CN202869949U - Optical system for enhancing optical excitation wave signal based on energy recovery principle - Google Patents
Optical system for enhancing optical excitation wave signal based on energy recovery principle Download PDFInfo
- Publication number
- CN202869949U CN202869949U CN 201220428515 CN201220428515U CN202869949U CN 202869949 U CN202869949 U CN 202869949U CN 201220428515 CN201220428515 CN 201220428515 CN 201220428515 U CN201220428515 U CN 201220428515U CN 202869949 U CN202869949 U CN 202869949U
- Authority
- CN
- China
- Prior art keywords
- pump light
- light
- pump
- sample
- optical system
- 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.)
- Withdrawn - After Issue
Links
Images
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The utility model discloses an optical system for enhancing an optical excitation wave signal based on the energy recovery principle. The optical system comprises a pump light outgoing part and a pump light reflection part, wherein the pump light outgoing part comprises a pump light source, a pump light polarization device, a polarizing beam splitting device and a pump light focusing lens, and the pump light reflection part comprises a pump light regulation lens, a quarter-wave plate, a first pump light reflector mirror and a second pump light reflector mirror. The optical system can greatly reduce the cost, the volume and the weight of the related detection and analysis instruments and imaging systems, and also can greatly improve the detection sensitivity of a related system under the condition of remaining the requirement on the power or the energy level of the pump light source unchanged.
Description
Technical field
The utility model relates to generation and the detection field of optical excitation ripple, is specially a kind of optical system that reclaims the enhancing optical excitation ripple signal of principle based on energy.
Background technology
Beam irradiation by interaction between light and matter, can excite to produce various effects to sample, comprises optical excitation heat wave, optical excitation sound wave, photoluminescence etc.Can obtain a lot of information about sample by the determination and analysis to these optical excitation wave effects, thereby derive various rigorous analysis testing tool and imaging devices based on the optical excitation ripple, be widely used in the every field such as new material, new forms of energy, electronic information, environmental science, biologic medical, advanced manufacturing industry.
Being used in actual applications the light beam of irradiation sample is commonly referred to as pump beam, and it can be ordinary beam of light, also can be laser beam.According to the difference of concrete applicable cases, pump beam can be simple continuous light, amplitude-modulated continuous light or pulsed light.When pump beam is amplitude-modulated continuous light or pulsed light, owing to can utilize phase-locked detection technique or Synchronous Detection, all kinds of rigorous analysis testing tools and imaging device based on the optical excitation wave effect have higher sensitivity and larger dynamic range usually, thereby use very extensive.
In all kinds of determination and analysis technology based on the optical excitation wave effect, the signal intensity of optical excitation wave effect generally all strengthens along with the enhancing of pump beam energy or power, therefore much need to carry out higher sensitivity detection and the occasion of analyzing, pump light source is all selected the higher LASER Light Source of power (perhaps single pulse energy).Owing to the volume of LASER Light Source, weight, cost usually all along with the raising of power (perhaps single pulse energy) improves, just have very important significance if therefore can in the situation that does not increase pump light source power (perhaps single pulse energy), strengthen optical excitation ripple signal.
Existing technology generally designs to improve optical excitation ripple signal intensity, the concrete Detection Techniques of optical excitation ripple signal are improved to strengthen sensitivity and improved signal to noise ratio (S/N ratio) etc. aspect electronic circuit and the signal processing nothing more than the pump light light path is optimized in the work aspect the enhancing optical excitation ripple signal.Take photoacoustic technique as example, a lot of effort all are on the optimal design that is placed on photoacoustic cell; Take photothermal technique as example, main effort all is to be placed in the design of the selection of the optimal design to the pump light light path, concrete detection method and detection light path and electronic circuit.
The utility model content
The utility model purpose provides and a kind ofly reclaims the optical system of the enhancing optical excitation ripple signal of principle based on energy, the problem of pumping light power or energy level being had relatively high expectations to solve all kinds of detection analytical instrument based on the optical excitation ripple and imaging device.
