CN108827988A - Non-local modulation of X-ray diffraction imaging device and method based on light field High order correletion - Google Patents

Non-local modulation of X-ray diffraction imaging device and method based on light field High order correletion Download PDF

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CN108827988A
CN108827988A CN201810603834.XA CN201810603834A CN108827988A CN 108827988 A CN108827988 A CN 108827988A CN 201810603834 A CN201810603834 A CN 201810603834A CN 108827988 A CN108827988 A CN 108827988A
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modulation
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modulator
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谈志杰
喻虹
陆荣华
韩申生
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Shanghai Institute of Optics and Fine Mechanics of CAS
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/20Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/05Investigating materials by wave or particle radiation by diffraction, scatter or reflection
    • G01N2223/056Investigating materials by wave or particle radiation by diffraction, scatter or reflection diffraction
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/10Different kinds of radiation or particles
    • G01N2223/101Different kinds of radiation or particles electromagnetic radiation
    • G01N2223/1016X-ray

Abstract

A kind of non-local modulation of X-ray diffraction imaging device and method based on light field High order correletion, device includes x-ray source, beam splitting chip, object under test, non-local modulator, X-ray surface detector, X-ray point detector and computer, and non-local modulator includes mask modulator and lens modulator.The light that x-ray source issues passes through beam splitting chip, and transmitted light passes through non-local modulator along optical axis direction, and intensity signal is recorded by X-ray surface detector, and along optical axis direction by object under test, intensity signal is recorded reflected light by X-ray point detector.X-ray source is equal to two detector distances.Computer is connected with X-ray surface detector and point detector, has the program that operation is associated to collected light intensity sequence.The present invention is based on the modulation of the non-local of light field High order correletion, can be improved picture quality and resolution ratio that X-ray diffraction imaging restores image.

