CN107941353A - A kind of mensuration based on the associated coherence vortex topological charge of two-photon - Google Patents
A kind of mensuration based on the associated coherence vortex topological charge of two-photon Download PDFInfo
- Publication number
- CN107941353A CN107941353A CN201711181534.9A CN201711181534A CN107941353A CN 107941353 A CN107941353 A CN 107941353A CN 201711181534 A CN201711181534 A CN 201711181534A CN 107941353 A CN107941353 A CN 107941353A
- Authority
- CN
- China
- Prior art keywords
- photons
- light modulator
- spatial light
- photon
- topological charge
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000005540 biological transmission Effects 0.000 claims abstract description 24
- 238000000034 method Methods 0.000 claims abstract description 9
- 230000001427 coherent effect Effects 0.000 claims description 13
- 238000000691 measurement method Methods 0.000 claims description 6
- 239000000835 fiber Substances 0.000 claims description 4
- 230000002596 correlated effect Effects 0.000 claims description 2
- 230000005428 wave function Effects 0.000 claims description 2
- 230000003287 optical effect Effects 0.000 abstract description 13
- 238000005259 measurement Methods 0.000 abstract description 9
- 239000013307 optical fiber Substances 0.000 abstract description 6
- 230000006870 function Effects 0.000 description 7
- 238000003384 imaging method Methods 0.000 description 4
- 238000004891 communication Methods 0.000 description 3
- 238000004364 calculation method Methods 0.000 description 2
- 230000001276 controlling effect Effects 0.000 description 2
- 230000000875 corresponding effect Effects 0.000 description 2
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- PCTMTFRHKVHKIS-BMFZQQSSSA-N (1s,3r,4e,6e,8e,10e,12e,14e,16e,18s,19r,20r,21s,25r,27r,30r,31r,33s,35r,37s,38r)-3-[(2r,3s,4s,5s,6r)-4-amino-3,5-dihydroxy-6-methyloxan-2-yl]oxy-19,25,27,30,31,33,35,37-octahydroxy-18,20,21-trimethyl-23-oxo-22,39-dioxabicyclo[33.3.1]nonatriaconta-4,6,8,10 Chemical compound C1C=C2C[C@@H](OS(O)(=O)=O)CC[C@]2(C)[C@@H]2[C@@H]1[C@@H]1CC[C@H]([C@H](C)CCCC(C)C)[C@@]1(C)CC2.O[C@H]1[C@@H](N)[C@H](O)[C@@H](C)O[C@H]1O[C@H]1/C=C/C=C/C=C/C=C/C=C/C=C/C=C/[C@H](C)[C@@H](O)[C@@H](C)[C@H](C)OC(=O)C[C@H](O)C[C@H](O)CC[C@@H](O)[C@H](O)C[C@H](O)C[C@](O)(C[C@H](O)[C@H]2C(O)=O)O[C@H]2C1 PCTMTFRHKVHKIS-BMFZQQSSSA-N 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000002050 diffraction method Methods 0.000 description 1
- 238000005315 distribution function Methods 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 238000005305 interferometry Methods 0.000 description 1
- 230000000877 morphologic effect Effects 0.000 description 1
- 238000012576 optical tweezer Methods 0.000 description 1
- 230000008447 perception Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 230000004304 visual acuity Effects 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J11/00—Measuring the characteristics of individual optical pulses or of optical pulse trains
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The present invention relates to a kind of measuring method based on the associated coherence vortex topological charge of two-photon.The measuring method based on the associated coherence vortex topological charge of two-photon includes the following steps:Produce incoherent entangled photon pairs;The entangled photon pairs are divided into i photons and s photons by beam splitter;Control computer makes to obtain vortex phase by the s photons of spatial light modulator, and optical signal then is coupled to single mode optical fiber, spot measurement is carried out with avalanche diode;Control computer makes to obtain specific amplitude and phase by the i photons of spatial light modulator, and optical signal then is coupled to single mode optical fiber, spot measurement is carried out with avalanche diode;Optical signal measured by two-way is associated and calculates and is recorded with computer;By varying the transmission coefficient of the spatial light modulator of light path where i photons, the maximum in output relating value is found;I photon transmission coefficients corresponding to the maximum are exactly the vortex topology charge values of s photons.The present invention, as light source, measures the topological charge of coherence vortex in single photon level, has the advantages that measurement result is accurate, measurement range is big using incoherent entangled photon pairs.
