CN105699356B - Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy - Google Patents

Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy Download PDF

Info

Publication number
CN105699356B
CN105699356B CN201610093394.9A CN201610093394A CN105699356B CN 105699356 B CN105699356 B CN 105699356B CN 201610093394 A CN201610093394 A CN 201610093394A CN 105699356 B CN105699356 B CN 105699356B
Authority
CN
China
Prior art keywords
fluorescence
comentropy
raman
signal
mixed signal
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.)
Active
Application number
CN201610093394.9A
Other languages
Chinese (zh)
Other versions
CN105699356A (en
Inventor
姚志湘
粟晖
刘柳
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.)
Oprah Winfrey, scientific instruments (Suzhou) Co. Ltd.
Original Assignee
Guangxi University of Science and Technology
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 Guangxi University of Science and Technology filed Critical Guangxi University of Science and Technology
Priority to CN201610093394.9A priority Critical patent/CN105699356B/en
Publication of CN105699356A publication Critical patent/CN105699356A/en
Application granted granted Critical
Publication of CN105699356B publication Critical patent/CN105699356B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65Raman scattering

Landscapes

  • Health & Medical Sciences (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Abstract

A method of judging that the fluorescence of Raman spectrum eliminates degree by comentropy, it is related to a kind of Raman spectrum fluorescence elimination method, it reduces criterion using the comentropy of discrete series as fluorescent component, fluorescence is gradually reduced from mixed signal, when comentropy reaches minimum, the fluorescence in mixed signal is completely eliminated.The present invention judges the elimination degree of fluorescence using comentropy, more scientific and reasonable, not by instrument wave number scope limitation, instrument performance is made to be not fully exerted, and increases the degree of freedom of Instrument Design and manufacture;And solve the limitation for needing that fluorescence residual condition is judged in particular range of wavelengths in prior art, to spectral region without particular/special requirement, it is suitable for the Instrument Design of different wave length setting.Also it can quickly and accurately obtain the Raman actual signal not interfered by fluorescence for meeting actual mechanism, application easy to spread in the case where not increasing equipment complexity and changing existing measurement custom.

