445 3 7 3 A7 B7 五、發明说明(1 ) 請 先I 33 I 讀! 背I 面 j 之 ί 事I I | 填I If 旋光物質溶液經過;參透膜(sem^_permeable membrane );參透,其淨透速 率與兩邊的壓力有關β由於旋光物質具有旋光性(optical acdv丨ty ), 它可讓入射的線偏極化雷射光產生旋轉(optical rotation ),旋光物質 的滲透速荜可藉由線偏極化的旋轉角度隨時間鈞變化而直接量得。 另外,滲透速率的變化也因渗透膜兩端的壓力增加而造成其速率的 改變。 1-丁 本專利主要在藉由量測旋光角度的方法直接量測旋光物質溶液濃 度的變化速率而獲得滲透膜兩端的壓力差。它寸應用於動物眼睛房 水中葡萄糖(aqueous glucose)濃度變化的速'率進而即時測得房水 中壓力的大Λ;、1並印時檢查出早期造成房水壓力變化的病因,特別 是對青光眼(glaucoma )病人的早期珍斷將可提供一種高敏感度偵 測眼壓的定量方法及技術。 經濟部中央揉準局MB;工消費合作社印裝 傳統中旋光性質對線偏極化光所造成的旋光角度均藉由光起偏器 (polarizer)以及光檢偏器(analyzer)並利闬機械方式直接量取因旋光 物質所造成的旋光角度改變而得到相關的物理量,例如光折射率或 旋光物質在溶液中的濃度等β在功能上因機械的振動以及較低的量 測速度而被直接由聲光(acousto-optic)或電光(electro-optic)調變器 (modulator)產生強度調變的入射光源而取代,它藉由直接量取強度 調變的輸ά光信號的振幅或相位而求得旋光角度的大小。然而在這 些系統中利用機械方式產生強度.調變信號易受振動以及調變頻率不 南的影響而無法得到較高的量測精度,但藉由聲光,電光調變器或 光彈調變器(photoelastic modulator,ΡΕΜ)而產生高頻率的強度調變 仏號或極化光調變信號(poiarization. modulation)則因調變器本身的不 本紙法尺度適用t國闺家祿举(CNS) A4^ ( 210x297公廣) t 44537 3 λ7 __ _ B7 I " ' " " -------*_:_ 五、發明説明(2) 穩定性而造成誤差。藉由聲光調變器而產生光學外差干涉是可達到 高的調變頻率以及較高的穩定度;然而因干涉儀(mterfe「ometer)對 外界環境的干擾相當破感而造成系統量測精度上的限制。本發明係 以一組相互垂直的線偏極化雙頻穩頻雷射(例如Zeeman雷射),簡稱 雙頻穩頻雷射(two-frequency laser)為光源,利用一極化光分光片 (polarized beam splitter)或極化光析光片產生外差干涉信 號’並利用信號振幅大小量測裝置直接量取強度調變信號的振幅大 小,而獲得旋光性物質的旋轉角度(如圖一)。因faf = -之 ’丁 / 關係’溶液中旋轉角度匕與溶液中旋光物質濃度c成線性關係, 進而可藉由量測旋轉角度而得到濃度。其中△為光程,為 旋光物質之specific rotation.在光學架構上它屬於共同路徑干涉儀 (common-path interferometer),因此系統對外界環境的干優有免疫能 力。而且構造較傳統方法簡單,同時擁有較高的量測精度及即時性。 本發明以雙頻穩頻雷射為光源,其頻率分為^與①:。調整極化光 分光片,使得X轴與入射雙頻率的相互垂直線偽極化雷射光中的P 波平行且Y軸與S波平行,如第二圖(a)。或將相互垂直之線偏極化 光分別與X軸及Y軸成一夹角,如第二圖(b)。雙頻率的相互垂 直線偏極化雷射光在通過旋光性物質後同時產生旋轉角的轉動 (如第二圖(c))。在經由極化分光片將P波與S波分開並分別由光偵 檢器DP與Ds所偵測。其所輸出的外差干涉信號可分別表示如下:445 3 7 3 A7 B7 V. Description of the invention (1) Please read I 33 I first! Back I and j of the matter II | Fill in I If the optically active substance solution passes through; see through membrane (sem ^ _permeable membrane); see through, its net permeation rate is related to the pressure on both sides β because optically active matter has optical acdv 丨 ty It can make the incident linearly polarized laser light rotate (optical rotation), and the penetration speed of the optically polarized material can be directly measured by the change of the rotation angle of the linearly polarized material with time. In addition, the change in the permeation rate is also caused by the increase in pressure at both ends of the permeation membrane. 1-D This patent mainly measures the rate of change of the concentration of the optically active substance solution directly by measuring the angle of optically active rotation to obtain the pressure difference across the membrane. It is applied to the rate of change in the concentration of aqueous glucose in the eye of an animal, and the instantaneous measurement of the large Λ of the pressure in the aqueous humor; and 1 to check the cause of the early change in aqueous humor pressure, especially for glaucoma. (Glaucoma) Early diagnosis of patients will provide a highly sensitive quantitative method and technology for detecting intraocular pressure. The Central Bureau of the Ministry of Economic Affairs, MB; the industrial and consumer cooperatives printed