CN107091730A - Estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions - Google Patents

Estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions Download PDF

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Publication number
CN107091730A
CN107091730A CN201710451588.6A CN201710451588A CN107091730A CN 107091730 A CN107091730 A CN 107091730A CN 201710451588 A CN201710451588 A CN 201710451588A CN 107091730 A CN107091730 A CN 107091730A
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attenuator
beam splitter
photomultiplier
shutter
photoelectric diode
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CN201710451588.6A
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CN107091730B (en
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赵永建
方晓华
张向平
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Jinhua Polytechnic
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Jinhua Polytechnic
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M11/00Testing of optical apparatus; Testing structures by optical methods not otherwise provided for

Abstract

The present invention relates to field of optical measurements, estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions, mainly include laser, attenuator I, camera bellows, beam splitter I, attenuator II, level crossing I, shutter I, shutter II, level crossing II, beam splitter II, magazine, silicon photoelectric diode, photomultiplier to be measured, the beam splitter I, attenuator II, level crossing I, shutter I, shutter II, level crossing II, beam splitter II, magazine, silicon photoelectric diode, photomultiplier to be measured is respectively positioned in camera bellows, the silicon photoelectric diode, photomultiplier to be measured is located in magazine, by laser, attenuator I, beam splitter I, shutter I, level crossing II, beam splitter II, silicon photoelectric diode composition light path I, by laser, attenuator I, beam splitter I, attenuator II, level crossing I, shutter II, beam splitter II, silicon photoelectric diode composition light path II, the attenuator I, attenuator II and the optical axis of measuring system are respectively provided with certain angle.