Description

Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy
Technical field
It is especially a kind of that Raman spectrum is judged by comentropy the present invention relates to a kind of Raman spectrum fluorescence elimination method The method that fluorescence eliminates degree.
Background technology
Laser Raman spectroscopy can provide molecular spectrum information, while having and being not easy by moisture interference, non-contact and not The advantages that destroying sample, is a kind of qualitative and quantitative analysis means of fast development.But generated while Raman scattering excitation Fluorescence generates interference to Raman spectrum identifiability and signal quality.
It has developed rapidly in recent years using the photosensitive miniature beam splitting type Raman spectrometer of array, advantage is simple in structure, is not necessarily to Complex maintenance, but it uses hardware elimination fluorescence to interfere the complexity that can increase equipment, for example, utilizing the migration of Raman light With stablizing relatively for fluorescence, is excited by dual wavelength and eliminate fluorescence, instrument cost and complexity can all be promoted.Baseline fitting is reduced It is that current such Raman spectrometer disappears the main thought of fluorescence, most methods are reduced using spectrum baseline fitting to initial position, It provides fluorescence and eliminates presentation, can not actually be explained from mechanism or substantially, it is as a result both untrue or unreasonable.
The another bleach effect for thering is technology to be gradually reduced using fluorescence intensity under strong illumination, fluorescence intensity entire lowering, this Part measurement reflects the fluorescent characteristic in signal, and is gradually deducted from signal, the final fluorescence interference for eliminating Raman signal. Using Raman signal between specific wave number migration area this flat characteristic is presented to judge whether fluorescence is cut down completely in the technology, But with the proviso that must include the spectrum that this section is free of effective information in Instrument Design, limitation be constituted to Instrument Design.
Invention content
The technical problem to be solved by the present invention is to:A kind of fluorescence elimination degree judging Raman spectrum by comentropy is provided Method, to solve, increase instrument cost and complexity, result of the existing technology are untrue, are construed as limiting to Instrument Design Shortcoming.
Solving the technical solution of above-mentioned technical problem is:It is a kind of to judge that the fluorescence of Raman spectrum eliminates degree by comentropy Method, this method is to reduce criterion as fluorescent component using the comentropies of discrete series, is gradually reduced from mixed signal Fluorescence, when comentropy reaches minimum, the fluorescence in mixed signal is completely eliminated.
The present invention further technical solution be:This approach includes the following steps:
A, using the mixed signal of raman laser probe measurement sample, fixed-focus sets the time of integration, 2 groups of record with Spectroscopic data under upper different momentsS
B, serial weights are multiplied by later moment in time spectroscopic data successively, calculate the difference with previous moment spectroscopic data, obtains Decline metric Δ to the fluorescence without Raman signalS
C, metric Δ is declined to fluorescenceSNoise reduction is carried out, the fluorescence after noise reduction declines metric ΔSAs mixed signalS In the fluorescence component that containsF S
D, it is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,To reduce step-length,F S For Fluorescence component, and calculate often step and reducen*△*F S Comentropy afterwards;
E, judge that often step is reducedn*△*F S Whether comentropy afterwards is minimum value, if it is not, then step D is repeated, if It is then to show that fluorescence reduces completion, obtains the pure Raman signal without fluorescence.
The present invention further technical solution be:In stepb, the serial weights are 0.95~1.05.
The present invention further technical solution be:It is described that metric Δ is declined to fluorescence in step CSIt is dropped It makes an uproar selectionSAvitzky-Golay filters, it is the 1/10 of overall signal length to select the filtering of 2 ranks, window width.
The present invention further technical solution be:The step D includes following specific method:
D1, according to formula, calculate the comentropy of mixed signalH(X), formula InP(a i ) it is mixed signalSTakeiThe probability of a luminous intensity,i=1,2 ...,Q, qValue is number of data points contained by spectrum;
Step-length △ is reduced in D2, setting, is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,F S For fluorescence component, and calculates often step and reducen*△*F S Comentropy afterwards.
The present invention further technical solution be:The step-length △ that reduces is 0.01~0.1.
Due to using the above structure, the present invention by comentropy judge the fluorescence of Raman spectrum eliminate the method for degree with The prior art is compared, and is had the advantages that:
1. the fluorescence of Raman spectrum really rationally, can be eliminated effectively:
The present invention is to reduce criterion as fluorescent component using the comentropy of discrete series, is gradually reduced from mixed signal Fluorescence, when comentropy reaches minimum, the fluorescence in mixed signal is completely eliminated.Excite Raman light also can be same since light irradiates Shi Jifa fluorescence, to generate interference to Raman light.However, Raman light and fluorescence and asynchronous, Raman information contained amount is apparent Higher than fluorescence;Research confirms that the uncertainty of the mixed signal containing fluorescence is always greater than pure Raman signal, i.e., signal is completely by drawing Graceful spectrum is constituted, and entropy is minimum.Therefore, the present invention really can rationally, effectively eliminate the fluorescence of Raman spectrum.
2. method is easy:
It is unrelated with amplitude since the size of the entropy of mixed signal is only related with the composition situation of the signal, it need not mark Other data preprocessing methods such as standardization are suitable for the processing of each single-measurement data;Therefore, the present invention is repeatedly surveyed with needs The methods of the order judgement that measuring could use is compared, and method of the invention is more easy.
3. the degree of freedom of Instrument Design and manufacture can be increased:
The present invention judges the elimination degree of fluorescence using comentropy, more scientific and reasonable, not by instrument wave number scope limitation, So that instrument performance is not fully exerted, increases the degree of freedom of Instrument Design and manufacture.Therefore, the present invention solves the prior art and needs The limitation that fluorescence residual condition is judged in particular range of wavelengths is suitable for different wave length and sets to spectral region without particular/special requirement The Instrument Design set.
4. equipment used in is simple, low cost:
The acquisition requirement of the present invention and acquisition step and existing acquisition method indifference, equipment is simple, low cost, not In the case of increasing equipment manufacturing cost, measurement attachment and changing existing acquisition step, quickly and accurately obtains and meet actual mechanism The Raman actual signal not interfered by fluorescence, application easy to spread.
In the following, judging that the fluorescence of Raman spectrum eliminates degree by comentropy to the present invention in conjunction with the accompanying drawings and embodiments The technical characteristic of method is further described.
Description of the drawings
Fig. 1:The spectrogram measured in one step A of embodiment,
Fig. 2:In one step B of embodiment, the spectrum comparison diagram subtracted using weighting subtractive and non-weighted difference,
Fig. 3:The spectrogram of the fluorescence component contained in mixed signal described in one step C of embodiment,
Fig. 4:In one step D of embodiment, comentropy with the amount of reducing figure of changing,
Fig. 5:In one step E of embodiment, the obtained Raman signal without fluorescenceRWith the mixed signal of original measurementSIt Between spectrum comparison diagram;
Fig. 6:In 200-1800cm-1When band signal, comentropy is with the amount of reducing figure of changing;
Fig. 7:The fluorescence for simulating Raman-fluorescence mixed signal is eliminated in experiment, is simulated respectively using Lorentzian pair Should in the spectral curve of Raman and fluorescence,
Fig. 8:The fluorescence for simulating Raman-fluorescence mixed signal is eliminated in experiment, 1 times of Raman signal and 5 times of fluorescence signals Design sketch is summed it up,
Fig. 9:The fluorescence for simulating Raman-fluorescence mixed signal is eliminated in experiment, and 1 times of Raman signal has summed it up -1 ~ 5 times Fluorescence comentropy figure of changing.
Specific implementation mode
A method of judging that the fluorescence of Raman spectrum eliminates degree by comentropy, this method is using discrete series Comentropy reduces criterion as fluorescent component, and fluorescence is gradually reduced from mixed signal, when comentropy reaches minimum, mixing letter Fluorescence in number is completely eliminated.
This approach includes the following steps:
A, using the mixed signal of raman laser probe measurement sample, fixed-focus sets the time of integration, 2 groups of record with Spectroscopic data under upper different momentsS
B, serial weights are multiplied by later moment in time spectroscopic data successively, which is 0.95~1.05, is calculated with before The difference of one moment spectroscopic data obtains the fluorescence without Raman signal and declines metric ΔS
C, it selectsSAvitzky-Golay filters decline metric Δ to fluorescenceSNoise reduction is carried out, the filtering of 2 ranks, window are selected Mouth width degree is the 1/10 of overall signal length, and the fluorescence after noise reduction declines metric ΔSAs mixed signalSIn the fluorescence that contains ComponentF S
D, it is gradually reduced from mixed signaln*△*F S, nFor the step number reduced,n=1,2 ...,To reduce step-length,F S For Fluorescence component, and calculate often step and reducen*△*F S Comentropy afterwards;