Description
Technical Field
The invention relates to a method for measuring coherent vortex topological charge based on two-photon correlation, and belongs to the field of quantum sensing.
Technical Field
The vortex beam is a special optical field with a spiral phase wavefront and the phase distribution function of the optical field is exp (il theta), and each photon of the optical field carries a specific orbital angular momentumWhere l is called the topological charge and θ is the azimuth. For partially coherent light with poor coherence, there is generally no optical vortex with zero intensity, but there is a coherent vortex with zero spectral coherence or mutual coherence function. The topological charge of the coherent vortex has important application prospect in optical tweezers, laser communication and quantum cryptography systems. Orbital angular momentum state | l of photon&With completeness, orthogonality and infinite dimensions, which has been demonstrated as an effective degree of freedom for application as high-dimensional hilbert space quantum information (see academic papers Franke-Arnold S, allen L, padgett m.advances in optical and regular expression. Laser Photon Rev 2008 2.
Two-photon entanglement means that two photons are not in a localized form, and when one of the photons is changed, the other photon is correspondingly changed under any condition. Entangled bifocal wavelets, which are quantum morphological coherent functions, can be used to reflect coherent vortices in the two-photon entangled state (see academic paper Li-garg Wang et al, ABCD law of two-mode Gaussian-oriented light fields in optical Communications 284 (2011) 5860-5865). Two-photon correlation imaging is a novel imaging mechanism which utilizes quantum entanglement characteristic of a light source to obtain diffraction images of an object in a light path without the object. Such correlated imaging, also known as ghost imaging, is now widely used in the fields of distributed image processing, distributed perception and communications.
The current methods for measuring the topological charge of the optical vortex mainly comprise the following steps: interferometry and diffraction. When the coherence of the light source is reduced, the interference method cannot accurately judge the topological charge value. When the light source topological charge value is large, the resolving power of the diffraction method is reduced. In addition, the above two methods employ pseudo-thermal laser as a light source. The improvement of the accuracy of the measurement signal is seriously restricted by the thermal noise of the light source, so that the vortex topological information of the light source is difficult to accurately identify on the single photon level.
Disclosure of Invention
The invention aims to provide a two-photon correlation-based coherent vortex topological charge measuring method aiming at the defects of the prior art.
The purpose of the invention is realized by the following technical scheme. A two-photon correlation-based measurement method of coherent vortex topological charge comprises the following steps:
(1) Generating incoherent entangled photon pairs;
(2) Splitting the entangled photon pair into i photons and s photons by a beam splitter;
(3) Controlling a computer to enable s photons passing through the spatial light modulator to obtain a vortex phase, then coupling an optical signal to a single-mode optical fiber, and carrying out single-point measurement by using an avalanche diode;
(4) Controlling a computer to enable i photons passing through the spatial light modulator to obtain specific amplitude and phase, then coupling an optical signal to a single-mode optical fiber, and carrying out single-point measurement by using an avalanche diode;
(5) Performing correlation calculation on the two paths of measured optical signals and recording the correlation calculation by using a computer;
(6) By changing the transmission coefficient l of the spatial light modulator on the light path where the i photon is located, the transmission coefficient corresponding to the maximum value in the output values is the vortex topological charge value of the s photon.
The incoherent entangled photon pair used in the present invention is generated by a dual mode laser.
The method has the beneficial effect that the vortex light beam can be measured on the single photon level. The measurement result is visual, and the measurement range is large.
Drawings
Fig. 1 shows a schematic diagram used in one embodiment of the present invention.
Detailed Description
The present invention will be described in further detail with reference to examples, which are illustrative of the present invention.
FIG. 1 is a schematic diagram for one embodiment of the present invention. It includes: a dual-mode correlation laser 1; a beam splitter 2; a first band-pass filter 3; a first spatial light modulator 4; a first computer 5; a second band-pass filter 6; a second spatial light modulator 7; a second computer 8; a first lens 9; a first single mode optical fiber 10; a first avalanche photodiode 11; a second lens 12; a second single mode optical fiber 13; a second avalanche photodiode 14; a correlation counter 15; a third computer 16.
