TW201403026A - Apparatus for low coherence optical imaging - Google Patents
Apparatus for low coherence optical imaging Download PDFInfo
- Publication number
- TW201403026A TW201403026A TW102137599A TW102137599A TW201403026A TW 201403026 A TW201403026 A TW 201403026A TW 102137599 A TW102137599 A TW 102137599A TW 102137599 A TW102137599 A TW 102137599A TW 201403026 A TW201403026 A TW 201403026A
- Authority
- TW
- Taiwan
- Prior art keywords
- sample
- low
- optical imaging
- unit
- imaging device
- Prior art date
Links
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
Description
本創作係關於一種低同調干涉光學成像裝置，尤指一種可同時取得樣本不同深度之資訊之低同調干涉光學成像裝置。 This creation is about a low-coherence interference optical imaging device, especially a low-coherence interference optical imaging device that can simultaneously obtain information on different depths of a sample.
光學同調性斷層攝影術(Optical Coherence Tomography；OCT)是近十年開始發展的影像技術，其技術的前身為光學低同調反射術(Optical Coherence Domain Reflectometry；OCDR)，該光學低同調反射術係利用低同調性光源(low coherence light source)在時間同調上的特性，其於一干涉儀中能產生極短干涉條紋之長度來達到造影的效果。 Optical Coherence Tomography (OCT) is an imaging technique that has been developed in the past decade. Its technology was formerly known as Optical Coherence Domain Reflectometry (OCDR), which is used in the optical coherence reflexology. The low coherence light source has a characteristic of time coherence, which can produce a very short interference fringe length in an interferometer to achieve the contrast effect.
其解析度如以下之方程式所示：lc=0.441 x(λ0 2/△λ) Its resolution is as shown in the following equation: l c =0.441 x(λ 0 2 /△λ)
其中，lc為光源的同調長度，亦即造影的縱向解析度，λ0為中心波長，△λ為頻譜寬度。 Where l c is the coherence length of the light source, that is, the longitudinal resolution of the contrast, λ 0 is the center wavelength, and Δλ is the spectrum width.
理論上，當光源的頻譜越寬，干涉條紋之長度越短，相對造影的解析度就越高。其主要係作為量測光學元件不同折射率界面的方法。 In theory, the wider the spectrum of the light source, the shorter the length of the interference fringes, and the higher the resolution of the contrast. It is mainly used as a method of measuring the different refractive index interfaces of optical elements.
光學同調性斷層攝影術主要係結合光學低同調反射術在縱向解析度上的技術，利用參考端上一維的縱向掃描，以及樣本端上二維的橫向掃描，並配合透鏡聚焦提高橫向解析度，即可實現待測物的三維斷層掃描影像。 Optical coherence tomography is a technique that combines the low resolution of optical homomorphism in the longitudinal resolution, using one-dimensional longitudinal scanning on the reference end, and two-dimensional lateral scanning on the sample end, combined with lens focusing to improve lateral resolution. , the three-dimensional tomographic image of the object to be tested can be realized.
請參閱第1圖，係習用光學同調性斷層攝影術之示意圖。如圖所示，其主要件利用一低同調光源12產生一光束121，該光束121經一準直鏡141 準直後投射至一分光鏡14上，由分光鏡14將光束121分為一樣本光束123及一參考光束125。 Please refer to Figure 1, which is a schematic diagram of a conventional optical tonal tomography. As shown, the main component utilizes a low coherent light source 12 to produce a beam 121 that passes through a collimating mirror 141. After collimation, it is projected onto a beam splitter 14, and the beam 121 is split by the beam splitter 14 into an equal beam 123 and a reference beam 125.
其中，樣本光束123經由一聚焦鏡143聚焦至一樣本17上，經樣本17反射或散射後，部分光線經該聚焦鏡143準直後，由分光鏡14反射，並經聚焦鏡147聚焦至一影像感測器181。參考光束125則由反射鏡145反射後，通過該分光鏡14由聚焦鏡147聚焦至該影像感測器181。利用參考光束125與樣本光束123之光程差造成的干涉現象，由影像感測器181感測訊號後，以一訊號處理單元183進行訊號分析，並由一顯示器185顯示分析結果。 The sample beam 123 is focused onto the same book 17 via a focusing mirror 143. After being reflected or scattered by the sample 17, a portion of the light is collimated by the focusing mirror 143, reflected by the beam splitter 14 and focused by an focusing mirror 147 to an image. Sensor 181. The reference beam 125 is reflected by the mirror 145, and is focused by the focusing mirror 14 to the image sensor 181 through the beam splitter 14. After the image sensor 181 senses the signal by using the interference phenomenon caused by the optical path difference between the reference beam 125 and the sample beam 123, the signal is analyzed by a signal processing unit 183, and the analysis result is displayed by a display 185.
