CN104849215A - Position triangular wave frequency coding plane array imaging light measurement system - Google Patents
Position triangular wave frequency coding plane array imaging light measurement system Download PDFInfo
- Publication number
- CN104849215A CN104849215A CN201510196507.3A CN201510196507A CN104849215A CN 104849215 A CN104849215 A CN 104849215A CN 201510196507 A CN201510196507 A CN 201510196507A CN 104849215 A CN104849215 A CN 104849215A
- Authority
- CN
- China
- Prior art keywords
- monochromatic
- photosensitive device
- group
- light
- triangular wave
- 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
Links
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention discloses a position triangular wave frequency coding plane array imaging light measurement system. The measurement system comprises: a group of monochromatic light sources, a group of light-sensitive devices, and a computer externally connected with the light-sensitive devices, the group of the monochromatic light sources is distributed on one side of a sample, and the group of the light-sensitive devices is distributed on the other side of the sample; each of the monochromatic light sources forms an n*n plane array light sources; each of the light-sensitive devices forms an n*n plane array light source receiving device; triangular waves with different frequencies and having a ratio doubling relationship are adopted to respectively drive all the monochromatic light sources, and all the light-sensitive devices receive monochromatic light combinations of all the monochromatic light sources permeating the sample; and the computer separates the monochromatic light combinations to obtain the contribution of all the monochromatic light sources in order to realize imaging of the sample. The system realizes high-speed comprehensive-information plane array imaging light high-precision measurement, and has the advantages of simple structure and circuit, low requirements on an apparatus and a technology, easy debugging and high reliability.
Description
Technical field
The present invention relates to battle array imaging measuring system field, face, particularly relate to the face battle array imaging measuring system of a kind of position triangular wave frequency coding.
Background technology
By light, imaging is carried out to interior of articles in prior art, particularly imaging is carried out to inside of human body, there is the harmless outstanding advantages radiationless without wound, but not yet there is the face battle array imaging measuring system that can enter Clinical practice so far, its reason is existing, and battle array imaging measuring system precision is low, quantity of information is less, cannot meet the needs in practical application.
Summary of the invention
The invention provides the face battle array imaging measuring system of a kind of position triangular wave frequency coding, present invention achieves the high-acruracy survey of high speed, greatly the face battle array imaging of information, meet the needs in practical application, described below:
The face battle array imaging measuring system of a kind of position triangular wave frequency coding, described battle array imaging measuring system comprises: one group of monochromatic source, one group of photosensitive device, and the computing machine external with photosensitive device, one group of monochromatic source is distributed in the one side of sample, and one group of photosensitive device is distributed in the another side of sample;
Wherein, each monochromatic source in one group of monochromatic source forms n × n area array light source; Realize coding to Different Light, each photosensitive device in one group of photosensitive device forms n × n area array light source receiving device, n >=3 and be odd number;
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochromatic source in one group of monochromatic source respectively, in one group of photosensitive device, each photosensitive device receives each monochromatic source and combines through the monochromatic light of sample;
Computing machine carries out to monochromatic light combination the contribution that demodulation is separated each monochromatic source obtained in monochromatic light combination, realizes the imaging to sample accordingly.
Further, each monochromatic source and even, the reciprocity arrangement of each photosensitive device.
Wherein, described monochromatic source is laser diode, and described photosensitive device is photodiode.
Another embodiment, described monochromatic source is monochrome photodiode, and described photosensitive device is photodiode.
Another embodiment, described monochromatic source be monochromatic filter plate to monochromatic light after white light filtering, described photosensitive device is photodiode.
Another embodiment, described monochromatic source is laser diode, and described photosensitive device is photomultiplier.
Another embodiment, described monochromatic source is monochrome photodiode, and described photosensitive device is photomultiplier.
Another embodiment, described monochromatic source be monochromatic filter plate to monochromatic light after white light filtering, described photosensitive device is photomultiplier.
The beneficial effect of technical scheme provided by the invention is: the present invention adopts the triangular wave of 2 overtones band relations to drive monochromatic source, the contribution that separation can obtain each monochromatic source in monochromatic light combination is carried out to the photosignal that photosensitive device detects, accordingly can to imaging of samples; Present invention achieves the high-acruracy survey of face battle array imaging of high speed, large information, and there is structure and circuit is simple, device and technological requirement is low, debugging easily, high reliability.
