CN105957034A - Scanning infrared imaging system scene non-uniformity correction based on registration - Google Patents
Scanning infrared imaging system scene non-uniformity correction based on registration Download PDFInfo
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Abstract
The invention relates to a scanning infrared imaging system scene non-uniformity correction based on registration, and the method comprises that registration is performed on previous and next frames of video streams, and longitudinal translation amount and transverse translation amount of the screen is calculated. The translation is performed on an image of the previous frame through utilizing Fourier transform operation, and the above image is subtracted by an image of next frame and divides an absolute value of the longitudinal translation amount to obtain a difference matrix. The elementary transformation is performed on the difference matrix to obtain a bias non-uniform difference matrix which aims at an appointed row, and each column of the matrix is partly accumulated to obtain a bias correction matrix. Average solving is performed on each column of the bias correction matrix, so that a bias correction vector is obtained and is used for non-uniform correction of a to-be-corrected image. The method has advantages of fast calculation speed and good quality of image and has good application prospect.
Description
Technical field
The present invention relates to the scene non-uniform correction method of a kind of infrared image, it is more particularly related to one is based on joining
Accurate sweep type infrared imaging system scene asymmetric correction method.
Background technology
Infrared imaging system capacity of resisting disturbance is strong, and hidden performance is good, and air penetration capacity is strong, adapts to multiple special occasions, in section
Grind, military affairs, medical science, industry, many aspects such as civilian in an increasingly wide range of applications.Now widely used infrared imaging
System is divided into two classes: a class is gazing type infrared imaging system, and in system, opticator focuses on infrared focus plane IR Scene
On;Another kind of is sweep type infrared imaging system, and system is enough become with alignment infrared focus plane two parts by optical mechaical scanning, system handle
Scene is progressively mapped in infrared imaging alignment along scanning direction.
Either in sweep type infrared imaging system or in gazing type infrared imaging system, affected by manufacturing process,
The response of each pixel of infrared focus plane is not consistent, there is heterogeneity, shows as fixing pattern noise (fixed in the picture
Pattern noise, referred to as FPN), cause infrared image signal to noise ratio low, poor image quality.It is thus desirable to infrared image is carried out
Nonuniformity correction processes removes FPN.Owing to FPN exists drift characteristic, self-adapting correction method energy based on scene in time domain
Enough it is corrected from heteropical form of expression, the correction error that response drift is brought can be overcome to a certain extent,
Do not require or have only to demarcate simply, adaptively updating correction coefficient according to scene information.
At present the most ripe self-adapting correction method based on scene have time domain processing algorithm, spatial processing algorithm and based on
The Processing Algorithm of estimation, but the proposition of these methods is both for what gazing type infrared imaging system proposed, and sweep type is red
The scene non-uniform correction method of outer imaging system is also not affected by paying attention to.Directly the scene gazing type infrared imaging system is non-homogeneous
Bearing calibration applies in sweep type infrared imaging system, there is certain defect: cause convergence rate slow;Do not account for sweeping
Retouch the noise behavior of type infrared imaging system, the poor image quality processed can be caused.
Summary of the invention
The present invention is directed to prior art defect, it is provided that a kind of sweep type infrared imaging system scene Nonuniformity Correction based on registration
Method.
Technical scheme provides a kind of sweep type infrared imaging system scene asymmetric correction method based on registration, bag
Include following steps:
(1) integer constant L more than zero that input is preset, if the resolution of the output image of Infrared Detectors is M × N, makes m, n represent
Space coordinates, has m=1 ..., M, n=1 ..., N, the memory space P that size is M × L is set;Counting variable t is set,
Line variable s is set, initializes s=1, frame number indexed variable k is set, initialize k=1;
(2) two two field pictures before and after obtaining continuously from the video flowing of Infrared Detectors, are designated as ykAnd yk+1;This two two field picture is registrated,
Calculate scene translation pixel count, including longitudinal translation dvWith transverse translation dh, it may be judged whether 0 < | dv| < 1,
It is to enter step (4),
Otherwise make k=k+2, two new two field pictures are re-executed step (2);
(3) to ykCalculate displacement images yk *It is as follows,
Wherein, m, n are image space coordinate, and u, v are frequency domain coordinate, Yk(u v) is ykFrequency domain figure picture,It is yk
Displacement images, j is imaginary unit;
Calculate difference matrix D as follows,
If dv> 0, the first row of D is set to 0;If dv< 0, last column of D is set to 0;
