirrors of each lens is an aspherical mirror. The aspherical lens is characterized in that: the curvature varies continuously from the center of the lens to the periphery of the lens. Unlike a spherical lens having a constant curvature from the center of the lens to the periphery of the lens, an aspherical lens has a better radius of curvature characteristic, and has advantages of improving distortion aberration and improving astigmatic aberration. By adopting the aspherical lens, aberration occurring at the time of imaging can be eliminated as much as possible, thereby improving imaging quality.
However, those skilled in the art will appreciate that the various results and advantages described in this specification can be obtained by varying the number of lenses making up a projection lens without departing from the technical solution claimed in the present application. For example, although four lenses are described as an example in the embodiment, the projection lens is not limited to include four lenses. The projection lens may also include other numbers of lenses, if desired.
Specific examples of projection lenses applicable to the above embodiments are further described below with reference to the accompanying drawings.
Example 1
A projection lens according to embodiment 1 of the present application is described below with reference to fig. 1 to 2. Fig. 1 shows a schematic configuration of a projection lens according to embodiment 1 of the present application.
As shown in fig. 1, a projection lens according to an exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 1 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 1, wherein the radii of curvature and thicknesses are each in millimeters (mm).
TABLE 1
As can be seen from table 1, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical. In the present embodiment, the surface shape x of each aspherical lens can be defined by, but not limited to, the following aspherical formula:
wherein x is the distance vector height from the vertex of the aspheric surface when the aspheric surface is at the position with the height h along the optical axis direction; c is an aspheric ballParaxial curvature of the face, c=1/R (i.e., paraxial curvature c is the inverse of radius of curvature R in table 1 above); k is the conic coefficient (given in table 1); ai is the correction coefficient of the aspherical i-th order. Table 2 below shows the higher order coefficients A that can be used for each of the aspherical mirror surfaces S1-S8 in example 1 4 、A 6 、A 8 、A 10 、A 12 、A 14 And A 16 。
TABLE 2
Table 3 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 1.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.50 | 1.45 | -0.59 | 5.96 | 2.31 |
TABLE 3 Table 3
The projection lens in embodiment 1 satisfies:
ff2= -7.63, where f is the total effective focal length of the projection lens and f2 is the effective focal length of the second lens E2;
ff1=3.10, where f is the total effective focal length of the projection lens and f1 is the effective focal length of the first lens E1;
f3/f=1.32, where f3 is the effective focal length of the third lens E3, and f is the total effective focal length of the projection lens;
r8/r1= -1.35, where R8 is the radius of curvature of the imaging side surface S8 of the fourth lens E4, and R1 is the radius of curvature of the image source side surface S1 of the first lens E1;
ff4=1.95, where f is the total effective focal length of the projection lens and f4 is the effective focal length of the fourth lens E4;
r4/r3= -1.25, where R4 is the radius of curvature of the imaging side surface S4 of the second lens E2, and R3 is the radius of curvature of the image source side surface S3 of the second lens E2;
t12/t23=0.91, where T12 is the distance between the first lens E1 and the second lens E2 on the optical axis, and T23 is the distance between the second lens E2 and the third lens E3 on the optical axis;
CT 4/ct2=2.14, wherein CT4 is the center thickness of the fourth lens element E4 on the optical axis, and CT2 is the center thickness of the second lens element E2 on the optical axis;
DT42/DT41 = 1.19, where DT42 is the maximum effective half-caliber of the imaging side surface S8 of the fourth lens E4 and DT41 is the maximum effective half-caliber of the image source side surface S7 of the fourth lens E4;
TTL/f=0.73, where TTL is the on-axis distance from the image source surface OBJ to the image side surface S8 of the fourth lens E4, and f is the total effective focal length of the projection lens.
Fig. 2 shows a distortion curve of the projection lens of embodiment 1, which represents distortion magnitude values at different angles of view. As can be seen from fig. 2, the projection lens according to embodiment 1 can achieve good imaging quality.
