CN102508142A - Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip - Google Patents

Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip Download PDF

Info

Publication number
CN102508142A
CN102508142A CN201110329133XA CN201110329133A CN102508142A CN 102508142 A CN102508142 A CN 102508142A CN 201110329133X A CN201110329133X A CN 201110329133XA CN 201110329133 A CN201110329133 A CN 201110329133A CN 102508142 A CN102508142 A CN 102508142A
Authority
CN
China
Prior art keywords
wavelength
ccd chip
sigma
image
ccd
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.)
Pending
Application number
CN201110329133XA
Other languages
Chinese (zh)
Inventor
邵晓鹏
吕斐
陈朝康
王杨
许宏涛
乔林
杨晓晖
徐大庸
马菁汀
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Xidian University
Original Assignee
Xidian University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Xidian University filed Critical Xidian University
Priority to CN201110329133XA priority Critical patent/CN102508142A/en
Publication of CN102508142A publication Critical patent/CN102508142A/en
Pending legal-status Critical Current

Links

Images

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The invention discloses a method for measuring quantum efficiency and a responsivity parameter of a charge coupled device (CCD) chip, and mainly solves the problem of low measurement precision in the prior art. The method comprises the following steps of: selecting a series of wavelengths at equal intervals, setting a tunable wavelength monochromatic uniform light source system by using the wavelength values respectively, generating monochromatic light with the corresponding wavelengths, shooting image information according to requirements, uploading to a computer, selecting needed images by using matched computer software, calculating the mean gray value mu and the image variance sigma<2> of the images, calculating a gain K of a control circuit respectively according to the calculated values, and calculating the quantum efficiency eta and the responsivity R according to the mean gray value mu, the image variance sigma<2> and the gain K. The method for measuring the quantum efficiency and the responsivity parameter of the CCD chip has the advantages of high precision and high stability in parameter measurement and is suitable for the precise measurement of the quantum efficiency and the responsivity parameter of the CCD chip.