DhIt is divided into integer part Int (dh) and fractional part ε (dh), i.e. dh=Int (dh)+ε(dh), if dh> 0, remove row in D and sit
It is designated as n=1 ..., 1+ | Int (dh) | row;If dh< 0, removing row coordinate in D is n=N-| Int (dh) | ..., the row of N;
(4) difference matrix D is carried out elementary transformation, obtain biasing heteropical difference matrix G for s row;
For dv> 0 situation, if s=1, it is not necessary to perform any operation;If 2≤s≤M, from 1 row to s-1 row, sequentially
The element of current line is set to the opposite number of next line element by ground;
For dv< situation of 0, if s=M, it is not necessary to would perform any operation;If 1≤s≤M-1, inverted order ground is by the element of current line
It is set to the opposite number of lastrow element;
(5) perform to add up to each column in G, obtain biasing heteropical correction matrix Q for s row, each in correction matrix Q
Element computational methods are as follows,
As m=s, make Q (m, n)=0;
Work as m=1 ..., during s-1,
Work as m=s+1 ..., during M,
(6) Q is averaging by row, obtains the updating vector c that dimension is M × 1s, m row element computing formula is as follows,
Updating vector csValue be saved in memory space P t row in;
(7) if s < M, s=s+1 is made;Otherwise, s=1 is made;
(8) if t < L, make t=t+1, make k=k+2, return step (2) and proceed new two continuous frames to process;Otherwise, to storage
Space P is averaging by row, obtains average correction vector cavg;
(9) average correction vector c is usedavgThe output image of Infrared Detectors is carried out Nonuniformity Correction;
(10) make t=1, memory space P is reset;
(11) make k=k+2, return step (2) and new two continuous frames is processed, dynamically update average correction vector cavg。
And, the described opposite number that sequentially element of current line is set to next line element, it is achieved as follows,
D (m, n)=-D (m+1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to 1,2 ..., s-1, gradually add 1.
And, the element of current line is set to the opposite number of lastrow element by described inverted order ground, it is achieved as follows,
D (m, n)=-D (m-1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to M, M-1 ..., s+1, gradually subtract 1;Finally the element of s row is set to 0, by the square after conversion
Battle array is designated as G.
The scene asymmetric correction method of the present invention has the advantage that
1. the amount of calculation needed for is little, and resource consumption is few.
2. calculation is succinct, it is easy to accomplish.
3. the image obtained after correction is clear, and uniformity is good.
Accompanying drawing explanation
Fig. 1 is the method flow diagram of the embodiment of the present invention.
Detailed description of the invention
For the ease of those of ordinary skill in the art understand and implement the present invention, below in conjunction with the accompanying drawings and embodiment the present invention is made into
The detailed description of one step, it will be appreciated that embodiment described herein is merely to illustrate and explains the present invention, is not used to limit
The present invention.
When being embodied as, method provided by the present invention can use computer software technology to realize automatically and run.As it is shown in figure 1, this
Inventive embodiments sweep type infrared imaging system scene asymmetric correction method based on registration comprises the following steps:
(1) input integer constant L more than zero, when being embodied as, this value can be by those skilled in the art according to heteropical noise
Level-preset, such as, arrange L=10 or L=20, etc..If the resolution of the output image of Infrared Detectors is M × N, order
M, n representation space coordinate, has m=1 ..., M, n=1 ..., N, the memory space P that size is M × L is set.Counting is set
Variable t.Line variable s is set, initializes s=1.Frame number indexed variable k is set, initializes k=1;
(2) two two field pictures before and after obtaining continuously from the video flowing of Infrared Detectors, are designated as ykAnd yk+1.This two two field picture is registrated,
Calculate scene translation pixel count, including longitudinal translation dvWith transverse translation dh, to there is the image of sub-pix longitudinal translation to entering
Row subsequent treatment, i.e. exist sub-pix longitudinal translation (0 < | dv| < 1, dhCan be arbitrarily).When being embodied as, it can be determined that whether
0<|dv| < 1, it is to enter step (4), otherwise make k=k+2, two new frames are re-executed step (2).
(3) to ykCarry out fast Fourier transform (FFT) and obtain its frequency domain figure as Yk, by YkIt is multiplied by with translation information dvAnd dhRelevant
Complex exponential, then carry out an inverse fast fourier (IFFT) and obtain ykDisplacement images yk *, i.e.
Wherein m, n are image space coordinate, and u, v are frequency domain coordinate, i.e. Yk(u v) is ykFrequency domain figure picture,It is yk
Displacement images, j is imaginary unit.
Again yk *With yk+1Subtract each other and divided by | dv|, obtaining difference matrix D, computing formula is
If dv> 0, the first row of D is set to 0;If dv< 0, last column of D is set to 0;
DhIt is divided into integer part Int (dh) and fractional part ε (dh), i.e. dh=Int (dh)+ε(dh), if dh> 0, remove row in D and sit
It is designated as n=1 ..., 1+ | Int (dh) | row;If dh< 0, removing row coordinate in D is n=N-| Int (dh) | ..., the row of N.
(4) difference matrix D is carried out elementary transformation, obtain biasing heteropical difference matrix G for s row.
For dv> 0 situation, if s=1, it is not necessary to perform any operation;If 2≤s≤M, from 1 row to s-1 row, sequentially
The element of current line is set to the opposite number of next line element by ground, it may be assumed that
D (m, n)=-D (m+1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to 1,2 ..., s-1, gradually add 1;
For dv< situation of 0, if s=M, it is not necessary to would perform any operation;If 1≤s≤M-1, inverted order ground is by the element of current line
It is set to the opposite number of lastrow element, it may be assumed that
D (m, n)=-D (m-1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to M, M-1 ..., s+1, gradually subtract 1;Finally the element of s row is set to 0, by the square after conversion
Battle array is designated as G.
(5) perform to add up to each column in G, thus obtain biasing heteropical correction matrix Q for s row;In matrix Q respectively
Element computational methods are as follows:
As m=s, make Q (m, n)=0;
Work as m=1 ..., during s-1,
Work as m=s+1 ..., during M,
(6) Q is averaging by row, obtains the updating vector c that dimension is M × 1s, wherein m row (m=1 ..., M) element computing formula
As follows:
Updating vector csValue be saved in memory space P t row in, i.e.
P (m, t)=cs(m,1)
(7) if s < M, make s from increasing 1, i.e. s=s+1;Otherwise, s=1 is made.The most often calculate once, make s=s+1, if s+1 > M,
Then make s=1.
(8) if t < L, make t from increasing 1, i.e. t=t+1, make k=k+2, return step (2) and proceed new two continuous frames to process;
Otherwise, then memory space P is averaging by row, obtains average correction vector cavg, i.e.
(9) average correction vector c is usedavgThe output image of Infrared Detectors is carried out Nonuniformity Correction, and updating formula is as follows:
yc(m, n)=y (m, n)+cavg(m,1)
Wherein m=1 ..., M, n=1 ..., N, y are the image to be corrected of M × N, ycFor image after the correction of M × N.
(10) t=1 is made.Memory space P is reset, i.e.
P (m, l)=0
Wherein, l is the row coordinate of P, l=1 ..., L.
(11) make k=k+2, return step (2) and new two continuous frames is processed, thus dynamically update average correction vector cavg, with
Just heteropical time drift problem is solved, until stopping flow process.
Using method provided by the present invention to test the emulating image with fixing pattern noise, this image is in video flowing
One frame, due to the time drift characteristic of fixing pattern noise, causes nonuniformity correction parameter undesirable, therefore exists big in image
Measure horizontal stripe noise as depicted.Design sketch after processing from using the inventive method, it is found that compare figure before treatment
Picture, horizontal stripe noise substantially disappears, it is possible to the detailed information being clearly observed in scene.As can be seen here, the present invention proposes
Method can improve heterogeneity effectively.
Claims (3)
1. a sweep type infrared imaging system scene asymmetric correction method based on registration, it is characterised in that comprise the following steps:
(1) integer constant L more than zero that input is preset, if the resolution of the output image of Infrared Detectors is M × N, makes m, n represent
Space coordinates, has m=1 ..., M, n=1 ..., N, the memory space P that size is M × L is set;Counting variable t is set,
Line variable s is set, initializes s=1, frame number indexed variable k is set, initialize k=1;
(2) two two field pictures before and after obtaining continuously from the video flowing of Infrared Detectors, are designated as ykAnd yk+1;This two two field picture is registrated,
Calculate scene translation pixel count, including longitudinal translation dvWith transverse translation dh, it may be judged whether 0 < | dv| < 1,
It is to enter step (4),
Otherwise make k=k+2, two new two field pictures are re-executed step (2);
(3) to ykCalculate displacement images yk *It is as follows,
Wherein, m, n are image space coordinate, and u, v are frequency domain coordinate, Yk(u v) is ykFrequency domain figure picture,It is yk
Displacement images, j is imaginary unit;
Calculate difference matrix D as follows,
If dv> 0, the first row of D is set to 0;If dv< 0, last column of D is set to 0;
DhIt is divided into integer part Int (dh) and fractional part ε (dh), i.e. dh=Int (dh)+ε(dh), if dh> 0, remove row in D and sit
It is designated as n=1 ..., 1+ | Int (dh) | row;If dh< 0, removing row coordinate in D is n=N-| Int (dh) | ..., the row of N;
(4) difference matrix D is carried out elementary transformation, obtain biasing heteropical difference matrix G for s row;
