CN101950915A - Resonant cavity capable of obtaining hollow laser beams - Google Patents
Resonant cavity capable of obtaining hollow laser beams Download PDFInfo
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- CN101950915A CN101950915A CN 201010274086 CN201010274086A CN101950915A CN 101950915 A CN101950915 A CN 101950915A CN 201010274086 CN201010274086 CN 201010274086 CN 201010274086 A CN201010274086 A CN 201010274086A CN 101950915 A CN101950915 A CN 101950915A
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- resonant cavity
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Abstract
The invention relates to a resonant cavity capable of obtaining hollow laser beams, which can directly output hollow conical laser beams, belonging to the field of laser technology. The current technology for obtaining the hollow laser beams uses an optical device outside the resonant cavity for reshaping the laser beams emitted by the resonant cavity to obtain the hollow laser beams, and the scheme not only has a complex structure, but also has large energy loss. The resonant cavity capable of obtaining the hollow laser beams of the invention comprises a reflector, a laser gain medium and an output coupling mirror, wherein the material of the output coupling mirror is biaxial crystal, and one optical axis of the biaxial crystal is parallel to the axial line of the resonant cavity.
Description
Technical field
The present invention relates to a kind of resonant cavity that can obtain hollow laser beam, can directly export open circles taper laser beam, belong to laser technology field.
Background technology
Along with the development of laser technology, hollow laser beam not only is used widely at aspects such as biology, laser processing and atom coolings, and can be applied to fields such as scanning imagery, remote sensing guidance, range finding.The existing technology that obtains hollow laser beam all is by an outer laser beam reshaping that Optical devices send resonant cavity of resonant cavity, obtain to form hollow laser beam, this class scheme is complex structure not only, and energy loss is also very big, also causes the degree of coherence of laser beam to reduce in addition.
In the optical crystal material field, biaxial crystal has conical surface refraction effect.
Summary of the invention
In order to realize directly exporting the purpose of hollow laser beam by resonant cavity, we have invented a kind of resonant cavity that can obtain hollow laser beam, can directly export open circles taper laser beam, have apparatus structure simultaneously and simply, do not have extra energy loss, keep the original degree of coherence of laser beam simultaneously.
The present invention's the resonant cavity that can obtain hollow laser beam is made up of speculum, gain medium and output coupling mirror, it is characterized in that, the output coupling mirror material is a biaxial crystal, and an optical axis of biaxial crystal is parallel with resonator axis.
Because biaxial crystal has conical surface refraction effect, the resonant cavity output coupling mirror that adopts this crystal to make, resonant cavity can directly be exported open circles taper laser beam, and with respect to prior art, its structure is very simple, just the material selected for use of the output coupling mirror of resonant cavity unlike the prior art, not adding Optical devices in addition, therefore just do not have extra energy loss yet, is not to obtain hollow laser beam by laser beam reshaping, therefore, the degree of coherence of laser beam does not reduce.
The harmonic light of incident biaxial crystal propagate put to
Parallel with resonator axis, see shown in Figure 1, by crystal optics as can be known:
Then:
k
xD
x+k
yD
y+k
zD
z=0,
∵D
x=ε
xE
x,D
y=ε
yE
y,D
z=ε
zE
z,
k
y=0,
So:
k
xD
x+k
zD
z=0,
ε
xk
xE
x+ε
zk
zE
z=0,
Make vector
If plane π is vertical
Intersection point is the Q point, plane Λ vertical vector
AB is the intersection of plane π and plane Λ, because
On the Λ plane,
Must on the intersection AB of plane π and plane Λ, do with the intersection point P of plane π
Meet at the R point with plane π, because of
Coplane, so, on the π plane, R, Q, P on same straight line, in Δ RPO,
So:
Therefore,
Anyway change, always satisfy formula (1), be unable to do without the Λ plane simultaneously,
Change, be equivalent to the P point and move on intersection AB, the mobile R point that is equivalent to of P point moves, and satisfies formula (1), and because of the track of P point on intersection AB is straight line, the track of R is circle, so, all
Constitute taper seat.Therefore, when harmonic light is propagated, electric displacement vector no matter
Get any direction, unique phase velocity is all arranged, still, because electric field strength
With electric displacement vector
Not not in the same way, unlimited a plurality of radiation direction will occur, these light surround a taper seat.Its effect shows as, harmonic light propagate put to
During with the biaxial crystal optical axis coincidence parallel with resonator axis, the Energy distribution of output is on the hollow conical surface, and therefore, the laser beam of resonant cavity output is the open circles taper, and hot spot therefore also just in the form of a ring; Conical surface wall is thin, the power density height of laser beam.
Description of drawings
Fig. 1 is that biaxial crystal produces hollow cone shaped light beam schematic diagram.Fig. 2 is the structural representation of the present invention's the resonant cavity that can obtain hollow laser beam, and this figure double as is a Figure of abstract.
Embodiment
The present invention's the resonant cavity that can obtain hollow laser beam is made up of speculum 1, gain medium 2 and output coupling mirror 3, sees shown in Figure 2ly, and output coupling mirror 3 materials are biaxial crystal, and an optical axis of biaxial crystal is parallel with resonator axis.Pumping source 4 is a 808nm 30W diode laser matrix.Pump light 4 is coupled in the gain medium 2 in the resonant cavity by coupled apparatus.Coupled apparatus is made up of coupled fiber 5, coupled lens 6.Coupled fiber 5 core diameters are 400 μ m, numerical aperture NA=0.22.Coupled lens 6 is made up of a pair of planoconvex spotlight, and convex surface is relative, and the convex surface radius is 50mm, each planoconvex spotlight two sides plating 808nm anti-reflection film, transmitance T>95%.Speculum 1 is the plano-concave mirror, and one side is a concave surface in the chamber, two sides plating 808nm anti-reflection film and 1064nm highly reflecting films, anti-reflection film transmitance T>95%, highly reflecting films reflectivity R>98%.Gain medium 2 is Nd:YAG crystal bars, and neodymium ion doped concentration N=1% is of a size of
Output coupling mirror 3 adopts KTP (KTP) crystal to make, and an optical axis of this biaxial crystal is parallel with resonator axis, and ktp crystal is of a size of 4mm * 4mm * 2mm, and ktp crystal skin covering of the surface system is 10% to the transmitance of 1064nm wavelength.