此外，再利用一縱向掃描單元161驅動該反射鏡145上下移動，藉以調整參考光束125之光程，可進行樣本17縱向(深度)的掃描。另以一橫向掃描單元163令樣本光束123在樣本17之表面上移動，可進行樣本17橫向兩個維度的掃描。 In addition, a longitudinal scanning unit 161 is used to drive the mirror 145 to move up and down, thereby adjusting the optical path of the reference beam 125 to perform longitudinal (depth) scanning of the sample 17. In addition, by a lateral scanning unit 163, the sample beam 123 is moved on the surface of the sample 17, and scanning of two lateral dimensions of the sample 17 can be performed.
本發明之一目的，在於提供一種低同調干涉光學成像裝置，尤指一種可同時取得樣本不同深度之資訊之低同調干涉光學成像裝置。 An object of the present invention is to provide a low-coherence interference optical imaging apparatus, and more particularly to a low-coherence interference optical imaging apparatus capable of simultaneously obtaining information of different depths of samples.
本發明之另一目的，在於提供一種低同調干涉光學成像裝置，其主要係利用一相位轉換反射單元，令參考光束於一橫截面上不同位置具有不同的相位，在於取樣光束產生干涉時，可同時取得不同深度之資訊者。 Another object of the present invention is to provide a low-coherence interference optical imaging apparatus, which mainly utilizes a phase-conversion reflection unit, so that the reference beam has different phases at different positions on a cross-section, when the sampling beam generates interference. At the same time, people who have obtained different depths of information.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，其相位轉換反射單元係為一微週期結構反射鏡，可令參考光束兩側產生相位差者。 Another object of the present invention is to provide a low coherence interference optical imaging device, wherein the phase conversion reflection unit is a micro-periodic structure mirror, which can cause phase difference on both sides of the reference beam.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，其微週期結構反射鏡係以一光柵為較佳者。 It is still another object of the present invention to provide a low coherence interference optical imaging apparatus in which a micro-periodic structure mirror is preferably a grating.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，利用一光束位移單元令參考光束與原光路產生空間位移，並以一光束曲折單元將 之與取樣光束疊合而產生千涉，可同時取得不同深度之資訊者。 Another object of the present invention is to provide a low-coherence interference optical imaging apparatus that utilizes a beam displacement unit to spatially shift a reference beam from an original optical path and to use a beam bending unit It is superimposed with the sampled beam to generate thousands of information, and can obtain information of different depths at the same time.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，其光束位移單元包含有一透鏡及一反射鏡，可令參考光束產生空間位移者。 Another object of the present invention is to provide a low coherence interference optical imaging apparatus, the beam displacement unit comprising a lens and a mirror for spatially displacing the reference beam.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，其透鏡係以徑向漸變折射率透鏡為較佳。 It is still another object of the present invention to provide a low coherence interference optical imaging apparatus in which the lens is preferably a radially graded index lens.
本發明之又一目的，在於提供一種低同調干涉光學成像裝置，其光束曲折單元係可以一稜鏡實施者。 It is still another object of the present invention to provide a low coherence interference optical imaging apparatus in which the beam meandering unit can be implemented.
為達成上述目的，本發明提供一種低同調干涉光學成像裝置，其主要係包含有：一低同調光源，用以提供一光束；一主分光器，將該光束分為一樣本光束及一參考光束，該樣本光束投射至一樣本後，部分反射及/或散射之光線形成一取樣光束，該取樣光束係藉由該主分光器導引至一光感測器；一相位轉換反射單元，用以反射該參考光束至一光感測器，並令反射後之參考光束於一橫截面上不同位置具有不同的相位；及一訊號處理單元，連接該光感測器，藉由來自該光感測器之訊號分析該樣本之資訊。 In order to achieve the above object, the present invention provides a low coherence interference optical imaging apparatus, which mainly comprises: a low coherent light source for providing a light beam; and a main optical splitter, the light beam is divided into the same present beam and a reference beam. The sample beam is projected to the same direction, and the partially reflected and/or scattered light forms a sample beam, and the sample beam is guided to the photo sensor by the main beam splitter; a phase conversion reflection unit is used for Reflecting the reference beam to a photo sensor, and causing the reflected reference beam to have different phases at different positions on a cross section; and a signal processing unit connecting the photo sensor by the light sensing The signal of the device analyzes the information of the sample.