Example 2
A projection lens according to embodiment 2 of the present application is described below with reference to fig. 3 to 4. In this embodiment and the following embodiments, descriptions of portions similar to embodiment 1 will be omitted for brevity. Fig. 3 shows a schematic structure of a projection lens according to embodiment 2 of the present application.
As shown in fig. 3, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 4 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 2, wherein the radii of curvature and thicknesses are each in millimeters (mm).
TABLE 4 Table 4
As is clear from table 4, in embodiment 2, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 5 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 2, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 8.0505E-01 | -4.6397E+00 | 2.2410E+01 | -5.7501E+01 | 6.0022E+01 | 1.3993E+01 | -5.6479E+01 |
| S2 | 4.0667E-01 | -5.2418E+00 | 4.3291E+01 | -2.4489E+02 | 7.6653E+02 | -1.2375E+03 | 8.0725E+02 |
| S3 | -6.2410E-02 | -3.5615E+01 | 8.5155E+02 | -1.2697E+04 | 1.0081E+05 | -3.6719E+05 | 4.9109E+05 |
| S4 | 5.6913E-01 | -2.4765E+01 | 9.0322E+02 | -1.9548E+04 | 2.3017E+05 | -1.3869E+06 | 3.4008E+06 |
| S5 | -1.1151E-01 | 3.6489E+00 | -6.7726E+01 | 6.7578E+02 | -3.5458E+03 | 9.2598E+03 | -9.2559E+03 |
| S6 | -1.3269E-01 | 5.7543E+00 | -7.3179E+01 | 4.1421E+02 | -1.1769E+03 | 1.5811E+03 | -7.5435E+02 |
| S7 | -2.3580E-02 | 2.2522E+00 | -2.7978E+01 | 1.4827E+02 | -3.9351E+02 | 5.0908E+02 | -2.5340E+02 |
| S8 | 1.3259E-02 | -1.8760E-01 | 1.5473E+00 | -6.4581E+00 | 1.4063E+01 | -1.5225E+01 | 6.4491E+00 |
TABLE 5
Table 6 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 2.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.50 | 1.50 | -0.67 | 6.59 | 2.76 |
TABLE 6
Fig. 4 shows a distortion curve of the projection lens of embodiment 2, which represents distortion magnitude values at different angles of view. As can be seen from fig. 4, the projection lens according to embodiment 2 can achieve good imaging quality.
Example 3
A projection lens according to embodiment 3 of the present application is described below with reference to fig. 5 to 6. Fig. 5 shows a schematic structural view of a projection lens according to embodiment 3 of the present application.
As shown in fig. 5, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 7 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 3, wherein the radii of curvature and thicknesses are each in millimeters (mm).
TABLE 7
As is clear from table 7, in embodiment 3, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 8 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 3, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
TABLE 8
Table 9 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 3.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.49 | 1.54 | -0.65 | 6.18 | 2.31 |
TABLE 9
Fig. 6 shows a distortion curve of the projection lens of embodiment 3, which represents distortion magnitude values at different angles of view. As can be seen from fig. 6, the projection lens according to embodiment 3 can achieve good imaging quality.
Example 4
A projection lens according to embodiment 4 of the present application is described below with reference to fig. 7 to 8. Fig. 7 shows a schematic configuration of a projection lens according to embodiment 4 of the present application.
As shown in fig. 7, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 10 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 4, in which the units of the radii of curvature and thicknesses are millimeters (mm).