Referring to fig. 1, the working steps of a two-photon correlation-based measurement method of coherent vortex topological charge are as follows:
1. the dual-mode correlation laser 1 generates a Gaussian entangled two-photon pair; the wave function of the gaussian entangled photon pair is:
ψ in (x 1 ,y 1 ;x 2 ,y 2 )=G 0 exp[-2(x 1 2 +y 1 2 )/σ s 2 ]δ(x 1 -x 2 )δ(y 1 -y 2 )
wherein G is 0 Is a constant number, x 1 ,y 1 Is the transverse coordinate, x, of one of the entangled photons 2 ,y 2 Is the transverse coordinate, σ, of another entangled photon s Represents the laser output spot radius; the Gaussian entangled photon pair is split into two photons by the beam splitter 2, and the two photons respectively enter a transmission light path s and a reflection light path i of the beam splitter 2; the photons entering the beam splitter 2 transmission path s are called s-photons, the photons entering the beam splitter 2 transmission path i are called i-photons;
2. the s photons enter a first spatial light modulator 4 after passing through a first band-pass filter 3; the distance between the beam splitter 2 and the first spatial light modulator 4 is q 1 (ii) a The first spatial light modulator 4 is connected with the first computer 5, and enables s photons emitted from the first spatial light modulator to obtain a vortex phase with a topological charge of m under the control of the first computer 5;
3. the i photons enter a second spatial light modulator 7 after passing through a second band-pass filter 6; the distance between the beam splitter 2 and the first spatial light modulator 4 is q 1 And q is 1 >q 2 (ii) a The second spatial light modulator 7 is connected with a second computer 8, and enables i photons emitted from the second spatial light modulator to obtain specific amplitude and phase under the control of the second computer 8; the transmission function of the second spatial light modulator 7 is:
where l is the transmission coefficient, p is a non-negative integer, v x Is the x-component, v, of the transverse coordinate of the transmission function y Is the y-component of the transverse coordinate of the transmission function, λ is the wavelength of the incoherent entangled photon pair, H a () Indicates that hermitian polynomial a is the corresponding order;
4. s photons exiting the first spatial light modulator 4 are coupled into a first single mode fiber 10 through a first lens 9 and received by a first avalanche photodiode 11; z is a radical of 1 Is the distance from the first spatial light modulator 4 to the first lens 9 and satisfies q 2 -q 1 =z 1 ;
5. I photons exiting the second spatial light modulator 7 are coupled into a second single mode fiber 13 through a second lens 12 and received by a second avalanche photodiode 14;
6. the output signals of the first avalanche photodiode 11 and the second avalanche photodiode 14 enter the associated counter 15 and are recorded by the third computer 16;
7. changing the coefficient l of the transmission function of the second spatial light modulator 7 by means of the second computer 8 and recording the output value of the correlation counter 15; when the correlation counter 15 obtains the maximum output signal, the transmission coefficient l taken by the second spatial light modulator 7 is the vortex topological charge value m of s photons;
8. the output value of the correlation counter 15 is the first order correlation signal of i photons to s photons:
where n and m are non-negative integers, δ () is the dirac function, l is the transmission coefficient of the second spatial light modulator 7, and m is the vortex topological charge value of the s photons.
Claims (4)
1. A two-photon correlation-based measurement method of coherent vortex topological charge is characterized by comprising the following steps:
(1) The incoherent entangled photon pair is split into two photons by the beam splitter 2, and the two photons respectively enter a transmission light path s and a reflection light path i of the beam splitter 2; the photons entering the beam splitter 2 transmission path s are called s-photons, the photons entering the beam splitter 2 transmission path i are called i-photons;
(2) The s photons enter a first spatial light modulator 4 after passing through a first band-pass filter 3; the distance between the beam splitter 2 and the first spatial light modulator 4 is q 1 (ii) a The first spatial light modulator 4 is connected with the first computer 5, and enables s photons emitted from the first spatial light modulator to obtain a vortex phase with a topological charge of m under the control of the first computer 5;
(3) The i photons enter a second spatial light modulator 7 after passing through a second band-pass filter 6; the distance between the beam splitter 2 and the first spatial light modulator 4 is q 2 And q is 1 >q 2 (ii) a The second spatial light modulator 7 is connected with a second computer 8, and enables i photons emitted from the second spatial light modulator to obtain specific amplitude and phase under the control of the second computer 8;
(4) S photons exiting the first spatial light modulator 4 are coupled into a first single mode fiber 10 through a first lens 9 and received by a first avalanche photodiode 11; z is a radical of 1 Is the distance from the first spatial light modulator 4 to the first lens 9 and satisfies q 2 -q 1 =z 1 ;
(5) I photons exiting the second spatial light modulator 7 are coupled into a second single mode fiber 13 through a second lens 12 and received by a second avalanche photodiode 14;
(6) The output signals of said first avalanche photodiode 11 and said second avalanche photodiode 14 enter into a correlated counter 15 and are recorded by a third computer 16;
(7) Changing the coefficient l of the transmission function of the second spatial light modulator 7 by means of the second computer 8 and recording the output value of the correlation counter 15; when the associated counter 15 obtains the maximum output signal, the transmission coefficient l taken by the second spatial light modulator 7 is the vortex topological charge value m of s photons.
