TW508437B - Optical rotation angle measurement device using phase method - Google Patents
Optical rotation angle measurement device using phase method Download PDFInfo
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508437 A7 B7 五、發明說明(/) 【發明領域】 本發明是關於一種旋光角度相位量測裝置,特別是指 一種利用雙頻率,雙偏極化雷射光即時量測旋光角度 置。 、 5 【背景技術】 經濟部智慧財產局員工消費合作社印製 具有旋光特性(optical activity)物質之溶液,如糖水等 可將一線偏極化光在通過該旋光溶液後產生線偏極光旋轉 一角度(optical rotation),因此可藉由旋轉角度的大小進 一步求得該溶液的濃度,和圓偏極化雙折射(circular 10 birefringence)等旋光特性之物理量。然而大部分量測旋光 角度的方法都是利用極化片(polarizer)和分析片(analyzer) 所組成之極化儀(polarimeter)直接量取輸出之線偏極化光 的強度變化而得到旋轉角度大小。這種方法常因雷射光源 輸出強度的不穩定而且亦很容易受外界環境的影響而不能 15 精確的測量旋轉角度。因此有研究提出利用空間(spatial) 或時間(temporal)的干涉儀並利用同步偵測(Synchronized detection)的方法用以提高信號訊雜比值(SNR)而達到提高 量測精確度的目的,然而這些方法在光學架構上比較#复雜 同時亦一樣容易受到環境的影響。 20 【發明内容】 故本發明之一目的係提供一種具環境穩定性之旋光角 度相位量測裝置。 〜本發明之另一目的係提供一種即時量測之旋光角度相 位量測裝置。 第4頁 本紙張尺度適用中國國家標準(CNS)A4规格(210 X 297公釐) 508437 五、發明說明(V) 依上述目的,本發明之主要特徵係在於利用雙頻率, 雙偏極化雷射光如Zeeman雷射以相位敏感(phase韻iti㈣ 的方法和裝置即時量測旋光角度,因採用共同路徑之光學 架構,使環i兄因素之景;^響被有效降低、穩定性及偵測靈敏 度大幅提升,而採同步偵測亦可迅速獲得即時資訊。 10 訂 15 經濟部智慧財產局員工消費合作社印製 本發明一種叙光角度相位量測裝置,係用以測試一待 測物之旋光角度,包括:一穩頻雷射光源,用來輸出一信 號光束和一參考光束,該信號光束和參考光束分別具有雙 頻率、而且偏極化方向相互垂直的圓偏極化雷射分量,該 信號光束是被入射到該待測物;一極化分光裝置,用來分 離牙過該待測物的k號光束所含的p波和S波分量;一極 化光分析片,用來調整來自分光元件的參考光束的極化方 向,使其P波和s波分量間可以產生外差干涉光學信號; 第一和第二光偵檢器,分別把來自該極化光分析片的參考 光束外差干涉光學信號、和穿過該待測物的信號光束的P 波或S波分量之至少一分量,轉換成一參考信號和一第一 資料信號;一組處理裝置,用來把該參考信號相對該第一 資料信號偏移7Γ/2,並把該偏移後之參考資料和第一資料 信號相乘,取該直流信號輸出,藉此獲得該待測物的旋光 20角度。 為供更詳盡明確瞭解本發明之目的、功效及構造特 徵,茲舉本發明之較佳實施例並配合圖示説明如后·· 【附圖說明】 第一圖是本案第一較佳實施例之光學架構示意圖。· ___ 第5頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) I* 508437 A7 B7 經濟部智慧財產局員工消費合作社印製 五、發明說明(3 ) 第二圖是圓偏極化光旋轉角度示意圖。 第三圖是本案第二較佳實施例之光學架構示意圖。 第四圖是本案第三較佳實施例之光學架構示意圖。 第五圖是本案第四較佳實施例之光學架構示意圖。 5 第六圖是本案第五較佳實施例之光學架構示意圖。 【具體實施方式】 請參閱第一圖所示,本發明是利用所發雷射光束具有 兩種不同頻率、而且彼此的偏極化方向相互垂直的穩頻雷 射光源裝置1作為光源,在第一較佳實施例中,裝置1包 10 括線偏極化Zeeman雷射1〇〇、二分之一波片iio、分光 元件120、四分之一波片130。其中,雷射1〇〇發出的線 偏極化雷射光束經由一二分之一波片丨丨〇,使得這兩種線 偏極化光P波和S波分篁的方位角angle),分別 平行於空間座標軸X軸和Y軸。由分光元件(BS) 12〇把 光源100輸出的線偏極化光分為參考光束與信號光束。 如第二圖所示,由於旋光角度的產生是基於左(^和 右(R)圓偏極化光在具有旋光特性的介質傳播時,因傳播 的速率不栢·同而造成線偏極化光旋轉,因此在第一圖中利 用一方位角為45之四分之一波片13〇將信號光束的p 波和S波分別轉換成圓偏極化的r波和l波。並同時入 射至具旋光特性之溶液中。其中p波和s波可以J〇ne,s ,(4,%)和(為,A) 15 20 矩碎表示成P波 V ,S波: 〇· 1 分別為P波和S波之振幅及頻率,再經過λ/4波片轉換 __^第ό頁 卜紙張尺度適用中國國豕&準(CNS)A4规格·(21〇 χ 297公爱) -•%層1 U ------^---------線 ---1 (請先閱讀背面之注意事項再填寫本頁) 508437 A7 B7 經濟部智慧財產局員工消費合作社印製 五、發明說明() 成R波和L波,分別可寫成R波··(Ι/Α)#— A.和L波 R波和L波在穿過具旋光性之待測物溶液140後可寫 成 R,波··(1 忑)Ape“t+a ;L’波··(1/λ/Ι;Μ〆(〜+〜) 5 其中和表示因R波和L波在旋光介質中 傳播速度不同所造成的相位變化,由第二圖中可得到線偏 極化光的旋轉角度5=(θκ—θ〇/2。當R’波和L’波再通 過一 50 : 50的極化光分光器(PBS) 150分光,其中在通過 Ρ波偏極化方向的R’波和L’將轉換成(Ap/W) 10 和(As/A) %ί(ω pt+ Θ R)508437 A7 B7 V. Description of the Invention (/) [Field of the Invention] The present invention relates to an optical rotation angle phase measurement device, and particularly to an instant measurement of optical rotation angle using dual-frequency, dual-polarization laser light. 5 [Background technology] The employee cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs prints a solution with optical activity, such as sugar water, which can rotate a linearly polarized light through the optically polarized solution to rotate an angle (Optical rotation). Therefore, the concentration of the solution and the physical quantities of optical rotation characteristics such as circular 10 birefringence can be further obtained by the magnitude of the rotation angle. However, most of the methods for measuring the