本發明尚提供一種低同調干涉光學成像裝置，其主要係包含有：一低同調光源，用以提供一光束；一主分光器，將該光束分為一樣本光束及一參考光束，該樣本光束投射至一樣本後，部分反射及/或散射之光線形成一取樣光束；一光束位移單元，用以反射該參考光束，並令該反射光束產生一位移；一光束曲折單元，反射位移後之參考光束被導引至該光束曲折單元之一端，該取樣光束經由該主分光器導引至該光束曲折單元之另一端，藉由該光束曲折單元令該參考光束與該取樣光束於一光感測器上疊合；及一訊號處理單元，連接該光感測器，藉由來自該光感測器之訊號分析該樣本之資訊。 The present invention further provides a low coherence interference optical imaging apparatus, which mainly comprises: a low coherent light source for providing a light beam; and a main optical splitter, the light beam is divided into the same present beam and a reference beam, the sample beam After being projected to the same, a portion of the reflected and/or scattered light forms a sample beam; a beam displacement unit for reflecting the reference beam and causing the reflected beam to produce a displacement; a beam bending unit, the reference after the reflection displacement The light beam is guided to one end of the beam bending unit, and the sampling beam is guided to the other end of the beam bending unit via the main beam splitter, and the beam bending unit causes the reference beam and the sampling beam to be in a light sensing The device is superimposed; and a signal processing unit is connected to the photo sensor, and the information of the sample is analyzed by a signal from the photo sensor.
10‧‧‧光學同調性斷層攝影裝置 10‧‧‧Optical tonal tomography apparatus
12‧‧‧低同調光源 12‧‧‧Low coherent light source
121‧‧‧光束 121‧‧‧ Beam
123‧‧‧樣本光束 123‧‧‧sample beam
125‧‧‧參考光束 125‧‧‧Reference beam
14‧‧‧分光鏡 14‧‧‧beam splitter
141‧‧‧準直鏡 141‧‧‧ collimation mirror
143‧‧‧聚焦鏡 143‧‧‧ focusing mirror
145‧‧‧反射鏡 145‧‧‧Mirror
147‧‧‧聚焦鏡 147‧‧‧ Focusing mirror
161‧‧‧縱向描單元 161‧‧‧ longitudinal drawing unit
163‧‧‧橫向描單元 163‧‧‧Horizontal drawing unit
17‧‧‧樣本 17‧‧‧ sample
181‧‧‧影像感測器 181‧‧‧Image Sensor
183‧‧‧訊號處理單視 183‧‧‧ Signal processing single vision
185‧‧‧顯示器 185‧‧‧ display
20‧‧‧低同調干涉光學成像裝置 20‧‧‧Low coherent interference optical imaging device
22‧‧‧低同調光源 22‧‧‧Low coherent light source
231‧‧‧光束 231‧‧‧ Beam
233‧‧‧參考光束近端 233‧‧‧Reference beam proximal end
234‧‧‧參考光束 234‧‧‧Reference beam
235‧‧‧參考光束遠端 235‧‧‧Reference beam distal
237‧‧‧樣本光束 237‧‧‧sample beam
239‧‧‧取樣光束 239‧‧‧Sampling beam
24‧‧‧主分光器 24‧‧‧Main splitter
241‧‧‧準直單元 241‧‧‧ Collimation unit
243‧‧‧聚焦單元 243‧‧‧ Focus unit
245‧‧‧單軸聚焦單元 245‧‧‧Single-axis focusing unit
25‧‧‧相位轉換反射單元 25‧‧‧ phase conversion reflection unit
251‧‧‧微週期結構反射鏡 251‧‧‧Microcycle structure mirror
253‧‧‧微結構 253‧‧‧Microstructure
26‧‧‧掃描單元 26‧‧‧Scan unit
27‧‧‧樣本 27‧‧‧ sample
281‧‧‧光感測器 281‧‧‧Light sensor
283‧‧‧訊號處理單元 283‧‧‧Signal Processing Unit
285‧‧‧顯示器 285‧‧‧ display
30‧‧‧低同調干涉光學成像裝置 30‧‧‧Low coherent interference optical imaging device
333‧‧‧參考光束內側 333‧‧‧ reference beam inside
335‧‧‧參考光束外側 335‧‧‧ outside the reference beam
35‧‧‧光束位移單元 35‧‧‧ Beam Displacement Unit
351‧‧‧透鏡 351‧‧‧ lens
353‧‧‧反射鏡 353‧‧‧Mirror
355‧‧‧光軸 355‧‧‧ optical axis
356‧‧‧光束曲折單元 356‧‧‧beam bending unit
357‧‧‧稜鏡 357‧‧‧稜鏡
39‧‧‧單軸散焦單元 39‧‧‧Single-axis defocusing unit
40‧‧‧低同調干涉光學成像裝置 40‧‧‧Low coherent interference optical imaging device
431‧‧‧觀測光束 431‧‧‧Observation beam
44‧‧‧觀測分光器 44‧‧‧Observing beam splitter
481‧‧‧影像感測器 481‧‧‧Image Sensor
50‧‧‧低同調干涉光學成像裝置 50‧‧‧Low coherent interference optical imaging device
531‧‧‧觀測光束 531‧‧‧Observation beam
54‧‧‧觀測分光器 54‧‧‧Observing beam splitter
581‧‧‧影像感測器 581‧‧‧Image Sensor
60‧‧‧低同調干涉光學成像裝置 60‧‧‧Low coherent interference optical imaging device
65‧‧‧光束位移單元 65‧‧‧ Beam Displacement Unit
651‧‧‧色散補償器 651‧‧‧Dispersion compensator
653‧‧‧背向反射鏡 653‧‧‧Back mirror
67‧‧‧光束曲折單元 67‧‧‧ beam bending unit
671‧‧‧第一反射鏡 671‧‧‧First mirror
673‧‧‧第二反射鏡 673‧‧‧second mirror
675‧‧‧第三反射鏡 675‧‧‧third mirror
第1圖：係習用光學斷層掃描裝置之示意圖。 Figure 1: Schematic diagram of a conventional optical tomography apparatus.
第2圖：係本發明一實施例之構造示意圖。 Fig. 2 is a schematic view showing the construction of an embodiment of the present invention.
第3圖：係本發明另一實施例之構造示意圖。 Fig. 3 is a schematic view showing the configuration of another embodiment of the present invention.
第4圖：係本發明又一實施例之構造示意圖。 Fig. 4 is a schematic view showing the configuration of still another embodiment of the present invention.
第5圖：係本發明又一實施例之構造示意圖。 Fig. 5 is a schematic view showing the configuration of still another embodiment of the present invention.
第6圖：係本發明又一實施例之構造示意圖。 Figure 6 is a schematic view showing the configuration of still another embodiment of the present invention.
請參閱第2圖，係本發明一實施例之構造示意圖。如圖所示，本發明之低同調干涉光學成像裝置20主要包含有：一低同調光源22、一主分光器24、一相位轉換反射單元25、一樣本27、一光感測器281及一訊號處理單元283。 Please refer to FIG. 2, which is a schematic structural view of an embodiment of the present invention. As shown in the figure, the low coherence interference optical imaging device 20 of the present invention mainly comprises: a low coherent light source 22, a main beam splitter 24, a phase conversion reflecting unit 25, the same 27, a light sensor 281 and a Signal processing unit 283.
其中，該低同調光源22可提供一低同調光束231，該低同調光束231投射至主分光器24後，分為一參考光束234及一樣本光束237。該樣本光束237投射至樣本27之後，部分反射及/或散射之光線形成一取樣光束239，該取樣光束239經主分光器24反射後投射至光感測器281上。該參考光束234經該相位轉換反射單元25反射之後，其參考光束內側233與參考光束外側235將產生相位差。 The low-coherent light source 22 can provide a low-coherent light beam 231. After the low-coherent light beam 231 is projected to the main beam splitter 24, it is divided into a reference beam 234 and an identical beam 237. After the sample beam 237 is projected onto the sample 27, the partially reflected and/or scattered light forms a sample beam 239 that is reflected by the main beam splitter 24 and projected onto the photo sensor 281. After the reference beam 234 is reflected by the phase conversion reflection unit 25, its reference beam inner side 233 and reference beam outer side 235 will produce a phase difference.
在本實施例中，該相位轉換反射單元25係以一微週期結構反射鏡251實施。其中，該微週期結構反射鏡251包含有複數個週期性重複之微結構253。由於參考光束234投射到該微週期結構反射鏡251時，在參考光束234的寬度範圍內涵蓋有複數個微結構253，各微結構253與主分光器24之距離不同，造成參考光束近端233至參考光束遠端235之間，每個微結構253所反射之參考光束皆具有不同的光程及相位。 In the present embodiment, the phase shifting reflection unit 25 is implemented by a micro period structural mirror 251. The micro-period structure mirror 251 includes a plurality of periodically repeating microstructures 253. Since the reference beam 234 is projected onto the micro-periodic structure mirror 251, a plurality of microstructures 253 are covered within the width of the reference beam 234, and the distances of the microstructures 253 from the main beam splitter 24 are different, resulting in the proximal end of the reference beam 233. Between the distal ends 235 of the reference beam, the reference beams reflected by each of the microstructures 253 have different optical paths and phases.
因此，當反射後之參考光束234與取樣光束239在光感測器281上產生干涉時，由於參考光束234具有不同的相位，故可同時與來自該樣本27 不同深度之取樣光束239產生建設性干涉條紋。光感測器281可產生與干涉條紋相對應之訊號，並傳送到訊號處理單元283進行分析，藉以同時獲取樣本27不同深度之資訊。 Therefore, when the reflected reference beam 234 and the sampled beam 239 interfere on the photo sensor 281, since the reference beam 234 has a different phase, it can be simultaneously with the sample 27 Sampled beams 239 of different depths produce constructive interference fringes. The light sensor 281 can generate a signal corresponding to the interference fringe and transmit it to the signal processing unit 283 for analysis, thereby simultaneously obtaining information of different depths of the sample 27.
