CN101744607A - Imaging system of compressed state light field - Google Patents
Imaging system of compressed state light field Download PDFInfo
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- CN101744607A CN101744607A CN200810188559A CN200810188559A CN101744607A CN 101744607 A CN101744607 A CN 101744607A CN 200810188559 A CN200810188559 A CN 200810188559A CN 200810188559 A CN200810188559 A CN 200810188559A CN 101744607 A CN101744607 A CN 101744607A
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- 238000003384 imaging method Methods 0.000 title claims abstract description 99
- 230000003287 optical effect Effects 0.000 claims abstract description 37
- 230000006835 compression Effects 0.000 claims abstract description 5
- 238000007906 compression Methods 0.000 claims abstract description 5
- 238000000034 method Methods 0.000 claims description 17
- 238000007654 immersion Methods 0.000 claims description 11
- 238000001228 spectrum Methods 0.000 claims description 11
- 238000005305 interferometry Methods 0.000 claims description 8
- 239000004065 semiconductor Substances 0.000 claims description 6
- 239000004568 cement Substances 0.000 claims description 4
- 239000007788 liquid Substances 0.000 claims description 4
- 239000004973 liquid crystal related substance Substances 0.000 claims description 4
- 239000013307 optical fiber Substances 0.000 claims description 4
- 238000010008 shearing Methods 0.000 claims description 4
- 239000007787 solid Substances 0.000 claims description 4
- 230000003595 spectral effect Effects 0.000 abstract description 5
- 230000010287 polarization Effects 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 238000004458 analytical method Methods 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000003760 hair shine Effects 0.000 description 2
- 230000005855 radiation Effects 0.000 description 2
- 206010052128 Glare Diseases 0.000 description 1
- 230000003044 adaptive effect Effects 0.000 description 1
- 238000003745 diagnosis Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005672 electromagnetic field Effects 0.000 description 1
- 238000005265 energy consumption Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
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- 230000007774 longterm Effects 0.000 description 1
- 230000005610 quantum mechanics Effects 0.000 description 1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3581—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using far infrared light; using Terahertz radiation
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/21—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour by interference
- G02F1/215—Michelson type
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Abstract
The invention relates to an imaging system of a compressed state light field, which comprises a laser, a compressed light device, an imaging system and a detector; the compression optical equipment is arranged on an output light path of the laser; the imaging system is arranged on an output optical path of the compression optical equipment; the detector is connected with the imaging system. The invention provides an imaging system of a compressed optical field with high image signal-to-noise ratio, high spatial resolution, high spectral resolution, high reliability, stable performance and low power consumption.
Description
Technical field
The present invention relates to a kind of imaging system, relate in particular to a kind of imaging system of compressed state optical field.
Background technology
In recent years, imaging technique extensively uses high s/n ratio, high-resolution formation method research more and more causing people's attention in the fields such as medical diagnosis, medicinal herb components analysis, biochemistry micro-structure and component analysis, integrated circuit detect, engineering nondestructive detecting and information are obtained.
The employed light source of existing active imaging mainly is the natural light light source, laser diode, fluorescent lamp etc., or imageable target self radiant light.When we handle the light field of this quasi-tradition light source as a quantum regime, there is random vacuum fluctuation (quantum noise) in the pairwise orthogonal component of describing electromagnetic field, even we adopt effective ways to remove the influence in all classical error sources in the measuring process, quantum noise still is present among the various forms of radiation, and this quantum noise derives from quantum mechanics intrinsic statistical property.Therefore, use squeezed light equipment that light source is improved, can realize high s/n ratio, high-resolution high-quality imaging.
Passive passive type imaging mainly is passive receiving target object reflection and self radiation signal light, realizes that target object detects.Because there are a large amount of veiling glares in target background, this has just limited the raising of signal to noise ratio and image resolution ratio.Utilize conventional light source, as realizations such as fluorescent lamp, laser instrument initiatively active imaging can overcome the shortcoming of passive imaging, the signal to noise ratio and the resolution of imaging increase, but the quantum noise in the light source can influence imaging effect.Therefore, realize further that high s/n ratio, high-resolution imaging must manage to reduce the light source quantum noise.