Description

Estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions
Technical field
It is particularly a kind of to be rung using non-liner revision estimation photomultiplier absolute light the present invention relates to field of optical measurements Should rate absolute light responsiveness of the estimation photomultiplier under low light-intensity conditions device.
Background technology
The measurement of extremely low power light is played an important role in scientific research and commercial Application, and such as astronomical observation, nuclear radiation is visited In terms of survey, bioluminescence detection and spectroscopy measurement, it is used for using photomultiplier visible to measure in photodetector The low-power light in light region;The method of the most frequently used accurate measurement absolute light responsiveness be by the measurement result of detector to be measured with The data of reference light source or photodetector after one calibration are contrasted.The defect of currently available technology is, to absolute light The estimation of responsiveness and linearity measure are carried out separately, and are only for some spectral region or some is narrower Reference optical power, by these experimental results be not enough to estimate photomultiplier measurement broad power band photoresponse rate, The device of absolute light responsiveness of the estimation photomultiplier under low light-intensity conditions can solve problem.
The responsiveness of one photodiode refers to the current signal and the ratio of the amount of radiation of input of its output, responsiveness The typically function of input radiation wavelength;If the responsiveness of a photodiode does not change with the amount of input radiation, It is called linear, the linearity is one of primary demand of optical radiation accurate measurement, especially in light measurement and actinometry Field, in linearity measuring method, the addition method is a kind of basic method, by document【Sanders, C.L.J.Res.Natl Bur.Stand.A 1972,76,437】And document【Sanders, C.L.Appl.Opt.1962,1,207】Understand, measure non-thread Property degree the principle of the addition method be that the photoresponse that the light that two light sources are sent is produced in photodiode to be measured respectively is N1With N2, the photoresponse that the summation of the light of two light sources is produced in photodiode to be measured is N12If, N1+N2=N12, then can be with It is linear to think photodiode to be measured, if N1+N2≠N12, then nonlinearity can be by N12/(N1+N2) provide.With top Two different light sources or a light source and two different diaphragms can be used in method.
The content of the invention
In order to solve the above problems, the present invention estimates photomultiplier absolute light responsiveness using non-liner revision, passes through The result obtained with the optical attenuator after calibration is compared to estimation, minimum light wide in the power bracket of visible-range Power can be close to single photon level.
The present invention proposes that the light under a kind of radiation of visible light of luminous power of estimation photomultiplier in single photon level rings Should rate method, based on three factors:The spectral responsivity of silicon photoelectric diode after calibration;Silicon photoelectric diode after calibration Conversion from responsiveness to photomultiplier;The non-liner revision of silicon photoelectric diode and photomultiplier.
The technical solution adopted in the present invention is:
The device of the absolute light responsiveness of the estimation photomultiplier under low light-intensity conditions, mainly including laser, Attenuator I, camera bellows, beam splitter I, attenuator II, level crossing I, shutter I, shutter II, level crossing II, beam splitter II, magazine, silicon Photodiode, photomultiplier to be measured, the beam splitter I, attenuator II, level crossing I, shutter I, shutter II, level crossing II, Beam splitter II, magazine, silicon photoelectric diode, photomultiplier to be measured are respectively positioned in the camera bellows, the silicon photoelectric diode, are treated Photomultiplier is surveyed to be located in the magazine, laser transmitting laser through attenuator I to beam splitter I, by the laser, Attenuator I, beam splitter I, shutter I, level crossing II, beam splitter II, silicon photoelectric diode composition light path I, by the laser, decline Subtract device I, beam splitter I, attenuator II, level crossing I, shutter II, beam splitter II, silicon photoelectric diode composition light path II, by adjusting H-section attenuator H I and attenuator II parameter measure the linearity under the conditions of different luminous powers, if shared n group attenuator parameters, The luminous power of the silicon photoelectric diode is incided from 10 to enable-6W to 10-16Change in the range of W, the attenuator I, attenuator II and measuring system optical axis are respectively provided with the inclination of certain angle to avoid interference with, and the silicon photoelectric diode is entering Penetrate luminous power 10-6Responsiveness under the conditions of W is known.The linear survey of the photomultiplier to be measured and the silicon photoelectric diode Amount is implemented under the conditions of 433 nanometers, 532 nanometers, 694 nanometers of lambda1-wavelength respectively.
The device step of the absolute light responsiveness of the estimation photomultiplier under low light-intensity conditions is:
One, is used as the ginseng for the absolute light power for calibrating the photomultiplier to be measured using the silicon photoelectric diode According to, incident optical power be 10-6W to 10-11The non-linear of the silicon photoelectric diode is calibrated under conditions of W scopes, method is successively For:Two-beam line is collimated by adjusting level crossing I, level crossing II and beam splitter II and in the identical point at optical sensor center Overlapping, under original state, shutter I and shutter II are turned off, next, opening shutter I, measure the now silicon photoelectric diode Output signal IA, shutter II is then turned on, the output signal I of the now silicon photoelectric diode is measuredA+B, shutter I is turned off, Measure the output signal I of the now silicon photoelectric diodeB, shutter I is then turned on, the defeated of the now silicon photoelectric diode is measured Go out signal I 'B+A, shutter II is turned off, the output signal I ' of the now silicon photoelectric diode is measuredA, obtained linearly by following formula DegreeWhereinPass through regulated attenuator I and attenuator II parameter measures the linearity under the conditions of different luminous powers, if shared n group attenuator parameters, to incide the silicon The luminous power of photodiode can be from 10-6W to 10-16Change in the range of W, k represents one group of condition in above-mentioned n groups, described Calculate the linearity method can eliminate by linearity measure test in attenuator produce laser drift effect, finally, will The linearity under the conditions of each luminous power is multiplied, and obtains the silicon photoelectric diode output signal IA+B(k) nonlinearity