Accompanying drawing explanation
Fig. 1 is the structural representation of the face battle array imaging measuring system of position triangular wave frequency coding;
Fig. 2 is monochromatic source, sample and photosensitive device relative position schematic diagram;
Fig. 3 is triangular wave pumping signal schematic diagram.
In accompanying drawing, the list of parts representated by each label is as follows:
1: one group of monochromatic source; 2: sample;
3: one groups of photosensitive devices.
Embodiment
For making the object, technical solutions and advantages of the present invention clearly, below embodiment of the present invention is described further in detail.
Embodiment 1
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, described battle array imaging measuring system comprises: one group n × n monochromatic source 1 (LD
1lD
n) and one group n × n photosensitive device 3 (PD
1pD
n), n>=3 and for odd number (n is odd number, then middle light source or photosensitive device can be used as center line, be convenient to aim at arrangement, wherein, the concrete value of n is relevant to the cross-sectional area of sample 2, and the embodiment of the present invention does not limit this); One group of monochromatic source 1 is distributed in the one side of sample 2, and one group of photosensitive device 3 is distributed in the another side of sample 2;
Wherein, each monochromatic source LD in one group of monochromatic source 1
1lD
nevenly, equity arrangement, form area array light source; Each photosensitive device PD in one group of photosensitive device 3
1pD
nevenly, equity arrangement, form area array light source receiving device.This face battle array imaging measuring system also comprises the computing machine (not shown) external with one group of photosensitive device 3.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochromatic source LD in one group of monochromatic source 1 respectively
ij, each photosensitive device PD in one group of photosensitive device 3
ijreceive each monochromatic source LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic source LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
That is, according to each just to the light intensity that the photosensitive device of monochromatic source receives, backprojection reconstruction obtains the transmission image of sample 2, and the photosensitive device of other positions obtains the information of this wavelength as auxiliary, strengthening image information.According to the organizational information in graphical analysis sample 2, determine the scattering degree information of sample tissue.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic source LD
ijthe step of contribution be specially:
1) LD to drive monochromatic source is supposed
jhighest frequency f
max(f in these cases
max=f
1) 4M speed sampling f is carried out to photosignal
s=4M × f
max, obtain sampled signal x (m), wherein M be more than or equal to 1 positive integer;
2) computing machine will add up to the sampled signal in the positive and negative half period in each triangular wave cycle corresponding to each wavelength respectively, and accumulation result carries out asking difference operation;
That is, obtain cumulative sum by cumulative for the sampled value of the positive half period of each triangular wave in certain hour (an integer triangular wave cycle), the sampled value of the negative half period of each triangular wave is cumulative obtains cumulative sum, and these two cumulative sums are subtracted each other.
3) difference of each wavelength above-mentioned is carried out k cycle or an integral multiple k periodic accumulation, the spectral value of each wavelength can be obtained.Wherein:
In formula: f
minfor the low-limit frequency in excitation triangular wave; A is preset constant, value be more than or equal to 1 positive integer, a/f
minfor the cycle of lower sampling; f
nfor the triangular wave excitation frequency of handled wavelength.
To amplitude be x be sampled value, if uniform sampling N (>>1) puts and is averaged within the regular hour, the mean value obtained is
Wherein, [x] is that analog to digital converter quantizes x, is also the positive integer that round off rounding obtains.X
ithe amplitude of i-th, [x
i] be that analog to digital converter is to x
iquantizing, is also the positive integer that round off rounding obtains.
(3) formula shows, the signal sampling one being compared to " totally " is repeatedly averaged, and can not improve its precision, and the error of the mean value obtained is identical with the error of unitary sampling, is Δ x
i.
If to amplitude be x be sampled sawtooth wave, within the regular hour, uniform sampling N (>>1) puts and is averaged equally, and the mean value obtained is
Wherein, x
i=m
i+ Δ x
i, m
i=[x
i].Also be m
ithat rounding obtains positive integer, and Δ x
iit is " at random " error of losing after being rounded.