In order to achieve the above object, the technical scheme that adopts of the utility model is:
A kind of optical system that reclaims the enhancing optical excitation ripple signal of principle based on energy, it is characterized in that: comprise pump light emission parts, pump light reflecting part, the pump light that described pump light emission parts comprises pump light source, be successively set on the pump light source emitting light path plays deflection device, plays the light splitting device that the pump light after deflection device rises partially sees through for pump light, and the pump light condenser lens, described pump light condenser lens is arranged on the light splitting device transmitted light path and aims at sample; Described pump light reflecting part comprises the pump light adjustment lens of the pump beam that receives sample reflection or transmission, be successively set on quarter-wave plate, the first pump light high reflective mirror on the pump light adjustment transmission light transmitted by lens road, and be arranged on the second pump light high reflective mirror on the light splitting device reflected light path in the pump light emission parts.
Describedly a kind ofly reclaim the optical system of the enhancing optical excitation ripple signal of principle based on energy, it is characterized in that: be coated with anti-reflection film on the described quarter-wave plate.
The utility model can reduce by a relatively large margin the requirement to power or the energy level of pump light source, thereby reduce by a relatively large margin cost, the volume and weight of coherent detection analytical instrument and imaging system in the constant situation of sensitivity keeping.To the fainter sample of some optical excitation ripple signals, the detection sensitivity that also can require to improve by a relatively large margin in the constant situation related system at the power or the energy level that keep pump light source.
Description of drawings
Fig. 1 is the schematic diagram of the utility model when being applied to the high-transmission rate sample.
Fig. 2 is the schematic diagram of the utility model when being applied to the high reflectance sample.
Fig. 3 is the example structure figure of the utility model when being applied to the high-transmission rate sample.
Fig. 4 is the example structure figure of the utility model when being applied to the high reflectance sample.
Embodiment
Principle of the present utility model is as follows:
As shown in Figure 1, for the sample of high-transmission rate, from the linearly polarized light of pump light light source, suppose it is the S polarisation, (supposing that polarization spectroscope is T to the transmitance of S polarisation through polarization spectroscope for the first time
s, be R to the reflectivity of P polarized light
p) all see through, incide on the sample.Pump beam through the sample outgoing is being supposed that by high reflectivity mirror 1(its reflectivity is R through behind the quarter wave plate
1) reflect, through inciding on the sample for the second time behind the quarter wave plate, this moment, 90 degree variations occured in the polarization direction of pump beam, had become the P polarized light again.Incide for the second time pump light on the sample and incide on the polarization spectroscope for the second time after the sample outgoing and be polarized the spectroscope reflection, reflected light is supposed that by high reflectivity mirror 2(its reflectivity is R
2) reflect, again be polarized and incide on the sample for the third time after spectroscope reflects.Pump beam through the sample outgoing is reflected by high reflectivity mirror 1 through behind the quarter wave plate again, and through inciding on the sample for the 4th time behind the quarter wave plate, the polarization direction of pump beam 90 degree occured again changed this moment, had been converted back into the S polarized light.Inciding pump light on the sample for the 4th time incides polarization spectroscope and all sees through effusion pump energy recycling system for the 4th time after the sample outgoing.
Through after such optical system, the pump energy of irradiation sample has totally been reused four times.If the quarter wave plate front and rear surfaces all is coated with anti-reflection film, its transmitance is approximately 100%, and then the pumping light power P of accumulative total can use following equation expression in sample:
P=P
oT
s+P
oT
sTR
1+P
oT
sTR
1TR
pR
2R
p+P
oT
sTR
1TR
pR
2R
pTR
1 （1）
P in the formula (1)
oThat pump light is at the incident power that enters polarization spectroscope for the first time, T
sThat polarization spectroscope is to the transmitance of S polarisation, R
pPolarization spectroscope is to the reflectivity to the P polarized light, R
1, R
2Be respectively the reflectivity of high reflectivity mirror 1 and high reflectivity mirror 2, T is the transmitance of sample.
Table 1 is for pumping light power P and the P of different sample transmitance situations to accumulative total in the sample in the formula (1)
oRatio done simple computation, suppose R in the calculating
1=R
2=99.95%, T
s=99.6%, R
p=99.6%, all be more feasible numerical value in the practice.