Summary of the invention
In order to solve the above-mentioned technical problem that exists in the background technology, the invention provides the imaging system of a kind of signal noise ratio (snr) of image height, spatial resolution height, spectral resolution height, reliability height, stable performance, compressed state optical field low in energy consumption.
Technical solution of the present invention is: the invention provides a kind of imaging system of compressed state optical field, its special character is: the imaging system of this compressed state optical field comprises laser instrument, squeezed light equipment, imaging system and detector; Described squeezed light equipment is arranged on the output light path of laser instrument; Described imaging system is arranged on the output light path of squeezed light equipment; Described detector links to each other with imaging system.
The imaging system of above-mentioned compressed state optical field also comprises data handling system, and described data handling system links to each other with detector.
Above-mentioned squeezed light equipment is quadrature position phase squeezed light equipment, intensity difference squeezed light equipment, Amplitude Squeezed Light or space compression light device.
Above-mentioned laser instrument is semiconductor laser, liquid laser, gas laser, solid state laser or optical fiber laser.
Above-mentioned detector is CCD, vacuum pickup tube, SSPD.
Above-mentioned imaging system is based on Sagnac type lateral shearing interference method, the michelson interferometry based on Michelson's interferometer, birefringent polarizing interferometric method, the interferometric method of liquid crystal tunable optical filter, the multiple beam interferometry of Fabry-Perot (Fabry-perot) and the imaging system of employing dispersing prism, diffraction grating, binary optical elements, acousto-optic tunable filter color dispersion-type spectrum imaging method or single photon imaging or how much imagings of Sagnac interferometer.
When above-mentioned imaging system was the imaging system of traditional single photon imaging or how much imagings, described detector also included the super hemisphere immersion lens of standard that is arranged on before the detector.
Above-mentioned super hemisphere immersion lens is by optical cement and detector close adhesion.
Advantage of the present invention is:
1, signal noise ratio (snr) of image, spatial resolution and spectral resolution can significantly improve.The present invention makes squeezed light suppress random vacuum fluctuation (quantum noise) after adopting squeezed light equipment, therefore utilizes the squeezed light light source to be embodied as picture, can improve the signal light intensity, improves signal to noise ratio, improves image resolution ratio.
2, stable performance, the reliability height.The present invention utilizes laser instrument to produce squeezed light, and light stability can be for a long time, continuous operation, the reliability height of imaging.
3, can realize the faint light imaging.The present invention is because be active imaging system, the watt level that can regulate light source, so this imaging system also can be under the faint light condition high s/n ratio, high-resolution imaging.
4, efficient height.The present invention also has adaptive improvement in sniffer, add an immersion lens before detector, can improve light path, under the identical situation of detector area, can improve the signal to noise ratio of whole system equivalently.
5, can realize continuous, fast imaging.The squeezed light that is adopted among the present invention can be realized continuous operation, therefore can realize continuous, fast imaging.
Description of drawings
Fig. 1 is the structural representation of system provided by the present invention;
Fig. 2 is the structural representation of squeezed light equipment provided by the present invention;
Fig. 3 is the present invention's first preferred embodiment structural representation;
Fig. 4 is an improved standard immersion lens structural representation in another embodiment of the present invention.
The specific embodiment
Referring to Fig. 1, the invention provides a kind of imaging system of compressed state optical field, the imaging system of this compressed state optical field comprises laser instrument 1, squeezed light equipment 2, imaging system 4, detector 5 and data handling system 6; Squeezed light equipment 2 is arranged on the output light path of laser instrument 1; Imaging system 4 is arranged on the output light path of squeezed light equipment 2; Detector 5 links to each other with imaging system 4; Data handling system 6 links to each other with detector 5.
Squeezed light equipment 2 can be quadrature position phase squeezed light equipment, intensity difference squeezed light equipment, Amplitude Squeezed Light or space compression light device.Laser instrument 1 is semiconductor laser, liquid laser, gas laser, solid state laser or optical fiber laser etc.Detector 5 can be image devices such as CCD, vacuum pickup tube, SSPD.