(4) formula can utilize arithmetic series sum formula to obtain further:
(5) the last item in formula is the value after quantizing, although less than the result of (3) formula half, according to theory of errors, the precision of data does not change because being multiplied by a fixing non-zero constant.But be the random number of zero-mean in one next, compare will reduce in (3) formula
doubly, therefore, the effect of the precision that can be improved equally after over-sampling is carried out to sawtooth wave or triangular wave pumping signal, and do not need another external high-frequency disturbing signal.
Wherein, the shape of the embodiment of the present invention to one group of monochromatic source 1 and one group of photosensitive device 3 does not limit, and is generally square.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 2
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment is using laser diode as monochromatic source LD
1lD
n, photodiode is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each laser diode LD in one group of monochromatic source 1 respectively
ij, each photosensitive device PD in one group of photosensitive device 3
ijreceive each laser diode LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each laser diode LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each laser diode LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 3
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment is using monochrome photodiode as monochromatic source LD
1lD
n, photodiode is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochrome photodiode LD in one group of monochromatic source 1 respectively
ij, each photodiode PD in one group of photosensitive device 3
ijreceive each monochrome photodiode LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochrome photodiode LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochrome photodiode LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 4
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment using monochromatic filter plate to monochromatic light after white light filtering as monochromatic source LD
1lD
n, photodiode is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochromatic filter plate in one group of monochromatic source 1 to monochromatic light LD after white light filtering respectively
ij, each photodiode PD in one group of photosensitive device 3
ijreceive each monochromatic light LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic light LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic light LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 5
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment is using laser diode as monochromatic source LD
1lD
n, photomultiplier is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each laser diode LD in one group of monochromatic source 1 respectively
ij, each photomultiplier PD in one group of photosensitive device 3
ijreceive each laser diode LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each laser diode LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each laser diode LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 6
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment is using monochrome photodiode as monochromatic source LD
1lD
n, photomultiplier is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochrome photodiode LD in one group of monochromatic source 1 respectively
ij, each photomultiplier PD in one group of photosensitive device 3
ijreceive each monochrome photodiode LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochrome photodiode LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochrome photodiode LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
Embodiment 7
A face battle array imaging measuring system for position triangular wave frequency coding, see Fig. 1, Fig. 2 and Fig. 3, this embodiment using monochromatic filter plate to monochromatic light after white light filtering as monochromatic source LD
1lD
n, photomultiplier is as photosensitive device PD
1pD
nfor example is described.
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochromatic filter plate in one group of monochromatic source 1 to monochromatic light LD after white light filtering respectively
ij, each photomultiplier PD in one group of photosensitive device 3
ijreceive each monochromatic light LD
ijthrough the monochromatic light combination I of sample 2
ij; Computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic light LD
ijcontribution, imaging can be carried out to sample 2 accordingly.
Wherein, computing machine combines I to monochromatic light
ijcarry out demodulation separation and can obtain monochromatic light combination I
ijin each monochromatic light LD
ijthe step of contribution identical with embodiment 1, the embodiment of the present invention does not repeat this.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
It will be appreciated by those skilled in the art that accompanying drawing is the schematic diagram of a preferred embodiment, the invention described above embodiment sequence number, just to describing, does not represent the quality of embodiment.
The foregoing is only preferred embodiment of the present invention, not in order to limit the present invention, within the spirit and principles in the present invention all, any amendment done, equivalent replacement, improvement etc., all should be included within protection scope of the present invention.
Claims (8)
1. the face battle array imaging measuring system of a position triangular wave frequency coding, described battle array imaging measuring system comprises: one group of monochromatic source, one group of photosensitive device, and the computing machine external with photosensitive device, it is characterized in that, one group of monochromatic source is distributed in the one side of sample, and one group of photosensitive device is distributed in the another side of sample;
Wherein, each monochromatic source in one group of monochromatic source forms n × n area array light source, realizes the coding to Different Light; Each photosensitive device in one group of photosensitive device forms n × n area array light source receiving device, n >=3 and be odd number;
Adopt different frequency and become the triangular wave of 2 times of ratio to drive each monochromatic source in one group of monochromatic source respectively, in one group of photosensitive device, each photosensitive device receives each monochromatic source and combines through the monochromatic light of sample;
Computing machine carries out to monochromatic light combination the contribution that demodulation is separated each monochromatic source obtained in monochromatic light combination, realizes the imaging to sample accordingly.