traditional polarized light to the polarized light caused by the polarized light (polarizer) and the optical analyzer (analyzer). The method directly measures the change of the optical rotation angle caused by the optically active substance and obtains the relevant physical quantities. For example, the optical refractive index or the concentration of the optically active substance in the solution, etc. β is directly functionally due to mechanical vibration and a low measurement speed. It is replaced by an acoustic light-optic or electro-optic modulator that generates an intensity-modulated incident light source. It directly measures the amplitude or phase of the input optical signal whose intensity is modulated. Find the magnitude of the rotation angle. However, in these systems, the strength is generated mechanically. The modulation signal is susceptible to vibration and the frequency of modulation is not high enough to obtain high measurement accuracy. However, it is modulated by acousto-optic, electro-optic, or photoelastic modulation. Photoelastic modulator (PEM) and high-frequency intensity modulation signal or poiarization. Modulation is applied due to the non-paper-based scale of the modulator itself (CNS) A4 ^ (210x297 public broadcasting) t 44537 3 λ7 __ _ B7 I " '" " ------- * _: _ 5. Explanation of the invention (2) Stability caused errors. The optical heterodyne interference generated by the acousto-optic modulator can achieve high modulation frequency and high stability; however, the system measurement is caused by the interference of the mterfe "ometer" on the external environment. Limitation on accuracy. The present invention uses a set of mutually orthogonal line-biased dual-frequency frequency-stable lasers (such as Zeeman laser), referred to as two-frequency lasers for short, as a light source, using one pole A polarized beam splitter or polarized light splitter generates a heterodyne interference signal and uses a signal amplitude measurement device to directly measure the amplitude of the intensity modulation signal to obtain the rotation angle of the optically active substance ( As shown in Figure 1), because the rotation angle of the solution in the solution of "f / =" is in a linear relationship with the concentration of the optically active substance c in the solution, the concentration can be obtained by measuring the rotation angle. Among them, △ is the optical path length, which is The specific rotation of optically active substances. It belongs to a common-path interferometer on the optical structure, so the system is immune to external interference. It is simpler to construct than traditional methods. At the same time, it has high measurement accuracy and instantaneity. The present invention uses a dual-frequency stable frequency laser as the light source, and its frequency is divided into ^ and ①: The polarized light beam splitter is adjusted so that the X-axis and the incident dual-frequency are mutually related. The P-wave in the vertical-line pseudo-polarized laser light is parallel and the Y-axis is parallel to the S-wave, as shown in