CN1727979A - Method for measuring Brillonin frequency shift value and velocity of sound of medium to be tested through Brillonin system - Google Patents
Method for measuring Brillonin frequency shift value and velocity of sound of medium to be tested through Brillonin system Download PDFInfo
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- CN1727979A CN1727979A CN 200510010051 CN200510010051A CN1727979A CN 1727979 A CN1727979 A CN 1727979A CN 200510010051 CN200510010051 CN 200510010051 CN 200510010051 A CN200510010051 A CN 200510010051A CN 1727979 A CN1727979 A CN 1727979A
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- shift value
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Abstract
A method for testing out Brillouin frequency shift value and sound speed of media to be tested by using Brillouin system includes placing media to be tested in amplifier, placing mixed media formed by two type of medias in folding zone, regulating volume ratio of said two medias, selecting polarized light energy at light output end of light beam detection device to be maximum to obtain result of mixed media Brillouin frequency shift value being the same as Brillourin frequency shift value of media to be tested and calculating out sound speed of media to be tested .
Description
Technical field:
What the present invention relates to is the nonlinear optics field, specifically is a kind ofly to measure the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system.
Background technology:
Because stimulated Brillouin scattering (SBS) has the phase conjugation characteristic, can eliminate the phase distortion in the optical transmission process, improve beam quality.SBS phase conjugation theory and experiment thereof for many years obtained research widely.Experimental study shows that medium has very big influence to the stimulated Brillouin scattering characteristic, and medium SBS parameter is the important symbol of medium SBS characteristic, so the measurement of medium SBS parameter just seems and is even more important.Usually used Fabry-Perot interferometer (Fabry-Perot interferometer) to measure the medium Brillouin shift in the past, the Fabry-Perot interferometer has resolution and precision advantages of higher, but interferometer is subjected to the restriction of bandwidth, and promptly a kind of Fabry-Perot interferometer can only be measured the medium Brillouin shift value under the specific lambda1-wavelength situation.Therefore, if the medium Brillouin shift of wanting to measure under the different lambda1-wavelength situations just needs different Fabry-Perot interferometers, this just makes troubles to measurement, and has improved the measurement cost.
Summary of the invention:
The objective of the invention is to use a kind of Fabry-Perot interferometer can only measure the medium Brillouin shift value and the velocity of sound under the specific lambda1-wavelength situation in order to solve, and to measure the medium Brillouin shift value and the velocity of sound under the different lambda1-wavelength situations, the F-P interferometer that just needs many different wave lengths, this makes troubles to measurement, and improved the problem of measuring cost, and then provide a kind of and measured the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system.The system that the present invention uses is made up of laser instrument 1, polaroid 2, quarter wave plate 3, first convex lens 4, amplification pond 5, second convex lens 6, vibration pond 7, light beam detector 8; The step of the Brillouin shift value of testing medium and the measuring method of the velocity of sound is: put into testing medium 001 in amplifying pond 5; In vibration pond 7, put into and mix the adjustable blending agent of forming of Brillouin shift value by two media, the p polarized light of laser instrument 1 output is input to the input end of polaroid 2 after polaroid 2 transmission and output to the input end of quarter wave plate 3 from the output terminal of the sheet 2 that shakes, behind quarter wave plate 3 propagation and transformations, obtain circularly polarized light and be input in the input end of first convex lens 4 at the output terminal of quarter wave plate 3, circularly polarized light through the transmission of first convex lens 4 focus on the back the output terminal of first convex lens 4 obtain contracting Shu Zengqiang circularly polarized light and be input in the input end in amplification pond 5, the circularly polarized light of testing medium transmission outputs to the input end of second convex lens 6 from the output terminal that amplifies pond 5 in amplifying pond 5, output to the input end in vibration pond 7 through the circularly polarized light of second convex lens 6 transmission output terminal from second convex lens 6, the focus point L of second convex lens, 6 output terminals is in the blending agent in the vibration pond 7, circularly polarized light is Brillouin scattering takes place in the blending agent and to produce the Stokes seed light at the focus point L place of second convex lens, 6 output terminals, the Stokes seed light that produces is along the transmission of former road second convex lens 6, amplify the amplification transmission of testing medium in the pond 5, the transmission of first convex lens 4, the transmission of quarter wave plate 3 also obtains the s polarized light after quarter wave plate 3 conversion, the s polarized light is input on the polaroid 2 and is reflexed in the light input end of light beam detector 8 002 by it; Adjust the volume ratio of the two media in the blending agent in the vibration pond 7, select the maximum luminous energy reading value that shows on the light beam detector 8, the Brillouin shift value of the blending agent of this volume ratio is promptly identical with the Brillouin shift value of testing medium in the amplification pond 5, the Brillouin shift value of its testing medium, just the Brillouin shift value of blending agent is calculated by following formula:
V is the Brillouin shift value of the blending agent in the vibration pond 7, just the Brillouin shift value of testing medium in the above-mentioned formula; λ is a lambda1-wavelength, n