2. the face battle array imaging measuring system of a kind of position according to claim 1 triangular wave frequency coding, is characterized in that, each monochromatic source and even, the reciprocity arrangement of each photosensitive device.
3. the face battle array imaging measuring system of a kind of position according to claim 1 and 2 triangular wave frequency coding, it is characterized in that, described monochromatic source is laser diode, and described photosensitive device is photodiode.
4. the face battle array imaging measuring system of a kind of position according to claim 1 and 2 triangular wave frequency coding, it is characterized in that, described monochromatic source is monochrome photodiode, and described photosensitive device is photodiode.
5. a kind of position according to claim 1 and 2 triangular wave frequency coding face battle array imaging measuring system, it is characterized in that, described monochromatic source be monochromatic filter plate to monochromatic light after white light filtering, described photosensitive device is photodiode.
6. the face battle array imaging measuring system of a kind of position according to claim 1 and 2 triangular wave frequency coding, it is characterized in that, described monochromatic source is laser diode, and described photosensitive device is photomultiplier.
7. the face battle array imaging measuring system of a kind of position according to claim 1 and 2 triangular wave frequency coding, it is characterized in that, described monochromatic source is monochrome photodiode, and described photosensitive device is photomultiplier.
8. a kind of position according to claim 1 and 2 triangular wave frequency coding face battle array imaging measuring system, it is characterized in that, described monochromatic source be monochromatic filter plate to monochromatic light after white light filtering, described photosensitive device is photomultiplier.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510196507.3A CN104849215A (en) | 2015-04-23 | 2015-04-23 | Position triangular wave frequency coding plane array imaging light measurement system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510196507.3A CN104849215A (en) | 2015-04-23 | 2015-04-23 | Position triangular wave frequency coding plane array imaging light measurement system |
Publications (1)
Publication Number | Publication Date |
---|---|
CN104849215A true CN104849215A (en) | 2015-08-19 |
Family
ID=53849026
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201510196507.3A Pending CN104849215A (en) | 2015-04-23 | 2015-04-23 | Position triangular wave frequency coding plane array imaging light measurement system |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN104849215A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106506906A (en) * | 2016-10-20 | 2017-03-15 | 天津大学 | CCD camera raises predetermined level triangular wave frequency coded imaging systems |
CN106510624A (en) * | 2016-10-20 | 2017-03-22 | 天津大学 | Raised preset level triangular wave frequency encoded plane array photosensitive device imaging system |
CN106546534A (en) * | 2016-10-20 | 2017-03-29 | 天津大学 | Face battle array launching light raises the triangular wave frequency coded imaging systems of predetermined level |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101479594A (en) * | 2006-06-28 | 2009-07-08 | 华威大学 | Imaging apparatus and method |
CN201277947Y (en) * | 2008-10-29 | 2009-07-22 | 西安科技大学 | Spectrum absorption detection apparatus for coal mine methane gas concentration |
CN101636782A (en) * | 2007-03-22 | 2010-01-27 | 高通股份有限公司 | Method and device for generating triangular waves |
CN101832815A (en) * | 2010-04-30 | 2010-09-15 | 天津大学 | Multi-channel single photon counting measuring system based on digital lock phase de-multiplex |
CN102169012A (en) * | 2011-01-11 | 2011-08-31 | 中国科学院上海光学精密机械研究所 | Method for improving vibration measurement precision of semiconductor laser sine phase modulation interferometer |
CN102258365A (en) * | 2011-08-17 | 2011-11-30 | 天津大学 | Sine-wave modulation photo plethysmo graphy measuring device and method |
-
2015
- 2015-04-23 CN CN201510196507.3A patent/CN104849215A/en active Pending
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101479594A (en) * | 2006-06-28 | 2009-07-08 | 华威大学 | Imaging apparatus and method |
CN101636782A (en) * | 2007-03-22 | 2010-01-27 | 高通股份有限公司 | Method and device for generating triangular waves |