D1, according to formula, calculate the comentropy of mixed signalH(X), formula InP(a i ) it is mixed signalSTakeiThe probability of a luminous intensity,i=1,2 ...,Q, qValue is number of data points contained by spectrum;
Step-length △ is reduced in D2, setting, is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,F S For fluorescence component, and calculates often step and reducen*△*F S Comentropy afterwards;
E, judge that often step is reducedn*△*F S Whether comentropy afterwards is minimum value, if it is not, then step D is repeated, if It is then to show that fluorescence reduces completion, obtains the pure Raman signal without fluorescence.
The following is specific embodiments of the present invention:
Embodiment one:
A method of judging that the fluorescence of sucrose Raman spectrum eliminates degree by comentropy, this method includes following step Suddenly:
A, using raman laser probe 785nm laser excitations, sucrose Raman spectrum, fixed-focus, when setting integrates are measured Between 10s, time interval 30s measures 2 times, record gained mixed signalS 1、 S 2, as shown in fig. 1,S 1For the measurement light at moment 1 Spectrum,S 2For the measure spectrum at moment 2;
B, the weights for adjusting 2 spectrum of moment are 1.028, with previous moment spectrum subtraction, obtain effectively eliminating drawing therein The fluorescence of graceful ingredient declines decreasing concentration magnitude ΔS, respectively by the spectrum of subtractive after weightingS 3With the spectrum for not weighting direct subtractiveS 4Make Comparison is as shown in Fig. 2, as can be seen from Figure 2, using weighting subtractive, can effectively eliminate Raman ingredient therein;
C, it selectsSAvitzky-Golay filters decline metric Δ to fluorescenceSNoise reduction is carried out, the filtering of 2 ranks, window are selected Mouth width degree is 91;Fluorescence after noise reduction declines metric ΔSAs mixed signalSIn the fluorescence component that containsF S , such as Fig. 3 institutes Show;
D, it is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,To reduce step-length,F S For Fluorescence component, and calculate often step and reducen*△*F S Comentropy afterwards, specific method are:
D1, according to formula, the comentropy of mixed signal is calculated, in formulaP (a i ) it is mixed signalSTakeiThe probability of a luminous intensity,i=1,2 ...,Q, qValue is number of data points contained by spectrum;
Step-length △ is reduced in D2, setting, is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,F S For fluorescence component, and calculates often step and reducen*△*F S Comentropy afterwards;
E, judge that often step is reducedn*△*F S Whether comentropy afterwards is minimum value, if it is not, then step D is repeated, if It is then to show that fluorescence reduces completion, obtains the pure Raman signal without fluorescence.Fig. 4 is comentropy with the amount of reducing situation of change,F S 5.83 times when, there is minimum value in comentropy, is from original mixed signalSIt is middle to deduct corresponding 5.83 timesF S Afterwards, it obtains Raman signal R without fluorescence;The Raman signal without fluorescence that Fig. 5 isRWith the mixed signal of original measurementSBetween Spectrum comparison diagram.
Present inventor also selects 200-1800cm-1Band signal calculates comentropy, as shown in fig. 6, in fluorescence ComponentF S 5.88 times there is minimum value, with using in embodiment one in 200-3000cm-1The comentropy of the calculating of band signal 5.83* when minimum valueF S Error be less than 1%, show that the present invention can not depend on specific range of signal, and obtain consistent Effective result.
The elimination degree of fluorescence is judged using comentropy, it is more scientific and reasonable, not by instrument wave number scope limitation, make instrument Performance is not fully exerted, and increases the degree of freedom of Instrument Design and manufacture.The present invention, which solves, to be needed in the prior art specific Wave-length coverage judges the limitation of fluorescence residual condition, to spectral region without particular/special requirement, is suitable for the instrument of different wave length setting Design.In the case of not increasing equipment complexity and changing existing measurement custom, it can quickly and accurately obtain and meet reality The Raman actual signal of mechanism not interfered by fluorescence.
In addition, fluorescence content is 0 when in order to demonstrate,prove comentropy with minimum value, present inventor has also made simulation and has drawn Fluorescence in graceful-fluorescence mixed signal eliminates experiment:
1. simulating the curve of spectrum corresponding to Raman and fluorescence respectively using Lorentzian, as shown in Figure 7.
2. the Raman of simulation and fluorescence signal are summed it up, the mixed signal that can be simulated.Fig. 8 is 1 times of Raman signal and 5 The adduction effect of times fluorescence signal.
3. calculating simulation Raman signal sums it up the information entropy after the fluorescence of different content respectively.The Raman that Fig. 9 is 1 times is believed Number adduction comentropy situation of change of -1 ~ 5 times of fluorescence, it can be seen that fluorescence content is 0 when comentropy has minimum value, Output is the Raman signal without fluorescence.

