CN105784334A - Fiber laser beam quality measurement method base on photoelectric detector and CCD camera - Google Patents
Fiber laser beam quality measurement method base on photoelectric detector and CCD camera Download PDFInfo
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Abstract
The invention relates to a fiber laser beam quality measurement method base on a photoelectric detector and a CCD camera. The method comprises: an optical axis of a measured light beam is adjusted to be in a horizontal state, and a beam splitter is arranged at an optical path and thus the measured light beam is divided into two parts that are used for measuring a near field and a far field of the light beam. On the basis of measurement of the near field and the far field of the measured light beam as well as a related data analysis, a near field width and a far field width of the light beam are calculated, so that light beam quality M <2> x and light beam quality M <2>y at a corresponding direction are obtained by calculation. An M<2> factor expression based on near field and far field light intensity distribution of a beam is deduced in theory, so that a defect that the existing M<2> factor measuring instrument can not evaluate the large-size fiber laser beam quality easily can be overcome. The provided fiber laser beam quality measurement method is suitable for fiber laser beam quality measurement including a few of high order modes and some cut fiber laser beam quality measurement.
Description
Technical field
The present invention relates to the measuring method of a kind of optical-fiber laser beam quality, especially a kind of method measuring optical-fiber laser beam quality based on photodetector and CCD camera.
Background technology
Beam quality is highly important index in laser practical application, it is generally recognized that it is from the aspect of matter to evaluate laser beam characteristic.The method at present laser beam quality being evaluated is a lot, such as M2The factor, the β factor, Si Telieer ratio etc. [Feng Guoying, Zhou Shouhuan, " discussion of laser beam quality overall merit ", Chinese laser, 36,1643-1653(2009)].In the nineties in 20th century, A.E.Siegman proposition M2The factor evaluates beam quality.M2The factor is defined as the waist width of actual light beam and the product of its far-field divergence angle ratio with the corresponding product of ideal beam, also it is current scientific research personnel and most commonly used evaluation methodology [A.E.Siegman that high-capacity optical fiber laser production firm adopts for optical-fiber laser beam quality, " Newdevelopmentinlaserresonator ", Proc.ofSPIE, 1990,2:1224].M2Factor value, be more than or equal to 1, works as M2The factor is closer to 1, and research worker thinks that the optical field distribution of output beam is closer to Gauss basic mode light beam, and beam quality is more good.
To laser beam M2The method of factor measurement generally includes following three classes: line-of-sight course, two-point method and hyperbolic fitting method.Line-of-sight course is measured more convenient with two-point method, but precision is not high;Hyperbolic fitting method is carried out hyperbolic fit by then passing through measurement multiple spot (5 available points should be at least respectively measured in usual far field, near field), thus precision is higher, but implementation is complicated, generally need to by relevant precision instrument.To optical-fiber laser M2Factor measurement generally adopts the M that Ophir-Spiricon company of the U.S. produces2Factor measuring instrument, its fundamental method of measurement adopted is hyperbolic fitting method, higher [the PengfeiMa of precision, RumaoTao, XiaolinWang, etal, " Coherentpolarizationbeamcombinationoffourmode-lockedfibe rMOPAsinpicosecondregime ", Opt.Express, 2014,22 (4): 4123-4130].But this M2Factor measuring instrument immobilizes because of its CCD limited resolution and convertible lens focal length, causes its scope of application critical constraints, and for the measurement of fundamental-mode gaussian beam, it is generally only available for precise measuring bundle waist width light beam [" M less than 5mm2-200/200s-FWUsersGuide”,2009,Ophir-SpiriconInc.DocumentNo:11382].Therefore, a kind of new method that can be used for measuring the beam quality of large-scale optical fiber laser is found, it appears particularly important.
Summary of the invention
The technical problem to be solved in the present invention is: provide the measuring method of a kind of optical-fiber laser beam quality based on photodetector and CCD camera.The method measures M2Factor principle is correct, and operation is simple, it is not necessary to special precision instrument, and the method is applicable to the optical-fiber laser that waist width is bigger.The laser beam quality of large-sized optical-fiber laser is significant.