Two, are 10 in incident optical power-6W to 10-11The non-thread of the photomultiplier to be measured is calibrated under conditions of W scopes Property, method is followed successively by:The silicon photoelectric diode is removed, the photomultiplier to be measured is placed in the position of former silicon photoelectric diode Put, collimate two-beam line by adjusting level crossing I, level crossing II and beam splitter II and in the identical point at optical sensor center Overlapping, under original state, shutter I and shutter II are turned off, next, opening shutter I, measure now photomultiplier to be measured Output signal IC, shutter II is then turned on, the output signal I of now photomultiplier to be measured is measuredC+D, shutter I is turned off, is measured The now output signal I of photomultiplier to be measuredD, shutter I is then turned on, the output signal of now photomultiplier to be measured is measured I′D+C, shutter II is turned off, the output signal I ' of now photomultiplier to be measured is measuredC, the linearity is obtained by following formulaWhereinPass through regulated attenuator I and attenuator II Parameter measure the linearity under the conditions of different luminous powers, if shared n group attenuator parameters, to incide the silicon light The luminous power of electric diode can be from 10-6W to 10-16Change in the range of W, k represents one group of condition in above-mentioned n groups, the meter Calculate the linearity method can eliminate by linearity measure test in attenuator produce laser drift effect, finally, will be every The linearity under the conditions of individual luminous power is multiplied, and obtains the photomultiplier output signal I to be measuredC+D(k) nonlinearity
Three, are 10 in incident optical power-11Under conditions of W, respectively with the silicon photoelectric diode and photoelectricity to be measured times after calibration Increase pipe measurement incident light and measured in the light path II, measure the luminous power data of the silicon photoelectric diode after calibration It is compared with the luminous power data of photomultiplier to be measured, method is followed successively by:First, the silicon photoelectric diode is placed in institute State in light path II, absolute incident laser power is measured using the silicon photoelectric diode after calibration, secondly, remove the pole of silicon photoelectricity two Pipe, photomultiplier to be measured is placed in the position of former silicon photoelectric diode, and measure photomultiplier for incident laser The position adjustment of photoresponse, wherein laser irradiation in the linearity measure of above-mentioned steps one to unanimously, being so repeated ten times, most Afterwards, the incident optical power that the incident optical power that the calculating photomultiplier to be measured is measured is measured with the silicon photoelectric diode Ratio, and determine the photomultiplier in incident optical power as 10 using this-11Absolute response rate under the conditions of W;
Four, estimate the photomultiplier to be measured in incident optical power 10-16Nonlinear characteristic under the conditions of W, and combine The responsiveness obtained in above-mentioned steps three-incident optical power curve, by approximating method, is estimated in luminous power as 10 using this-16W When absolute light responsiveness;
Five, finally obtain the photomultiplier to be measured 10-11W to 10-16The absolute light responsiveness of W scopes.
The beneficial effects of the invention are as follows:
The present invention can be 10 in visible power-11W to 10-16The photoresponse rate of photomultiplier, institute are estimated in the range of W State calculate the linearity method can eliminate by linearity measure test in attenuator produce laser drift effect, can disappear Except a series of dependence of the attenuator transmittance to wavelength and time in linearity measures.
Brief description of the drawings
Further illustrated with reference to the figure of the present invention:
Fig. 1 is schematic diagram of the present invention.
In figure, 1. lasers, 2. attenuator I, 3. camera bellows, 4. beam splitter I, 5. attenuator II, 6. level crossing I, 7. shutters I, 8. shutter II, 9. level crossing II, 10. beam splitter II, 11. magazines, 12. silicon photoelectric diodes, 13. photomultipliers to be measured.
Embodiment
If Fig. 1 is schematic diagram of the present invention, mainly include laser 1, attenuator I2, camera bellows 3, beam splitter I4, attenuator II5, level crossing I6, shutter I7, shutter II8, level crossing II9, beam splitter II10, magazine 11, silicon photoelectric diode 12, treat light-metering Electric multiplier tube 13, the beam splitter I4, attenuator II5, level crossing I6, shutter I7, shutter II8, level crossing II9, beam splitter II10, magazine 11, silicon photoelectric diode 12, photomultiplier to be measured 13 are respectively positioned in the camera bellows 3, the silicon photoelectric diode 12nd, photomultiplier 13 to be measured is located in the magazine 11, and the laser 1 launches laser through attenuator I2 to beam splitter I4, By the laser 1, attenuator I2, beam splitter I4, shutter I7, level crossing II9, beam splitter II10,12 groups of silicon photoelectric diode Into light path I, by the laser 1, attenuator I2, beam splitter I4, attenuator II5, level crossing I6, shutter II8, beam splitter II10, the composition light path II of silicon photoelectric diode 12, work(of not sharing the same light is measured by regulated attenuator I2 and attenuator II5 parameter The linearity under the conditions of rate, if shared n group attenuator parameters, the luminous power of the silicon photoelectric diode 12 is incided to enable It is enough from 10-6W to 10-16Change in the range of W, the optical axis of the attenuator I2, attenuator II5 and measuring system is respectively provided with necessarily The inclination of angle is to avoid interference with, and the silicon photoelectric diode 12 is in incident optical power 10-6Responsiveness under the conditions of W is known. The linear measurement of the photomultiplier to be measured 13 and the silicon photoelectric diode 12 is received 433 nanometers, 532 nanometers, 694 respectively Implement under the conditions of the lambda1-wavelength of rice.
The device of the absolute light responsiveness of the estimation photomultiplier under low light-intensity conditions using non-liner revision come The absolute light responsiveness of photomultiplier is estimated, the responsiveness of the incident light compared with broad power band, and minimum light intensity can be estimated Close to single photon level.