Table 10
As is clear from table 10, in embodiment 4, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 11 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 4, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 5.9190E-01 | -9.5682E-01 | 1.5246E+00 | 1.4408E+00 | -1.8549E+00 | 0.0000E+00 | 0.0000E+00 |
| S2 | 6.7315E-01 | 5.7754E+00 | -6.1253E+01 | 4.1049E+02 | -1.2852E+03 | 1.8107E+03 | -9.4551E+02 |
| S3 | -6.1430E-02 | -1.4837E+01 | 5.6080E+02 | -1.2459E+04 | 1.4614E+05 | -8.9912E+05 | 2.2470E+06 |
| S4 | 1.7728E+00 | -7.6106E+00 | 9.0300E+01 | -1.0970E+03 | 8.7712E+03 | -3.8775E+04 | 7.1022E+04 |
| S5 | -3.5555E-01 | 8.0956E-01 | 8.4511E+00 | -7.6330E+01 | 3.0721E+02 | -5.9416E+02 | 4.4787E+02 |
| S6 | 1.4957E-01 | -7.1230E-02 | 2.7423E+00 | -1.2480E+01 | 3.4176E+01 | -4.7353E+01 | 2.8473E+01 |
TABLE 11
Table 12 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 4.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.49 | 1.86 | -0.68 | 7.74 | 1.92 |
Table 12
Fig. 8 shows a distortion curve of the projection lens of embodiment 4, which represents distortion magnitude values at different angles of view. As can be seen from fig. 8, the projection lens according to embodiment 4 can achieve good imaging quality.
Example 5
A projection lens according to embodiment 5 of the present application is described below with reference to fig. 9 to 10. Fig. 9 shows a schematic configuration of a projection lens according to embodiment 5 of the present application.
As shown in fig. 9, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 13 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 5, in which the units of the radii of curvature and thicknesses are millimeters (mm).
TABLE 13
As is clear from table 13, in embodiment 5, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 14 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 5, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
TABLE 14
Table 15 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 5.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.47 | 1.55 | -0.67 | 8.98 | 2.23 |
TABLE 15
Fig. 10 shows a distortion curve of the projection lens of embodiment 5, which represents distortion magnitude values at different angles of view. As can be seen from fig. 10, the projection lens according to embodiment 5 can achieve good imaging quality.
Example 6
A projection lens according to embodiment 6 of the present application is described below with reference to fig. 11 to 12. Fig. 11 shows a schematic structural view of a projection lens according to embodiment 6 of the present application.
As shown in fig. 11, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 16 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 6, in which the radii of curvature and thicknesses are each in millimeters (mm).
Table 16
As is clear from table 16, in embodiment 6, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 17 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 6, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 7.7309E-01 | -1.2329E+00 | 1.5965E+00 | 6.2851E+00 | -1.3052E+01 | 0.0000E+00 | 0.0000E+00 |
| S2 | 9.4646E-01 | 5.7194E+00 | -1.0454E+02 | 1.0912E+03 | -5.6163E+03 | 1.2871E+04 | -1.0593E+04 |
| S3 | 8.1481E-01 | 1.6495E+01 | -1.2105E+03 | 2.5863E+04 | -2.9970E+05 | 1.6837E+06 | -3.4325E+06 |
| S4 | 3.9765E+00 | -2.6956E+01 | 2.7356E+02 | -3.5215E+03 | 3.2010E+04 | -1.6161E+05 | 3.4395E+05 |
| S5 | -3.5554E-01 | 2.6437E+00 | -1.5112E+01 | 7.9214E+01 | -2.3434E+02 | 3.5795E+02 | -2.1981E+02 |
| S6 | -2.3670E-02 | -3.0676E+00 | 3.4836E+01 | -1.9511E+02 | 5.7765E+02 | -8.3985E+02 | 4.8062E+02 |
| S7 | -2.8650E-02 | -1.8915E+00 | 1.7194E+01 | -8.4513E+01 | 2.1753E+02 | -2.7457E+02 | 1.3378E+02 |
| S8 | -2.2260E-02 | -1.4160E-02 | -4.6485E-01 | 2.4129E+00 | -6.2830E+00 | 7.6431E+00 | -3.5857E+00 |
TABLE 17
Table 18 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 6.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.90 | 1.47 | -0.50 | 8.80 | 2.05 |
TABLE 18
Fig. 12 shows a distortion curve of the projection lens of example 6, which represents distortion magnitude values at different angles of view. As can be seen from fig. 12, the projection lens according to embodiment 6 can achieve good imaging quality.