Description

Non-local modulation of X-ray diffraction imaging device and method based on light field High order correletion
Technical field
The present invention relates to X-ray diffraction imaging, especially a kind of non-local modulation of X-ray based on light field High order correletion Diffraction imaging device and method.
Background technique
Existing X-ray Fourier transformation diffraction imaging method, only X-ray coherent diffraction imaging (XCDI) are a kind of, it It is to be radiated on object under test using coherent X-ray, using the Fraunhofer diffraction intensity distribution of object light field, obtain the object The Fourier transformation intensity distribution of transmittance function, then amplitude and phase letter using Phase Retrieve Algorithm recovery object under test Breath.This X-ray coherent diffraction imaging technology mainly has following limitation:
1) imaging beam must be coherent X-ray, and sample to be tested size is limited by X-ray lateral coherence scale.To For three generations's synchrotron radiation X-ray imaging device, maximum sample to be tested size is only 10 micron dimensions;For using X-ray tube Conventional compact x-ray imaging device can not carry out X-ray coherent diffraction imaging since its spatial coherence is poor completely.
2) imaging beam must transmit longer distance (meeting fraunhofer condition) after object, can just detect The Fourier transformation strength information of object transmittance function.For forth generation synchrotron radiation X-ray imaging device, although energy Meet the relevant condition of light beam large area, but sample to be tested size is limited by Fraunhofer diffraction condition, such as:Using wavelength 1nm Coherent X-ray diffraction imaging is carried out to the sample of size 1mm, required detection range reaches 1 kilometer.
3) it since X-ray has high penetrability, carries out corresponding in detector center when X-ray coherent diffraction imaging There is high-intensitive transmitted light in position, often absorbed using beam stop in actual imaging device, therefore, obtained to spread out Penetrate in intensity distribution that there are the direct current of image and low-frequency components to lack.
4) the Fourier transformation intensity distribution for the object transmittance function that detection obtains, needs to carry out Phase Retrieve Algorithm Restore the amplitude and phase of object under test.The algorithm of extensive utilization is HIO algorithm at present, which cannot be guaranteed to converge to complete Office's optimal solution, and it is more sensitive for initial value.
For the phase retrieval problem in X-ray coherent diffraction imaging, Candas of Stanford University et al. proposes one Phase Retrieve Algorithm (E.J.Candes, et., al, " the Phase retrieval from that kind is modulated based on random coded coded diffraction patterns,”Appl.Comput.Harmon.Anal.,vol.39,no.2,pp. 277–299, 2015).The algorithm can significantly improve the recovery picture quality of phase recovery.However the algorithm is needed in object plane to light field It is modulated, non-local modulator is needed to be completely coincident with object under test, it is relatively difficult to achieve in practice.
Analogy rainbow of Shanghai Optics and Precision Mechanics institute, Chinese Academy of Sciences et al. devises incoherent X-ray diffraction imaging Device (Noncoherent X ray diffraction imaging device, 201110148476.6), and X-ray Fourier transformation was completed in 2016 The principle demonstration of relevance imaging (XFGI) tests (H.Yu et al., " Fourier-Transform Ghost Imaging with Hard X Rays,"Phys.Rev.Lett.,vol.117,no. 11,2016).The imaging method does not need coherent light Source can be obtained by the Fourier transformation intensity distribution of object transmittance function, recover object by Phase Retrieve Algorithm later Body, obtained result are similarly limited to Phase Retrieve Algorithm.
Summary of the invention
The technical problem to be solved in the present invention is that overcoming the defect of above-mentioned first technology, provide a kind of based on non-local The incoherent light X-ray diffraction imaging device and method of modulation, by adding non-local on the reference arm of light beam Free propagation Modulator, to obtain better phase recovery result using new Phase Retrieve Algorithm.
Technical solution of the invention is as follows:
A kind of non-local modulation of X-ray diffraction imaging device based on light field High order correletion, feature are that its composition includes X-ray source, beam splitting chip, object under test, non-local modulator, X-ray surface detector, X-ray point detector and computer, it is non- Local modulator includes mask modulator and lens modulator, and the light that the X radiographic source issues is divided into transmission by beam splitting chip Light and reflected light are successively non-local modulator and X-ray surface detector along transmission light direction, are to be measured along reflection light direction Object and X-ray point detector, the distance of the x-ray source to the X-ray surface detector and the x-ray source To being equidistant for the X-ray point detector, the input terminal of the computer and the X-ray surface detector and The output end of point detector is connected, and the computer has the program that operation is associated to collected light intensity sequence.