1And n
2Be respectively the refractive index of the two media in the blending agent; ρ
1And ρ
2Be respectively the density of the two media in the blending agent;
1And
2Be respectively the volume ratio of the two media in the blending agent,
1=V
1/ (V
1+ V
2),
2=V
2/ (V
1+ V
2), V wherein
1And V
2Be respectively the volume of the two media in the blending agent; υ
1And υ
2Be respectively the velocity of sound of the two media in the blending agent; L
1And L
2Be respectively the molecular free path of the two media in the blending agent; S
1And S
2Be respectively the internal surface area mark of the two media in the blending agent, S
1=x
1γ
1/ (x
1γ
1+ x
2γ
2), S
2=x
2γ
2/ (x
1γ
1+ x
2γ
2), x
1And x
2Be respectively the mole fraction of the two media in the blending agent, γ
1And γ
2Be respectively the internal surface area 003 of the two media in the blending agent; The velocity of sound of testing medium is calculated according to following formula:
V is the Brillouin shift value of testing medium in the above-mentioned formula, and λ is a lambda1-wavelength, and n is a medium refraction index 004.The present invention is as long as change different blending agents, just can measure whole Brillouin shift values and the velocity of sound of different testing mediums when different lambda1-wavelength, need not change system, also not be subjected to the restriction of lambda1-wavelength, the equipment of its use is single, and method is simple, accurate, cost is low.
Description of drawings:
Fig. 1 is the system architecture synoptic diagram that the present invention uses, and Fig. 2 is the Brillouin shift value of testing medium and the measuring method flow chart of steps of the velocity of sound.
Embodiment:
Embodiment one: in conjunction with Fig. 1, Fig. 2 present embodiment is described, the system that the present invention uses is made up of laser instrument 1, polaroid 2, quarter wave plate 3, first convex lens 4, amplification pond 5, second convex lens 6, vibration pond 7, light beam detector 8; The step of the Brillouin shift value of testing medium and the measuring method of the velocity of sound is: put into testing medium 001 in amplifying pond 5; In vibration pond 7, put into and mix the adjustable blending agent of forming of Brillouin shift value by two media, the p polarized light of laser instrument 1 output is input to the input end of polaroid 2 after polaroid 2 transmission and output to the input end of quarter wave plate 3 from the output terminal of polaroid 2, behind quarter wave plate 3 propagation and transformations, obtain circularly polarized light and be input in the input end of first convex lens 4 at the output terminal of quarter wave plate 3, circularly polarized light through the transmission of first convex lens 4 focus on the back the output terminal of first convex lens 4 obtain contracting Shu Zengqiang circularly polarized light and be input in the input end in amplification pond 5, the circularly polarized light of testing medium transmission outputs to the input end of second convex lens 6 from the output terminal that amplifies pond 5 in amplifying pond 5, output to the input end in vibration pond 7 through the circularly polarized light of second convex lens 6 transmission output terminal from second convex lens 6, the focus point L of second convex lens, 6 output terminals is in the blending agent in the vibration pond 7, circularly polarized light is Brillouin scattering takes place in the blending agent and to produce the Stokes seed light at the focus point L place of second convex lens, 6 output terminals, the Stokes seed light that produces is along the transmission of former road second convex lens 6, amplify the amplification transmission of testing medium in the pond 5, the transmission of first convex lens 4, the transmission of quarter wave plate 3 also obtains the s polarized light after quarter wave plate 3 conversion, the s polarized light is input on the polaroid 2 and is reflexed in the light input end of light beam detector 8 002 by it; Adjust the volume ratio of the two media in the blending agent in the vibration pond 7, select the maximum luminous energy reading value that shows on the light beam detector 8, the Brillouin shift value of the blending agent of this volume ratio is promptly identical with the Brillouin shift value of testing medium in the amplification pond 5, the Brillouin shift value of its testing medium, just the Brillouin shift value of blending agent is calculated by following formula:
V is the Brillouin shift value of the blending agent in the vibration pond 7, just the Brillouin shift value of testing medium in the above-mentioned formula; λ is a lambda1-wavelength, n
1And n
2Be respectively the refractive index of the two media in the blending agent; ρ
1And ρ
2Be respectively the density of the two media in the blending agent;
1And
2Be respectively the volume ratio of the two media in the blending agent,
1=V
1/ (V
1+ V
2),
2=V
2/ (V
1+ V
2), V wherein
1And V
2Be respectively the volume of the two media in the blending agent; υ
1And υ
2Be respectively the velocity of sound of the two media in the blending agent; L
1And L
2Be respectively the molecular free path of the two media in the blending agent; S
1And S
2Be respectively the internal surface area mark of the two media in the blending agent, S
1=x
1γ
1/ (x
1γ
1+ x
2γ
2), S
2=x
2γ
2/ (x
1γ
1+ x
2γ
2), x
1And x
2Be respectively the mole fraction of the two media in the blending agent, γ
1And γ
2Be respectively the internal surface area 003 of the two media in the blending agent; The velocity of sound of testing medium is calculated according to following formula:
V is the Brillouin shift value of testing medium in the above-mentioned formula, and λ is a lambda1-wavelength, and n is a medium refraction index 004.The model that light beam detector 8 is selected for use is the ED200 energy meter; Two media in the described blending agent can be selected benzene, CCl respectively for use
4Two media; Testing medium is a cyclohexane in the example test.