the second figure (a). Or, the orthogonally-polarized linearly polarized light forms an angle with the X-axis and Y-axis, respectively, such as Second figure (b). Polarized laser light with two mutually perpendicular polarized lines passes through the optically active substance and simultaneously generates a rotation of the rotation angle (as shown in the second figure (c)). The P wave and the The S waves are separated and detected by the optical detectors DP and Ds. The heterodyne interference signals output by them can be expressed as follows:
Jp (Δωί) = ax2z sin[ 2(θν +θώ)] c〇s( Δω[)+ DC............(ι).Jp (Δωί) = ax2z sin [2 (θν + θώ)] c〇s (Δω () + DC ............ (ι).
Is ( Δωί )^aia2m^^2{0(i+9m )] cos( ΑωΙ)+ DC ......(2) j 其f A是旋光物質所造成的旋轉角:孕’冬分別為兩線偽極先的 振幅大小:=q —必,.;/X7為直流項° 當碇光性物f所造成的旋轉角度很小,Eq. (i)和Eq. (2)可改寫為:j I八Δω〇 二 la也十 认Λ①DC .................(3) 本纸杀尺度適用尹国®家揉準(CVS ) A4说格ί 210X297公釐) (诗先閱讀背面之注意事項再填写太f 訂 1 ------—線,-- 經濟部尹央標筚局員工消費合作社印裝 44537 3 A 7 ____B7_____, 五、發明説明(i ) Is (Αωΐ) = ~^axa2 {^+9m)c〇s(Δωί)+ DC ..................(4) 藉由帶通遽波器濾出強度調變信號(中心頻率設定在△£〇 ),再利 用光電信號處理器將與/5相減而得到 Ι{Δω〇 = IP~ Is= 43l22 {eQ+9m)cos(Δωί)...............(5) 我們可由振幅量測裝置量測該信號振幅大小。根據Eq.(5),當光束 通過無旋光性物質時,所得信號振幅大小為,當光束通過旋 光性物質時,則輸出信號振幅大小為+D ^本專利之極 化光分光片(PBS)可以一極化角(azimuth angle)為之極化光析光片 (analyzer)取代,(如第三圖)所輸出外差干涉信號可表示為Is (Δωί) ^ aia2m ^^ 2 {0 (i + 9m)] cos (ΑωΙ) + DC ...... (2) j where f A is the rotation angle caused by the optically active substance: pregnant and winter are respectively The amplitude of the two-wire pseudo pole first: = q —must,.; / X7 is the DC term ° When the rotation angle caused by the photoluminescence object f is small, Eq. (I) and Eq. (2) can be rewritten as : J I eight Δω〇 two la also recognize Λ①DC ....... (3) The paper killing scale is applicable to Yin Guo® Home Kneading Standard (CVS) A4. 210X297 mm) (Read the notes on the back of the poem first and then fill in too f. Order 1 -------- line,-printed by Yinyang Biaoju Bureau of the Ministry of Economic Affairs Consumer Cooperatives 44537 3 A 7 ____B7_____, V. Description of the invention ( i) Is (Αωΐ) = ~ ^ axa2 {^ + 9m) c〇s (Δωί) + DC ........ (4) by bandpass chirp The filter filters out the intensity modulation signal (the center frequency is set to △ £ 〇), and then subtracts / 5 with the photoelectric signal processor to obtain Ι {Δω〇 = IP ~ Is = 43l22 {eQ + 9m) cos (Δωί) ......... (5) The amplitude of the signal can be measured by the amplitude measuring device. According to Eq. (5), when the light beam passes through the non-optical material, the amplitude of the obtained signal is: when the light beam passes through the optically active substance, the output signal amplitude is + D ^ Polarized light beam splitter (PBS) of this patent It can be replaced by a polarization light analyzer (azimuth angle), and the heterodyne interference signal (as shown in the third picture) can be expressed as