The x-ray source is true thermal X-rays source or counterfeit thermal X-rays source.
The size of the non-local modulator is greater than object under test, and there are mainly two types of modulation types:
<1>Mask modulation:Mask modulator and object under test away from the x-ray source apart from identical, in one experiment In the same size there may be multiple random mask modulators, structure distribution is different, and a kind of structure distribution is a kind of non-local Modulation;
<2>Lens modulation:With fixed focal length.
It is special using the imaging method of the above-mentioned non-local modulation of X-ray diffraction imaging device based on light field High order correletion Point is that the imaging method includes the following steps:
<1>It adjusts x-ray source and beam splitting chip, X-ray surface detector, X-ray point detector is coaxial, and two detectors Apart from being equidistant for x-ray source, distance is d, object under test is put into optical path, the distance away from X-ray point detector is d2, adjust object under test and light path coaxial;
<2>Within a coherence time of x-ray source, the X-ray surface detector and the exposure of X-ray point detector Once, it obtains without modulation reference picture and detection light intensity, respectivelyWith
<3>Within the coherence time of x-ray source, the lens modulator is put into optical path, focal length f, with Distance d of the lens modulator apart from X-ray surface detector2' meet following relationship:
The exposure of X-ray surface detector is primary, obtains lens and modulates reference picture
<4>Within the coherence time of x-ray source, lens modulator is removed into optical path, mask modulator is moved into light Road, the exposure of X-ray surface detector is primary, obtains mask and modulates reference picture
<5>Different mask modulators is replaced by the way of moving in and out, and obtains mask on X-ray surface detector Reference picture is modulated,N therein is the quantity of whole mask modulators, N be 3 or more it is just whole Number;
<6>Step is repeated several times<2>,<3>,<4>,<5>, obtain relevance imaging sequenceWith Wherein n=1 ..., N, k=1 ..., K, K are total pendulous frequency;
<7>Operation is associated to relevance imaging sequence, specific practice is:
1. by a certain group of relevance imaging sequence without modulation reference pictureOn different location xrThe light intensity value at placeWith detection light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation in relevance imaging sequence DistributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
2. calculating detection light intensity sequenceThe average value of k=1 ..., KIt calculates without modulation reference image sequenceThe average value of k=1 ..., KFinally calculate? To the information without the object under test under modulation, i.e. Fourier's information of object under test;
3. a certain group of relevance imaging sequence lens are modulated reference pictureOn different location xrThe light intensity value at placeWith detection light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation in relevance imaging sequence DistributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
4. calculating lens reference image sequenceThe average value of k=1 ..., KFinally calculateObtain the information of the object under test under lens modulation, i.e. object under test Low resolution real space information;
5. the mask of a certain group of relevance imaging sequence certain structure is modulated reference pictureOn different location xrPlace Light intensity valueWith detection light intensityIt is associated operation, it is unmodulated to obtain a certain moment in relevance imaging sequence Intensity correlation distributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
6. calculating the mask modulation reference image sequence of certain structureThe average value of k=1 ..., K Finally calculateObtain the object under test under the mask modulation of certain structure Information, that is, modulate after object under test Fourier's information;
<8>It utilizes<7>Obtained in Fourier's information of object under test, the low resolution real space information of object under test with And Fourier's information of object under test carries out phase recovery after N kind difference mask modulation, obtains the high-resolution occupied space of object under test Between be distributed.
Technical effect of the invention is as follows:
The present invention utilizes incoherent X-ray, can realize X-ray Fourier transformation diffraction imaging in Fresnel region, have The existing advantage of Noncoherent X ray diffraction imaging device based on light field High order correletion.
The present invention in reference arm addition non-local modulation, can be improved the image that X-ray diffraction imaging restores image simultaneously Quality and resolution ratio.
Detailed description of the invention
Fig. 1 is the structural representation of the non-local modulation of X-ray diffraction imaging device the present invention is based on light field High order correletion Scheme, in figure:
1:X-ray source, 2:Beam splitting arrangement, 3:Object under test, 4:Non-local modulator, 401:Mask modulator, 402:Thoroughly Mirror modulator;5:X-ray planar array detector, 6:X-ray point detector, 7:Computer.
Fig. 2 is the non-local modulation of X-ray diffraction imaging technology mask modulating mode the present invention is based on light field High order correletion Flowering structure schematic diagram.
Fig. 3 is the non-local modulation of X-ray diffraction imaging device lens modulating mode the present invention is based on light field High order correletion Flowering structure schematic diagram.
Fig. 4 is the phase distribution structural schematic diagram of the mask modulator of certain distribution.
Specific embodiment
The present invention is based on the non-local modulation of X-ray diffraction imaging devices of light field High order correletion, as shown in Figure 1, including X Radiographic source 1, beam splitting arrangement 2, object under test 3, non-local modulator 4, X-ray surface detector 5, X-ray point detector 6 and meter Calculation machine 7.X-ray source 1, beam splitting arrangement 2, object under test 3, random non-local modulator 4, X-ray surface detector 5 and point detection Device 6 is in sustained height.Non-local modulator 4 includes mask modulator 401 and lens modulator 402.X-ray source 1 is penetrated to X The distance of line surface detector 5 and being equidistant to X-ray point detector 6.It is penetrated by the intensity information of object under test 3 by X Line point detector 6 receives record, is recorded and receives by X-ray surface detector 5 by the intensity information of non-local modulator.Institute The computer 7 stated is connected with the output end of two X-ray detectors, has and is associated operation to collected light intensity sequence Program, more object informations are obtained using the modulation of different non-locals, so as to preferably recover object under test.
Non-local modulation of X-ray diffraction imaging device of the present embodiment based on light field High order correletion mainly includes three kinds of works Operation mode:
(1) without modulating mode (as shown in Figure 1):Mask modulator 401 and lens modulator 402 are removed into optical path, X is penetrated The direct recording light intensity information of line surface detector 5.
(2) mask modulating mode (as shown in Figure 2):The amplitude of mask modulator 401 is 1 in the present embodiment, and phase is random The modulator of distribution, mask modulator 401 are equidistant with object under test 3 away from x-ray source 1.May exist in one experiment Multiple mask modulators, structure distribution are different, and a kind of structure distribution is that a kind of non-local is modulated, and Fig. 3 show a kind of mask The schematic diagram of distributed architecture.A kind of Fourier that mask modulation passes through object under test 3 after the association available coded modulation of operation Strength information.
(3) lens modulating mode (as shown in Figure 3):With fixed focal length.Lens modulator 402 is along optical axis direction Can be with vertical adjustment, each lengthwise position is a kind of modulation of non-local.A kind of lens modulation is available by association operation The low resolution real space information of object under test 3, the low real space information of differentiating can be used as the supported collection quickening phase of phase recovery Bit recovery convergence rate.
It is imaged using the non-local modulation of X-ray diffraction imaging device based on light field High order correletion of the present embodiment, Its imaging method includes the following steps:
<1>It adjusts x-ray source 1 and beam splitting chip 2, X-ray surface detector 5, X-ray point detector 6 is coaxial, and two spies Survey device being equidistant apart from x-ray source 1, distance be d, object under test 3 is put into optical path, away from X-ray point detector away from From for d2, adjust itself and light path coaxial;
The distance d of two detector distance x-ray sources is 40 centimetres in the present embodiment, and object under test is apart from X-ray point The distance d of detector2It is 30 centimetres;
<2>Within a coherence time of x-ray source 1, X-ray surface detector 5 and the exposure of X-ray point detector 6 one It is secondary, it obtains without modulation reference picture and detection light intensity, respectivelyWith
<3>Within the coherence time of x-ray source 1, lens modulator 402 is put into optical path, focal length f, with it Distance d apart from X-ray surface detector 52' meet following relationship:
X-ray surface detector 5 exposes once, obtains lens and modulates reference picture;
In the present embodiment, the focal length of lens is 4.16 centimetres, and the distance away from X-ray surface detector 5 is 25 centimetres, full It is enough co-relation.
<4>Within the coherence time of x-ray source 1, lens modulator 402 is removed into optical path, by mask modulator 401 Optical path is moved into, X-ray surface detector 5 exposes once, obtains mask and modulates reference picture
<5>Different mask modulators 401 is replaced by the way of moving in and out, and is obtained on X-ray surface detector 5 Mask modulates reference picture,N therein is the quantity of whole mask modulators 401;