Example 7
A projection lens according to embodiment 7 of the present application is described below with reference to fig. 13 to 14. Fig. 13 shows a schematic structural view of a projection lens according to embodiment 7 of the present application.
As shown in fig. 13, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is convex, and the image forming side surface S2 thereof is concave; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 19 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 7, in which the units of the radii of curvature and thicknesses are millimeters (mm).
TABLE 19
As is clear from table 19, in embodiment 7, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 20 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 7, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 4.8361E-01 | -3.2341E-01 | 2.6070E-01 | -3.1058E-01 | -9.5350E-02 | 0.0000E+00 | 0.0000E+00 |
| S2 | 4.5980E-01 | 4.4671E+00 | -4.1977E+01 | 2.5620E+02 | -1.0182E+03 | 2.0564E+03 | -1.5903E+03 |
| S3 | -1.9670E-01 | 1.0073E+01 | -6.5709E+02 | 1.4866E+04 | -1.9436E+05 | 1.3028E+06 | -3.4935E+06 |
| S4 | 2.4263E+00 | -4.4909E+00 | -1.3788E+02 | 3.0152E+03 | -3.0798E+04 | 1.5720E+05 | -3.1835E+05 |
| S5 | -5.6710E-01 | 4.6274E+00 | -3.0735E+01 | 1.7618E+02 | -6.1353E+02 | 1.1174E+03 | -8.1790E+02 |
| S6 | 1.8892E-01 | -1.0114E+00 | 1.0131E+01 | -5.1681E+01 | 1.5016E+02 | -2.2435E+02 | 1.3825E+02 |
| S7 | 1.2243E-01 | -1.3146E+00 | 9.3104E+00 | -4.0508E+01 | 9.3836E+01 | -1.0927E+02 | 5.0130E+01 |
| S8 | -5.0800E-03 | -1.0316E-01 | 2.0290E-01 | 1.4868E-01 | -2.2665E+00 | 3.9620E+00 | -2.2084E+00 |
Table 20
Table 21 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 7.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.50 | 1.71 | -0.68 | 11.51 | 2.00 |
Table 21
Fig. 14 shows a distortion curve of the projection lens of embodiment 7, which represents distortion magnitude values at different angles of view. As can be seen from fig. 14, the projection lens according to embodiment 7 can achieve good imaging quality.
Example 8
A projection lens according to embodiment 8 of the present application is described below with reference to fig. 15 to 16. Fig. 15 shows a schematic structural view of a projection lens according to embodiment 8 of the present application.
As shown in fig. 15, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an image forming side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is a convex surface, and the image forming side surface S2 thereof is a convex surface; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 22 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 8, in which the radii of curvature and thicknesses are each in millimeters (mm).
Table 22
As is clear from table 22, in embodiment 8, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 23 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 8, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 2.0451E-01 | -7.6718E-01 | 1.3377E-01 | 3.0263E+00 | -7.9566E+00 | 0.0000E+00 | 0.0000E+00 |
| S2 | 3.9981E-01 | -1.2211E+00 | 4.9526E+00 | -1.7683E+01 | 3.8928E+00 | 5.0109E+01 | -4.2296E+01 |
| S3 | 1.3489E-01 | -7.5732E+00 | 5.2784E+01 | -8.8773E+02 | 9.8831E+03 | -6.1758E+04 | 1.6268E+05 |
| S4 | 3.0761E+00 | -2.1121E+01 | 2.3813E+02 | -2.9466E+03 | 2.6793E+04 | -1.3781E+05 | 2.9792E+05 |
| S5 | -6.1013E-01 | 4.1908E+00 | -1.7786E+01 | 5.3101E+01 | -8.4057E+01 | 3.3219E+01 | 4.2226E+01 |
| S6 | -4.0151E-01 | 2.4365E-01 | 1.8245E+01 | -1.1416E+02 | 3.3874E+02 | -4.9319E+02 | 2.8408E+02 |
| S7 | -3.4922E-01 | -1.1731E-01 | 1.0731E+01 | -5.9213E+01 | 1.5296E+02 | -1.9217E+02 | 9.2682E+01 |
| S8 | -5.8220E-02 | -2.9410E-02 | -8.0880E-02 | 1.1590E+00 | -4.7132E+00 | 7.4302E+00 | -4.3784E+00 |
Table 23
Table 24 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 8.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.00 | 1.43 | -0.74 | 12.16 | 2.24 |
Table 24
Fig. 16 shows a distortion curve of the projection lens of embodiment 8, which represents distortion magnitude values at different angles of view. As can be seen from fig. 16, the projection lens according to embodiment 8 can achieve good imaging quality.