rotation angle are to directly measure the intensity change of the output linearly polarized light using a polarimeter composed of a polarizer and an analyzer to obtain the rotation angle. size. This method often cannot accurately measure the rotation angle due to the unstable output intensity of the laser light source and it is also easily affected by the external environment. Therefore, some studies have proposed the use of spatial or temporal interferometers and the use of synchronous detection to improve the signal-to-noise ratio (SNR) to improve the measurement accuracy. However, these The method is more complicated in terms of optical architecture and is also easily affected by the environment. [Summary of the Invention] Therefore, an object of the present invention is to provide an optical rotation angle phase measurement device with environmental stability. ~ Another object of the present invention is to provide an optical rotation angle phase measurement device for instant measurement. Page 4 This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 508437 V. Description of the invention (V) According to the above purpose, the main feature of the present invention is the use of dual-frequency, double-biased polarized mines Laser light such as Zeeman laser uses phase-sensitive (phase rhyme) methods and devices to measure the rotation angle in real time. The use of a common path optical architecture makes the scene of the ring-shaped factor; the response is effectively reduced, the stability and the detection sensitivity It is greatly improved, and real-time information can also be obtained quickly by using synchronous detection. 10 Order 15 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, a narrative angle phase measurement device of the present invention is used to test the rotation angle of an object Including: a stable frequency laser light source for outputting a signal beam and a reference beam, the signal beam and the reference beam respectively having a circularly polarized laser component with dual frequencies and polarization directions perpendicular to each other, the signal The light beam is incident on the object to be measured; a polarization beam splitting device is used to separate the p-wave and S-wave components contained in the k-number beam passing through the object; a polarized light analysis , Used to adjust the polarization direction of the reference beam from the spectroscopic element so that heterodyne interference optical signals can be generated between the P-wave and s-wave components; the first and second optical detectors respectively analyze the polarized light from the The reference optical heterodyne interference optical signal of the sheet and at least one component of the P-wave or S-wave component of the signal beam passing through the object to be measured are converted into a reference signal and a first data signal; a set of processing devices for The reference signal is shifted by 7Γ / 2 from the first data signal, and the shifted reference data is multiplied by the first data signal, and the DC signal is output to obtain the optical rotation 20 angle of the object to be measured. In order to provide a more detailed and clear understanding of the purpose, efficacy and structural features of the present invention, the preferred embodiments of the present invention are illustrated in conjunction with