The imaging mode of imaging system 4 can be based on the Sagnac type lateral shearing interference method of Sagnac interferometer, michelson interferometry based on Michelson's interferometer, the birefringent polarizing interferometric method, the interferometric method of liquid crystal tunable optical filter, the interference spectrum imaging method of the multiple beam interferometry of Fabry-Perot (Fabry-perot) etc., and employing dispersing prism, diffraction grating, binary optical elements, the color dispersion-type spectrum imaging method of acousto-optic tunable filter etc., single photon imaging or how much imaging systems such as imaging can be used among the present invention, finish goal of the invention of the present invention.
When if the imaging mode of imaging system 4 is traditional single photon imaging or how much imaging systems such as imaging, detector 5 also includes the super hemisphere immersion lens 7 of standard that is arranged on before the detector 5.Super hemisphere immersion lens 7 is by optical cement and detector 5 close adhesion.
Referring to Fig. 2, it can be semiconductor laser, liquid laser, gas laser, solid state laser or optical fiber laser etc. that the present invention selects laser instrument 1 in use.In order to say something, in the cited implementation column of the present invention, the DABOLO laser instrument LD that adopts Germany to produce, it is the continuous single-frequency green (light) laser of laser diode pumped total solidsization, 532nm green glow Maximum Power Output is 800mW, the angle of polarization direction and vertical direction is 45 °, and the long-term power stability of 5h is less than ± 1%; Can export the infrared peak power 400mW of 1064nm simultaneously.Behind squeezed light equipment 2, obtain Amplitude Squeezed Light, squeezed light shines target 3 to be measured, with traditional lens mode 4 imagings, detects the flashlight of transmission at target to be measured 3 rears then with detector 5.The operation principle that squeezed light equipment provided by the present invention produces squeezed light is:
1, the infrared light of laser emitting (1064nm) elder generation process focal length is that the planoconvex lens f1 collimation of f=450mm is approximate collimated light beam.The half-wave plate H1 of back is used for realizing the phase place modulation.Light beam passes through polarization splitting prism P1 again.
2, the green glow of laser emitting (532nm) elder generation process focal length is that the planoconvex lens f2 collimation of f=300mm is approximate directional light.Form beam splitter with half-wave plate H4 and polarization splitting prism P2, the power of control institute divided beams.The half-wave plate H5 of back is used for realizing the phase place modulation.
3, half-wave plate H2, H3 and Faraday rotator IS form optoisolator.When the polarization direction of green glow and infrared light all is adjusted to vertical after, light beam after converging incides resonator cavity through lens f3.
4, the concave surface of the input mirror M1 of resonator cavity is high anti-to 1064nm, and the plane is anti-reflection to 532nm, and whole eyeglass is 70% to the transmitance of 532nm; The concave surface of outgoing mirror M2 is 96.7% to the reflectance of 1064nm, and high anti-to 532nm, the plane is anti-reflection to 1064nm.Focal length of resonator cavity external is that f=148mm and the lens f4 that is coated with the 1064nm anti-reflection film are approximate directional light with the emergent light collimation, is exactly Amplitude Squeezed Light.
Referring to Fig. 3, be that the present invention utilizes the interference spectrum formation method to come target to be measured is carried out first embodiment of imaging, the present invention in use, at first target 3 to be measured is arranged in the imaging system 4 of compressed state optical field of the present invention, and it is target to be measured 3 is fixing or be placed between squeezed light equipment 2 and the imaging system 4, and be on the output light path of squeezed light equipment 2, the present invention in this embodiment, the laser that can utilize semiconductor laser 1 to produce prepares the Amplitude Squeezed Light light source, realizes target acquisition.The squeezed light that is produced by Amplitude Squeezed Light equipment 2 shines target to be measured, reflected light or transillumination become the collimated beam of a branch of electric vector and inject Sagnac interference beam splitting system after preposition optical system, this light wave is divided into a branch of transillumination and a branch of reflected light, through M after arriving beam-splitting board
1And M
2Return beam-splitting board after the reflection again, arrive detector 5 through transmission and reflection respectively.Each bundle in the two bundle light has all experienced a transmission and primary event respectively on beam-splitting board when arriving detector 5.
