CN107101722A - A kind of broadband linear polarization imaging method based on Mach Zehnder interferometer - Google Patents

A kind of broadband linear polarization imaging method based on Mach Zehnder interferometer Download PDF

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Publication number
CN107101722A
CN107101722A CN201710221519.6A CN201710221519A CN107101722A CN 107101722 A CN107101722 A CN 107101722A CN 201710221519 A CN201710221519 A CN 201710221519A CN 107101722 A CN107101722 A CN 107101722A
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CN
China
Prior art keywords
light
polarization
diffraction grating
plane mirror
reflected light
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Pending
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CN201710221519.6A
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Chinese (zh)
Inventor
朱京平
张宁
张云尧
宗康
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Xian Jiaotong University
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Xian Jiaotong University
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Priority to CN201710221519.6A priority Critical patent/CN107101722A/en
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/2823Imaging spectrometer
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/447Polarisation spectrometry
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/45Interferometric spectrometry
    • G01J3/453Interferometric spectrometry by correlation of the amplitudes

Abstract

The present invention discloses a kind of broadband linear polarization imaging method based on Mach Zehnder interferometer, the light of extraterrestrial target polarization information is carried through being incided by preposition optics microscope group in Polarization Detection imaging system, light beam is divided into reflected light (p light) and transmitted light (s light) in the presence of polarization beam apparatus, two-beam is respectively through diffraction grating, realize dispersion, by plane mirror, change the direction of propagation, then incident in polarization beam apparatus, wherein p light reflects, s light transmissions, pass through after two-beam convergence after polarizer, direction of vibration is mutually perpendicular to, in the presence of imaging len, stable interference fringe can be obtained on CCD detection array, Fourier transform finally is carried out to interference fringe, filtering and Fourier's inverse transform, so as to obtain the two dimensional image of linear polarization component.The present invention is in astronomical observation, and earth remote sensing, the field such as machine vision and biomedical diagnostic has potential using value.