本發明之低同調干涉光學成像裝置20尚可包含有一掃描單元26，設置於分光器24與樣本27之間，可改變樣本光束237在樣本27上的落點，藉以進行該樣本27之橫向掃描。 The low-coherence interference optical imaging device 20 of the present invention may further include a scanning unit 26 disposed between the beam splitter 24 and the sample 27 to change the falling point of the sample beam 237 on the sample 27, thereby performing lateral scanning of the sample 27. .
另外，本發明之低同調干涉光學成像裝置20尚可包含有一準直單元241、一聚焦單元243及一單軸聚焦單元245。可利用準直單元341準直該低同調光源22所產生之光束231。聚焦單元243可將樣本光束237聚焦於樣本27上，同時可將取樣光束239予以準直。單軸聚焦單元245則可將參考光束234與取樣光束239於光感測器281上聚焦為一直線。而訊號處理單元283分析所得之樣本資訊，則可利用一顯示器285加以顯示。 In addition, the low coherence interference optical imaging device 20 of the present invention may further include a collimation unit 241, a focusing unit 243, and a single axis focusing unit 245. The collimating unit 341 can be used to collimate the light beam 231 generated by the low coherent light source 22. Focusing unit 243 can focus sample beam 237 onto sample 27 while collimating sample beam 239. The uniaxial focusing unit 245 can focus the reference beam 234 and the sample beam 239 onto the photo sensor 281 in a straight line. The signal processing unit 283 analyzes the obtained sample information, and can display it by using a display 285.
本實施例中，該微週期結構反射鏡251係可以一光柵實施。 In this embodiment, the micro-period structure mirror 251 can be implemented by a grating.
請參閱第3圖，係本發明另一實施例之構造示意圖。如圖所示，本實施例之低同調干涉光學成像裝置30，其主要構造與第2圖所示實施例大致相同，惟，本實施例採用一光束位移單元35及一光束曲折單元356進行參考光束334之相位轉換及其與取樣光束239之疊合。 Please refer to FIG. 3, which is a schematic structural view of another embodiment of the present invention. As shown in the figure, the main configuration of the low-coherence interference optical imaging device 30 of the present embodiment is substantially the same as that of the embodiment shown in FIG. 2, but the present embodiment uses a beam displacement unit 35 and a beam bending unit 356 for reference. The phase transition of beam 334 and its superposition with sample beam 239.
其中，該光束位移單元35包含有一透鏡351及一反射鏡353。當參考光束334通過透鏡351時，參考光束內側333與參考光束外側335被偏折的角度不同，而經由該反射鏡353反射後再次通過透鏡351，導致參考光束334離開該光束位移單元35時，參考光束內側333之光程與參考光束外側335之光程不相同。故，參考光束334離開相位轉換反射單元35時，同一橫截面中不同的位置具有不同的相位。本實施例中，係以參考光束內側333之光程小於參考光束外側335之狀況為例進行說明。 The beam displacement unit 35 includes a lens 351 and a mirror 353. When the reference beam 334 passes through the lens 351, the reference beam inner side 333 is different from the reference beam outer side 335 by an angle, and is reflected by the mirror 353 and then passes through the lens 351 again, causing the reference beam 334 to exit the beam displacement unit 35. The optical path of the inner side 333 of the reference beam is different from the optical path of the outer side 335 of the reference beam. Therefore, when the reference beam 334 leaves the phase conversion reflection unit 35, different positions in the same cross section have different phases. In this embodiment, the case where the optical path of the inner side 333 of the reference beam is smaller than the outer side 335 of the reference beam is taken as an example.
由於參考光束334通過該光束位移單元35時，產生一空間位移而離開 原來的光路，故本發明利用一光束曲折單元356將參考光束334與取樣光束239加以曲折而可於光感測器281上疊合。此時，由於參考光束334自其內側333至外側335分別具有不同的相位，可同時與來自該樣本27不同深度之取樣光束239產生建設性的干涉條紋。藉由光感測器281產生對應該干涉條紋之訊號，並以訊號處理單元283進行分析，即可同時取得該樣本27不同深度之資訊，並以顯示器285加以顯示。 When the reference beam 334 passes through the beam displacement unit 35, a spatial displacement is generated to leave The original optical path, the present invention utilizes a beam bending unit 356 to bend the reference beam 334 and the sample beam 239 to be superimposed on the photo sensor 281. At this time, since the reference beam 334 has different phases from the inner side 333 to the outer side 335, respectively, constructive interference fringes can be generated simultaneously with the sample beam 239 having a different depth from the sample 27. The signal corresponding to the interference fringe is generated by the photo sensor 281, and analyzed by the signal processing unit 283, and the information of the different depths of the sample 27 can be simultaneously acquired and displayed on the display 285.