Example 9
A projection lens according to embodiment 9 of the present application is described below with reference to fig. 17 to 18. Fig. 17 shows a schematic configuration of a projection lens according to embodiment 8 of the present application.
As shown in fig. 17, the projection lens according to the exemplary embodiment of the present application sequentially includes, along an optical axis from an image source side to an imaging side: a first lens E1, a second lens E2, a third lens E3, a fourth lens E4, and a stop STO.
The first lens E1 has positive optical power, the image source side surface S1 thereof is a convex surface, and the image forming side surface S2 thereof is a convex surface; the second lens E2 has negative focal power, the image source side surface S3 is a concave surface, and the image forming side surface S4 is a concave surface; the third lens E3 has positive optical power, the image source side surface S5 thereof is concave, and the image forming side surface S6 thereof is convex; the fourth lens element E4 has positive refractive power, and has a concave image-source-side surface S7 and a convex image-side surface S8. The projection lens has a light transmittance of greater than 85% in the light wave band of about 800nm to about 1000 nm. Light from the image source passes sequentially through the respective surfaces S1 to S8 and is finally imaged on a projection surface (not shown) such as a projection screen.
Table 25 shows the surface types, radii of curvature, thicknesses, materials, and cone coefficients of the respective lenses of the projection lens of example 9, in which the units of the radii of curvature and thicknesses are millimeters (mm).
Table 25
As is clear from table 25, in embodiment 9, the image source side surface and the image side surface of any one of the first lens E1 to the fourth lens E4 are aspherical surfaces. Table 26 shows the higher order coefficients that can be used for each of the aspherical mirror surfaces in example 9, wherein each of the aspherical surface types can be defined by the formula (1) given in example 1 above.
| Face number | A4 | A6 | A8 | A10 | A12 | A14 | A16 |
| S1 | 3.6323E-01 | -9.6699E-01 | 1.9994E-01 | 2.8178E+00 | -7.4025E+00 | 0.0000E+00 | 0.0000E+00 |
| S2 | 4.4282E-01 | -1.3810E-01 | -4.5518E+00 | 2.8758E+01 | -1.2061E+02 | 2.1459E+02 | -1.2413E+02 |
| S3 | 3.3197E-01 | -9.9161E+00 | 1.0597E+02 | -1.7647E+03 | 1.8742E+04 | -1.1157E+05 | 2.8453E+05 |
| S4 | 3.0244E+00 | -1.9525E+01 | 2.1702E+02 | -2.7327E+03 | 2.5851E+04 | -1.3854E+05 | 3.1237E+05 |
| S5 | -9.2369E-01 | 7.0146E+00 | -3.5276E+01 | 1.2828E+02 | -2.9140E+02 | 3.6266E+02 | -1.7435E+02 |
| S6 | -3.6876E-01 | -7.5200E-03 | 2.3023E+01 | -1.4295E+02 | 4.3183E+02 | -6.6276E+02 | 4.1416E+02 |
| S7 | -3.3232E-01 | -1.4068E-01 | 1.2417E+01 | -7.2617E+01 | 2.0287E+02 | -2.8620E+02 | 1.6007E+02 |
| S8 | -4.6560E-02 | -3.6610E-02 | -1.1030E-02 | 6.6582E-01 | -3.3885E+00 | 6.1323E+00 | -4.2951E+00 |
Table 26
Table 27 gives the total effective focal length f of the projection lens and the effective focal lengths f1 to f4 of the respective lenses in embodiment 9.