The technical scheme is that
M2The definition of the factor is:
(1)
In above formula, ω is the waist width of actual light beam, and θ is the far-field divergence angle of actual light beam, ω0、θ0The respectively waist width of ideal beam (taking fundamental-mode gaussian beam in Siegman theory is ideal beam) and far-field divergence angle, and meet:
(2)
Wherein λ is optical wavelength.Bring (2) formula into M2The definition of the factor can obtain:
(3)
(4)
ωx(θx)、ωy(θy) respectively actual light beam x, waist width (far-field divergence angle) on y direction.Therefore the M to light beam2The factor is measured and is just converted to the near field size (ω to light beamx、ωy) and far-field divergence angle (θx、θy) measurement.
In the spatial domain, the definition of width of light beam generally has three kinds, i.e. 1/n definition, encircled power and second-order moments.Encircled power and second-order moments mode are both needed to accurately obtain near-field beam hot spot full figure to be measured, and then draw near-field beam width by correlation computations.For obtaining light field whole audience information accurately, generally need to utilize the CCD that target surface is completely covered hot spot that the light intensity of tested light beam is measured, but CCD target surface size is generally only several millimeter, it is impossible to measure large scale hot spot.And with 1/n definition, the measurement of near field light beam width is only needed to measure and obtains the curve of light distribution through beam center largest light intensity point.1/n definition refers on curve of light distribution I (r), maximum ImaxThe half of place's distance between two points be defined as width of light beam, common n value has e2, e and 2 etc..For desirable fundamental-mode gaussian beam, 1/e2The width of light beam that definition calculates with 86.5% encircled power, second-order moments is completely the same, thus we select 1/e2Define and near field light beam width is measured, ω can be obtainedxAnd ωy。
Owing to tested light beam is generally collimated beam, collimator distance, generally at about hundred meters, is basically unchanged in collimator distance inner light beam size, therefore in laboratory, the measurement of the far field beam angle of divergence can not be passed through two-point method or line-of-sight course measurement draws.Condenser lens must be utilized, tested light beam is focused on lens focus position namely the desirable far field of tested light beam, by the measurement of far-field spot being drawn the width of light beam ω on x, y direction of far-field spotx-farAnd ωy-farHerein owing to utilizing CCD that far-field measurement can obtain the whole audience light distribution of focal beam spot, thus the width of light beam in far field is calculated the defined formula adopting second moment, as shown in (5), (6) two formulas, this definition make use of the whole audience intensity signal of light beam, calculates more accurate.
(5)
(6)
(7)
I in two formulas abovefar(x, y) far-field intensity distribution detected for CCD camera.Calculate far-field spot width of light beam ω on x, y directionx-farAnd ωy-farAfterwards, available following (8), (9) two formulas, the far-field divergence angle θ of light beam can be calculatedxAnd θy, in formula, f is the focal length of condenser lens.
(8)
(9)
(8), (9) two formulas are substituted into (3), (4) two formulas respectively, obtains the M of tested light beam2The factor is:
(10)
(11)
Utilize (5) ~ (7) and (10) ~ (11) formula can calculate the M of tested light beam2The factor, calculated M2The factor may be used for evaluating the beam quality of tested light beam.
Concrete technical scheme is as follows:
This method utilizes M2Large-scale optical fiber laser beam quality evaluated by factor measuring instrument, tested light beam first carries out beam quality measurement, builds optical path.First by the optical axis level-off of tested light beam 1, put into spectroscope 2 in the optical path, tested light beam is divided into reflection light beam 3 and transmitted light beam 4 two parts, is respectively used near field and the far field of measuring beam.