The x-ray source 1 of the present embodiment is counterfeit thermal light source, coherence time T0It is 40 seconds.Mask modulator 401 shares 3 kinds not Same distributed architecture, i.e. N=3, lens modulator 402 have a determining position, replace 401 time of mask modulator every time It is 5 seconds, the time of replacement lens modulator 402 is 8 seconds, and X-ray surface detector 5 and each time for exposure of point detector 6 are 1 Second.Therefore obtaining 4 width modulation reference arm image in one group of relevance imaging and detecting the time interval T of light intensity is 28 seconds, meets and closes Join image-forming condition:T < T0
<6>Step is repeated several times<2>,<3>,<4>,<5>, obtain relevance imaging sequenceWith Wherein n=1 ..., N, k=1 ..., K, K are total pendulous frequency;
<7>Operation is associated to relevance imaging sequence, specific practice is:
1. by a certain group of relevance imaging sequence without modulation reference pictureOn different location xrThe light intensity value at placeWith detection light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation in relevance imaging sequence DistributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
2. calculating detection light intensity sequenceThe average value of k=1 ..., KIt calculates without modulation reference image sequenceThe average value of k=1 ..., KFinally calculate? To certain information without the object under test under modulation, i.e. Fourier's information of object under test.
Without under modulating mode, cross-correlation intensity distribution function and object transmitance distribution function (including amplitude and phase) Between relationship (J.Cheng and S.Han, " Incoherent coincidence can be indicated with formula below imaging and its applicability in X-ray diffraction,”Phys Rev Lett,vol.92, no.9,p.93903,2004.):
Wherein xrFor the position on reference picture, xtFor the position on detection image, x in the present embodimentr=0 is solid for one Fixed point, d are distance of the object under test to X-ray point detector, and t is the transmittance function of object under test, and F is that object under test is saturating Cross the Fourier transformation of rate function.
3. a certain group of relevance imaging sequence lens are modulated reference pictureOn different location xrThe light intensity value at placeWith detection light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation in relevance imaging sequence DistributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
4. calculating lens reference image sequenceThe average value of k=1 ..., KFinally calculateObtain the information of the object under test under the modulation of certain lens, i.e., it is to be measured The low resolution real space information of object.
Under lens modulating mode, relationship between cross-correlation intensity distribution function and object transmitance distribution function can be with It is indicated with formula below:
Wherein d2The distance of X-ray point detector 6, d are arrived for object under test 32' it is that lens modulator 402 arrives X-ray face battle array The distance of detector 5.The enlargement ratio of low-resolution image is 5 times in the present embodiment, by adjusting the focal length and lens of lens Lengthwise position, other enlargement ratios can be obtained.
5. the mask of a certain group of relevance imaging sequence certain structure is modulated reference pictureOn different location xrPlace Light intensity valueWith detection light intensityIt is associated operation, it is unmodulated to obtain a certain moment in relevance imaging sequence Intensity correlation distributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
6. calculating the mask modulation reference image sequence of certain structureThe average value of k=1 ..., K Finally calculateObtain the object under test under the mask modulation of certain structure Information, that is, modulate after object under test Fourier's information.
Under mask modulating mode, relationship between cross-correlation intensity distribution function and object transmitance distribution function can be with It is indicated with formula below:
Wherein SnFor the transmitance of the mask modulator 401 of n distributed architecture, in the present embodiment, non-local modulation Device is phase-only modulation, and phase difference π, the minimum unit size of modulation is 1.5 × 1.5 μm, and total size is 15 × 15 μm, Phase distribution such as Fig. 4.
<8>It utilizes<7>Obtained in Fourier's information of object under test, the low resolution real space information of object under test with And Fourier's information of object under test carries out phase recovery after N kind difference mask modulation, obtains the high-resolution occupied space of object under test Between be distributed.
It is to sum up told, the present invention is a kind of based on the non-local modulation of X-ray diffraction imaging device of light field High order correletion and side Method can realize X-ray Fourier transformation diffraction imaging in Fresnel region, have based on light field height using incoherent X-ray The existing advantage of the associated Noncoherent X ray diffraction imaging device of rank.Simultaneously in reference arm addition non-local modulation, Neng Gouyou Improve picture quality and resolution ratio in effect ground.