2. The method of claim 1, wherein the incoherent entangled photon pair is generated by a dual-mode correlation laser with a wave function of:
ψ in (x 1 ,y 1 ;x 2 ,y 2 )=G 0 exp[-2(x 1 2 +y 1 2 )/σ s 2 ]δ(x 1 -x 2 )δ(y 1 -y 2 )
wherein G is 0 Is a constant number, x 1 ,y 1 Is the transverse coordinate, x, of one of the entangled photons 2 ,y 2 Is the transverse coordinate, σ, of another entangled photon s Representing the spot radius of the laser output beam.
3. The two-photon correlation-based measurement method of the coherent vortex topological charge according to claim 1, wherein the transmission function of the second spatial light modulator 7 is as follows:
where l is the transmission coefficient of said second spatial light modulator 7, j is an imaginary unit, p is a non-negative integer, v x Is the x-component, v, of the transverse coordinate of the transmission function y Is the y-component of the transverse coordinate of the transmission function, λ is the wavelength of the incoherent entangled photon pair, H a () Expressing hermite polynomials, wherein the following table a indicates the order.
4. The measurement method of coherent vortex topological charge based on two-photon correlation according to claim 1, characterized in that the output value of said correlation counter 15 is a first order correlation signal of i photon and s photon:
where n and p are non-negative integers, δ () is the dirac function, l is the transmission coefficient of the second spatial light modulator 7, and m is the vortex topological charge value of the s photons.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711181534.9A CN107941353B (en) | 2018-03-06 | 2018-03-06 | Two-photon correlation-based coherent vortex topology charge measurement method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201711181534.9A CN107941353B (en) | 2018-03-06 | 2018-03-06 | Two-photon correlation-based coherent vortex topology charge measurement method |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107941353A true CN107941353A (en) | 2018-04-20 |
CN107941353B CN107941353B (en) | 2024-01-09 |
Family
ID=61930931
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201711181534.9A Active CN107941353B (en) | 2018-03-06 | 2018-03-06 | Two-photon correlation-based coherent vortex topology charge measurement method |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107941353B (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110187487A (en) * | 2019-06-13 | 2019-08-30 | 福建师范大学 | Single wavelength two-photon STED and dual wavelength single photon STED coupling imaging device and method |
CN110441787A (en) * | 2019-08-23 | 2019-11-12 | 中国科学院重庆绿色智能技术研究院 | A kind of quantum radar method for realizing three-dimensional accuracy enhancing |
CN110441262A (en) * | 2019-08-28 | 2019-11-12 | 中国地质大学(北京) | A kind of non-localized phase object edge enhancing method and its system |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102944312A (en) * | 2012-11-23 | 2013-02-27 | 苏州大学 | Method for measuring partially coherent vortex light beam topological charge number |
CN103954367A (en) * | 2014-04-18 | 2014-07-30 | 河南科技大学 | Device for measuring fractional-order optical vortex topology charge values and measuring method thereof |
CN104121996A (en) * | 2014-07-21 | 2014-10-29 | 河南科技大学 | Measuring device for measuring vortex light beam high-order topological charge |
US20150212308A1 (en) * | 2012-04-13 | 2015-07-30 | Bioaxial Sas | Optical Measurement Method and Device |
CN106932107A (en) * | 2017-04-07 | 2017-07-07 | 哈尔滨工业大学 | A kind of topological charge measurement apparatus based on far field construction principle |
CN206583537U (en) * | 2017-01-20 | 2017-10-24 | 中国计量大学 | A kind of device of utilization light distribution information measurement Gaussian vortex light topological charge |
-
2018
- 2018-03-06 CN CN201711181534.9A patent/CN107941353B/en active Active
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20150212308A1 (en) * | 2012-04-13 | 2015-07-30 | Bioaxial Sas | Optical Measurement Method and Device |
CN102944312A (en) * | 2012-11-23 | 2013-02-27 | 苏州大学 | Method for measuring partially coherent vortex light beam topological charge number |