For the measurement of near-field beam, we utilize the photodetector 6 on the three-dimensional regulation platform 5 being positioned over micrometer caliper to measure.Photodetector 6 can convert the intensity signal detected to information of voltage, is shown in real time by oscillograph 7, and the response of the light of Same Wavelength is linear by photodetector 6, and therefore the magnitude of voltage of oscillograph 7 display can be equivalent to light intensity value.Concrete method of testing is as shown in Figure 2.By regulating with the micrometer caliper in the X-direction of the three-dimensional regulation platform 5 of micrometer caliper, photodetector can be positioned over tested light beam edge by the diverse location of the X-direction of beam center, and then the magnitude of voltage that the light intensity obtaining diverse location is corresponding can be measured.Take an interval and keep certain, take a number and ensure that minimum light intensity values is less than the 10% of largest light intensity value, to ensure the reliability that follow-up data processes.The magnitude of voltage that multimetering is obtained does Gaussian function fitting, draws near-field beam width ω according to fitting functionx.Measuring principle and the step of Y-direction are same as described above.
For the measurement of far field beam, we adopt condenser lens 8 as shown in Figure 1 that transmitted light beam 4 is focused on lens focus position, i.e. far field beam, and by CCD camera 9 to focal beam spot imaging, by computer 10, imaging facula are displayed and data acquisition.CCD camera 9 resolution is sufficiently high, and condenser lens 8 focal distance f answers long enough, with coordinating of focal length, resolution should ensure that far-field spot at least occupies 20 pixels.
By to tested near-field beam, the measurement in far field and Correlative data analysis, near-field beam width (ω can be calculatedxAnd ωy) and far field width (ωx-farAnd ωy-far), and then utilize formula (10) ~ (11) that the beam quality M in respective direction can be calculatedx 2And My 2。
Adopt the present invention can reach techniques below effect:
1. it is deduced the M in the near field based on light beam and far-field intensity distribution theoretically2Factor expression, solves M2Factor measuring instrument is difficult to evaluate the defect of large-scale optical fiber laser beam quality.
2. simply correct based on the optical-fiber laser beam quality measuring method principle of photodetector and CCD camera, and owing to measuring method being discrete photoelectric device, it is not necessary to other precision instruments, easy to operate, light path can easily be accommodated.
3. it is applicable to the optical-fiber laser beam quality containing a small amount of higher order mode based on the optical-fiber laser beam quality measuring method of photodetector and CCD camera measure.
4. it is applicable to, based on the optical-fiber laser beam quality measuring method of photodetector and CCD camera, the optical-fiber laser beam quality measurement that part is blocked.
Accompanying drawing explanation
Fig. 1 is the optical-fiber laser beam quality new method of measuring principle schematic based on photodetector and CCD camera,
The tested light beam of 1-;2 spectroscopes;3-reflects light beam;4-transmitted light beam;5-is with the three-dimensional regulation platform of micrometer caliper;6-photodetector;7-oscillograph;8-condenser lens;9-CCD camera;10-computer.
Fig. 2 is the near-field beam measuring principle schematic diagram based on photodetector,
Fig. 3 is the near field intensity distribution figure in the X-direction of tested light beam,
Fig. 4 is the near field intensity distribution figure in the Y-direction of tested light beam,
Fig. 5 is the tested far field beam surface of intensity distribution after lens focus,
Fig. 6 is for utilizing M2The beam quality result figure that-200s-FW measuring instrument is measured.