Claims (4)

1. a kind of non-local modulation of X-ray diffraction imaging device based on light field High order correletion is characterized in that its composition is penetrated including X Line source (1), beam splitting chip (2), object under test (3), non-local modulator (4), X-ray surface detector (5), X-ray point detector (6) and computer (7), non-local modulator include mask modulator (401) and lens modulator (402), the x-ray source (1) light issued is divided into transmitted light and reflected light by beam splitting chip (2), is successively non-local modulator (4) along transmission light direction It is object under test (3) and X-ray point detector (6), the x-ray source along reflection light direction with X-ray surface detector (5) (1) the X-ray point detector (6) is arrived to the distance of the X-ray surface detector (5) and the x-ray source (1) It is equidistant, the output end of the input terminal of the computer (7) and the X-ray surface detector (5) and point detector (6) It is connected, the computer (7) has the program that operation is associated to collected light intensity sequence.
2. the non-local modulation of X-ray diffraction imaging device according to claim 1 based on light field High order correletion, feature It is that the x-ray source (1) is true thermal X-rays source or counterfeit thermal X-rays source.
3. the non-local modulation of X-ray diffraction imaging device according to claim 1 based on light field High order correletion, feature It is that the size of the non-local modulator (4) is greater than object under test (3), there are mainly two types of modulation types:
<1>Mask modulation:Mask modulator and object under test (3) apart from identical, are once being tested away from the x-ray source (1) In may exist multiple random mask modulators, in the same size, structure distribution is different, and a kind of structure distribution is a kind of non-local Modulation;
<2>Lens modulation:With fixed focal length.
4. the non-local modulation of X-ray diffraction imaging technology based on light field High order correletion told using claim 1, feature It is that the imaging method includes the following steps:
<1>Adjust x-ray source (1) and beam splitting chip (2), X-ray surface detector (5), X-ray point detector (6) coaxially, and two Detector distance x-ray source (1) is equidistant, and distance is d, and object under test (3) is put into optical path, is visited away from X-ray point The distance for surveying device (6) is d2, adjust object under test (3) and light path coaxial;
<2>Within a coherence time of x-ray source (1), the X-ray surface detector (5) and X-ray point detector (6) Exposure is primary, obtains without modulation reference picture and detection light intensity, respectivelyWith
<3>Within the coherence time of x-ray source (1), the lens modulator (402) is put into optical path, focal length is F, the distance d with lens modulator (402) apart from X-ray surface detector (5)2' meet following relationship:
X-ray surface detector (5) exposure is primary, obtains lens and modulates reference picture
<4>Within the coherence time of x-ray source (1), lens modulator (402) are removed into optical path, by mask modulator (401) Optical path is moved into, X-ray surface detector (5) exposure is primary, obtains mask and modulates reference picture
<5>Different mask modulators (401) is replaced by the way of moving in and out, and is obtained on X-ray surface detector (5) Mask modulates reference picture,N therein is the quantity of whole mask modulators (401), N be 3 with On positive integer;
<6>Step is repeated several times<2>,<3>,<4>,<5>, obtain relevance imaging sequenceWithWherein N=1 ..., N, k=1 ..., K, K are total pendulous frequency;
<7>Operation is associated to relevance imaging sequence, specific practice is:
1. by a certain group of relevance imaging sequence without modulation reference pictureOn different location xrThe light intensity value at placeWith Detect light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation distribution in relevance imaging sequenceThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
2. calculating detection light intensity sequenceK=1 ..., the average value of KIt calculates without modulation reference image sequenceK=1 ..., the average value of KFinally calculate? To the information without the object under test under modulation, i.e. Fourier's information of object under test;
3. a certain group of relevance imaging sequence lens are modulated reference pictureOn different location xrThe light intensity value at place With detection light intensityIt is associated operation, obtains a certain moment unmodulated intensity correlation distribution in relevance imaging sequenceThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
4. calculating lens reference image sequenceK=1 ..., the average value of KFinally calculateObtain the information of the object under test under lens modulation, i.e. object under test Low resolution real space information.
5. the mask of a certain group of relevance imaging sequence certain structure is modulated reference pictureOn different location xrThe light intensity at place ValueWith detection light intensityIt is associated operation, a certain moment unmodulated intensity in relevance imaging sequence is obtained and closes Connection distributionThe intensity correlation distribution of different moments is subjected to statistical average again, is obtained
6. calculating the mask modulation reference image sequence of certain structureK=1 ..., the average value of KFinally It calculatesObtain the letter of the object under test under the mask modulation of certain structure Breath, that is, Fourier's information of object under test after modulating.
<8>It utilizes<7>Obtained in Fourier's information of object under test, the low resolution real space information of object under test and N kind Fourier's information of object under test carries out phase recovery after different mask modulation, obtains the high-resolution real space point of object under test Cloth.
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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110243398A (en) * 2019-06-27 2019-09-17 南京邮电大学 A kind of relevance imaging method of the phase object based on relevant detection
CN110715944A (en) * 2019-10-21 2020-01-21 中国科学院高能物理研究所 Device and method for stable X-ray imaging
CN111044541A (en) * 2019-12-26 2020-04-21 苏州光隐科技有限公司 X-ray high-resolution imaging method based on high-order stack association
CN111398318A (en) * 2018-12-14 2020-07-10 中国科学院物理研究所 X-ray single-pixel camera based on X-ray calculation correlation imaging
CN111435194A (en) * 2019-01-15 2020-07-21 南京理工大学 Method for regulating and controlling three-dimensional space structure of light field
CN112198176A (en) * 2020-09-24 2021-01-08 中国科学院上海光学精密机械研究所 Single exposure X-ray diffraction imaging device and method based on light field high-order spatial correlation
CN112229397A (en) * 2020-09-11 2021-01-15 中国科学院上海光学精密机械研究所 Satellite angular position intensity correlation measurement system and method based on spatial modulation
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US11402342B2 (en) * 2018-02-21 2022-08-02 Bar-Ilan University System and method for high-resolution high contrast x-ray ghost diffraction