Relation between table 1. pump energy recovering effect and the sample transmissivity
| T | P/Po |
| 90.00% | 341.11% |
| 91.00% | 346.32% |
| 92.00% | 351.60% |
| 93.00% | 356.96% |
| 94.00% | 362.39% |
| 95.00% | 367.89% |
| 96.00% | 373.47% |
| 97.00% | 379.13% |
| 98.00% | 384.87% |
| 99.00% | 390.68% |
| 99.95% | 396.28% |
Can be found out that by above calculating and analysis the utility model can make pumping light power strengthen more than 3 times even near 4 times in the measured point to the sample with good transmissivity with comparalive ease.
As shown in Figure 2, for the sample of high reflectance, suppose that the sample reflectivity is R among the figure, then the pumping light power P in sample surface accumulative total can use following equation expression:
P=P
oT
s+P
oT
sRR
1+P
oT
sRR
1RR
pR
2R
p+P
oT
sRR
1RR
pR
2R
pRR
1 （2）
Formula (2) and formula (1) all fours: replace sample transmissivity T at formula (1) with sample reflectivity R, formula (1) has just become formula (2).
Utilize formula (2) to calculate and analyze equally and can find out, the utility model also can make pumping light power strengthen more than 3 times even near 4 times in the measured point to the sample with good reflection rate with comparalive ease.
Specific embodiment 1:
As shown in Figure 3.The utility model comprises pump light source 1, pump light plays deflection device 2, light splitting device 3, pump light condenser lens 4, pump light adjustment lens 5, quarter-wave plate 6, the first pump light high reflective mirror 7, the second pump light high reflective mirror 8, probe source 9, surveys light condenser lens 10, detection light adjustment lens 11, spatial filter 12, surveys light filtering apparatus 13 and detection light detection device 14, and sample 15 is placed on pump light condenser lens 4 and pump light is adjusted between the lens 5.
The pump beam that is sent by pump light source 1 is linearly polarized light after having passed through deflection device 2, and the polarization direction is set to be in transmissive state for light splitting device 3; Converge to zone to be measured on the sample 13 by the pump beam of light splitting device 3 transmissions by pump light condenser lens 4; After the pump beam of process sample 15 is adjusted lens 5, quarter-wave plate 6 through pump light for the first time, by returning along original optical path after 7 reflections of the first pump light high reflective mirror, and again adjust lens 5 through quarter-wave plate 6 and pump light, and adjust lens 5 by pump light and converge on the sample 15, the irradiation area with for the first time through sample 15 time overlaps; Being set to of quarter-wave plate 6: for the second time rotated 90 degree through the polarization direction of the pump light of quarter-wave plate with respect to the polarization direction through the pump light before the quarter-wave plate for the first time;
For the second time behind the pump beam process pump light condenser lens 4 through sample, again via after light splitting device 3 reflections, incide on the second pump light high reflective mirror 8, again by returning along original optical path after 8 reflections of the second pump light high reflective mirror, and again via after light splitting device 3 reflections, assembled by pump light condenser lens 4, shine for the third time on the sample 15, and overlap with front twice irradiation area; After the pump beam of process sample 15 is adjusted lens 5, quarter-wave plate 6 through pump light again, by returning along original optical path after 7 reflections of the first pump light high reflective mirror, and again adjust lens 5 through quarter-wave plate 6 and pump light, and adjust lens 5 by pump light and assemble, shine on the sample 15 for the 4th time, overlap with the irradiation area of first three time; Because quarter-wave plate, the polarization direction of the pump light of the 4th irradiation sample with shine for the first time sample before consistent, therefore, after the pump light of the 4th process sample passes through pump light condenser lens 4 again, export via light splitting device 3 transmissions.
Send detecting light beam by probe source 9 and assemble, shine on the sample 15 by surveying light condenser lens 10, overlap with the irradiation area of pump light on sample; The detecting light beam of process sample through after surveying light adjustment lens 11, spatial filter 12, filtering apparatus 13, enters and surveys light detection device 14 again.The effect of spatial filter 12 be make survey the light part by after enter and survey light detection device 14, the effect of filtering apparatus 13 is other parasitic lights that filter except detection light.Because the interaction of pump light and sample, change has occured in the irradiation area properties of materials on the sample, such as refractive index etc.Because these change, the propagation characteristic of the detection light of process irradiation area can change, as produces newly-increased convergence or the effect of dispersing.Because corresponding variation can occur through entering the detection luminous energy of surveying light detection device 14 behind the spatial filter 12 in this newly-increased convergence or effect weakening, by the measurement that changes surveying luminous energy, just can obtain accordingly the information that material behavior changes.