the illustrations below. [Brief Description of the Drawings] The first figure is the first preferred implementation of the present case. Schematic diagram of the optical structure of the example. · ___ page 5 This paper is in accordance with Chinese National Standard (CNS) A4 (210 X 297 mm) I * 508437 A7 B7 Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 3) The second diagram is a schematic diagram of the rotation angle of circularly polarized light. The third diagram is a schematic diagram of the optical architecture of the second preferred embodiment of the case. The fourth diagram is the schematic diagram of the optical architecture of the third preferred embodiment of the case. The fifth diagram It is a schematic diagram of the optical architecture of the fourth preferred embodiment of the present case. 5 The sixth diagram is a schematic diagram of the optical architecture of the fifth preferred embodiment of the present case. [Detailed Description] Please refer to the first figure, the present invention uses the lightning As a light source, a stable frequency laser light source device 1 having two different frequencies and polarizing directions perpendicular to each other is used as a light source. In a first preferred embodiment, the device 1 includes a linearly polarized Zeeman laser 1 00, a half-wave plate iio, a spectroscopic element 120, and a quarter-wave plate 130. Among them, the linearly polarized laser beam emitted by the laser 100 passes through a half-wave plate, so that the two azimuth angles of the linearly polarized light P-wave and S-wave deflection angle), Parallel to the X and Y axes of the space coordinate axis, respectively. The linearly polarized light output from the light source 100 is divided into a reference beam and a signal beam by a beam splitting element (BS) 120. As shown in the second figure, because the rotation angle is generated based on the left (^ and right (R) circularly polarized light when propagating in a medium with optical rotation characteristics, the linear polarization is caused by the propagation rate being different. The light rotates, so in the first figure, a quarter-wave plate 13 with an azimuth angle of 45 is used to convert the p-wave and S-wave of the signal beam into circularly polarized r-waves and l-waves, respectively. To a solution with optical rotation characteristics, where p wave and s wave can be expressed as J wave, s, (4,%) and (A, 15) 15 20 moment broken into P wave V, S wave: 〇 · 1 respectively Amplitude and frequency of P wave and S wave, and then converted by λ / 4 wave plate. __ ^ Page ¢ The paper size is applicable to China National Standards & (CNS) A4 specifications (21〇χ 297 公 爱)-• % Tier 1 U ------ ^ --------- Line --- 1 (Please read the notes on the back before filling out this page) 508437 A7 B7 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs Fifth, the description of the invention () into R wave and L wave, which can be written as R wave · (Ι / Α) # — A. and L wave R wave and L wave pass through the solution of the object under test 140 Can be written as R, wave ·· (1 忑) Ape t + a; L 'wave ... (1 / λ / 1, Μ〆 (~ + ~) 5 where sum represents the phase change caused by the different propagation speeds of the R wave and the L wave in the optically active medium. The rotation angle of linearly polarized light can be obtained in 5 = (θκ—θ〇 / 2. When the R 'wave and L' wave pass through a 50:50 polarized light splitter (PBS), the light is split into 150, and The R 'wave and L' in the polarization direction of the P wave will be converted into (Ap / W) 10 and (As / A)% ί (ω pt + Θ R)