Description

Measure the method for CCD chip quantum efficiency and responsiveness parameter
Technical field
The invention belongs to field of measuring technique, be specifically related to measurement, be used for development, assessment and the screening of CCD chip CCD chip quantum efficiency and responsiveness parameter.
Background technology
In the middle of the development and application of CCD chip; Because the restriction of processing and measuring technique; Cause actual quantum efficiency and the responsiveness parameter of CCD chip and measured value that manufacturer provides to have certain difference, and, need quantitatively to understand the actual performance parameter of CCD chip in some key application fields; Thereby, obtain data better more accurately to collecting to such an extent that data are reasonably proofreaied and correct.Therefore, be necessary to propose quantum efficiency and the responsiveness parameter that a kind of method effectively measures the CCD chip,, the CCD output data handled the data that more geared to actual circumstances through these performance parameters.
Traditional CCD chip quantum efficiency and responsiveness measurement method of parameters generally adopt laser instrument as the monochromatic light light source; Yet; Owing to also can't adopt laser instrument to realize the continuous variation of wavelength at present, cause to produce the monochromatic light of some wavelength coverage, thereby make the quantum efficiency of these wavelength coverages can only use the quantum efficiency of other wavelength to derive; Cause the quantum efficiency and the actual value of measurement that the bigger gap that gets is arranged, can't reflect quantum efficiency and responsiveness parameter that the CCD chip is actual.
Summary of the invention
The objective of the invention is to deficiency to above-mentioned prior art; A kind of method of measuring CCD chip quantum efficiency and responsiveness parameter is proposed; With the quantum efficiency that reduces to measure and the gap of actual value, improve the quantum efficiency of reality and the measuring accuracy of responsiveness parameter.
For realizing above-mentioned purpose, the present invention includes following steps:
1) CCD chip to be measured is placed in the middle of the Dewar flask that has entrance window, the CCD chip is linked to each other with the control circuit corresponding interface, this control circuit is used to control the imaging of CCD chip;
2) near the CCD chip, place the good detector of demarcation, be used for the nominal light source power, for measurement provides the luminous power reference value;
3) placing the monochromatic uniform source of light of wavelength-tunable system apart from CCD chip 80cm place, the monochromatic light that this light-source system sends shines directly into CCD and demarcates above the good detector;
4) electronic shutter that carries through shutter device or CCD chip is adjusted the integral time of CCD chip, the exposure of control CCD chip;
5) choose monochromatic wavelength width Δ λ, scanning wavelength scope [λ according to application demand s, λ e], scanning wavelength λ at interval Int, it is λ that initial wavelength is set s, cutoff wavelength is λ e, from initial wavelength X sBeginning, the scanning wavelength that superposes successively is λ at interval Int, reach cutoff wavelength λ up to wavelength eTill, obtain a series of wavelength value, as parameter, the control light-source system produces the monochromatic light of respective wavelength with these wavelength value;
6) every monochromatic wavelength that is provided with a time is taken two picture group pictures with the CCD chip, and every group of image number of taking is greater than 5; Wherein take first picture group as the time integral time of choosing need make the CCD chip reach 50% exposure or more than; The gained image is called bright image, take second picture group as the time, use with shooting first picture group as identical integral time; But need close shutter this moment, and the gained image is called dark image;
7) two bright images and two dark images in the middle of each extracts from the first picture group picture and the second picture group picture;
8) utilize the image calculation CCD chip of extraction and total gain K of control circuit thereof, be called system-gain:
8a) from two dark images and two bright images, respectively choose one, calculate the bright image choose and the average gray value μ of dark image respectively Y1And μ Y2:
&mu; y 1 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 1 [ m ] [ n ] , &mu; y 2 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 2 [ m ] [ n ]
Wherein, y 1, y 2Represent the bright image and dark image chosen respectively, M, N are respectively the capable pixel count and the row pixel count of photographic images;
8b) use the bright image variance of two bright image calculation that extracts
&sigma; y 1 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y A [ m ] [ n ] - y B [ m ] [ n ] ) 2
Y wherein A, y BRepresent first and second in the bright image respectively;
8c) use the dark image variance of two dark image calculation
Figure BDA0000102390080000025
that extracts
&sigma; y 2 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y C [ m ] [ n ] - y D [ m ] [ n ] ) 2
Wherein, y C, y DRepresent first and second in the dark image respectively;
The calculation of parameter system-gain K that 8d) obtains more than the basis:
K = &sigma; y 1 2 - &sigma; y 2 2 &mu; y 1 - &mu; y 2 ;
9) utilize the responsiveness R of four image calculation CCD chips that extract in the step 7):
R = &mu; y 1 - &mu; y 2 &mu; p
Wherein
Figure BDA0000102390080000033