Because the same area that pump light successively shines on the sample for four times, the synergistic effect of these four times irradiations is so that the detectable signal that optical excitation produces has had the increase of corresponding multiple than under the identical energy during single fraction irradiation; This is equivalent in the situation that does not increase pump energy, raising by a relatively large margin signal intensity, for efficient and accuracy that improve to survey important meaning is arranged.
Specific embodiment 2:
As shown in Figure 4.The utility model comprises pump light source 1, pump light plays deflection device 2, the first light splitting device 3, pump light condenser lens 4, pump light adjustment lens 5, quarter-wave plate 6, the first pump light high reflective mirror 7, the second pump light high reflective mirror 8, probe source 9, light splitting device 2 16, quarter-wave plate 2 17, surveys light condenser lens 10, detection light adjustment lens 11, spatial filter 12, surveys light filtering apparatus 13 and detection light detection device 14.
Pump light irradiation process in the specific embodiment 2 and energy removal process and specific embodiment 1 are basic identical, and just pump light is repeatedly to be reflected by sample surfaces, rather than picture is implemented in the allusion quotation example one repeatedly by the sample transmission.
Send detecting light beam by light splitting device 2 16 transmissions, through behind the quarter-wave plate 2 17 by probe source 9, assemble by surveying light condenser lens 10, shine on the surface of sample 15, overlap with the irradiation area of pump light on sample; Detecting light beam through the sample surfaces reflection returns along original optical path, again through surveying light condenser lens 10, quarter-wave plate 2 17, at this moment, 90 degree of having surveyed light polarization direction deflection, again by light splitting device 2 16 reflections, by after 11 collections of detection light adjustment lens, through behind spatial filter 12, the filtering apparatus 13, enter detection light detection device 14.Because the interaction of pump light and sample, change has occured in the irradiation area properties of materials on the sample, such as refractive index etc.Because these change, the propagation characteristic of the detection light of process irradiation area can change, as produces newly-increased convergence or the effect of dispersing.Because corresponding variation can occur through entering the detection luminous energy of surveying light detection device 14 behind the spatial filter 12 in this newly-increased convergence or effect weakening, by the measurement that changes surveying luminous energy, just can obtain accordingly the information that material behavior changes.
Claims (2)
1. optical system that reclaims the enhancing optical excitation ripple signal of principle based on energy, it is characterized in that: comprise pump light emission parts, pump light reflecting part, the pump light that described pump light emission parts comprises pump light source, be successively set on the pump light source emitting light path plays deflection device, plays the light splitting device that the pump light after deflection device rises partially sees through for pump light, and the pump light condenser lens, described pump light condenser lens is arranged on the light splitting device transmitted light path and aims at sample; Described pump light reflecting part comprises the pump light adjustment lens of the pump beam that receives sample reflection or transmission, be successively set on quarter-wave plate, the first pump light high reflective mirror on the pump light adjustment transmission light transmitted by lens road, and be arranged on the second pump light high reflective mirror on the light splitting device reflected light path in the pump light emission parts.