For dv> 0 situation, if s=1, it is not necessary to perform any operation;If 2≤s≤M, from 1 row to s-1 row, sequentially
The element of current line is set to the opposite number of next line element by ground;
For dv< situation of 0, if s=M, it is not necessary to would perform any operation;If 1≤s≤M-1, inverted order ground is by the element of current line
It is set to the opposite number of lastrow element;
(5) perform to add up to each column in G, obtain biasing heteropical correction matrix Q for s row, each in correction matrix Q
Element computational methods are as follows,
As m=s, make Q (m, n)=0;
Work as m=1 ..., during s-1,
Work as m=s+1 ..., during M,
(6) Q is averaging by row, obtains the updating vector c that dimension is M × 1s, m row element computing formula is as follows,
Updating vector csValue be saved in memory space P t row in;
(7) if s < M, s=s+1 is made;Otherwise, s=1 is made;
(8) if t < L, make t=t+1, make k=k+2, return step (2) and proceed new two continuous frames to process;Otherwise, to storage
Space P is averaging by row, obtains average correction vector cavg;
(9) average correction vector c is usedavgThe output image of Infrared Detectors is carried out Nonuniformity Correction;
(10) make t=1, memory space P is reset;
(11) make k=k+2, return step (2) and new two continuous frames is processed, dynamically update average correction vector cavg。
Sweep type infrared imaging system scene asymmetric correction method based on registration the most according to claim 1, it is characterised in that:
The described opposite number that sequentially element of current line is set to next line element, it is achieved as follows,
D (m, n)=-D (m+1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to 1,2 ..., s-1, gradually add 1.
Sweep type infrared imaging system scene asymmetric correction method based on registration the most according to claim 1, it is characterised in that:
The element of current line is set to the opposite number of lastrow element by described inverted order ground, it is achieved as follows,
D (m, n)=-D (m-1, n), n=1 ..., N-| Int (dh)|-1
Wherein row-coordinate m be changed to M, M-1 ..., s+1, gradually subtract 1;Finally the element of s row is set to 0, by the square after conversion
Battle array is designated as G.
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Cited By (5)
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CN106768383A (en) * | 2017-01-21 | 2017-05-31 | 浙江红相科技股份有限公司 | A kind of automatic blind element detection of infrared focal plane array and compensation method |
CN107450347A (en) * | 2017-07-14 | 2017-12-08 | 西安电子科技大学 | A kind of GPU Real-time Nonuniformity Correction methods based on infrared semi-matter simulating system |
CN111047521A (en) * | 2019-11-01 | 2020-04-21 | 北京空间机电研究所 | Infrared image nonuniformity parameterization correction optimization method based on image entropy |
CN111983710A (en) * | 2020-08-14 | 2020-11-24 | 西安应用光学研究所 | Non-uniformity correction method for scanning type infrared search system |
CN114913096A (en) * | 2022-06-10 | 2022-08-16 | 中国科学院长春光学精密机械与物理研究所 | Non-uniform correction method and system for characteristic initialization |
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Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
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CN106768383A (en) * | 2017-01-21 | 2017-05-31 | 浙江红相科技股份有限公司 | A kind of automatic blind element detection of infrared focal plane array and compensation method |
CN106768383B (en) * | 2017-01-21 | 2019-10-29 | 浙江红相科技股份有限公司 | A kind of automatic blind element detection of infrared focal plane array and compensation method |
CN107450347A (en) * | 2017-07-14 | 2017-12-08 | 西安电子科技大学 | A kind of GPU Real-time Nonuniformity Correction methods based on infrared semi-matter simulating system |
CN107450347B (en) * | 2017-07-14 | 2019-10-22 | 西安电子科技大学 | A kind of GPU Real-time Nonuniformity Correction method based on infrared semi-matter simulating system |
CN111047521A (en) * | 2019-11-01 | 2020-04-21 | 北京空间机电研究所 | Infrared image nonuniformity parameterization correction optimization method based on image entropy |
CN111047521B (en) * | 2019-11-01 | 2023-08-11 | 北京空间机电研究所 | Infrared image non-uniformity parameterization correction optimization method based on image entropy |
CN111983710A (en) * | 2020-08-14 | 2020-11-24 | 西安应用光学研究所 | Non-uniformity correction method for scanning type infrared search system |
CN114913096A (en) * | 2022-06-10 | 2022-08-16 | 中国科学院长春光学精密机械与物理研究所 | Non-uniform correction method and system for characteristic initialization |
CN114913096B (en) * | 2022-06-10 | 2024-04-23 | 中国科学院长春光学精密机械与物理研究所 | Feature initialization non-uniform correction method and system thereof |
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