Ιχ (Δωί) = 2axa2 sin(cos( Δωί)+ DC ...............(6) 當旋光角恨小時,Eq (6)可寫成 Ι^Δωΐ)^ laya2 (<90 + ^)cos(Δωΐ)^ DC.....................(7) 由振幅量測裝置測量信號振幅大小為 2响(θ0 +D ....................:..............................⑻ «I (請先M讀背面之注意事項再填寫太頁> • y- 經濟部中央標牮局貝工消f合作社印裝 將Θ設定為1° *且當旋光物質濃度為零時"振幅大小可表示為 /〇 = ^3^2 ...............................................................(9) 以為零;農度校正之用β利用振幅量測裝置連續測量外差干涉信號大 小隨時間的變化量為 \ΑΙ(Δωί)\ = j/, = ^az9m =\h\-〇m..........(10) 或 .....................................(11) 由於旋轉角度與濃度的線性關係,可即時量測旋光性物質在溶液 ; 中濃度的時間變化及滲透速率。 本發明特徵說明如下:第一圖為本發明之光學組件配置a系統中所 使用的光源為一線偏極化雙頻率穩頻雷射光(10),其中兩線偏極化 光相互垂直(Orthogonal) ’經分光片(20)將雷射光分成兩束光,一束為: 參考光束,另一束為信號光束。參考光束經過一固定方位角的極化 光析光片(ana丨yzer) Ar (45),再經由一抉速頻荜反應的光儐檢器(55) ----千-----------Γ_____ 本.紙孩又度逋月tSli家標孪(G\S ) A4規·格(210X297公釐) V Λ4537 3 A7 五、發明説明(斗) 接收,並產生外差干涉信號9在光偵檢器(55)的後面設置一帶通濾 波為(65)並將過渡之電子信號輸入振幅量測裝置(7〇p帶通濾波器 (請先閲請背面之注意事項再填寫本頁) if) 1中〜頻率設定等於雙頻率雷射光的差頻頻率 ω —ω2)。同時當雙頻率穩頻且相互垂直的線偏極化信號光 束雷射光通過待測旋紐物質Ρ〇)後,因旋光物質本身具有旋光性: 而使通過之光束其線偏極化方向改變纥角度。極化光分光片的乂軸 與入射雷射光的Ρ波平行,γ軸與s波平行(如第二圖⑷)。極化 先分光片(40)產生外差干涉信號,分別由光偵檢器(4丨)及(43)接收’ 再經過帶通濾波器(42),(44)直接輸出到光電信號處理裝置⑽,而得 到/()(』6>ί)外差干涉信號,並直接輸入到振幅量測裝置(7〇)中讀取 固疋拍頻率Δω外差干涉信號振幅大小,而即時量測被測試旋光物 質溶液旋轉角的時間變化及澡透速率。在第_圖中,參考外差干涉 信號輸入振幅量測裝置(70)直接量取參考光束的振幅大小,可做= 铪射光源強度後;化的監控及校正之用。第一圖中可將參考外差干; 信號做為以鎖相放大器(lock in amplifier)為振幅量測裝置的參考光 信號,而直接量取外差干涉信號的振幅大小。_______Ιχ (Δωί) = 2axa2 sin (cos (Δωί) + DC ............... (6) When the rotation angle is small, Eq (6) can be written as ^^ Δωΐ) ^ laya2 (< 90 + ^) cos (Δωΐ) ^ DC .............. (7) The amplitude of the signal measured by the amplitude measuring device is 2 ( θ0 + D .....: ............................ .... ⑻ «I (Please read the precautions on the back before filling in the page> • y- Printed by the Central Bureau of Standards, Ministry of Economic Affairs, Bei Gong Xiao Cooperative, and set Θ to 1 ° * and when the concentration of optically active substances When it is zero " the amplitude can be expressed as / 〇 = ^ 3 ^ 2 ............. .............. (9) As zero; for the correction of agronomy, β uses the amplitude measurement device to continuously measure the outside The change of the magnitude of the difference interference signal with time is \ ΑΙ (Δωί) \ = j /, = ^ az9m = \ h \ -〇m .... (10) or ... ......... (11) Due to the linear relationship between the rotation angle and the concentration, the optically active substance can be measured immediately The time variation of the concentration in solution and the permeation rate. The features of the present invention are described as follows: The first figure is the position of the optical component configuration a system of the present invention. The light source used is a linearly polarized dual-frequency stable frequency laser light (10), where the two linearly polarized lights are perpendicular to each other (Orthogonal) 'The laser light is divided into two beams by a beam splitter (20), one beam is: Reference Light beam, the other is a signal beam. The reference beam passes through a polarized light analyzer (ana 丨 yzer) Ar (45) with a fixed azimuth angle, and then passes through a photodetector (55)- --- Thousands ----------- Γ _____ Ben. The paper child spends another month tSli family standard twin (G \ S) A4 rule · Grid (210X297 mm) V Λ4537 3 A7 V. Description of the invention (Doo) Receive and generate heterodyne