Be the average photon number of the single pixel of CCD chip, A is the area of the single pixel of CCD chip, and E is the monochromatic light power that shines on the CCD chip, t ExpUsed integral time when take extracting bright image, λ shines the monochromatic wavelength on the CCD chip when extracting bright image for taking, and h is a Planck's constant, and c is the light velocity;
10) try to achieve the quantum efficiency of CCD chip by system-gain K and responsiveness R:
&eta; ( &lambda; ) = R K .
The present invention has following advantage:
1) The data chosen of the present invention is taken many, chooses the method for center section image, has well got rid of the error of imaging system, has improved the precision of measurement parameter.
2) the present invention gets many images for the calculating employing of space variance and asks average mode, has got rid of the influence of time domain variance basically, makes the space heterogeneity of measurement more accurate.
3) the present invention can calculate the absolute value of quantum efficiency and responsiveness owing to use the detector of demarcating that incident monochromatic light light intensity is demarcated, and with respect to relative quantum efficient and relative response degree, the user is more had reference value.
4) owing to adopt the monochromatic uniform source of light of wavelength-tunable system, can produce the monochromatic light of each wavelength, thereby can measure the quantum efficiency and the responsiveness parameter of each wavelength.
Description of drawings
Fig. 1 is the used hardware acquisition system of a present invention block diagram;
Fig. 2 is the process flow diagram that the present invention measures CCD chip quantum efficiency η and responsiveness parameter K.
Embodiment
The CCD chip is a kind of widely used image device; Be widely used in many fields such as uranology, Aero-Space, biology and medical research, molecular dynamics, spectroscopy, underwater photography, X ray detection, it is vital assessing for this performance parameter to the CCD chip.At present, the CCD chip assessed mainly contained following these parameters:
1. quantum efficiency η: CCD is at wavelength X the irradiation photoelectron number of generation and the ratio of incident light subnumber down, this parameter characterization the CCD chip to the monochromatic responding ability of specific wavelength.
2. responsiveness parameters R: CCD is under the setted wavelength monochromation illumination, the ratio of signal voltage and exposure.This parameter has been described CCD quantum efficiency and system-gain on the whole.
3. saturation degree μ P.sat: the photon number that can receive when CCD reaches capacity.
4. system-gain K: the electron number that system's pixel produces and the ratio of gray-scale value.
5. dark noise
Figure BDA0000102390080000041
the noise summation relevant with CCD chip sensing circuit.
6. signal to noise ratio snr: signal that photon produces and the ratio between the noise signal.
7. absolute sensitivity threshold value μ P.min: signal to noise ratio (S/N ratio) equals 1 o'clock required average photon number.
8. dynamic range DR: saturation degree is in the ratio of absolute sensitivity threshold value.
9. the error that departs from linear concerns between the output signal of nonlinearity error LE:CCD chip and the incident optical signal.
10. the ratio of the standard deviation of dark signal heterogeneity DSNU:CCD chip each pixel output gray level value under unglazed photograph and its average.
photo response heterogeneity PRNU:CCD chip under 50% saturated conditions of exposure, the standard deviation of each pixel output gray level value and the ratio of average.
Figure BDA0000102390080000043
Dark current μ I: the CCD chip unglazed according under the situation the output current size.
Figure BDA0000102390080000044
Double thermal constant T d: unglazed according under the situation, corresponding temperature when dark current is increased to reference temperature and goes out a times of dark current value.
Below will combine accompanying drawing, clear, intactly describe among the present invention to the 1. 2. perfect measurement flow process of responsiveness parameters R of quantum efficiency η and parameter of parameter.
With reference to Fig. 1, the used hardware acquisition system of the present invention block diagram, total system comprises the monochromatic uniform source of light of wavelength-tunable system, Dewar flask temperature controlled compartment, CCD chip, standard detector, control circuit and computing machine.CCD chip and standard detector are placed in the Dewar flask temperature controlled compartment; Its working temperature can be controlled by the Dewar flask temperature controlled compartment; Regulate the monochromatic uniform source of light of wavelength-tunable system and export even monochromatic light, be radiated on CCD chip and the standard detector, the CCD chip is driven into picture by control circuit; And the output information of CCD chip uploaded on the computing machine, computing machine calculates the performance parameter of CCD chip to be measured according to image information.For different measurement parameters, through regulating wavelength-tunable monochromatic source system, integral time and CCD chip operation temperature, gather corresponding image and intensity signal, basis calculates measurement parameter with the specific step of parameter correlation again.
With reference to Fig. 2, the present invention measures the method for CCD chip quantum efficiency η and responsiveness parameters R, comprises the steps:
Step 1, CCD chip to be measured is placed in the Dewar flask temperature controlled compartment of test macro; This Dewar flask temperature controlled compartment has entrance window; The transmitance of entrance window requires the transmitance of incident light is reached more than 98%; The CCD chip is linked to each other with the control circuit corresponding interface, and this control circuit is used to control the temperature of imaging of CCD chip and adjusting Dewar flask temperature controlled compartment, and the temperature of Dewar flask temperature controlled compartment is the working temperature of CCD chip.