Embodiment two: in the step 003 in embodiment one, during the maximum luminous energy reading value that on judging light beam detector 8, shows, make the percent by volume from 1% to 99% of a kind of medium in the blending agent and change, the percent by volume of another kind of medium changes from 99% to 1% accordingly, and finds the maximum luminous energy reading value that shows on the light beam detector 8.
Embodiment three: when measuring the Brillouin shift value of testing medium, occur temperature error for preventing system described in the embodiment one, in the present embodiment amplification pond 5, vibration pond 7 are arranged in the high-precision thermostat bath.Other composition is identical with embodiment one with method step.The model that high-precision thermostat bath is selected for use is CH1015.
Embodiment four: the difference of present embodiment and embodiment three is, velocity of sound temperature coefficient, the Brillouin shift value that thermal refractive index coefficient is proofreaied and correct its blending agent, i.e. the Brillouin shift value of testing medium with the blending agent in the vibration pond 7.Other composition is identical with embodiment one with method step.
Claims (4)
1, measure the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system, native system is made up of laser instrument (1), polaroid (2), quarter wave plate (3), first convex lens (4), amplification pond (5), second convex lens (6), vibration pond (7), light beam detector (8); The step that it is characterized in that the measuring method of the Brillouin shift value of testing medium and the velocity of sound is: put into testing medium (001) in amplifying pond (5); In vibration pond (7), put into and mix the adjustable blending agent of forming of Brillouin shift value by two media, the p polarized light of laser instrument (1) output is input to the input end of polaroid (2) after polaroid (2) transmission and output to the input end of quarter wave plate (3) from the output terminal of polaroid (2), behind quarter wave plate (3) propagation and transformation, obtain circularly polarized light and be input in the input end of first convex lens (4) at the output terminal of quarter wave plate (3), circularly polarized light through first convex lens (4) transmission focus on the back the output terminal of first convex lens (4) obtain contracting Shu Zengqiang circularly polarized light and be input in the input end in amplification pond (5), the circularly polarized light of testing medium transmission outputs to the input end of second convex lens (6) from the output terminal that amplifies pond (5) in amplifying pond (5), output to the input end in vibration pond (7) through the circularly polarized light of second convex lens (6) transmission output terminal from second convex lens (6), the focus point (L) of second convex lens (6) output terminal is in the interior blending agent in vibration pond (7), it is Brillouin scattering takes place in the blending agent and to produce the Stokes seed light that circularly polarized light is located at the focus point (L) of second convex lens (6) output terminal, the Stokes seed light that produces is along the transmission of former road second convex lens (6), amplify the amplification transmission of testing medium in the pond (5), the transmission of first convex lens (4), the transmission of quarter wave plate (3) also obtains the s polarized light after quarter wave plate (3) conversion, the s polarized light is input to that polaroid (2) is gone up and is reflexed in the light input end of light beam detector (8) (002) by it; Adjust the volume ratio of the two media in the blending agent in the vibration pond (7), select light beam detector (8) and go up the maximum luminous energy reading value that shows, the Brillouin shift value of the blending agent of this volume ratio is promptly identical with the Brillouin shift value of amplifying the middle testing medium in pond (5), the Brillouin shift value of its testing medium, just the Brillouin shift value of blending agent is calculated by following formula:
V is the Brillouin shift value of the blending agent in the vibration pond (7), just the Brillouin shift value of testing medium in the above-mentioned formula; λ is a lambda1-wavelength, n
1And n
2Be respectively the refractive index of the two media in the blending agent; ρ
1And ρ
2Be respectively the density of the two media in the blending agent;
1And
2Be respectively the volume ratio of the two media in the blending agent,
1=V
1/ (V
1+ V
2),
2=V
2/ (V
1+ V
2), V wherein
1And V
2Be respectively the volume of the two media in the blending agent; υ
1And υ
2Be respectively the velocity of sound of the two media in the blending agent; L
1And L
2Be respectively the molecular free path of the two media in the blending agent; S
1And S
2Be respectively the internal surface area mark of the two media in the blending agent, S
1=x
1γ
1/ (x
1γ
1+ x
2γ
2), S
2=x
2γ
2/ (x
1γ
1+ x
2γ
2), x
1And x
2Be respectively the mole fraction of the two media in the blending agent, γ
1And γ
2Be respectively the internal surface area (003) of the two media in the blending agent; The velocity of sound of testing medium is calculated according to following formula:
V is the Brillouin shift value of testing medium in the above-mentioned formula, and λ is a lambda1-wavelength, and n is medium refraction index (004).