interference signal 9 Set a band-pass filter to (65) behind the optical detector (55) and input the transitional electronic signal to the amplitude measurement device (70p band-pass filter ( Please read the notes on the back before filling in this page) if) 1 ~~ The frequency setting is equal to the difference frequency ω —ω2 of the dual-frequency laser light. At the same time, when the dual-frequency is stable and perpendicular to each other, the linearly polarized signal beams After the laser light passes through the spin button substance P0), the optically polarized substance itself has optical rotation: the polarization direction of the passing beam is changed by the angleThe chirp axis of the polarized beam splitter is parallel to the P wave of the incident laser light, and the gamma axis is parallel to the s wave (see the second figure ⑷). The polarization first beam splitter (40) generates heterodyne interference signals, which are received by the optical detectors (4 丨) and (43), respectively, and then output directly to the photoelectric signal processing device through a band-pass filter (42), (44). ⑽, to obtain / () (『6 > ί) heterodyne interference signal, and directly input it to the amplitude measurement device (7〇) to read the fixed beat frequency Δω heterodyne interference signal amplitude, and the instant measurement is The time change of the rotation angle of the optically active substance solution and the bath penetration rate were measured. In the figure _, the reference heterodyne interference signal is input to the amplitude measurement device (70) to directly measure the amplitude of the reference beam, which can be used for monitoring and correction after the intensity of the radioactive light source. In the first figure, the reference heterodyne can be used; the signal is used as a reference optical signal with a lock in amplifier as the amplitude measurement device, and the amplitude of the heterodyne interference signal is directly measured. _______
ί. I i. ϋ丨 經濟部中央標準局員工消費合作社印製 /知沒(¾. i - iD^ ^^ 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) d45373 C9 D9 圖式 第一圖本發明之光學組件流程圖(I) 10-線偏極化雙頻穩頻雷射(linearpolarized two-frequency 丨aser) 2〇·分光鏡(beam splitter) J 〇 · % 先性物質(optical ac five material) 極化光分光片(polarized beam splitter PBS) 41. 光偵檢器 D (photo detector) 43.元{貞檢器 Ds (photo detector) 42. 帶通;慮波器(bandpass filter) .帶通渡波器(bandpass filter) $5,極化光析光片八細咖挪) 元電信號處理器(signal processor) 5).光 貞檢器 Dr (photo detector) 65. f 通渡波器(bandpass filter) 7〇-振幅量測裝置(voltmeter or lock in amplifier) 肌個人電猫(personal computer) 第三圖本發明之光學組件流程圖(Π) 10.線偏極化雙頻穩頻雪射(Ihear polarized two-frequency laser) 20.分光鏡(beam splitter) 〕〇旋光性物質(optical active material) 4〇.極化光析光片(analyzer) 42.帶通;慮波器(bandpass fiter) 經濟部中央標準局员工消費合作社印製 45-極化光析光片Ar (analyzer) 55.光痛檢器 £)r (photo detector) 65-帶通;慮波器(bandpass filter) 70.振幅量測裝置(voltmeter or 丨ock in amplifier) 80.個人電腦(personai compUter) 本紙張尺度適用中國國家榡準(CNS ) M規格{ 21〇χ29"7公釐) 圖式 第四圖旋光物質溶液滲透速率'測量儀 10.線偏極化雙頻穩頻雪射(linear ρο丨arized two-frequency laser) 2 0.分光鏡(beam splitter) 30.反身于鏡(mirror) 40. 極化光分光片(polarized beam splitter, PBS) 41. 光伯檢器 Dp(photo detector) 43. 