CN103954367A (en) * | 2014-04-18 | 2014-07-30 | 河南科技大学 | Device for measuring fractional-order optical vortex topology charge values and measuring method thereof |
CN104121996A (en) * | 2014-07-21 | 2014-10-29 | 河南科技大学 | Measuring device for measuring vortex light beam high-order topological charge |
CN206583537U (en) * | 2017-01-20 | 2017-10-24 | 中国计量大学 | A kind of device of utilization light distribution information measurement Gaussian vortex light topological charge |
CN106932107A (en) * | 2017-04-07 | 2017-07-07 | 哈尔滨工业大学 | A kind of topological charge measurement apparatus based on far field construction principle |
Non-Patent Citations (2)
Title |
---|
周洋;李新忠;王静鸽;王辉;李贺贺;: "涡旋光束拓扑荷值的干涉测量方法", 河南科技大学学报(自然科学版), vol. 37, no. 03 * |
柯熙政;胥俊宇;: "涡旋光束轨道角动量干涉及检测的研究", 中国激光, vol. 43, no. 09 * |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110187487A (en) * | 2019-06-13 | 2019-08-30 | 福建师范大学 | Single wavelength two-photon STED and dual wavelength single photon STED coupling imaging device and method |
CN110187487B (en) * | 2019-06-13 | 2021-07-27 | 福建师范大学 | Single-wavelength two-photon STED and dual-wavelength single-photon STED coupling imaging device and method |
CN110441787A (en) * | 2019-08-23 | 2019-11-12 | 中国科学院重庆绿色智能技术研究院 | A kind of quantum radar method for realizing three-dimensional accuracy enhancing |
CN110441262A (en) * | 2019-08-28 | 2019-11-12 | 中国地质大学(北京) | A kind of non-localized phase object edge enhancing method and its system |
Also Published As
Publication number | Publication date |
---|---|
CN107941353B (en) | 2024-01-09 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN102944312B (en) | Method for measuring partially coherent vortex light beam topological charge number | |
CN101846745B (en) | Laser radar based on highly-correlated quantum imaging principle | |
CN106896498A (en) | Generation/the three-dimensional reconstruction apparatus and method of Laguerre Gauss vortex beams | |
CN107179132B (en) | Optical fiber image transmission beam velocity interferometer and shock wave velocity calculation method | |
CN103616165B (en) | Loss measurement of optic fibre system | |
CN102289152B (en) | Optical system wave aberration detection device | |
CN101634571B (en) | Optical pulse raster distributed fiber sensing device | |
CN107941353A (en) | A kind of mensuration based on the associated coherence vortex topological charge of two-photon | |
CN102998260B (en) | Two-photon entanglement-based terahertz wave imaging device | |
CN115494479B (en) | Single photon radar system based on pulse sequence extraction and 3D imaging method | |
CN101476978B (en) | Method for measuring geometric parameter of single mode fiber | |
CN102564612B (en) | Component prism-based phase diversity wavefront sensor | |
CN207798009U (en) | A kind of device of the radial displacement sensing based on Gauss vortex light | |
CN105444679B (en) | It can inhibit the inclined symmetrical laser displacement sensor of laser drift and surface | |
CN102401691A (en) | All-fibre laser Doppler three-dimensional vibration meter | |
CN110161528A (en) | A kind of scene of fire complex environment laser three-dimensional imaging method based on optical coherence tomography | |
CN105333815A (en) | Super lateral resolution surface three-dimensional online interference measuring system based on spectral dispersion line scanning | |
CN105571826A (en) | Evaluation method of laser beam quality of low-numerical aperture large-mode field area fiber | |
CN114333522A (en) | Single-photon and double-photon interference device and control method thereof | |
CN105717322B (en) | A kind of underwater high-speed target velocity test device | |
CN102410809B (en) | Complete common-path type microchip laser feedback interferometer | |
CN106646758A (en) | Self-adaption coupling system for single mode optical fiber based on two-dimensional scanning of optical fiber end surface | |
CN203929276U (en) | A kind of optical signal detecting disposal system based on resonance technique | |
KR100996140B1 (en) | cross correlator for measuring ultrashort laser pulse and method thereof | |
CN114460045B (en) | Method for measuring optical transmission matrix of scattering medium |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |