CN203828901U - Spectrometer for frequency domain OCT system - Google Patents

Abstract

A spectrometer for a frequency-domain OCT system, the structure of which includes a single-mode optical fiber, an achromatic lens, a blazed grating, a photodetector and a spectrometer base plate, and the single-mode optical fiber, an achromatic lens, a blazed grating and a photodetector are all fixed on the spectrometer bottom plate. The interference light of the OCT system is input to the single-mode fiber, and the output light of the single-mode fiber is collimated by an achromatic lens and irradiated onto the blazed grating. The first-order diffracted light of the diffraction grating is focused by the same achromatic lens and then detected by a photodetector. The system of the utility model has a simple and compact structure, and uses an achromatic lens to simultaneously realize the collimation of the incident light and the focusing of the first-order diffraction light of the diffraction grating, which is beneficial to the miniaturization of the frequency domain OCT system.

Description

Spectrometers for Frequency-Domain OCT Systems

technical field

The utility model relates to a spectrometer, in particular to a spectrometer used in a frequency domain OCT system.

Background technique

Optical coherence tomography (Optical Coherence Tomography, OCT) is a non-invasive high-resolution tomography technology based on low-coherence optical interferometry, which has been widely used in the fields of living biological tissue imaging and subsurface nondestructive testing. Time-domain OCT is the first OCT technology proposed, and the frequency-domain OCT developed later has greater advantages in imaging speed and sensitivity than time-domain OCT, and is the development direction of OCT technology. The frequency-domain OCT system and the time-domain OCT system are both based on the principle of low-coherence optical interference. The difference lies in the detection method of the interference signal: the time-domain OCT detects the interference signal in the time domain, while the frequency-domain OCT uses a spectrometer instead of the time-domain OCT. The point photodetector detects the spectrum of the interfering signal in the frequency domain. In the frequency-domain OCT system, the interference light signals of the reference arm and the detection arm are collimated and incident on the grating, and after being diffracted by the grating, they are focused by an objective lens on the line array photodetector to obtain the interference spectrum of the signal; by inverting the interference spectrum The Fourier transform can obtain the depth-resolved reflectivity information of the measured sample.

Since the frequency-domain OCT technology uses a spectrometer instead of a point photodetector, it reduces one-dimensional scanning compared to the time-domain OCT technology, and has a higher imaging speed. The imaging speed of current ultrafast frequency-domain OCT systems is two orders of magnitude faster than that of the fastest time-domain OCT systems. Frequency-domain OCT technology makes real-time three-dimensional tissue imaging truly possible, which is its most important advantage over time-domain OCT.

Frequency-domain OCT technology was first applied in the diagnosis of ophthalmic diseases. With the continuous improvement of system performance and the development of various functional OCT technologies, the application of frequency-domain OCT technology has become more extensive. It has been widely used in ophthalmology, gastrointestinal Medical, cardiovascular, dental and dermatological disease detection. Various clinical applications have also put forward higher and higher requirements for the frequency-domain OCT system, including the miniaturization and portability of the system and its instrumentation, especially in mature clinical application fields such as ophthalmology. It is hoped that the OCT instrument can be small into a portable handheld.

However, in the spectrometer of the current frequency-domain OCT system, the OCT interference signal is first collimated by a collimator and then incident on the diffraction grating. Interferometric detection. In the spectrometer with this structure, the collimation of the incident beam and the focusing of the diffracted beam are respectively realized by a collimating lens and a focusing lens. The collimation of the incident beam and the focusing of the diffracted beam are separated into two separate optical paths. It is not conducive to the compactness and portability of OCT instruments.

Contents of the invention

The purpose of this utility model is to provide a spectrometer for frequency-domain OCT system. The spectrometer has a simple and compact structure, and uses an achromatic lens to simultaneously realize the collimation of incident light and the focusing of diffracted light by a diffraction grating, which is beneficial to frequency-domain OCT. System miniaturization and portability.

The technical solution of the utility model is as follows:

A spectrometer for a frequency-domain OCT system, the structure of which includes a single-mode fiber, an achromatic lens, a blazed grating, a photodetector and a spectrometer base plate; the interference light of the OCT system is input to the single-mode fiber, and the output light of the single-mode fiber passes through The collimated light beam collimated by the achromatic lens is irradiated onto the blazed grating, and the first-order diffracted light of the blazed grating is detected by the photodetector after the first-order diffracted light of the blazed grating is focused by the achromatic lens; the single-mode optical fiber, the achromatic lens, the blazed Both the grating and the photodetector are fixed on the spectrometer base plate.

The output end face of the single-mode fiber output port is located at the front focus of the achromatic lens, and the output port is a PC or APC connector.

The blaze angle of the blazed grating is γ degrees, and the direction of the scribed lines of the blazed grating is parallel to the intersection line between the plane where the spectrometer base plate is located and the plane where the blazed grating is located.

The determination of the position of the blazed grating on the base plate is as follows: first, the angle between the plane of the spectrometer base plate and the plane of the blazed grating is equal to (90-γ) degrees, that is, the incident angle of the incident light on the blazed grating is equal to the diffraction angle; then The blazed grating is rotated by an angle θ with a straight line passing through the center of the blazed grating in the plane of the blazed grating and perpendicular to the direction of the blazed grating’s lines as the rotation axis, so that the first-order diffracted light is separated from the collimated beam irradiated on the blazed grating, where θ is less than 5 degrees.

The photosensitive surface of the photodetector is located on the focal plane after the first-order diffracted light of the blazed grating is focused by the achromatic lens.

The photodetector is a linear array CCD, a linear array CMOS linear array photodetection device.

Compared with the prior art, the utility model has the following advantages and positive effects:

1. The utility model uses an achromatic lens to simultaneously realize the collimation of the incident light and the focusing of the first-order diffracted light of the diffraction grating. Compared with the spectrometer structure commonly used in the OCT system, an achromatic lens for beam focusing is omitted .

2. The utility model has a simple structure and can realize a compact spectrometer, which is beneficial to the miniaturization of the frequency domain OCT system.

Description of drawings

Fig. 1 is a structural schematic diagram of a spectrometer used in a frequency-domain OCT system according to the present invention.

Fig. 2 is a schematic diagram of the OCT system where the spectrometer used in the frequency domain OCT system of the present invention is located.

Detailed ways

Below in conjunction with embodiment and accompanying drawing, the utility model will be further described, but should not limit the protection scope of the utility model with this.

The structural schematic diagram of the spectrometer used in the frequency domain OCT system of the present invention is shown in FIG. 1 . It can be seen from the figure that the utility model is used for the spectrometer of the frequency domain OCT system, and its structure includes a single-mode optical fiber 1, an achromatic lens 2, a blazed grating 3, a photodetector 4 and a spectrometer base plate 5; the interference light of the OCT system is input to the single Mode fiber 1, the output light 6 of single-mode fiber 1 is irradiated on the blazed grating 3 by the collimated beam 7 collimated by the achromat lens 2, and the first-order diffracted light 8 of the blazed grating 3 is focused by the achromat lens 2 The light beam 9 is detected by the photodetector 4; the single-mode optical fiber 1, the achromatic lens 2, the blazed grating 3 and the photodetector 4 are all fixed on the spectrometer base plate 5.

The output end face of the output port of the single-mode optical fiber 1 is located at the front focus of the achromatic lens 2, and the output port is a PC or APC connector.

The blaze angle of the blazed grating 3 is γ degrees, and the direction of the scribe line of the blazed grating 3 is parallel to the intersection line between the plane where the spectrometer base plate 5 is located and the plane where the blazed grating 3 is located.

The determination of the position of the blazed grating 3 on the base plate 5 is as follows: first, the angle between the plane where the spectrometer base plate 5 is located and the plane where the blazed grating 3 is located is equal to (90-γ) degrees, that is, the angle of incidence of the incident light on the blazed grating 3 and Diffraction angle is equal; Then take the straight line perpendicular to the line direction of blazed grating 3 through the center of blazed grating 3 in the plane of blazed grating 3 as rotation axis to rotate blazed grating 3 angle θ, so that the first-order diffracted light 8 is irradiated to The collimated beam 7 splits on the blazed grating where θ is less than 5 degrees.

The photosensitive surface of the photodetector 4 is located on the focal plane where the first-order diffracted light of the blazed grating 3 is focused by the achromatic lens 2 .

The photodetector 4 is a linear array CCD, a linear array CMOS linear array photodetection device.

In the frequency domain OCT system shown in Figure 2, the light emitted by the broadband light source 11 is input to the port 12a of the fiber coupler 12, and the two paths of light output by the fiber coupler 12 are respectively input to the reference arm and the sample arm: the light output from the port 12b Input to the reference arm, output to the collimator lens 14 after the polarization controller 13, reflect by the mirror 15 after being collimated by the collimator lens 14, and return to the lens 14 and the polarization controller 13, and enter the fiber coupler 12 again Port 12b of port 12c; the light output from port 12c is input to the sample arm, after being collimated by the lens 16, it is reflected by the scanning galvanometer 17 to the focusing lens 18, and the beam is focused and incident on the sample 19, and the beam reflected by the sample 19 passes through the lens 18 in turn , the scanning galvanometer 17 and the lens 16, and enter the port 12c of the fiber coupler 12 again. The interference signal output by the port 12d of the fiber coupler 12 is input into the single-mode optical fiber 1 of the compact spectrometer used in the frequency domain OCT system of the present utility model, and the electrical signal output by the photodetector 4 is collected by the computer 20 and processed. Finally, the tomographic structure image of sample 19 was obtained.

The central wavelength of the broadband light source 11 is 830nm, and the bandwidth is ±10nm; the light emitted by the broadband light source is respectively injected into the reference arm and the sample arm through a 50/50 fiber coupler. The light output from the optical fiber at the end of the reference arm is collimated and irradiated on the reference mirror. The light output from the fiber optic of the sample arm passes through the galvanometer after being collimated, and is focused on the sample by the objective lens. The axis of rotation of the galvanometer is located at the front focal plane of the objective lens to form an approximate telecentric optical path, ensuring that no additional phase shift is introduced when scanning the sample. The scattered light returned by the reference mirror and the sample is coupled into the optical fiber again, and is connected to the single-mode optical fiber of the compact spectrometer used in the frequency domain OCT system of the present invention through the output end of the optical fiber coupler. The single-mode fiber output port is an APC connector; the focal length of the achromatic lens is 200mm, and the diameter is about Ф50mm. The number of lines is 1200 lines/mm, the side length is 50mm, and the blazed angle at 830nm wavelength is 29.87°; determine the position of the blazed grating on the base plate: first make the angle between the plane of the spectrometer base plate and the plane of the blazed grating equal to ( 90-29.87)=60.13 degrees, at this time, the incident angle of the incident light on the blazed grating is equal to the diffraction angle, and then the rotation axis is rotated by a straight line passing through the center of the blazed grating in the plane of the blazed grating and perpendicular to the line direction of the blazed grating The angle of the blazed grating is 1 degree, so that the diffracted beam is separated from the incident beam; the photodetector is a linear array CCD, the number of pixels is 1024, and the pixel size is 14 microns. Under the above conditions, the spectral resolution of the compact spectrometer used in the frequency domain OCT system of the present invention is 0.05nm, which meets the system requirements.

Claims (6)

1. for the spectrogrph of frequency domain OCT system, its structure comprises single-mode fiber (1), achromat (2), balzed grating, (3), photodetector (4) and spectrogrph base plate (5); The interference light of OCT system inputs to single-mode fiber (1), it is upper that the collimated beam (7) of the output light (6) of this single-mode fiber (1) after achromat (2) collimation is radiated at described balzed grating, (3), and the focused beam (9) of the first-order diffraction light (8) of this balzed grating, (3) after achromat (2) focuses on surveyed by photodetector (4); Described single-mode fiber (1), achromat (2), balzed grating, (3) and photodetector (4) are all fixed on spectrogrph base plate (5).

2. spectrogrph according to claim 1, it is characterized in that the output end face of described single-mode fiber (1) output port is positioned at the front focus of achromat (2), and output port is PC or APC joint.

3. spectrogrph according to claim 1, it is characterized in that the flare angle of described balzed grating, (3) is γ degree, and the groove direction of balzed grating, (3) is parallel to the intersection of spectrogrph base plate (5) place plane and balzed grating, (3) place plane.

4. spectrogrph according to claim 1, it is characterized in that described balzed grating, (3) is as follows at determining of the upper position of base plate (5): first make the angle of spectrogrph base plate (5) place plane and balzed grating, (3) place plane equal (90-γ) degree, the angle of incidence of the upper incident illumination of balzed grating, (3) equates with the angle of diffraction; Then take in the plane of balzed grating, (3) is (3) θ angles of rotating shaft rotation balzed grating, through the vertical straight line of the groove direction with balzed grating, (3) at balzed grating, (3) center, first-order diffraction light (8) and the collimated beam (7) exposing on balzed grating, are separated, and wherein θ is less than 5 degree.

5. spectrogrph according to claim 1, on the focal plane of the first-order diffraction light that the photosurface that it is characterized in that described photodetector (4) is positioned at balzed grating, (3) after achromat (2) focuses on.

6. spectrogrph according to claim 1, is characterized in that described photodetector (4) is for line array CCD, linear array CMOS photodiode array part.