〜產生外差干涉並由第二光偵檢器D 160所接收、轉換為第一資料信號之電信號輸出。Dp所輸 出的第一資料信號可寫成~ An electrical signal that generates heterodyne interference and is received by the second optical detector D 160 and converted into a first data signal is output. The first data signal output by Dp can be written as
Ip( 全 As2+ApAscos( Ay t+ΑΘ)· •⑴Ip (Full As2 + ApAscos (Ay t + ΑΘ) · • ⑴
其中ΔΘ = 0R — 0L ’=% - % ;同理’通過S波偏極化方向的R e’Kt+θβ和《八〆*) 〇 e i(cost+0L)。 >參考光束經過光分析片121而產生外差干涉,並由第 光偵檢器A 122接收轉換為一參考信號,A所輸出的 笫7頁 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) —「TIT·——!· --------t---------線· (請先,閲讀背面之注意事項再填寫本頁) - 508437 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明(Γ ) 參考信號可寫成Wherein ΔΘ = 0R — 0L ′ =%-%; the same way ′ passes through the polarization direction of S wave R e ′ Kt + θβ and “Hachi〆 *) 〇 e i (cost + 0L). > The reference beam passes through the light analysis sheet 121 to generate heterodyne interference, and is received and converted into a reference signal by the first photodetector A 122. The A7 pages output by A are in accordance with Chinese National Standard (CNS) A4 specifications. (210 X 297 mm) — "TIT · ——! · -------- t --------- line · (Please read the notes on the back before filling this page)- 508437 Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7 V. Description of invention (Γ) The reference signal can be written as
Ir(z^t)=(Ap’)2+(As’)2+2Ap’As’cos( J 必/)...................(2) 其中(Ap,,As’)為參考光中P波和S波的振幅。Ir (z ^ t) = (Ap ') 2+ (As') 2 + 2Ap'As'cos (J must /) ... (2 ) Where (Ap, As') is the amplitude of the P and S waves in the reference light.
Ip(*t),和Ir (如0分別輸入處理裝置2,先經過以咖為 5 中心頻率之帶通濾波器161和123將直流信號濾除,則 Ιρ(」Μ) =ApAscos(ztot+ ΔΘ)...................................(3) ΙΓ( ζίώ; t)=2 Ap J As ? c o s (^ 〇.......................................(4) 其中將Ir (如t)通過一 tt/2相位偏移器124,使其相對於 第一資料信號偏移π/2,使得 10 ΙΓ( Δω t)=2 Ap J As 5 sin( ζΐώ; /).......................................(5) 再輸入乘法器190和Ip(zto〇信號相乘而得到 I1(zi^i)=ApAscos(zkyi+A^) · 2Ap,As,sin(.............(6) 在低濃度的條件下Δ&〇,則 Ιχ{Αωί)^ 2I0[cos( zky/)- A^sin( J^/)]sin( Δωϊ) 15 =I〇[sin(2 Αωί)+ A^cos(2 Δωί)]Λ0 ί^θ..................(7) 通過一低通濾波器200後,輸出的直流輸出信號為 Ιι^Κδ^Ι〇|^~4|=^Ι〇|4........................................(8) 其中I〇=ApAp,AsAs,,5為旋轉角度。由本發明可得 到一放大21。倍之旋轉角度信號,就可以由後續的計算處 20理裝置210計算出旋光角度和相關之物理量。 當然,如熟於此技者所能輕易理解,前述較佳實施例 中’穿過待測物140的信號光束在經過極化分光器15〇分 光*後’ S波偏極化方向產生的外差干涉也可由第三光偵檢 器Ds 170接收並轉換為第二資料信號,並可寫成 --— :—^ 第 8頁 本紙張尺度過用1F回囵豕“準(CNS)A4規恪(210 X 297公釐) J.— ^ 7* 1 ^------------1. (請t閱讀背面之注意事項再填寫本頁) 508437 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明(么)Ip (* t), and Ir (such as 0 are input to the processing device 2 respectively, and the DC signal is filtered through the band-pass filters 161 and 123 with the center frequency of 5 as the first, then Ιρ (″ Μ) = ApAscos (ztot + ΔΘ ) ............ (3) ΙΓ (ζίώ; t) = 2 Ap J As ? cos (^ 〇 ....................................... (4) where Ir (Such as t) by a tt / 2 phase shifter 124, which is shifted by π / 2 from the first data signal, so that 10 Γ (Δω t) = 2 Ap J As 5 sin (ζΐώ; /) .. ..................................... (5) Input the multiplier 190 and Ip (zto〇 again. Multiply the signals to get I1 (zi ^ i) = ApAscos (zkyi + A ^) 2Ap, As, sin (............. (6) Δ & under low concentration conditions 〇 , Ιχ {Αωί) ^ 2I0 [cos (zky /)-A ^ sin (J ^ /)] sin (Δωϊ) 15 = I〇 [sin (2 Αωί) + A ^ cos (2 Δωί)] Λ0 ί ^ θ ............ (7) After passing a low-pass filter 200, the output DC output signal is Ιι ^ Κδ ^ Ι〇 | ^ ~ 4 | = ^ Ι〇 | 4 .............. (8) where I 〇 = ApAp, AsAs ,, 5 is the rotation angle. According to the present invention, a magnification of 21. is obtained. The signal can be calculated by the subsequent computing unit 20 processing device 210 to calculate the angle of rotation and related physical quantities. Of course, as those skilled in the art can easily understand, the signal passing through the object 140 in the foregoing preferred embodiment can be easily understood. After the beam has passed through the polarization beam splitter 15o *, the heterodyne interference generated by the polarization direction of the S wave can also be received by the third optical detector Ds 170 and converted into a second data signal, which can be written as ---: — ^ P. 8 This paper has passed the standard of 1F. “CNS” A4 (210 X 297 mm) J.— ^ 7 * 1 ^ ------------ 1 (Please read the notes on the back before filling out this page) 508437 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7 V. Description of the invention (?)
Is(^t)=iAp2+lAs2-ApAscos(^t+A0).....................(9) 隨後把第一資料信號Ιρ(Δα〇和第二資料信號以 輸入差動放大器180相減並放大,形成一 Balance detector 平衡電路而能有效的降低系統雜訊(c〇imn〇n mode noise) 5提南SNR值,差動放大器i8〇所輸出的信號為 Id(^〇 = 2 r [ApAscos(zI^/+a^)] ..................(10) 將差動放大器180輸出的信號輸入乘法器190,和經 過冗/2相位偏輕器124偏移後的參考信號Ir (」以)相乘, 同樣經過低通濾波器200後得到 10 12 = 2Ι0 γ |Δ^ = 4Ι〇 γ |4..................................(11) 其中7為差動放大器之增益。由I〆 Eq(8)和Ι2,Eq(l 1) 得知’本發明可大幅提昇旋轉角5之偵測靈敏度並可偵測 相關之物理量。 另外,如第四圖本案第三較佳實施例所示,當光源為 15 雙頻率相互垂直圓偏極化(circular polarization)雷射光 源’例如圓偏極化Zeeman雷射101,則穩頻雷射光源裝 置1可簡化,為雷射101和一分光元件120,參考光束的光 路上,也要對應設置極化方向可調整在P波(X-軸)方向或 S波(y-軸)方向的極化光分析片121,以產生和Eq(2)同性 20質的外差干涉參考信號。 同樣把第二實施例中的穩頻雷射光源裝置用第三較佳 賓^施例的光源裝置取代,就成為第五圖本案第四較佳實施 例的悲樣。 _ 第9頁 本纸張尺度適用中國國家標準(CNS)A4規恪(210 X 297公釐) ΊΊ M —i I · 11-----^-----— III (請先閱讀背面之注意事項再填寫本頁) · 508437 經濟部智慧財產局員工消費合作社印製 120.. .分光元件 122、160、170···光偵檢器 124··· 7Γ/2相位偏移器 140.. .待測物 180.. .差動放大器 200.. .低通濾波器 300.. .鎖相放大器 A7 B7 五、發明說明(7) 當然,如第六圖本發明第五較佳實施例,把第一較佳 實施例中的處理裝置以鎖相放大器300取代,量取相位差 ,並求出旋光角度5的大小。 綜上所述’本發明確能藉上揭之構造將旋光角度放大 5 並以DC信號大小量測,無論在偵測靈敏度和有效量測範 圍均大幅提高,本發明係一開創性發明,符合發明專利之 新穎進步要件’惟上揭圖示及說明僅為了解本發明實施例 而已,非為限定本發明之實施,凡熟悉該項技藝人士依本 發明特徵範圍因素所作之其他等效變化或修飾皆應涵蓋在 10 以下申請專利範圍内。附件即為利用第六圖的光學架構完 成之糖溶液之濃度和相位差變化的線性圖形,可供證明本 發明方法的可行性。 【元件標號對照表】 1···穩頻雷射光源裝置 2···處理裝置 15 1 〇〇…線偏極化Zeeman雷射101···圓偏極化Zeeman雷射 110···二分之一波片 121···極化光分析片 123、161…帶通濾波器 130···四分之一波片 20 150···極化光分光器 190…乘法器 210···計算處理裝置 第10頁 本紙張尺度適用中國國豕標準(CNS)A4規格(210 X 297公爱) —ΓΙΤ — U----------------^--------- (請先閱讀背面之注意事項再填寫本頁)Is (^ t) = iAp2 + lAs2-ApAscos (^ t + A0) ......... (9) Then the first data signal Ιρ (Δα 〇 Subtract and amplify the second data signal with the input differential amplifier 180 to form a Balance detector, which can effectively reduce system noise (coimn〇n mode noise) 5 Raise the SNR value of the south, the differential amplifier i8 〇 The output signal is Id (^ 〇 = 2 r [ApAscos (zI ^ / + a ^)] .. (10) The differential amplifier 180 The output signal is input to the multiplier 190, and is multiplied by the reference signal Ir ("by") after being shifted by the redundant / 2 phase biaser 124. Similarly, after passing the low-pass filter 200, 10 12 = 2Ι0 γ | Δ ^ = 4Ι〇γ 4 .............. (11) where 7 is the gain of the differential amplifier From I〆Eq (8) and I2, Eq (l 1), it is learned that the present invention can greatly improve the detection sensitivity of the rotation angle 5 and can detect the relevant physical quantity. In addition, as shown in the fourth figure, the third one is better in this case. As shown in the embodiment, when the light source is a 15-frequency mutual circular circular polarization laser light source, such as a circularly polarized Zeeman laser 101, the stable frequency laser light source device 1 may Simplified, for the laser 101 and a beam splitter 120, the optical path of the reference beam must also be set correspondingly. The polarization direction can be adjusted in the P-wave (X-axis) direction or S-wave (y-axis) direction. Slice 121 to generate a heterodyne interference reference signal of the same quality as Eq (2). Similarly, the frequency-stabilized laser light source device in the second embodiment is replaced with the light source device in the third preferred embodiment, and becomes the first. Five pictures The sad example of the fourth preferred embodiment of this case. _ Page 9 This paper size applies Chinese National Standard (CNS) A4 (210 X 297 mm) ΊΊ M —i I · 11 ----- ^ -----— III (Please read the notes on the back before filling this page) · 508437 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 120.. 124 ... 7Γ / 2 phase shifter 140 ... DUT 180 ... Differential amplifier 200 ... Low pass filter 300 ... Phase-locked amplifier A7 B7 V. Description of the invention (7) Of course, as shown in the sixth preferred embodiment of the present invention in FIG. 6, the processing device in the first preferred embodiment is replaced by a lock-in amplifier 300, and the phase difference is measured and calculated. The size of the rotation angle 5. In summary, the present invention can indeed enlarge the rotation angle by 5 and measure it with the size of the DC signal. The detection sensitivity and the effective measurement range are greatly improved. A groundbreaking invention conforms to the novel and progressive requirements of the invention patent. However, the illustrations and descriptions disclosed above are only for understanding the embodiments of the present invention, and are not intended to limit the implementation of the present invention. All other equivalent changes or modifications should be covered by the scope of patent application below 10. The appendix is a linear graph of the changes in the concentration and phase difference of the sugar solution completed using the optical architecture of Figure 6, which can prove the feasibility of the method of the present invention. [Comparison of component numbers] 1 ··· Stable frequency laser light source device 2 ···· Processing device 15 1 〇〇 ... Linearly polarized Zeeman laser 101 ··· Circularly polarized Zeeman laser 110 ·· 二Half-wave plate 121 ... Polarized light analysis plates 123, 161 ... Bandpass filter 130 ... Quarter-wave plate 20 150 ... Polarized light beam splitter 190 ... Multiplier 210 ... Calculation and processing device page 10 This paper size applies to China National Standard (CNS) A4 specification (210 X 297 public love) —ΓΙΤ — U ---------------- ^ --- ------ (Please read the notes on the back before filling this page)
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