Because two light beams split the relevant essential condition that satisfies same frequency, direction of vibration non-orthogonal (direction of vibration is identical) herein and have fixed bit to differ from same incident beam; And satisfy amplitude again and differ the relevant sufficient condition that not greatly different (two amplitudes equate) herein and optical path difference can not be too big, so when two light beams meet, will inevitably produce interference pattern.By fourier lense interferogram is converted into spectrogram, utilizes planar array detector 5CCD that spectrogram is surveyed again, restore, just can obtain the image information and the spectral information of target to be measured through later data processing system 6 spectrograms with the survey data.
The beam splitting system of the imaging spectrometer in the last example is the Sagnac type lateral shearing interference method that adopts based on the Sagnac interferometer, same interference spectrum imaging experiment scheme based on the squeezed state light source also can adopt the michelson interferometry based on Michelson's interferometer, and the birefringent polarizing interferometric method, adopt the interferometric method of liquid crystal tunable optical filter and the multiple beam interferometry of employing Fabry-Perot (Fabry-perot).
Also can adopt non-interference spectrum imaging method, come imaging etc. such as employing color dispersion-type imaging spectral technology, and can adopt traditional non-spectrum imaging methods such as lens imaging to come imaging.
Fig. 4 is that the present invention utilizes improved immersion lens structural representation in another preferred embodiment that traditional lens imaging principle proposed.Different with Fig. 3 is, present embodiment is to adopt traditional lens imaging mode, the present invention is existing except that being used in proof, commonly used some interference spectrum imaging systems 4 are outer can also to be used in non-interference spectrum imaging method and the traditional non-spectrum imaging methods such as lens imaging, certainly when utilizing traditional lens imaging mode to carry out imaging, except using semiconductor laser 1 and Amplitude Squeezed Light equipment 2, only before detector 5, add a super hemisphere immersion lens 7, so not only can improve light path, reduce the area of detector 5, improve the signal to noise ratio of whole system equivalently.Also can shorten optical path length, make structure of the present invention compact more.And, detector 5 closely is bonded on the super hemisphere immersion lens 7 with optical cement in order to make structure more stable.
Claims (8)
1. the imaging system of a compressed state optical field, it is characterized in that: the imaging system of described compressed state optical field comprises laser instrument, squeezed light equipment, imaging system and detector; Described squeezed light equipment is arranged on the output light path of laser instrument; Described imaging system is arranged on the output light path of squeezed light equipment; Described detector links to each other with imaging system.
2. the imaging system of compressed state optical field according to claim 1, it is characterized in that: the imaging system of described compressed state optical field also comprises data handling system, described data handling system links to each other with detector.
3. the imaging system of compressed state optical field according to claim 2, it is characterized in that: described squeezed light equipment is quadrature position phase squeezed light equipment, intensity difference squeezed light equipment, Amplitude Squeezed Light or space compression light device.
4. the imaging system of compressed state optical field according to claim 3, it is characterized in that: described laser instrument is semiconductor laser, liquid laser, gas laser, solid state laser or optical fiber laser.
5. the imaging system of compressed state optical field according to claim 4, it is characterized in that: described detector is CCD, vacuum pickup tube, SSPD.
6. according to the imaging system of claim 1 or 2 or 3 or 4 or 5 described compressed state optical fields, it is characterized in that: described imaging system is based on the Sagnac type lateral shearing interference method of Sagnac interferometer, michelson interferometry based on Michelson's interferometer, the birefringent polarizing interferometric method, the interferometric method of liquid crystal tunable optical filter, the multiple beam interferometry of Fabry-Perot (Fabry-perot) and employing dispersing prism, diffraction grating, binary optical elements, the imaging system of acousto-optic tunable filter color dispersion-type spectrum imaging method or single photon imaging or how much imagings.
7. the imaging system of compressed state optical field according to claim 6 is characterized in that: when described imaging system was the imaging system of traditional lens mode imaging, described detector also included the super hemisphere immersion lens of standard that is arranged on before the detector.