光偵檢器 Ds (photo detector) 42. 帶通滤波器(bandpass filter) 44. 帶通濾波器(bandpass filter)· 45. 極化光析光片(analyzer) 50.光電信號處理器(signal processor) 55.光偵、檢器(photo detector) 6 5.帶通遽波器(bandpass filter) 70.振幅量測裝置(voltmeter or lock in amplifier) 80.個人電腦(persona丨 computer) 介電子開關(electronic shutter) 100.眼球(human eye) 110.透鏡(lens) 120.圖形顯示版 經濟部中央標準局負工消費合作社印装 (a) 極化光分光片之X軸與入射雷射光P波平行,Y軸與S波行。 (b) 極化光分光片之X軸和Y軸分別與入射雷射光P波和S波成一 Θ 〇夾角a (c)入射雷射光中P波和S波經過旋光物質並旋轉θ ηι角度。 本纸張尺度適用中國國家標準(CNS ) A4见格(2】0><297公釐)ί. I i. ϋ 丨 Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs / Cognizance (¾. i-iD ^ ^^ This paper size applies to the Chinese National Standard (CNS) A4 specification (210X297 mm) d45373 C9 D9 Figure The first diagram of the formula (I) 10-linearly polarized two-frequency 丨 aser 2.Beam splitter J % (optical ac five material) polarized beam splitter PBS 41. light detector 43 (photo detector) 43. Yuan {Chasser Ds (photo detector) 42. Bandpass; wave filter (bandpass filter) .bandpass filter ($ 5, polarized light analysis sheet), signal processor (signal processor) 5), photo detector 65 (f detector) (bandpass filter) 70-amplitude measuring device (voltmeter or lock in amplifier) muscle personal electric cat (personal computer) Figure 3 Optical component flow chart of the present invention (Π) 10. Linear polarization dual frequency stabilization frequency snow (Ihear polarized two-frequency laser) 20. Beam splitter 〔〇 Optical act (optical act ive material) 4〇. Polarized light analyzer (analyzer) 42. Bandpass; waveband (bandpass fiter) Printed 45-polarized light analyzer Ar (analyzer) 55 Photodetector £) r (photo detector) 65-bandpass; bandpass filter 70. Amplitude measuring device (voltmeter or 丨 ock in amplifier) 80. Personal computer (personai compUter) China National Standard (CNS) M specification {21〇χ29 " 7 mm) The fourth diagram of the optical rotation solution's permeation rate 'measuring instrument 10. Linear polarized dual-frequency stable frequency snow injection (linear ρο 丨 arized two- frequency laser) 2 0. beam splitter 30. mirror 40. polarized beam splitter (PBS) 41. optical detector Dp (photo detector) 43. light detection Ds (photo detector) 42. Bandpass filter (bandpass filter) 44. Bandpass filter (bandpass filter) 45. Polarized light analyzer (analyzer) 50. Photoelectric signal processor (signal processor) 55. Photo detector 6 5. Bandpass filter 70. Amplitude measuring device (voltmeter or loc k in amplifier) 80. personala computer electronic shutter 100. human eye 110 lens 120. Graphic display version Printed by the Consumers ’Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs a) The X-axis of the polarized beam splitter is parallel to the P-wave of the incident laser light, and the Y-axis is parallel to the S-wave. (b) The X-axis and Y-axis of the polarized light beam splitter form an included angle a with the incident laser light P wave and S wave, respectively. (c) The P wave and S wave in the incident laser light pass through the optically active substance and rotate through the angle of θ ηι. This paper size is applicable to Chinese National Standard (CNS) A4 (2) > < 297 mm