2. according to claim 1ly a kind ofly reclaim the optical system of the enhancing optical excitation ripple signal of principle based on energy, it is characterized in that: be coated with anti-reflection film on the described quarter-wave plate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN 201220428515 CN202869949U (en) | 2012-08-27 | 2012-08-27 | Optical system for enhancing optical excitation wave signal based on energy recovery principle |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN 201220428515 CN202869949U (en) | 2012-08-27 | 2012-08-27 | Optical system for enhancing optical excitation wave signal based on energy recovery principle |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN202869949U true CN202869949U (en) | 2013-04-10 |
Family
ID=48036658
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN 201220428515 Withdrawn - After Issue CN202869949U (en) | 2012-08-27 | 2012-08-27 | Optical system for enhancing optical excitation wave signal based on energy recovery principle |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN202869949U (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102854134A (en) * | 2012-08-27 | 2013-01-02 | 合肥知常光电科技有限公司 | Energy recovery principle based optical system for enhancing optical excitation wave signal |
| CN104184025A (en) * | 2013-05-23 | 2014-12-03 | 福州高意通讯有限公司 | Multi-pumping fiber laser structure |
| CN115047383A (en) * | 2022-08-15 | 2022-09-13 | 之江实验室 | Reflection-type SERF atomic magnetometer and integrated gauge head device thereof |
-
2012
- 2012-08-27 CN CN 201220428515 patent/CN202869949U/en not_active Withdrawn - After Issue
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102854134A (en) * | 2012-08-27 | 2013-01-02 | 合肥知常光电科技有限公司 | Energy recovery principle based optical system for enhancing optical excitation wave signal |
| CN102854134B (en) * | 2012-08-27 | 2015-12-02 | 合肥利弗莫尔仪器科技有限公司 | A kind of optical system of the enhancing optical excitation ripple signal based on energy recovery principle |
| CN104184025A (en) * | 2013-05-23 | 2014-12-03 | 福州高意通讯有限公司 | Multi-pumping fiber laser structure |
| CN115047383A (en) * | 2022-08-15 | 2022-09-13 | 之江实验室 | Reflection-type SERF atomic magnetometer and integrated gauge head device thereof |
| CN115047383B (en) * | 2022-08-15 | 2022-11-15 | 之江实验室 | Reflection-type SERF atomic magnetometer and integrated gauge head device thereof |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN102169050B (en) | Method for comprehensively measuring reflectivity | |
| CN100526856C (en) | Page quantitative determination device and methods based on terahertz time-domain spectroscopic technology | |
| CN101726362B (en) | Terahertz polarization analyzer and terahertz polarization measurement method | |
| CN100565099C (en) | Be used for improving the method and apparatus of the signal to noise ratio (S/N ratio) of optoacoustic film thickness measuring system | |
| US20220252497A1 (en) | Method and system for measuring refractive index of particle sample by using polarization difference of scattered light distribution | |
| CN101846506B (en) | Roll angle measurement method based on common path parallel beams | |
| CN101699265A (en) | Device and method for measuring scattering particles by using dynamic polarized light | |
| CN202869949U (en) | Optical system for enhancing optical excitation wave signal based on energy recovery principle | |
| CN103364090B (en) | Measure the device and method that ultra-short pulse laser propagates phase velocity in media as well | |
| JP2012141311A (en) | Apparatus for measuring transmissivity of patterned glass substrate | |
| CN101832910B (en) | Reverse collinear transient heat reflection measurement system | |
| CN102854134A (en) | Energy recovery principle based optical system for enhancing optical excitation wave signal | |
| CN115494479A (en) | Single photon radar system based on pulse sequence extraction and 3D imaging method | |
| CN1786659A (en) | Method and apparatus for enhancing measuring sensitivity of rotating corner | |
| CN102636337A (en) | Method for measuring optical fiber dispersion | |
| CN108489607A (en) | Water body optical attenuation coefficient measuring device and method | |
| CN108088815A (en) | Highly sensitive multiple beam refractive index detection device and method based on graphene surface ripple | |
| CN102944537B (en) | A kind of detection system based on SPR and detection method thereof | |
| CN104330053A (en) | Micro angle measurement method and device | |
| CN103454074A (en) | Method for measuring reflectivity of small-bore-diameter high-reflectivity mirror | |
| CN109407365B (en) | Device and method for measuring diffraction efficiency of liquid crystal grating device under laser action | |
| CN103471815A (en) | Method for simultaneously measuring S-polarized light reflectivity and P-polarized light reflectivity of high reflecting mirror | |
| CN204028004U (en) | A kind of substance detecting apparatus based on Raman filtering | |
| CN106342212B (en) | High reflection mirror laser back scattering measurement mechanism | |
| CN100340869C (en) | Electro-optic double modulation polarized light laser distance measuring method and its device |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| AV01 | Patent right actively abandoned |
Granted publication date: 20130410 Effective date of abandoning: 20151202 |
|
| C25 | Abandonment of patent right or utility model to avoid double patenting |