其中，該透鏡351係以徑向漸變折射率(Radial Gradient Index；RGIN)透鏡之態樣為較佳。光束曲折單元356則可以一稜鏡357實施，令取樣光束239與參考光束334分別由稜鏡357之兩側通過，經曲折之後於光感測器281上疊合。 Among them, the lens 351 is preferably in the form of a Radial Gradient Index (RGIN) lens. The beam bending unit 356 can be implemented at one turn 357, so that the sample beam 239 and the reference beam 334 are respectively passed by the sides of the crucible 357, and are folded over the photo sensor 281 after being meandered.
本實施例尚可於該光束曲折單元356與光感測器281之間設置一單軸聚焦單元245，藉以將取樣光束239及參考光束334聚焦於一直線上，而該光感測器281則可使用一維光感測器。 In this embodiment, a single-axis focusing unit 245 is disposed between the beam bending unit 356 and the photo sensor 281, so that the sampling beam 239 and the reference beam 334 are focused on a straight line, and the photo sensor 281 can be Use a one-dimensional light sensor.
另可於該單軸聚焦單元245與光束曲折單元357之間，或單軸聚焦單元245與光感測器281之間增設一單軸散焦單元39，並令其散焦的維度與單軸聚焦單元245之聚焦維度垂直。如此之設置，可擴大參考光束334與取樣光束239在光感測器281上聚焦之寬度，可有效提高低同調干涉光學成像裝置之縱向掃描範圍。 Alternatively, a single-axis defocusing unit 39 may be added between the single-axis focusing unit 245 and the beam bending unit 357, or between the single-axis focusing unit 245 and the photo sensor 281, and the defocusing dimension and the single axis may be The focus dimension of the focusing unit 245 is vertical. With such an arrangement, the width of the reference beam 334 and the sample beam 239 on the photo sensor 281 can be enlarged, which can effectively improve the longitudinal scanning range of the low coherence interference optical imaging device.
請參閱第4圖，係本發明又一實施例之構造示意圖。如圖所示，本實施例之低同調干涉光學成像裝置40，其主要構造與第2圖所述實施例大致相同，惟，本實施例之主分光器24與樣本27之間尚設有一觀測分光器44，並設置有一影像感測器481，連接至該訊號處理單元283。 Please refer to FIG. 4, which is a schematic structural view of still another embodiment of the present invention. As shown in the figure, the main structure of the low-coherence interference optical imaging device 40 of the present embodiment is substantially the same as that of the embodiment shown in FIG. 2, but there is still an observation between the main beam splitter 24 and the sample 27 of this embodiment. The optical splitter 44 is provided with an image sensor 481 connected to the signal processing unit 283.
該觀測分光器44可將取樣光束239分出一部分，成為一觀測光束431。該觀測光束431投射至影像感測器481上，影像感測器481取得影像訊號後，傳送至訊號處理單元283，即可於顯示器285上顯示樣本27表面之狀 態。 The observation beam splitter 44 splits the sample beam 239 into a portion of the observation beam 431. The observation beam 431 is projected onto the image sensor 481. After the image sensor 481 obtains the image signal, the image sensor 481 transmits the image signal to the signal processing unit 283, and the surface of the sample 27 is displayed on the display 285. state.
請參閱第5圖，係本發明又一實施例之構造示意圖。如圖所示，本實施例之低同調干涉光學成像裝置50，其主要構造與第3圖所述實施例大致相同，惟，本實施例之主分光器24與樣本27之間尚設有一觀測分光器54，並設置有一影像感測器581，連接至該訊號處理單元283。 Please refer to FIG. 5, which is a schematic structural view of still another embodiment of the present invention. As shown in the figure, the main structure of the low-coherence interference optical imaging device 50 of the present embodiment is substantially the same as that of the embodiment shown in FIG. 3, but there is still an observation between the main beam splitter 24 and the sample 27 of this embodiment. The beam splitter 54 is provided with an image sensor 581 connected to the signal processing unit 283.
該觀測分光器54可將取樣光束239分出一部分，成為一觀測光束531。該觀測光束531投射至影像感測器581上，影像感測器581取得影像訊號後，傳送至訊號處理單元283，即可於顯示器285上顯示樣本27表面之狀態。 The observation beam splitter 54 splits the sample beam 239 into a portion of the observation beam 531. The observation beam 531 is projected onto the image sensor 581. After the image sensor 581 acquires the image signal, the image sensor 581 transmits the image signal to the signal processing unit 283 to display the state of the surface of the sample 27 on the display 285.
請參閱第6圖，係本發明又一實施例之構造示意圖。如圖所示，本實施例之低同調干涉光學成像裝置60，其主要構造與第3圖所述實施例大致相同，惟，本實施例之光束位移單元65使用一色散補償器651與背向反射器653之組合，而光束曲折單元67則使用一反射鏡組實施。 Please refer to FIG. 6 , which is a schematic structural view of still another embodiment of the present invention. As shown in the figure, the low-coherence interference optical imaging device 60 of the present embodiment has a main structure substantially the same as that of the embodiment shown in FIG. 3. However, the beam displacement unit 65 of the present embodiment uses a dispersion compensator 651 and a back direction. The combination of reflectors 653, and the beam meandering unit 67 is implemented using a mirror set.
該反射鏡組包含有一第一反射鏡671、第二反射鏡673及第三反射鏡675。首先利用第一反射鏡671改變參考光束334與取樣光束239之方向，再分別以第二反射鏡673與第三反射鏡675以適當角度將參考光束334與取樣光束239反射至光感測器281，藉以形成干涉圖形。 The mirror group includes a first mirror 671, a second mirror 673, and a third mirror 675. First, the direction of the reference beam 334 and the sample beam 239 is changed by the first mirror 671, and the reference beam 334 and the sample beam 239 are reflected to the photo sensor 281 at an appropriate angle by the second mirror 673 and the third mirror 675, respectively. In order to form an interference pattern.
本實施例中，同樣可使用一單軸聚焦單元245將參考光束334與取樣光束239聚焦於一直線上，而該光感測器281亦可使用一維光感測器。 In this embodiment, a single-axis focusing unit 245 can also be used to focus the reference beam 334 and the sample beam 239 on a straight line, and the photo sensor 281 can also use a one-dimensional photo sensor.
此外，尚可於光束曲折單元67與光感測器281之間設置一單軸散焦單元39，並令其散焦的維度與單軸聚焦單元245之聚焦維度垂直。如此之設置，可擴大參考光束334與取樣光束239在光感測器281上聚焦之寬度，可有效提高低同調干涉光學成像裝置之縱向掃描範圍。 In addition, a single-axis defocusing unit 39 is disposed between the beam meandering unit 67 and the photo sensor 281, and the defocusing dimension is perpendicular to the focusing dimension of the uniaxial focusing unit 245. With such an arrangement, the width of the reference beam 334 and the sample beam 239 on the photo sensor 281 can be enlarged, which can effectively improve the longitudinal scanning range of the low coherence interference optical imaging device.
上述第3圖及第6圖所示實施例中，光束位移單元35、65及光束曲折單元356、67可交互搭配使用，皆可達到同時獲取樣本27不同深度資訊之 目的。 In the embodiments shown in FIG. 3 and FIG. 6 , the beam displacement units 35 and 65 and the beam bending units 356 and 67 can be used in combination to obtain different depth information of the sample 27 at the same time. purpose.
以上所述者，僅為本發明之實施例而已，並非用來限定本發明實施之範圍，即凡依本發明申請專利範圍所述之形狀、構造、特徵、方法及精神所為之均等變化與修飾，均應包括於本發明之申請專利範圍內。 The above is only the embodiment of the present invention, and is not intended to limit the scope of the present invention, that is, the equivalent changes and modifications of the shapes, structures, features, methods and spirits described in the claims of the present invention. All should be included in the scope of the patent application of the present invention.
22‧‧‧低同調光源 22‧‧‧Low coherent light source
231‧‧‧光束 231‧‧‧ Beam
237‧‧‧樣本光束 237‧‧‧sample beam
239‧‧‧取樣光束 239‧‧‧Sampling beam
24‧‧‧主分光器 24‧‧‧Main splitter
241‧‧‧準直單元 241‧‧‧ Collimation unit
243‧‧‧聚焦單元 243‧‧‧ Focus unit
245‧‧‧聚焦單元 245‧‧‧ Focus unit
26‧‧‧掃描單元 26‧‧‧Scan unit
27‧‧‧樣本 27‧‧‧ sample
281‧‧‧光感測器 281‧‧‧Light sensor
283‧‧‧訊號處理單元 283‧‧‧Signal Processing Unit
285‧‧‧顯示器 285‧‧‧ display
30‧‧‧低同調干涉光學成像裝置 30‧‧‧Low coherent interference optical imaging device
333‧‧‧參考光束內側 333‧‧‧ reference beam inside
335‧‧‧參考光束外側 335‧‧‧ outside the reference beam
35‧‧‧光束位移單元 35‧‧‧ Beam Displacement Unit
351‧‧‧透鏡 351‧‧‧ lens
353‧‧‧反射鏡 353‧‧‧Mirror
355‧‧‧光軸 355‧‧‧ optical axis
356‧‧‧光束曲折單元 356‧‧‧beam bending unit
357‧‧‧稜鏡 357‧‧‧稜鏡
39‧‧‧單軸散焦單元 39‧‧‧Single-axis defocusing unit
Claims (13)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| TW102137599A TWI494540B (en) | 2010-03-29 | 2010-03-29 | Apparatus for low coherence optical imaging |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| TW102137599A TWI494540B (en) | 2010-03-29 | 2010-03-29 | Apparatus for low coherence optical imaging |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| TW201403026A true TW201403026A (en) | 2014-01-16 |
| TWI494540B TWI494540B (en) | 2015-08-01 |
Family
ID=50345487
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| TW102137599A TWI494540B (en) | 2010-03-29 | 2010-03-29 | Apparatus for low coherence optical imaging |
Country Status (1)
| Country | Link |
|---|---|