2, according to claim 1ly measure the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system, it is characterized in that in the step (003), when judging that light beam detector (8) is gone up the maximum luminous energy reading value that shows, make the percent by volume from 1% to 99% of a kind of medium in the blending agent and change, the percent by volume of another kind of medium changes from 99% to 1% accordingly, and finds the maximum luminous energy reading value that shows on the light beam detector (8).
3, according to claim 1ly measure the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system, it is characterized in that amplify a pond (5), vibration pond (7) is arranged in the high-precision thermostat bath.
4, according to claim 1ly measure the Brillouin shift value of testing medium and the method for the velocity of sound with the Brillouin system, it is characterized in that velocity of sound temperature coefficient, the Brillouin shift value that thermal refractive index coefficient is proofreaied and correct its blending agent, i.e. the Brillouin shift value of testing medium with the blending agent in the vibration pond (7).
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| CNB2005100100513A CN100349058C (en) | 2005-05-31 | 2005-05-31 | Method for measuring Brillonin frequency shift value and velocity of sound of medium to be tested through Brillonin system |
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|---|---|---|---|
| CNB2005100100513A CN100349058C (en) | 2005-05-31 | 2005-05-31 | Method for measuring Brillonin frequency shift value and velocity of sound of medium to be tested through Brillonin system |
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| CN1727979A true CN1727979A (en) | 2006-02-01 |
| CN100349058C CN100349058C (en) | 2007-11-14 |
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN100409096C (en) * | 2006-06-21 | 2008-08-06 | 哈尔滨工业大学 | Method for measuring Brillouin frequency-shift and line-width based on double-tank system and mixed medium |
| CN102012515A (en) * | 2010-11-10 | 2011-04-13 | 南昌航空大学 | Method and device for detecting solid target in atmosphere through Brillouin scattering |
| CN102809437A (en) * | 2012-08-31 | 2012-12-05 | 哈尔滨工业大学 | Device for measuring medium brillouin gain linetype and line width and a method for measuring medium brillouin gain linetype and line width based on device |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2004125520A (en) * | 2002-09-30 | 2004-04-22 | Ando Electric Co Ltd | Apparatus and method for measuring characteristics of optical fiber |
| CN1328624C (en) * | 2004-09-29 | 2007-07-25 | 哈尔滨工业大学 | Method of different medium of mixed medium selected by double-pond excited Brillouin scattering system |
-
2005
- 2005-05-31 CN CNB2005100100513A patent/CN100349058C/en not_active Expired - Fee Related
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN100409096C (en) * | 2006-06-21 | 2008-08-06 | 哈尔滨工业大学 | Method for measuring Brillouin frequency-shift and line-width based on double-tank system and mixed medium |
| CN102012515A (en) * | 2010-11-10 | 2011-04-13 | 南昌航空大学 | Method and device for detecting solid target in atmosphere through Brillouin scattering |
| CN102012515B (en) * | 2010-11-10 | 2012-10-24 | 南昌航空大学 | Method and device for detecting solid target in atmosphere through Brillouin scattering |
| CN102809437A (en) * | 2012-08-31 | 2012-12-05 | 哈尔滨工业大学 | Device for measuring medium brillouin gain linetype and line width and a method for measuring medium brillouin gain linetype and line width based on device |
| CN102809437B (en) * | 2012-08-31 | 2014-06-04 | 哈尔滨工业大学 | Device for measuring medium brillouin gain linetype and line width and a method for measuring medium brillouin gain linetype and line width based on device |
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| CN100349058C (en) | 2007-11-14 |
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