Claims (2)

1. the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions is estimated, mainly including laser (1), decay Device I (2), camera bellows (3), beam splitter I (4), attenuator II (5), level crossing I (6), shutter I (7), shutter II (8), level crossing II (9), beam splitter II (10), magazine (11), silicon photoelectric diode (12), photomultiplier to be measured (13), the beam splitter I (4), Attenuator II (5), level crossing I (6), shutter I (7), shutter II (8), level crossing II (9), beam splitter II (10), magazine (11), Silicon photoelectric diode (12), photomultiplier to be measured (13) are respectively positioned in the camera bellows (3), the silicon photoelectric diode (12), Photomultiplier (13) to be measured is located in the magazine (11), and the silicon photoelectric diode (12) is in incident optical power 10-6W conditions Under responsiveness be, it is known that it is characterized in that:The laser (1) launches laser through attenuator I (2) to beam splitter I (4), by institute State laser (1), attenuator I (2), beam splitter I (4), shutter I (7), level crossing II (9), beam splitter II (10), silicon photoelectricity two Pole pipe (12) constitutes light path I, by the laser (1), attenuator I (2), beam splitter I (4), attenuator II (5), level crossing I (6), shutter II (8), beam splitter II (10), silicon photoelectric diode (12) composition light path II, by regulated attenuator I (2) and decline Subtract device II (5) parameter to measure the linearity under the conditions of different luminous powers, if shared n group attenuator parameters, to cause incidence Luminous power to the silicon photoelectric diode (12) can be from 10-6W to 10-16Change in the range of W, the attenuator I (2), decline The optical axis for subtracting device II (5) and measuring system is respectively provided with the inclination of certain angle to avoid interference with.
2. the device of absolute light responsiveness of the estimation photomultiplier according to claim 1 under low light-intensity conditions, its It is characterized in:The linear measurement of the photomultiplier to be measured (13) and the silicon photoelectric diode (12) respectively 433 nanometers, 532 nanometers, implement under the conditions of 694 nanometers of lambda1-wavelength.
CN201710451588.6A 2017-06-08 2017-06-08 Device for estimating absolute light response rate of photomultiplier Active CN107091730B (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111398762A (en) * 2020-03-31 2020-07-10 北方夜视技术股份有限公司 Photomultiplier tube linear range testing device and method