| Parameters (parameters) | f(mm) | f1(mm) | f2(mm) | f3(mm) | f4(mm) |
| Numerical value | 4.25 | 1.61 | -0.74 | 22.92 | 2.04 |
Table 27
Fig. 18 shows a distortion curve of the projection lens of embodiment 9, which represents distortion magnitude values at different angles of view. As can be seen from fig. 18, the projection lens according to embodiment 9 can achieve good imaging quality.
In summary, examples 1 to 9 each satisfy the relationship shown in table 28.
Table 28
The above description is only illustrative of the preferred embodiments of the present application and of the principles of the technology employed. It will be appreciated by persons skilled in the art that the scope of the application referred to in the present application is not limited to the specific combinations of the technical features described above, but also covers other technical features formed by any combination of the technical features described above or their equivalents without departing from the inventive concept. Such as the above-mentioned features and the technical features disclosed in the present application (but not limited to) having similar functions are replaced with each other.
Claims (10)
1. The projection lens is characterized by sequentially comprising, along an optical axis from an image source side to an imaging side:
a first lens having positive optical power, the image source side surface of which is convex;
a second lens having negative optical power, the image source side surface and the image side surface of which are both concave;
a third lens having positive or negative optical power;
a fourth lens having positive optical power, an imaging side surface of which is convex;
the number of lenses with focal power of the projection lens is four; and
the total effective focal length f of the projection lens and the effective focal length f4 of the fourth lens satisfy 1.5 < f/f4 < 2.5.
2. The projection lens of claim 1, wherein the total effective focal length f of the projection lens and the effective focal length f1 of the first lens satisfy 2.0 < f/f1 < 3.5.
3. The projection lens of claim 1, wherein the total effective focal length f of the projection lens and the effective focal length f2 of the second lens satisfy f/f2 +.4.0.
4. The projection lens of claim 1, wherein the third lens has positive optical power, and an effective focal length f3 and a total effective focal length f of the projection lens satisfy 1.0 < f3/f < 5.5.
5. The projection lens of any one of claims 1 to 4, wherein the projection lens has a light transmittance of greater than 85% in the light wave band of 800nm to 1000 nm.
6. The projection lens according to any one of claims 1 to 4, characterized in that a distance TTL of an image source surface of the projection lens to an imaging side surface of the fourth lens on the optical axis and a total effective focal length f of the projection lens satisfy TTL/f < 1.0.
7. The projection lens according to any one of claims 1 to 4, wherein a maximum effective half-caliber DT42 of an imaging side surface of the fourth lens and a maximum effective half-caliber DT41 of an image source side surface of the fourth lens satisfy 1.0 < DT42/DT41 < 1.4.
8. The projection lens according to any one of claims 1 to 4, wherein a separation distance T12 of the first lens and the second lens on the optical axis and a separation distance T23 of the second lens and the third lens on the optical axis satisfy 0.8 < T12/T23 < 2.2.
9. The projection lens according to any one of claims 1 to 4, wherein a center thickness CT4 of the fourth lens on the optical axis and a center thickness CT2 of the second lens on the optical axis satisfy 1.5 < CT4/CT2 < 3.0.