Step 2, near the CCD chip, place standard detector, this detector is demarcated, and is used for measurement light source power, for thereafter calculating provides the luminous power reference value.
Step 3, placing the monochromatic uniform source of light of wavelength-tunable system apart from CCD chip 80cm place; The monochromatic uniform source of light of this wavelength-tunable system is made up of broad spectrum light source, monochromator, integrating sphere; Its wavelength regulation area requirement covers the response wave length scope of CCD chip; The monochromatic wavelength width requirement that produces is less than 50nm, and the monochromatic light that the monochromatic uniform source of light of this wavelength-tunable system sends shines directly into CCD and above the standard detector.
The integral time of step 4, the electronic shutter adjustment CCD chip that carries through the CCD chip; The exposure of control CCD chip; If the electronic shutter of CCD chip does not satisfy application demand; Then need add shutter device in the middle of the input path, generally be added on before the entrance window or before the monochromatic uniform source of light of the wavelength-tunable system, use this shutter device to regulate the exposure of CCD chip.
Step 5, choose wavelength width Δ λ, scanning wavelength scope [λ according to the response wave length scope of application demand and CCD chip s, λ e], scanning wavelength λ at interval Int, wherein wavelength width Δ λ need be less than 50nm, and in the scanning wavelength scope will be included in the wavelength response range of CCD chip, scanning wavelength is λ at interval IntBe less than the wavelength width of twice, it is λ that initial wavelength is set s, cutoff wavelength is λ e, beginning from initial wavelength, the scanning wavelength that superposes successively is λ at interval Int, reach λ up to wavelength eTill, obtain a series of wavelength value, as parameter, the control light-source system produces the monochromatic light of respective wavelength with these wavelength value.
Step 6, every monochromatic wavelength that is provided with a time are taken two picture group pictures with the CCD chip, and every group of image number of taking is greater than 5; Wherein take first picture group as the time integral time of choosing need make the CCD chip reach 50% exposure or more than; The gained image is called bright image, take second picture group as the time, use with shooting first picture group as identical integral time; But need close shutter this moment; The gained image is called dark image, and the image of all shootings all uploads in the middle of the computing machine through control circuit, next uses supporting computer software that these data are handled and obtains measurement parameter.
Step 7, two bright images and two dark images from the first picture group picture and the second picture group picture in the middle of the extraction, these four images will be used for follow-up calculating, and remaining image abandons need not.
Image calculation CCD chip and the total gain K of control circuit thereof that step 8, utilization are extracted are called system-gain:
8a) from two dark images and two bright images, respectively choose one, calculate the bright image choose and the average gray value μ of dark image respectively Y1And μ Y2:
&mu; y 1 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 1 [ m ] [ n ] , &mu; y 2 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 2 [ m ] [ n ]
Wherein, y 1, y 2Represent the bright image and dark image chosen respectively, M, N are respectively the capable pixel count and the row pixel count of photographic images, and these two sizes can obtain from the product manual of CCD chip or from image information, come out;
8b) use the bright image variance of two bright image calculation
Figure BDA0000102390080000063
that extracts
&sigma; y 1 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y A [ m ] [ n ] - y B [ m ] [ n ] ) 2
Y wherein A, y BRepresent first and second in the bright image respectively;
8c) use the dark image variance of two dark image calculation
Figure BDA0000102390080000065
that extracts
&sigma; y 2 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y C [ m ] [ n ] - y D [ m ] [ n ] ) 2
Wherein, y C, y DRepresent first and second in the dark image respectively;
The calculation of parameter system-gain K that 8d) obtains more than the basis:
K = &sigma; y 1 2 - &sigma; y 2 2 &mu; y 1 - &mu; y 2 .
Step 9, utilize resulting average gray parameter μ in the step 8 Y1And μ Y2Calculate the responsiveness R of CCD chip:
R = &mu; y 1 - &mu; y 2 &mu; p
Wherein
Figure BDA0000102390080000072
Be the average photon number of the single pixel of CCD chip, A is the area of the single pixel of CCD chip, and E is the monochromatic light power that shines on the CCD chip, t ExpUsed integral time when take extracting bright image, λ shines the monochromatic wavelength on the CCD chip when extracting bright image for taking, and h is a Planck's constant, and c is the light velocity.
Step 10, try to achieve the quantum efficiency of CCD chip by system-gain K and responsiveness R:
&eta; ( &lambda; ) = R K .
More than describing only is an instantiation of the present invention; Do not constitute any restriction of the present invention; Obviously to those skilled in the art, after having understood content of the present invention and principle, all maybe be under the situation that does not deviate from the principle of the invention, structure; Carry out various corrections and change on form and the details, but these are based on the correction of inventive concept with change still within claim protection domain of the present invention.

Claims (2)

1. a method of measuring CCD chip quantum efficiency and responsiveness parameter comprises the steps:
1) CCD chip to be measured is placed in the middle of the Dewar flask temperature controlled compartment that has entrance window, the CCD chip is linked to each other with the control circuit corresponding interface, this control circuit is used to control the imaging of CCD chip;
2) near the CCD chip, place the good detector of demarcation, be used for the nominal light source power, for measurement provides the luminous power reference value;
3) placing the monochromatic uniform source of light of wavelength-tunable system apart from CCD chip 80cm place, the monochromatic light that this light-source system sends shines directly into CCD and demarcates above the good detector;
4) electronic shutter that carries through shutter device or CCD chip is adjusted the integral time of CCD chip, the exposure of control CCD chip;
5) choose monochromatic wavelength width Δ λ, scanning wavelength scope [λ according to application demand s, λ e], scanning wavelength λ at interval Int, it is λ that initial wavelength is set s, cutoff wavelength is λ e, from initial wavelength X sBeginning, the scanning wavelength that superposes successively is λ at interval Int, reach cutoff wavelength λ up to wavelength eTill, obtain a series of wavelength value, as parameter, the control light-source system produces the monochromatic light of respective wavelength with these wavelength value;
6) every monochromatic wavelength that is provided with a time is taken two picture group pictures with the CCD chip, and every group of image number of taking is greater than 5; Wherein take first picture group as the time integral time of choosing need make the CCD chip reach 50% exposure or more than; The gained image is called bright image, take second picture group as the time, use with shooting first picture group as identical integral time; But need close shutter this moment, and the gained image is called dark image;
7) two bright images and two dark images in the middle of each extracts from the first picture group picture and the second picture group picture;
8) utilize the image calculation CCD chip of extraction and total gain K of control circuit thereof, be called system-gain:
8a) from two dark images and two bright images, respectively choose one, calculate the bright image choose and the average gray value μ of dark image respectively Y1And μ Y2:
&mu; y 1 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 1 [ m ] [ n ] , &mu; y 2 = 1 MN &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 y 2 [ m ] [ n ]
Wherein, y 1, y 2Represent the bright image and dark image chosen respectively, M, N are respectively the capable pixel count and the row pixel count of photographic images;
8b) use the bright image variance of two bright image calculation
Figure FDA0000102390070000021
that extracts
&sigma; y 1 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y A [ m ] [ n ] - y B [ m ] [ n ] ) 2
Y wherein A, y BRepresent first and second in the bright image respectively;
8c) use the dark image variance of two dark image calculation
Figure FDA0000102390070000023
that extracts
&sigma; y 2 2 = 1 2 NM &Sigma; m = 0 M - 1 &Sigma; n = 0 N - 1 ( y C [ m ] [ n ] - y D [ m ] [ n ] ) 2
Wherein, y C, y DRepresent first and second in the dark image respectively;
The calculation of parameter system-gain K that 8d) obtains more than the basis:
K = &sigma; y 1 2 - &sigma; y 2 2 &mu; y 1 - &mu; y 2 ;
9) utilize the responsiveness R of four image calculation CCD chips that extract in the step 7):
R = &mu; y 1 - &mu; y 2 &mu; p
Wherein
Figure FDA0000102390070000027
Be the average photon number of the single pixel of CCD chip, A is the area of the single pixel of CCD chip, and E is the monochromatic light power that shines on the CCD chip, t ExpUsed integral time when take extracting bright image, λ shines the monochromatic wavelength on the CCD chip when extracting bright image for taking, and h is a Planck's constant, and c is the light velocity;
10) try to achieve the quantum efficiency of CCD chip by system-gain K and responsiveness R:
&eta; ( &lambda; ) = R K .
2. measuring method according to claim 1, wherein the described control light-source system of step 5) produces the monochromatic light of respective wavelength, carries out as follows:
2a) choose monochromatic wavelength width: Δ λ<50nm;
2b) choose scanning wavelength [λ s, λ e], this wavelength need cover the wavelength response range of CCD chip;
2c) choosing sweep spacing is: λ Int<2* Δ λ;
2d) from initial wavelength X sBeginning, the scanning wavelength that superposes successively is λ at interval Int, reach cutoff wavelength λ up to wavelength eTill, obtain a series of wavelength value;
The a series of wavelength value that 2f) obtain more than the basis are provided with light-source system and produce corresponding monochromatic light.
CN201110329133XA 2011-10-26 2011-10-26 Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip Pending CN102508142A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201110329133XA CN102508142A (en) 2011-10-26 2011-10-26 Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201110329133XA CN102508142A (en) 2011-10-26 2011-10-26 Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip

Publications (1)

Publication Number Publication Date
CN102508142A true CN102508142A (en) 2012-06-20

Family

ID=46220247

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201110329133XA Pending CN102508142A (en) 2011-10-26 2011-10-26 Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip

Country Status (1)

Country Link
CN (1) CN102508142A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103308280A (en) * 2013-05-24 2013-09-18 中国电子科技集团公司第四十一研究所 Quantum efficiency calibration device and calibrating method for CCD (charge coupled device)
CN104142226A (en) * 2014-08-12 2014-11-12 中国电子科技集团公司第四十一研究所 CCD device quantum efficiency measuring device and method
CN105738073A (en) * 2016-02-03 2016-07-06 中国科学院国家空间科学中心 Method for performing pixel response function measurement in spatial frequency domain
CN105841925A (en) * 2016-03-22 2016-08-10 中国科学院国家空间科学中心 Detector pixel response Fourier spectrum acquisition-based image reconstruction method
CN106932174A (en) * 2017-03-07 2017-07-07 中国科学院新疆理化技术研究所 For the general method for fast measuring of focal plane imaging device absolute spectral response
CN110044928A (en) * 2019-04-23 2019-07-23 华中科技大学 A kind of detection device of space encoding light field to bend glass surface defect

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
EUROPEAN MACHINE VISION ASSOCIATION: "EMVA Standard 1288:Standard for Characterization of Image Sensors and Cameras", 《WWW.EMVA.ORG》 *
许宏涛等: "CCD芯片性能参数测量系统", 《仪器仪表学报》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103308280A (en) * 2013-05-24 2013-09-18 中国电子科技集团公司第四十一研究所 Quantum efficiency calibration device and calibrating method for CCD (charge coupled device)
CN104142226A (en) * 2014-08-12 2014-11-12 中国电子科技集团公司第四十一研究所 CCD device quantum efficiency measuring device and method
CN105738073A (en) * 2016-02-03 2016-07-06 中国科学院国家空间科学中心 Method for performing pixel response function measurement in spatial frequency domain
CN105738073B (en) * 2016-02-03 2019-02-26 中国科学院国家空间科学中心 A method of pixel response function measurement is carried out in spatial frequency domain
CN105841925A (en) * 2016-03-22 2016-08-10 中国科学院国家空间科学中心 Detector pixel response Fourier spectrum acquisition-based image reconstruction method
CN105841925B (en) * 2016-03-22 2019-02-26 中国科学院国家空间科学中心 A kind of image rebuilding method obtained based on detector pixel response Fourier spectrum
CN106932174A (en) * 2017-03-07 2017-07-07 中国科学院新疆理化技术研究所 For the general method for fast measuring of focal plane imaging device absolute spectral response
CN110044928A (en) * 2019-04-23 2019-07-23 华中科技大学 A kind of detection device of space encoding light field to bend glass surface defect

Similar Documents

Publication Publication Date Title
CN102508144A (en) Method for measuring dark signal non-uniformity and photon response non-uniformity of photons of CCD (charge coupled device) chip
EP2637004B1 (en) Multispectral imaging color measurement system and method for processing imaging signals thereof
CN102508147A (en) Method for measuring related parameters of sensitivity, linearity and dark noise of charge coupled device (CCD) chip
CN102508142A (en) Method for measuring quantum efficiency and responsivity parameter of charge coupled device (CCD) chip
US7489396B1 (en) Spectrophotometric camera
Downing et al. CCD riddle: a) signal vs time: linear; b) signal vs variance: non-linear
Kurtz et al. Measuring diffuse, direct, and global irradiance using a sky imager
CN102300057B (en) Method for correcting response inconsistency of linear array CCD (Charge Coupled Device) image elements
JP5834938B2 (en) Spectral characteristic acquisition apparatus, image evaluation apparatus, image forming apparatus, and spectral characteristic acquisition method
Carlson Comparison of modern CCD and CMOS image sensor technologies and systems for low resolution imaging
CN109313080B (en) Method for the contactless determination of temperature and infrared measuring system
US20070177230A1 (en) Methods and apparatuses for determining a color calibration for different spectral light inputs in an imaging apparatus measurement
WO2016071909A1 (en) Spectral imaging method and system
Farrell et al. Sensor calibration and simulation
Daigle et al. The darkest EMCCD ever
CN108174127A (en) Relative radiometric correction methods of the face battle array CMOS under global shutter working method
US10969275B2 (en) On-chip spectrometer employing pixel-count-modulated spectral channels and method of manufacturing the same
CN107782447B (en) Space dimension automatic identifying method and system in imaging spectrometer spectral calibration
TW201034442A (en) Gradation image capture for testing image sensors
CN114061766A (en) Multispectral reconstruction temperature measuring device and method in particle combustion process
WO2021179226A1 (en) Spectrum information obtaining method and spectrum detection device
CN106932174A (en) For the general method for fast measuring of focal plane imaging device absolute spectral response
Erz et al. Radiometric and spectrometric calibrations, and distance noise measurement of ToF cameras
Fu et al. CMOS neuromorphic optical sensor chip with color change-intensity change disambiguation (CCICD)
Bell et al. An evaluation framework for the accuracy of camera transfer functions estimated from differently exposed images

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C12 Rejection of a patent application after its publication
RJ01 Rejection of invention patent application after publication

Application publication date: 20120620