Detailed description of the invention
As shown in Figure 1, first by the optical axis level-off of tested light beam 1, put into spectroscope 2 in the optical path, tested light beam is divided into reflection light beam 3 and transmitted light beam 4 two parts, is respectively used near field and the far field of measuring beam.For the measurement of near-field beam, we utilize the photodetector 6 on the three-dimensional regulation platform 5 being positioned over micrometer caliper to measure.Photodetector 6 can convert the intensity signal detected to information of voltage, is shown in real time by oscillograph 7, and the magnitude of voltage of oscillograph 7 display can be equivalent to light intensity value.Concrete method of testing is as shown in Figure 2.By the micrometer caliper in the X-direction of adjustment 5, photodetector can be positioned over tested light beam edge by the diverse location of the X-direction of beam center, and then the magnitude of voltage that the light intensity obtaining diverse location is corresponding can be measured.The magnitude of voltage that multimetering is obtained does Gaussian function fitting, draws near-field beam width ω according to fitting functionx.Measuring principle and the step of Y-direction are same as described above.For the measurement of far field beam, we adopt condenser lens 8 as shown in Figure 1 that transmitted light beam 4 is focused on lens focus position, i.e. far field beam, and by CCD camera 9 to focal beam spot imaging, by computer 10, imaging facula are displayed and data acquisition.By to tested near-field beam, the measurement in far field and Correlative data analysis, near-field beam width (ω can be calculatedxAnd ωy) and far field width (ωx-farAnd ωy-far), and then utilize formula (10) ~ (11) that the beam quality M in respective direction can be calculatedx 2And My 2。
This laboratory has built experiment porch as shown in Figure 1 according to design above, measures near field and the far field of tested light beam.Near field light intensity values is accompanying drawing 3(X direction such as) and accompanying drawing 4(Y direction) shown in, data point is photodetector measured data value, and curve is Gauss curve fitting curve.X and light path in Y-direction test process have certain adjustment, thus X is different with Y-direction light intensity value, but unidirectional test carries out under identical conditions, therefore measurement data can reflect the light distribution of tested near-field beam.X and the Intensity of Gaussian fitting function respectively (12) of Y-direction, (13) formula.Utilize foregoing 1/e2Near field light beam width is calculated by definition, can obtain ωxAnd ωyRespectively 7.20mm and 7.16mm.
(12)
(13)
The measurement of far field beam is realized by condenser lens and CCD camera imaging.Condenser lens focal distance f is 1.04m, CCD target surface resolution is 4.4 μm/pixel.Far-field spot image is as shown in Figure 5.Utilize second-order moments far field beams width recited above, through can be calculated ωx-farAnd ωy-farRespectively 66.25 μm and 60.70 μm.And then by ωx/ωyAnd ωx-far/ωy-farBring formula (10)/(11) into, the beam quality M in respective direction can be calculatedx 2/My 2For 1.35/1.24.
In order to verify the result that above-mentioned beam quality measuring method calculates, we utilize the M of Ophir-Spiricon company2The beam quality of tested light beam has been measured by-200s-FW measuring instrument, measurement result as shown in Figure 6, Mx 2/My 2For 1.34/1.30.By contrasting it is found that the optical-fiber laser beam quality measuring method based on photodetector and CCD camera can realize optical-fiber laser beam quality is comparatively accurately measured.
Claims (3)
1., based on the optical-fiber laser beam quality measuring method of photodetector and CCD camera, utilize M2Large-scale optical fiber laser beam quality evaluated by factor measuring instrument, tested light beam is carried out beam quality measurement, build optical path, it is characterized in that, first by the optical axis level-off of tested light beam (1), put into spectroscope (2) in the optical path, tested light beam is divided into reflection light beam (3) and transmitted light beam (4) two parts, it is respectively used near field and the far field of measuring beam
For the measurement of near-field beam, utilize photodetector (6) measurement on the three-dimensional regulation platform (5) being positioned over micrometer caliper,
For the measurement of far field beam, adopt condenser lens (8) that transmitted light beam (4) is focused on lens focus position, i.e. far field beam, and by CCD camera (9) to focal beam spot imaging, by computer (10), imaging facula is displayed and data acquisition,
By to tested near-field beam, the measurement in far field and data analysis, namely calculating near-field beam width ωxAnd ωyWith far field width ωx-farAnd ωy-far, and then calculate the beam quality M in respective directionx 2And My 2。
null2. the optical-fiber laser beam quality measuring method based on photodetector and CCD camera according to claim 1,It is characterized in that,Described photodetector (6) converts the intensity signal detected to information of voltage,Shown in real time by oscillograph (7),The response of the light of Same Wavelength is linear by photodetector (6),Therefore the magnitude of voltage that oscillograph (7) shows is equivalent to light intensity value,By regulating with the micrometer caliper in the X-direction of the three-dimensional regulation platform (5) of micrometer caliper,Photodetector is positioned over tested light beam along by the diverse location of the X-direction of beam center,And then measure the magnitude of voltage that the light intensity obtaining diverse location is corresponding,Take an interval and keep fixing,Take a number and ensure that minimum light intensity values is less than the 10% of largest light intensity value,The magnitude of voltage that multimetering is obtained does Gaussian function fitting,Near-field beam width ω is drawn according to fitting functionx, the measuring process of Y-direction is identical with X-direction.