Claims (5)

1. a kind of method judging that the fluorescence of Raman spectrum eliminates degree by comentropy, it is characterised in that:This method is to use The comentropy of discrete series reduces criterion as fluorescent component, and fluorescence is gradually reduced from mixed signal, when comentropy reaches most Hour, the fluorescence in mixed signal is completely eliminated;This approach includes the following steps:
A, using the mixed signal of raman laser probe measurement sample, fixed-focus sets the time of integration, and 2 groups of record or more is no Spectroscopic data under in the same timeS
B, serial weights are multiplied by later moment in time spectroscopic data successively, calculate the difference with previous moment spectroscopic data, obtains not Fluorescence containing Raman signal declines metric ΔS
C, metric Δ is declined to fluorescenceSNoise reduction is carried out, the fluorescence after noise reduction declines metric ΔSAs mixed signalSIn contain Some fluorescence componentsF S
D, it is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,To reduce step-length,F S For fluorescence Component, and calculate often step and reducen*△*F S Comentropy afterwards;
E, judge that often step is reducedn*△*F S Whether comentropy afterwards is minimum value, if it is not, then step D is repeated, if it is, table Bright fluorescence reduces completion, obtains the pure Raman signal without fluorescence.
2. the method according to claim 1 for judging that the fluorescence of Raman spectrum eliminates degree by comentropy, feature exist In:In stepb, the serial weights are 0.95~1.05.
3. the method according to claim 1 for judging that the fluorescence of Raman spectrum eliminates degree by comentropy, feature exist In:It is described that metric Δ is declined to fluorescence in step CSCarry out noise reduction selectionSAvitzky-Golay filters select 2 Rank filters, and window width is the 1/10 of overall signal length.
4. the method according to claim 1 for judging that the fluorescence of Raman spectrum eliminates degree by comentropy, feature exist In:The step D includes following specific method:
D1, according to formula, calculate the comentropy of mixed signalH(X), in formulaP(a i ) it is mixed Close signalSTakeiThe probability of a luminous intensity,i=1,2 ...,Q, qValue is number of data points contained by spectrum;
Step-length △ is reduced in D2, setting, is gradually reduced from mixed signaln*△*F S ,nFor the step number reduced,n=1,2 ...,F S For Fluorescence component, and calculate often step and reducen*△*F S Comentropy afterwards.
5. the method according to claim 4 for judging that the fluorescence of Raman spectrum eliminates degree by comentropy, feature exist In:The step-length △ that reduces is 0.01~0.1.
CN201610093394.9A 2016-02-19 2016-02-19 Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy Active CN105699356B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610093394.9A CN105699356B (en) 2016-02-19 2016-02-19 Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610093394.9A CN105699356B (en) 2016-02-19 2016-02-19 Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy

Publications (2)

Publication Number Publication Date
CN105699356A CN105699356A (en) 2016-06-22
CN105699356B true CN105699356B (en) 2018-10-19

Family

ID=56222324

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610093394.9A Active CN105699356B (en) 2016-02-19 2016-02-19 Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy

Country Status (1)

Country Link
CN (1) CN105699356B (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108169201B (en) * 2016-12-08 2020-07-28 同方威视技术股份有限公司 Raman spectrum detection method for deducting package interference
CN108195817B (en) * 2016-12-08 2020-09-15 同方威视技术股份有限公司 Raman spectrum detection method for removing solvent interference
CN109752364B (en) * 2019-03-11 2021-06-08 广西科技大学 Asynchronous fading fluorescence elimination method of multi-component system Raman spectrum
CN109765212B (en) * 2019-03-11 2021-06-08 广西科技大学 Method for eliminating asynchronous fading fluorescence in Raman spectrum
CN110108689B (en) * 2019-05-17 2021-07-30 广西科技大学 Method for rapidly eliminating 3D fluorescence background noise

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60113132A (en) * 1983-11-25 1985-06-19 Agency Of Ind Science & Technol Raman spectrum measuring device
CN1425911A (en) * 2003-01-17 2003-06-25 南京师范大学 Raman test method for quick eliminating biologichal molecular fluorescence
CN103901014A (en) * 2014-03-10 2014-07-02 华南师范大学 Method for obtaining true Raman spectrum of cell by multiple linear regression fitting
CN104198463A (en) * 2014-09-22 2014-12-10 中国科学院重庆绿色智能技术研究院 Raman spectrum preprocessing method and system
WO2015096779A1 (en) * 2013-12-27 2015-07-02 同方威视技术股份有限公司 Raman spectrum detection method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7177022B2 (en) * 2005-02-18 2007-02-13 Axsun Technologies, Inc. Method and system removing fluorescence and other slowly varying baseline in Raman spectra

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60113132A (en) * 1983-11-25 1985-06-19 Agency Of Ind Science & Technol Raman spectrum measuring device
CN1425911A (en) * 2003-01-17 2003-06-25 南京师范大学 Raman test method for quick eliminating biologichal molecular fluorescence
WO2015096779A1 (en) * 2013-12-27 2015-07-02 同方威视技术股份有限公司 Raman spectrum detection method
CN103901014A (en) * 2014-03-10 2014-07-02 华南师范大学 Method for obtaining true Raman spectrum of cell by multiple linear regression fitting
CN104198463A (en) * 2014-09-22 2014-12-10 中国科学院重庆绿色智能技术研究院 Raman spectrum preprocessing method and system