8. the imaging system of compressed state optical field according to claim 7, it is characterized in that: the super hemisphere immersion lens of described standard is by optical cement and detector close adhesion.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN200810188559A CN101744607A (en) | 2008-12-17 | 2008-12-17 | Imaging system of compressed state light field |
| PCT/CN2009/000439 WO2010069116A1 (en) | 2008-12-17 | 2009-04-24 | Imaging system with squeezed state light field |
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| Application Number | Priority Date | Filing Date | Title |
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| CN200810188559A CN101744607A (en) | 2008-12-17 | 2008-12-17 | Imaging system of compressed state light field |
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| WO (1) | WO2010069116A1 (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106225666A (en) * | 2016-07-13 | 2016-12-14 | 南京大学 | A kind of quantum fibre optic interferometer |
| CN106932767A (en) * | 2017-04-17 | 2017-07-07 | 浙江神州量子网络科技有限公司 | Quantum radar and radar detection method based on squeezed light |
| CN109361833A (en) * | 2018-10-08 | 2019-02-19 | 南昌大学 | A kind of transmitting device and method of single photon compression video |
| CN111896103A (en) * | 2020-07-02 | 2020-11-06 | 西安交通大学 | Signal amplification device and method based on multipath quantum interference |
| CN113093166A (en) * | 2021-04-07 | 2021-07-09 | 毕思文 | Detection imaging optical system based on compressed-state light field |
| CN114414505A (en) * | 2022-01-22 | 2022-04-29 | 山东润一智能科技有限公司 | Intelligent monitoring terminal for quantum spectrum microorganisms |
| CN114545643A (en) * | 2022-04-22 | 2022-05-27 | 北京航空航天大学 | Single photon imaging system based on polarization noise reduction |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5574557A (en) * | 1995-05-08 | 1996-11-12 | The Board Of Trustees Of The Leland Stanford Junior University | Apparatus and method for performing sub-poissonian interference measurements using an intensity-squeezed state |
| CN1129869C (en) * | 2000-10-31 | 2003-12-03 | 中国科学院上海光学精密机械研究所 | Fingerprint Image Display and Acquisition Device |
| CN1170142C (en) * | 2002-03-19 | 2004-10-06 | 天津大学 | High-speed optical interference chromatographic imaging apparats |
| US7453626B2 (en) * | 2007-03-01 | 2008-11-18 | The United States Of America As Represented By The Secretary Of Commerce | Four-wave mixing source of squeezed light for image processing and interferometry |
| CN100549676C (en) * | 2007-11-14 | 2009-10-14 | 哈尔滨工业大学 | 4f phase coherent imaging device based on michelson interferometer |
-
2008
- 2008-12-17 CN CN200810188559A patent/CN101744607A/en active Pending
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- 2009-04-24 WO PCT/CN2009/000439 patent/WO2010069116A1/en active Application Filing
Cited By (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106225666A (en) * | 2016-07-13 | 2016-12-14 | 南京大学 | A kind of quantum fibre optic interferometer |
| CN106225666B (en) * | 2016-07-13 | 2017-05-03 | 南京大学 | Quantum optical fiber interferometer |
| CN106932767A (en) * | 2017-04-17 | 2017-07-07 | 浙江神州量子网络科技有限公司 | Quantum radar and radar detection method based on squeezed light |
| CN106932767B (en) * | 2017-04-17 | 2023-08-11 | 浙江神州量子网络科技有限公司 | Quantum radar based on compressed light and radar detection method |
| CN109361833A (en) * | 2018-10-08 | 2019-02-19 | 南昌大学 | A kind of transmitting device and method of single photon compression video |
| CN109361833B (en) * | 2018-10-08 | 2020-08-11 | 南昌大学 | Transmission method of single photon compression video transmission device |
| CN111896103A (en) * | 2020-07-02 | 2020-11-06 | 西安交通大学 | Signal amplification device and method based on multipath quantum interference |
| CN111896103B (en) * | 2020-07-02 | 2021-06-29 | 西安交通大学 | Signal amplification device and method based on multipath quantum interference |
| CN113093166A (en) * | 2021-04-07 | 2021-07-09 | 毕思文 | Detection imaging optical system based on compressed-state light field |
| CN114414505A (en) * | 2022-01-22 | 2022-04-29 | 山东润一智能科技有限公司 | Intelligent monitoring terminal for quantum spectrum microorganisms |
| CN114545643A (en) * | 2022-04-22 | 2022-05-27 | 北京航空航天大学 | Single photon imaging system based on polarization noise reduction |
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| WO2010069116A1 (en) | 2010-06-24 |
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Open date: 20100623 |