CN201277947Y (en) * | 2008-10-29 | 2009-07-22 | 西安科技大学 | Spectrum absorption detection apparatus for coal mine methane gas concentration |
CN101832815A (en) * | 2010-04-30 | 2010-09-15 | 天津大学 | Multi-channel single photon counting measuring system based on digital lock phase de-multiplex |
CN102169012A (en) * | 2011-01-11 | 2011-08-31 | 中国科学院上海光学精密机械研究所 | Method for improving vibration measurement precision of semiconductor laser sine phase modulation interferometer |
CN102258365A (en) * | 2011-08-17 | 2011-11-30 | 天津大学 | Sine-wave modulation photo plethysmo graphy measuring device and method |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106506906A (en) * | 2016-10-20 | 2017-03-15 | 天津大学 | CCD camera raises predetermined level triangular wave frequency coded imaging systems |
CN106510624A (en) * | 2016-10-20 | 2017-03-22 | 天津大学 | Raised preset level triangular wave frequency encoded plane array photosensitive device imaging system |
CN106546534A (en) * | 2016-10-20 | 2017-03-29 | 天津大学 | Face battle array launching light raises the triangular wave frequency coded imaging systems of predetermined level |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Cameron et al. | Bars in early-and late-type discs in COSMOS | |
CN103234735B (en) | Measure the apparatus and method of electro-optic intensity modulator chirp parameter frequency response characteristic | |
Morozov et al. | Ultrahigh-resolution optical vector analyzers | |
CN104792706A (en) | Image-forming light measurement system based on position triangular wave frequency coded excitation of area array CCD (charge coupled device) | |
CN104811617A (en) | Position triangular wave frequency encoded excitation imaging light measurement system of CCD camera | |
CN104849215A (en) | Position triangular wave frequency coding plane array imaging light measurement system | |
EP2857796A3 (en) | Methods and apparatus of tracking/locking resonator free spectral range and its application in resonator fiber optic gyroscope | |
Hong et al. | Photon-counting underwater optical wireless communication for reliable video transmission using joint source-channel coding based on distributed compressive sensing | |
CN105136672A (en) | Area array emission light position triangle wave frequency coding imaging light measuring system | |
US20200145111A1 (en) | Method and apparatus for tuning lookup table circuits in a transmitter of optical and electrical communication systems | |
Sticklus et al. | Experimental characterization of single-color power LEDs used as photodetectors | |
CN111175574B (en) | Measuring system and measuring method | |
Sandrolini et al. | Signal transformations for analysis of supraharmonic EMI caused by switched-mode power supplies | |
CN104865184A (en) | Position triangle wave frequency coding linear array imaging light measuring system | |
CN104819964A (en) | Position triangular wave frequency coding type imaging light measurement system | |
Umair et al. | Strong Noise Rejection in VLC Links under Realistic Conditions through a Real-Time SDR Front-End | |
CN105158211A (en) | Linear CCD position triangular wave frequency coded-excitation imaging light measurement system | |
CN104792712A (en) | Position triangle wave coding array type transmission light measurement system | |
CN1932442A (en) | Frequency divider adapted to optical fiber top | |
CN104783762A (en) | Imaging optical measurement device for position sine wave frequency coding | |
CN104814721A (en) | Triangular wave frequency coding high spectral imaging measurement system applied to mammary gland | |
Ricci et al. | FPGA-based pulse compressor for ultra low latency visible light communications | |
CN103471817A (en) | Rapid measurement device and method for multi-field space luminosity distribution | |
Zhou et al. | Design and Research of Laser Power Converter (LPC) for Passive Optical Fiber Audio Transmission System Terminal | |
CN104613988B (en) | A kind of sufficient center wavelength accuracy apparatus and method based on FBG optical fiber |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
EXSB | Decision made by sipo to initiate substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
RJ01 | Rejection of invention patent application after publication |
Application publication date: 20150819 |
|
RJ01 | Rejection of invention patent application after publication |