| TW (1) | TWI494540B (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI494536B (en) * | 2014-04-01 | 2015-08-01 | Crystalvue Medical Corp | Optical measuring device and method |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5489984A (en) * | 1994-04-01 | 1996-02-06 | Imra America, Inc. | Differential ranging measurement system and method utilizing ultrashort pulses |
| JP4786027B2 (en) * | 2000-12-08 | 2011-10-05 | オリンパス株式会社 | Optical system and optical apparatus |
| DE10142001A1 (en) * | 2001-08-28 | 2003-03-20 | Zeiss Carl Jena Gmbh | Method and arrangement for obtaining topographs and tomographs of the eye structure using multiple simultaneous short-coherence interferometric deep scans of the pupil that are obtained simultaneously |
| DE10302849A1 (en) * | 2003-01-23 | 2004-07-29 | Carl Zeiss Meditec Ag | Measuring thickness and dispersion in tissues or bodily fluids using short-coherence interferometry, determines content of substance from its influence on optical characteristics |
| TW200739033A (en) * | 2006-04-07 | 2007-10-16 | Chien Chou | Cross-sectional scanning method using optical image and the apparatus thereof |
| US7460248B2 (en) * | 2006-05-15 | 2008-12-02 | Carestream Health, Inc. | Tissue imaging system |
| US20080100848A1 (en) * | 2006-10-25 | 2008-05-01 | Koji Kobayashi | Optical tomograph |
| US7929144B1 (en) * | 2008-12-16 | 2011-04-19 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Optical system and method for gas detection and monitoring |
-
2010
- 2010-03-29 TW TW102137599A patent/TWI494540B/en active
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI494536B (en) * | 2014-04-01 | 2015-08-01 | Crystalvue Medical Corp | Optical measuring device and method |
Also Published As
| Publication number | Publication date |
|---|---|
| TWI494540B (en) | 2015-08-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| TWI418762B (en) | Apparatus for low coherence optical imaging | |
| JP4505807B2 (en) | Multiplexed spectral interferometric optical coherence tomography | |
| JP6014166B2 (en) | Spectroscopic apparatus and spectral analysis method | |
| JP4916573B2 (en) | Optical interference measurement method and optical interference measurement apparatus | |
| CN102818786B (en) | Sinusoidal phase modulation parallel complex frequency domain optical coherence tomography imaging system and method | |
| JP2007512541A (en) | Method and apparatus for three-dimensional spectrally encoded imaging | |
| US20120232821A1 (en) | Multi-channel optical coherence tomography for imaging and temperature and force sensing | |
| JP2013545113A (en) | Image map optical coherence tomography | |
| CN104204775A (en) | Optical coherence tomography apparatus and optical coherence tomography method | |
| EP2932187A2 (en) | Interferometric apparatus with dispersive element and sample characteristic determining apparatus using such apparatus | |
| Hendargo et al. | Synthetic wavelength based phase unwrapping in spectral domain optical coherence tomography | |
| US20120105861A1 (en) | Device and method for determining optical path lengths | |
| JP2005283155A (en) | Dispersion correcting apparatus in light interference sectional image imaging method | |
| JP4852651B2 (en) | Multiplexed spectral interferometric optical coherence tomography | |
| JP2016017762A (en) | Optical delay device and optical coherence tomography device | |
| US20150077759A1 (en) | Compact, Slope Sensitive Optical Probe | |
| TWI494540B (en) | Apparatus for low coherence optical imaging | |
| JP3934131B2 (en) | Coaxial spatial optical coherence tomographic image measurement device | |
| JP5149923B2 (en) | Multiplexed spectral interferometric optical coherence tomography | |
| JP6917663B2 (en) | Optical interference unit for optical coherence tomography equipment | |
| JP5740701B2 (en) | Interferometer | |
| KR101407062B1 (en) | Optical coherence tomography apparatus for enhanced axial contrast and reference mirror having multiple plane for the same | |
| Mekonnen et al. | Wavelength-encoded multi-channel spectral domain optical coherence tomography (SD-OCT) for spatiotemporally resolved imaging | |
| JP3634327B2 (en) | Optical chromatic dispersion spatial coherence tomographic imaging system | |
| Pernechele et al. | Optical plate thickness measurement with single-shot low coherence interferometry |