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
Application of Band-Target Entropy Minimization to On-Line Raman Monitoring of an Organic Synthesis. An Example of New Technology for Process Analytical Technology;Effendi Widjaja et al;《Organic Process Research & Development》;20061224;第11卷(第1期);第98-103页 *
SNR Enhancement and Deconvolution of Raman Spectra Using a Two-Point Entropy Regularization Method;L. SHANE GREEK et al;《APPLIED SPECTROSCOPY》;19951231;第49卷(第4期);第426页右栏第2段至第5段,第427末段至428首段 *
乙醇含量拉曼光谱检测中噪声与背景同时消除方法研究;韩庆阳 等;《光谱学与光谱分析》;20151231;第35卷(第12期);第3406-3409页 *

Also Published As

Publication number Publication date
CN105699356A (en) 2016-06-22

Similar Documents

Publication Publication Date Title
CN105699356B (en) Judge the method that the fluorescence of Raman spectrum eliminates degree by comentropy
Conroy et al. Metal-rich, metal-poor: updated stellar population models for old stellar systems
Shen et al. The Sloan digital sky survey reverberation mapping project: first broad-line Hβ and Mg II Lags at z≳ 0.3 from six-month spectroscopy
Wilkinson et al. P-MaNGA: full spectral fitting and stellar population maps from prototype observations
Coatman et al. C IV emission-line properties and systematic trends in quasar black hole mass estimates
Vincenzi et al. Spectrophotometric templates for core-collapse supernovae and their application in simulations of time-domain surveys
Finkelstein et al. CANDELS: The evolution of galaxy rest-frame ultraviolet colors from z= 8 to 4
Maxwell et al. Coherent-Radiation Spectroscopy of Few-Femtosecond Electron Bunches<? format?> Using a Middle-Infrared Prism Spectrometer
Glikman et al. A near-infrared spectral template for quasars
Finkelstein et al. Dust Extinction and metallicities of star-forming Lyα emitting galaxies at low redshift
Grier et al. THE SLOAN DIGITAL SKY SURVEY REVERBERATION MAPPING PROJECT: RAPID C iv BROAD ABSORPTION LINE VARIABILITY
Thorp et al. Testing the consistency of dust laws in SN Ia host galaxies: a BAYESN examination of Foundation DR1
Barman et al. Effect of photobleaching on calibration model development in biological Raman spectroscopy
CA2299285A1 (en) Method and apparatus for generating basis sets for use in spectroscopic analysis
WO2018184262A1 (en) Dynamic calibration method for echelle spectrometer for laser induced breakdown spectrum collection
JP2008539417A (en) Spectroscopy for determining the amount of analyte in a mixture of analytes.
JP4911409B2 (en) Method and apparatus for measuring pulse rate and oxygen saturation during exercise
CN105241866B (en) The method for eliminating baseline interference in Raman spectrum using fluorescence bleach effect
JP2007292665A (en) Glare evaluation device and program
Cava et al. SHARDS: A Global View of the Star Formation Activity at z∼ 0.84 and z∼ 1.23
CN104345049B (en) Threshold correction method applied to wavelet threshold noise reduction of laser-induced breakdown spectroscopy
Rakshit et al. The Seoul National University AGN monitoring project. II. BLR size and black hole mass of two AGNs
Sirressi et al. CLusters in the UV as EngineS (CLUES). I. Survey Presentation and FUV Spectral Analysis of the Stellar Light
CN105606589B (en) The Raman spectrum that fluorescence colour fading metric is asked for by kurtosis judgement disappears fluorescent method
Talbot et al. Correction approach for delta function convolution model fitting of fluorescence decay data in the case of a monoexponential reference fluorophore

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right

Effective date of registration: 20191107

Address after: 215011 north side, floor 3, building 1, No. 8, Keling Road, high tech Zone, Suzhou City, Jiangsu Province

Patentee after: Oprah Winfrey, scientific instruments (Suzhou) Co. Ltd.

Address before: 545006 No. 268 East Ring Road, the Guangxi Zhuang Autonomous Region, Liuzhou

Patentee before: Guangxi University of Science and Technology

TR01 Transfer of patent right