Citations (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2092743A (en) * 1981-02-10 1982-08-18 Ceat Cavi Spa Apparatus for Measuring Attenuation in an Optical Fibre
CN1726664A (en) * 2002-12-16 2006-01-25 阿斯顿光学技术有限公司 Optical interrogation system and sensor system
JP2006133146A (en) * 2004-11-09 2006-05-25 National Institute Of Advanced Industrial & Technology Spectral responsivity measuring device for photodetector, measuring method therefor, and spectral irradiance calibration method of light source
US20060257896A1 (en) * 2005-02-24 2006-11-16 Compugen Ltd. Novel diagnostic markers, especially for in vivo imaging, and assays and methods of use thereof
CN101013062A (en) * 2007-01-30 2007-08-08 北京理工大学 Transmittance ratio test system for folding-shaft periscopic telescope optical system
JP2009257820A (en) * 2008-04-14 2009-11-05 Otsuka Denshi Co Ltd Optical characteristic measurement apparatus and optical characteristic measurement method
US20100219327A1 (en) * 2009-03-01 2010-09-02 Arbore Mark A High speed quantum efficiency measurement apparatus utilizing solid state lightsource
EP2410309A1 (en) * 2010-07-20 2012-01-25 U2t Photonics Ag Method and system for characterizing an optical device
WO2014036002A1 (en) * 2012-08-28 2014-03-06 Northeastern University Tunable heterojunction for multifunctional electronics and photovoltaics
CN104165756A (en) * 2014-08-27 2014-11-26 中国科学院半导体研究所 High-sensitivity optical vector network analyzer based on stimulated Brillouin scattering
CN104568391A (en) * 2015-01-21 2015-04-29 中国科学院上海技术物理研究所 Performance testing method and device for dual optical path switching mutual reference high precession AOTF
CN204679246U (en) * 2015-01-21 2015-09-30 中国科学院上海技术物理研究所 Double light path switches mutually with reference to high-precision A OTF performance testing device
CN107314887A (en) * 2017-06-08 2017-11-03 金华职业技术学院 The method for estimating absolute light responsiveness of the photomultiplier under low light-intensity conditions
CN207540768U (en) * 2017-06-08 2018-06-26 金华职业技术学院 Estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions

Patent Citations (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2092743A (en) * 1981-02-10 1982-08-18 Ceat Cavi Spa Apparatus for Measuring Attenuation in an Optical Fibre
CN1726664A (en) * 2002-12-16 2006-01-25 阿斯顿光学技术有限公司 Optical interrogation system and sensor system
JP2006133146A (en) * 2004-11-09 2006-05-25 National Institute Of Advanced Industrial & Technology Spectral responsivity measuring device for photodetector, measuring method therefor, and spectral irradiance calibration method of light source
US20060257896A1 (en) * 2005-02-24 2006-11-16 Compugen Ltd. Novel diagnostic markers, especially for in vivo imaging, and assays and methods of use thereof
CN101013062A (en) * 2007-01-30 2007-08-08 北京理工大学 Transmittance ratio test system for folding-shaft periscopic telescope optical system
JP2009257820A (en) * 2008-04-14 2009-11-05 Otsuka Denshi Co Ltd Optical characteristic measurement apparatus and optical characteristic measurement method
US20100219327A1 (en) * 2009-03-01 2010-09-02 Arbore Mark A High speed quantum efficiency measurement apparatus utilizing solid state lightsource
EP2410309A1 (en) * 2010-07-20 2012-01-25 U2t Photonics Ag Method and system for characterizing an optical device
WO2014036002A1 (en) * 2012-08-28 2014-03-06 Northeastern University Tunable heterojunction for multifunctional electronics and photovoltaics
CN104165756A (en) * 2014-08-27 2014-11-26 中国科学院半导体研究所 High-sensitivity optical vector network analyzer based on stimulated Brillouin scattering
CN104568391A (en) * 2015-01-21 2015-04-29 中国科学院上海技术物理研究所 Performance testing method and device for dual optical path switching mutual reference high precession AOTF
CN204679246U (en) * 2015-01-21 2015-09-30 中国科学院上海技术物理研究所 Double light path switches mutually with reference to high-precision A OTF performance testing device
CN107314887A (en) * 2017-06-08 2017-11-03 金华职业技术学院 The method for estimating absolute light responsiveness of the photomultiplier under low light-intensity conditions
CN207540768U (en) * 2017-06-08 2018-06-26 金华职业技术学院 Estimate the device of absolute light responsiveness of the photomultiplier under low light-intensity conditions

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
周泉: "具有高响应率宽响应范围的硅光电晶体管的设计与研究", 《CNKI优秀硕士学位论文》 *
杨晓娅: "微弱光信号检测系统的设计与研究", 《CNKI优秀硕士学位论文》 *
杨永宾: "硅光电管光谱特性测试系统的研究", 《万方学位论文》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111398762A (en) * 2020-03-31 2020-07-10 北方夜视技术股份有限公司 Photomultiplier tube linear range testing device and method
CN111398762B (en) * 2020-03-31 2022-07-08 北方夜视技术股份有限公司 Photomultiplier tube linear range testing device and method

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