3. the optical-fiber laser beam quality measuring method based on photodetector and CCD camera according to claim 1, it is characterised in that M2The calculating process of the factor is as follows:
M2Factor definition is:
(1)
In above formula, ω is the waist width of actual light beam, and θ is the far-field divergence angle of actual light beam, ω0、θ0The respectively waist width of ideal beam and far-field divergence angle, and meet:
(2)
Wherein λ is optical wavelength, brings (2) formula into M2The definition of the factor can obtain:
(3)
(4)
ωx(θx)、ωy(θy) respectively actual light beam x, waist width on y direction, i.e. far-field divergence angle, the therefore M to light beam2The factor is measured and is just converted to the near field size (ω to light beamx、ωy) and far-field divergence angle (θx、θy) measurement,
Use 1/e2Define and near field light beam width is measured, namely obtain near field size ωxAnd ωy;
The width of light beam in far field is calculated the defined formula adopting second moment, as shown in (5), (6) two formulas,
(5)
(6)
(7)
I in formula abovefar(x, y) far-field intensity distribution detected for CCD camera calculate far-field spot width of light beam ω on x, y directionx-farAnd ωy-farAfterwards, utilize formula (8), (9), namely calculate the far-field divergence angle θ of light beamxAnd θy, in formula, f is the focal length of condenser lens,
(8)
(9)
(8), (9) two formulas are substituted into (3), (4) two formulas respectively, obtains the M of tested light beam2The factor is:
(10)
(11)
Utilize (5) ~ (7) and (10) ~ (11) formula can calculate the M of tested light beam2The factor.
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Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN2890864Y (en) * | 2006-01-18 | 2007-04-18 | 中国科学院上海光学精密机械研究所 | Laser Beam Quality Measuring Device |
CN2890863Y (en) * | 2005-09-28 | 2007-04-18 | 中国科学院上海光学精密机械研究所 | Laser beam mass M2Factor real-time detector |
JP2010115680A (en) * | 2008-11-12 | 2010-05-27 | Suzuki Motor Corp | Method and apparatus for determining quality of laser beam machining |
CN105222992A (en) * | 2015-09-17 | 2016-01-06 | 西安科技大学 | A kind of Laser Beam Quality Factor measuring method |
-
2016
- 2016-04-08 CN CN201610215402.2A patent/CN105784334B/en active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN2890863Y (en) * | 2005-09-28 | 2007-04-18 | 中国科学院上海光学精密机械研究所 | Laser beam mass M2Factor real-time detector |
CN2890864Y (en) * | 2006-01-18 | 2007-04-18 | 中国科学院上海光学精密机械研究所 | Laser Beam Quality Measuring Device |
JP2010115680A (en) * | 2008-11-12 | 2010-05-27 | Suzuki Motor Corp | Method and apparatus for determining quality of laser beam machining |
CN105222992A (en) * | 2015-09-17 | 2016-01-06 | 西安科技大学 | A kind of Laser Beam Quality Factor measuring method |
Non-Patent Citations (1)
Title |
---|
陈日升 等: "一台染料激光器光束质量因子M2 的测量", 《光学技术》 * |
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CN115683576B (en) * | 2022-12-28 | 2023-03-10 | 中国科学院长春光学精密机械与物理研究所 | Detection device and method of optical coupling device |
CN116067629A (en) * | 2023-03-07 | 2023-05-05 | 度亘核芯光电技术(苏州)有限公司 | Optical lens detection device |
CN116067629B (en) * | 2023-03-07 | 2023-08-22 | 度亘核芯光电技术(苏州)有限公司 | Optical lens detection device |
CN117974640A (en) * | 2024-03-28 | 2024-05-03 | 莱森光学(深圳)有限公司 | Method and system for testing quality far field of light beam |
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