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101021621A (en) * 2007-02-02 2007-08-22 中国科学院上海光学精密机械研究所 Intensity relevant diffraction imaging device and image recovery method thereof
CN102353689A (en) * 2011-06-03 2012-02-15 中国科学院上海光学精密机械研究所 Noncoherent X ray diffraction imaging device
CN103323396A (en) * 2013-06-28 2013-09-25 中国科学院空间科学与应用研究中心 Two-dimensional compression ghost imaging system and method based on coincidence measurement
CN104021522A (en) * 2014-04-28 2014-09-03 中国科学院上海光学精密机械研究所 Target image separating device and method based on intensity correlated imaging
CN106371201A (en) * 2016-11-03 2017-02-01 清华大学 Fourier overlapping correlation imaging system and method based on computational ghost imaging
CN107219638A (en) * 2017-05-27 2017-09-29 辽宁大学 Super-resolution relevance imaging system and imaging method based on LPF

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101021621A (en) * 2007-02-02 2007-08-22 中国科学院上海光学精密机械研究所 Intensity relevant diffraction imaging device and image recovery method thereof
CN102353689A (en) * 2011-06-03 2012-02-15 中国科学院上海光学精密机械研究所 Noncoherent X ray diffraction imaging device
CN103323396A (en) * 2013-06-28 2013-09-25 中国科学院空间科学与应用研究中心 Two-dimensional compression ghost imaging system and method based on coincidence measurement
CN104021522A (en) * 2014-04-28 2014-09-03 中国科学院上海光学精密机械研究所 Target image separating device and method based on intensity correlated imaging
CN106371201A (en) * 2016-11-03 2017-02-01 清华大学 Fourier overlapping correlation imaging system and method based on computational ghost imaging
CN107219638A (en) * 2017-05-27 2017-09-29 辽宁大学 Super-resolution relevance imaging system and imaging method based on LPF

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
HONG YU 等: "X-ray Fourier-transform Ghost Imaging via Sparsity Constraints", 《2017 IEEE NCLEAR SCIENCE SYMPOSIUM AND SYMPOSIUM AND MEDICAL IMAGING CONFERENCE》 *
张二峰: "二阶和高阶关联成像研究", 《中国优秀硕士学位论文全文数据库 基础科学辑》 *

Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11402342B2 (en) * 2018-02-21 2022-08-02 Bar-Ilan University System and method for high-resolution high contrast x-ray ghost diffraction
CN111398318A (en) * 2018-12-14 2020-07-10 中国科学院物理研究所 X-ray single-pixel camera based on X-ray calculation correlation imaging
US11255800B1 (en) 2018-12-14 2022-02-22 Institute Of Physics, Chinese Academy Of Sciences X-ray single-pixel camera based on x-ray computational correlated imaging
CN111435194A (en) * 2019-01-15 2020-07-21 南京理工大学 Method for regulating and controlling three-dimensional space structure of light field
CN111435194B (en) * 2019-01-15 2022-04-15 南京理工大学 Method for regulating and controlling three-dimensional space structure of light field
CN110243398A (en) * 2019-06-27 2019-09-17 南京邮电大学 A kind of relevance imaging method of the phase object based on relevant detection
CN110243398B (en) * 2019-06-27 2021-04-20 南京邮电大学 Coherent detection-based phase object correlation imaging method
CN110715944B (en) * 2019-10-21 2021-03-30 中国科学院高能物理研究所 Device and method for stable X-ray imaging
CN110715944A (en) * 2019-10-21 2020-01-21 中国科学院高能物理研究所 Device and method for stable X-ray imaging
CN111044541A (en) * 2019-12-26 2020-04-21 苏州光隐科技有限公司 X-ray high-resolution imaging method based on high-order stack association
CN112229397A (en) * 2020-09-11 2021-01-15 中国科学院上海光学精密机械研究所 Satellite angular position intensity correlation measurement system and method based on spatial modulation
CN112229397B (en) * 2020-09-11 2022-08-30 中国科学院上海光学精密机械研究所 Satellite angular position intensity correlation measurement system and method based on spatial modulation
CN112198176A (en) * 2020-09-24 2021-01-08 中国科学院上海光学精密机械研究所 Single exposure X-ray diffraction imaging device and method based on light field high-order spatial correlation
CN112198176B (en) * 2020-09-24 2022-12-02 中国科学院上海光学精密机械研究所 Single exposure X-ray diffraction imaging device and method based on light field high-order spatial correlation
CN113758952A (en) * 2021-08-20 2021-12-07 中国科学院上海光学精密机械研究所 X-ray diffraction imaging device and method based on momentum coding
CN113758952B (en) * 2021-08-20 2022-10-11 中国科学院上海光学精密机械研究所 X-ray diffraction imaging device and method based on momentum coding

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Application publication date: 20181116