Description

A kind of broadband linear polarization imaging method based on Mach Zehnder interferometer
【Technical field】
The invention belongs to optical remote sensing field of detecting, be related to a kind of broadband linear polarization based on Mach Zehnder interferometer into Image space method.
【Background technology】
Polarization imaging is a kind of can to carry while obtain the advanced Detection Techniques of the strength information and polarization information of target There are certain potentiality in terms of the detection of high target, identification, classification effectiveness and precision, military surveillance, earth resource generaI investigation, Many necks such as environmental health monitoring and surveilliance, natural calamity forecast, Atmospheric Survey, astronomical observation, machine vision are freeed, biomedical diagnostic Domain all has great application value and development prospect.Channel modulation type polarization imaging technology is used as a new remote sensing Technology, has caused the attention of domestic and international mechanism with its unique remote sensing advantage, foreign study mechanism be concentrated mainly on it is beautiful, The large project of the country such as day, Europe relies on unit, the military, university etc.;Mainly there are Anhui ray machine institute, west in studies in China mechanism Pacify ray machine institute, Xi'an Communications University etc., the polarization imaging Detection Techniques reported differ from one another.
The core devices of channel modulation type polarization imager typically use birefringece crystal or interferometer.According to imaging side Formula, can be divided into Active Imaging and imaging and passive imaging, Active Imaging using Muller matrix polarization imaging as representative, its light source it is known or It is controllable, so as to detect the polarization state of target;Imaging and passive imaging is general based on natural light, due to not limited by light source, actual to answer It is wider with scope.It can be divided into data reduction pattern, Fourier analysis method, channel modulation pattern according to data processing method.Press According to time sequencing, timing polarization imaging can be divided into again, with non-sequential polarization imaging.Timing mainly includes rotatory polarization piece Type and liquid crystal regulation type:Rotatory polarization piece type is that turntable is placed before image camera, and rotatory polarization piece is to obtain target polarization State;Liquid crystal regulation type is the sequence of electrically-controlled liquid crystal, realizes polarizer function, it is also possible to obtain the polarization state of target, the two lack Point is that dynamic object can not be imaged;Non-sequential can be divided into a point amplitude type, point aperture type, point focal plane type and channel modulation again Type.Amplitude type is divided to generally require multiple detectors, data syn-chronization is more difficult, and equipment instrument is than larger and more complicated, robustness It is relatively low;Point aperture type is to be divided into the aperture of optical system multiple, and each aperture separately detects the polarization information of target, detection The utilization rate of device is relatively low, makes difficult;Point focal plane type adds polarization plates before the detectors, and every four pixels can detect one The polarization information of target pixel points, spatial resolution is low, and technique manufacture difficulty is big.
【The content of the invention】
It is an object of the invention to provide a kind of broadband linear polarization imaging method based on Mach Zehnder interferometer, utilize The dispersion and interferometer light splitting of transmissive diffraction grating obtain the light beam shearing displacement being directly proportional to wavelength, are interfered by two-beam, Obtain the stokes parameters (S of linear polarization information0、S1、S2) it is modulated to the image of interference fringe amplitude, interference fringe frequency It is inversely proportional, is directly proportional to shearing displacement with wavelength, so as to eliminates the influence of wavelength.
To reach above-mentioned purpose, the present invention is achieved using following technical scheme:
A kind of broadband linear polarization imaging method based on Mach Zehnder interferometer, comprises the following steps:
The light for carrying extraterrestrial target polarization information is incided in Polarization Modulation module by preposition optics microscope group, incident light Beam is divided into reflected light and transmitted light in the presence of the first polarization beam apparatus, reflected light and transmitted light respectively through diffraction grating, Dispersion is produced, respectively through the first plane mirror and the second plane mirror, changes the direction of propagation;Then reflected light and transmission Light is incided in the second polarization beam apparatus respectively, wherein reflected light back, incident light transmission, by polarization after two-beam convergence After piece, direction of vibration is mutually perpendicular to, in the presence of imaging len, and stable interference fringe is obtained on planar array detector, Fourier transform, filtering and Fourier's inverse transform are carried out to interference fringe finally by data acquisition processing system, so as to obtain The two dimensional image of linear polarization component.
Compared with prior art, the invention has the advantages that:
Channel modulation type is that the polarization information of target is being modulated in different spatial frequencys, so that on a sub-picture The target polarization information of acquisition, the polarization imaging method can obtain the polarization information of target simultaneously, with making simple, light path Simply, it is with low cost, the advantages of spatial resolution is high;The invention belongs to snapshot-type channel modulation polarization imaging method, first, sheet Invention imaging band is wide, can obtain the strength information and polarization information of target simultaneously under low light condition;Secondly, the present invention Need a two field picture of extraterrestrial target, you can to obtain its linear polarization image-forming information, dynamic object can be detected, operating efficiency It is high;Finally, data processing of the present invention is simple and quick, and target can be detected in real time.
【Brief description of the drawings】
Fig. 1 is color dispersion-type Mach Zehnder interferometer molded line polarization imaging device of the invention;
Fig. 2 is the schematic diagram that transmissive diffraction grating of the present invention carries out dispersion compensation;
Beam distribution figures of the Fig. 3 for the present invention Jing Guo Polarization Modulation module.
Wherein:The preposition optics microscope groups of 10-;11- object lens;12- field stops;13- collimation lenses;20- Polarization Modulation modules; 211/4 wave plate;The polarization beam apparatus of 22- first;The diffraction grating of 23- first;The diffraction grating of 24- second;The plane reflections of 25- first Mirror;The diffraction grating of 26- the 3rd;The diffraction grating of 27- the 4th;The plane mirrors of 28- second;The polarization beam apparatus of 29- second;30- is inclined Galvanometer;40- imaging lens;50- planar array detectors;60- data acquisition processing systems.
【Embodiment】
The present invention is described in further detail below in conjunction with the accompanying drawings:
Referring to Fig. 1-3, the broadband linear polarization imaging device of the invention based on Mach Zehnder interferometer, including set gradually In in light path for the preposition optics microscope group 10 of collimated incident light, Polarization Modulation module 20, imaging len 40 and face battle array visit Survey device 50;Incident light, which enters, enters Polarization Modulation module 20 after preposition optics microscope group 10, formed after Polarization Modulation module 20 The two orthogonal light of beam direction of vibration, and in the presence of imaging len 40, interference bar is formed on planar array detector 50 Line;The number for carrying out Fourier transform, filtering and Fourier's inverse transform to interference fringe is also associated with planar array detector 50 According to acquisition processing system 60;Polariscope 30 is provided between imaging len 40 and Polarization Modulation module 20.