10. The projection lens according to claim 9, wherein a radius of curvature R8 of an imaging side surface of the fourth lens and a radius of curvature R1 of an image source side surface of the first lens satisfy-1.5.ltoreq.r8/r1.ltoreq.1.0.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202310803357.2A CN116819728A (en) | 2017-12-15 | 2017-12-15 | projection lens |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202310803357.2A CN116819728A (en) | 2017-12-15 | 2017-12-15 | projection lens |
| CN201711348942.9A CN107831630B (en) | 2017-12-15 | 2017-12-15 | Projection lens |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201711348942.9A Division CN107831630B (en) | 2017-12-15 | 2017-12-15 | Projection lens |
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| Publication Number | Publication Date |
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| CN116819728A true CN116819728A (en) | 2023-09-29 |
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| Application Number | Title | Priority Date | Filing Date |
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| CN201711348942.9A Active CN107831630B (en) | 2017-12-15 | 2017-12-15 | Projection lens |
| CN202310803357.2A Pending CN116819728A (en) | 2017-12-15 | 2017-12-15 | projection lens |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201711348942.9A Active CN107831630B (en) | 2017-12-15 | 2017-12-15 | Projection lens |
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| CN (2) | CN107831630B (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108227149B (en) * | 2018-01-30 | 2024-04-02 | 江西联益光学有限公司 | Collimation lens |
| US20190302596A1 (en) * | 2018-03-30 | 2019-10-03 | Anteryon Wafer Optics B.V. | Optical module |
| CN108427183B (en) * | 2018-05-04 | 2024-06-18 | 浙江舜宇光学有限公司 | Projection lens |
| CN109975955A (en) * | 2019-04-08 | 2019-07-05 | 广东弘景光电科技股份有限公司 | The pre- police monitoring optical system of fatigue driving and its camera module of application |
| CN112596218B (en) * | 2020-12-01 | 2021-11-16 | 浙江大学 | Large-depth-of-field infrared wavelength scanning lens |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JPH01261615A (en) * | 1988-04-12 | 1989-10-18 | Minolta Camera Co Ltd | Lens system for projection |
| JP2706946B2 (en) * | 1988-06-07 | 1998-01-28 | 旭光学工業株式会社 | Front aperture projection lens |
| JP2003066330A (en) * | 2001-08-29 | 2003-03-05 | Hitachi Ltd | Projection lens unit and back projection type picture display device using the same |
| KR101499981B1 (en) * | 2008-11-19 | 2015-03-06 | 엘지이노텍 주식회사 | Imaging Lens |
| JP5259503B2 (en) * | 2009-06-16 | 2013-08-07 | 富士フイルム株式会社 | Projection optical system and projection display device using the same |
| TWM390465U (en) * | 2010-04-30 | 2010-10-11 | E-Pin Optical Industry Co Ltd | Four-piece projection lens system and the projection apparatus using the same |
| CN102566014A (en) * | 2010-12-17 | 2012-07-11 | 中强光电股份有限公司 | Lens module |
| US8976466B2 (en) * | 2011-03-11 | 2015-03-10 | Olympus Corporation | Imaging optical system and imaging apparatus using the same |
| JP5795363B2 (en) * | 2011-04-19 | 2015-10-14 | 富士フイルム株式会社 | Projection lens and projection display device using the same |
| KR101281368B1 (en) * | 2011-09-23 | 2013-07-02 | 엘지이노텍 주식회사 | Imaging lens |
| CN103869450B (en) * | 2012-12-18 | 2016-07-13 | 广景科技有限公司 | LED digital micro projection lens of projector |
| JP5937036B2 (en) * | 2013-03-29 | 2016-06-22 | 富士フイルム株式会社 | Imaging lens and imaging device provided with imaging lens |
| CN106646829B (en) * | 2017-01-04 | 2018-08-14 | 浙江舜宇光学有限公司 | Telephoto lens and photographic device |
| CN106990505B (en) * | 2017-05-12 | 2022-05-24 | 浙江舜宇光学有限公司 | Imaging lens |
| CN107219614B (en) * | 2017-08-07 | 2022-09-06 | 浙江舜宇光学有限公司 | Optical imaging lens |
| CN207516711U (en) * | 2017-12-15 | 2018-06-19 | 浙江舜宇光学有限公司 | Projection lens |
-
2017
- 2017-12-15 CN CN201711348942.9A patent/CN107831630B/en active Active
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| CN107831630B (en) | 2023-12-29 |
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