As shown in figure 1, preposition optics microscope group 10 includes object lens 11, field stop 12 and the standard set gradually along incident ray Straight lens 13.Object lens 11 are telephotolens, microcobjective or common object lens.
Polarization Modulation module 20 includes the quarter wave plate 21 and first of the 0 ° of placement of quick shaft direction set gradually along incident ray Polarization beam apparatus 22;Incident light is divided into transmitted light and reflected light, between reflected light and transmitted light after the first polarization beam apparatus 22 Angle be 90 °;The first diffraction grating 23, the second diffraction grating 24 and the first plane mirror are disposed with transmitted light path 25, transmitted light is after the first plane mirror 25, with the reflection parallel light after the first polarization beam apparatus 22;Reflected light path On be disposed with the 3rd diffraction grating 26, the 4th diffraction grating 27 and the second plane mirror 28, reflected light is flat by second After face speculum 28, with the transmission parallel light after the first polarization beam apparatus 22;By the transmission of the first plane mirror 25 The reflected light of the second plane mirror 28 of light and process is converged at the second polarizing beam splitter mirror 29, is passed through by transmitted light and reflected light Direction of vibration after the second polarizing beam splitter mirror 29 is crossed to be mutually perpendicular to.First diffraction grating 23, the second diffraction grating 24, the 3rd diffraction light Grid 26 and, the 4th diffraction grating 27 be transmissive diffraction grating.
Polarization Modulation module 20 is by the quarter wave plate 21 of 0 ° of placement, the first polarization beam apparatus 22, the first diffraction grating 23, the Two diffraction grating 24, the first plane mirror 25, the 3rd diffraction grating 26, the 4th diffraction grating 27, the second plane mirror 28 And second polarization beam apparatus 29 constitute;Wherein four diffraction grating are located in Mach Zehnder light path branch, between two groups of gratings Distance it is identical, and two leg lengths are equal;Light beam passes through after quarter wave plate 21, its linear polarization information S carried1It is inclined with circle Information of shaking S3Transposition, polarization state is by S=[S0,S1,S2,S3]TIt is changed into S=[S0,S3,S2,S1]T, in the first polarization beam splitting Mirror 22 under effect, transmitted light (S light) transmission, reflected light (P light) reflection, wherein by taking S light as an example, light beam passes through the first diffraction Dispersion phenomenon occurs after grating 23, different wavelength is diffracted into different directions, after the second diffraction grating 24, light The direction of propagation of line changes again, is changed into directional light;After the first plane mirror 25 by 45 ° of placements, change and propagate Route;Similarly, P light experience identical changes, and is met with S light at the second polarization beam apparatus 29, by the second polarization beam apparatus After 29, two-beam direction of vibration is mutually perpendicular to, in theory the two phase difference (machining accuracy herein that there is wavelength And its it is high, Mach Zehnder interferometer four edges, brachium is essentially equal), when interfering, center striped has been offset, but not Influence measurement result;Afterwards, light beam passes through polariscope 30, and direction of vibration is mutually perpendicular to;In the presence of imaging len 40, face battle array Interference is obtained on detector 50 decent;Gather, extract and handle that to can obtain line inclined finally by data acquisition processing system 60 The corresponding two-dimensional space distribution map of information of shaking.
Broadband linear polarization imaging method of the invention based on Mach Zehnder interferometer, comprises the following steps:
The light for carrying extraterrestrial target polarization information is incided in Polarization Modulation module by preposition optics microscope group, incident light Beam is divided into reflected light and transmitted light in the presence of the first polarization beam apparatus, reflected light and transmitted light respectively through diffraction grating, Dispersion is produced, respectively through the first plane mirror and the second plane mirror, changes the direction of propagation;Then reflected light and transmission Light is incided in the second polarization beam apparatus respectively, wherein reflected light back, incident light transmission, by polarization after two-beam convergence After piece, direction of vibration is mutually perpendicular to, in the presence of imaging len, and stable interference fringe is obtained on planar array detector, Fourier transform, filtering and Fourier's inverse transform are carried out to interference fringe finally by data acquisition processing system, so as to obtain The two dimensional image of linear polarization component.
Transmissive diffraction grating is the ideal situation of transmission-type binary optical elements, will be high using diffraction efficiency in method First-order diffraction light.There is lateral shear effect by the light of color dispersion-type Mach Zehnder interferometer, shearing displacement is directly proportional to wavelength.
Such as Fig. 2, Mach Zehnder interferometer generation and the key technology of the positively related horizontal shear capacity of wavelength are complete by two What exactly the same transmissive diffraction grating 23 was constituted:Beam orthogonal is incided in transmissive diffraction grating 23, occurs diffraction phenomena, Wherein there is dsin θ in the angle of diffraction with wavelengthλ=m λ relation (the d diffraction grating cycles, θλFor the angle of diffraction, m is diffraction time, and λ is Wavelength), another shearing displacement Δ/2=Ltan θλ, when angle is sufficiently small, above-mentioned relation is approximately Δ/2=Lsin θ=Lm λ/d, i.e., Obtain and the positively related shearing displacement of wavelength.
Such as Fig. 3, two-beam passes through after Polarization Modulation module 20, shearing displacement and the wavelength positive correlation of each wave band, and adjusts The out of phase factor in system.
The principle of the present invention:
The light of extraterrestrial target polarization information is carried through being incided by preposition optics microscope group 10 in Polarization Modulation module 20, Light beam is incided after the quarter wave plate 21 of 0 ° of placement, linear polarization information S1With circular polarization information S3Exchange, in polarization beam splitting It is divided into reflected light (s light) and transmitted light (p light) in the presence of device 22, two-beam occurs diffraction and showed respectively through diffraction grating 23 As, dispersion is realized, by plane mirror 24, changes the direction of propagation, then incident in polarization beam apparatus 22, wherein P light Reflection, S light transmissions, pass through after polarizer 30, direction of vibration is mutually perpendicular to, in the work of imaging len 40 after two-beam convergence Under, stable interference fringe can be obtained on CCD detection array 50, Fourier transform, filter are finally carried out to interference fringe Involve Fourier's inverse transform, so as to obtain the two dimensional image of linear polarization component.
The technological thought of above content only to illustrate the invention, it is impossible to which protection scope of the present invention is limited with this, it is every to press According to technological thought proposed by the present invention, any change done on the basis of technical scheme each falls within claims of the present invention Protection domain within.

Claims (1)

1. a kind of broadband linear polarization imaging method based on Mach Zehnder interferometer, it is characterised in that this method is based on one kind Broadband linear polarization imaging device, the broadband linear polarization imaging device include be set in turn in light path be used for collimate into Penetrate preposition optics microscope group (10), Polarization Modulation module (20), imaging len (40) and the planar array detector (50) of light;Incident light Enter Polarization Modulation module (20) afterwards into preposition optics microscope group (10), the vibration of two beams is formed after Polarization Modulation module (20) The orthogonal light in direction, and in the presence of imaging len (40), interference fringe is formed on planar array detector (50);Face It is also associated with adopting for carrying out interference fringe the data of Fourier transform, filtering and Fourier's inverse transform on array detector (50) Collect processing system (60);
Polarization Modulation module (20) includes the broadband quarter wave plate (21) and the first polarization beam apparatus set gradually along incident ray (22);Incident light is divided into transmitted light and reflected light after the first polarization beam apparatus (22), the angle between reflected light and transmitted light For 90 °;The first diffraction grating (23), the second diffraction grating (24) and the first plane mirror are disposed with transmitted light path (25), transmitted light is after the first plane mirror (25), with the reflection parallel light after the first polarization beam apparatus (22);Instead Penetrate in light path and be disposed with the 3rd diffraction grating (26), the 4th diffraction grating (27) and the second plane mirror (28), reflect Light is after the second plane mirror (28), with the transmission parallel light after the first polarization beam apparatus (22);It is flat by first The transmitted light of face speculum (25) and the reflected light of the second plane mirror of process (28) are converged at the second polarizing beam splitter mirror (29) place Poly-, by transmitted light and reflected light, direction of vibration is mutually perpendicular to after the second polarizing beam splitter mirror (29);
It the described method comprises the following steps:
The light for carrying extraterrestrial target polarization information is incided in Polarization Modulation module by preposition optics microscope group, and incident beam exists It is divided into reflected light and transmitted light in the presence of first polarization beam apparatus, reflected light and transmitted light are produced respectively through diffraction grating Dispersion, respectively through the first plane mirror and the second plane mirror, changes the direction of propagation;Then reflected light and transmitted light are divided Do not incide in the second polarization beam apparatus, wherein reflected light back, incident light transmission, after two-beam convergence by polarizer it Afterwards, direction of vibration is mutually perpendicular to, in the presence of imaging len, stable interference fringe is obtained on planar array detector, finally Fourier transform, filtering and Fourier's inverse transform are carried out to interference fringe by data acquisition processing system, so that it is inclined to obtain line Shake the two dimensional image of component.
CN201710221519.6A 2017-04-06 2017-04-06 A kind of broadband linear polarization imaging method based on Mach Zehnder interferometer Pending CN107101722A (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109489579A (en) * 2018-11-16 2019-03-19 暨南大学 A kind of Sagnac polarization imaging device and method based on high dencity grating
CN111194419A (en) * 2017-09-21 2020-05-22 高新技术学习公司 Additional imaging module for off-axis recording of polarization encoded waves
CN113280916A (en) * 2021-05-31 2021-08-20 中国科学院长春光学精密机械与物理研究所 Fourier transform spectrometer

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111194419A (en) * 2017-09-21 2020-05-22 高新技术学习公司 Additional imaging module for off-axis recording of polarization encoded waves
CN109489579A (en) * 2018-11-16 2019-03-19 暨南大学 A kind of Sagnac polarization imaging device and method based on high dencity grating
CN113280916A (en) * 2021-05-31 2021-08-20 中国科学院长春光学精密机械与物理研究所 Fourier transform spectrometer
CN113280916B (en) * 2021-05-31 2022-08-05 中国科学院长春光学精密机械与物理研究所 Fourier transform spectrometer

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Application publication date: 20170829