When diode laser matrix was injected into power in the Nd:YAG crystal bar and surpasses the laser generation threshold value, the 1064nm harmonic light in the optical axis transmission of optical direction along ktp crystal, just can obtain open circles taper laser beam by outgoing mirror outside the chamber.
According to crystal optics, the cone angle of open circles taper laser beam is determined by formula (2):
In the formula: n
x, n
y, n
zBe three major axes orientation refractive indexes of ktp crystal, and, n
x=1.7416, n
y=1.7496, n
z=1.8323, get α=1.7 ° by formula.
Claims (2)
1. the resonant cavity that can obtain hollow laser beam is made up of speculum, gain medium and output coupling mirror, it is characterized in that, the output coupling mirror material is a biaxial crystal, and an optical axis of biaxial crystal is parallel with resonator axis.
2. the resonant cavity that can obtain hollow laser beam according to claim 1, it is characterized in that, output coupling mirror (3) adopts KTP (KTP) crystal to make, an optical axis of this biaxial crystal is parallel with resonator axis, ktp crystal is of a size of 4mm * 4mm * 2mm, and ktp crystal skin covering of the surface system is 10% to the transmitance of 1064nm wavelength.
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Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
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CN102570262A (en) * | 2012-02-29 | 2012-07-11 | 中国科学院上海光学精密机械研究所 | Hollow ring-shaped light beam output solid laser and using method therefor |
CN102891431A (en) * | 2012-02-09 | 2013-01-23 | 清华大学 | Solid laser oscillator capable of outputting annular laser distribution |
CN103572341A (en) * | 2013-09-23 | 2014-02-12 | 江苏大学 | Electrochemical composite decomposition manufacturing method and device of laser light tube electrode |
CN104942435A (en) * | 2015-07-14 | 2015-09-30 | 中国工程物理研究院激光聚变研究中心 | Laser machining head and laser machining method thereof |
CN105071206A (en) * | 2015-09-17 | 2015-11-18 | 江苏师范大学 | Vortex laser based on laser medium center zero gain structure |
CN105958311A (en) * | 2016-06-24 | 2016-09-21 | 长春理工大学 | Dual-rectangular hollow laser based on spherical aberration regulation-control thermal-stability region and laser shaping and amplification |
CN109217077A (en) * | 2018-11-15 | 2019-01-15 | 云南大学 | A kind of tunable hollow laser of self-mixing |
CN109217096A (en) * | 2018-11-15 | 2019-01-15 | 云南大学 | A kind of double half anti-gauss hollow Q-switched lasers of the adjustable polarization based on electro-optic crystal |
CN114336241A (en) * | 2021-12-30 | 2022-04-12 | 云南大学 | Tunable hollow laser based on electro-optic crystal axial cone |
CN114498272A (en) * | 2021-12-16 | 2022-05-13 | 深圳大学 | Intermediate infrared vector vortex optical rotation generating device and method |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1560666A (en) * | 2004-03-04 | 2005-01-05 | 中国科学院上海光学精密机械研究所 | Device for generating single pyramid collimation hollow ligt beam |
CN1866645A (en) * | 2006-06-09 | 2006-11-22 | 中国科学院上海光学精密机械研究所 | Pulse width adjustable acoustic-optic Q-switched double cladded fiber laser |
CN101232147A (en) * | 2007-01-25 | 2008-07-30 | 四川大学 | Hollow beam gas laser |
CN101567520A (en) * | 2009-05-26 | 2009-10-28 | 长春理工大学 | Hollow beam pumping emission semiconductor laser of vertical external chamber surface |
-
2010
- 2010-09-07 CN CN 201010274086 patent/CN101950915A/en active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1560666A (en) * | 2004-03-04 | 2005-01-05 | 中国科学院上海光学精密机械研究所 | Device for generating single pyramid collimation hollow ligt beam |
CN1866645A (en) * | 2006-06-09 | 2006-11-22 | 中国科学院上海光学精密机械研究所 | Pulse width adjustable acoustic-optic Q-switched double cladded fiber laser |
CN101232147A (en) * | 2007-01-25 | 2008-07-30 | 四川大学 | Hollow beam gas laser |
CN101567520A (en) * | 2009-05-26 | 2009-10-28 | 长春理工大学 | Hollow beam pumping emission semiconductor laser of vertical external chamber surface |
Non-Patent Citations (1)
Title |
---|
《光子学报》 20100831 武志超 等 晶体锥折射空心光束的位相差及偏振特性 第39卷, 第8期 2 * |
Cited By (16)
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CN102891431A (en) * | 2012-02-09 | 2013-01-23 | 清华大学 | Solid laser oscillator capable of outputting annular laser distribution |
CN102570262B (en) * | 2012-02-29 | 2013-11-20 | 中国科学院上海光学精密机械研究所 | Hollow ring-shaped light beam output solid laser and using method therefor |
CN102570262A (en) * | 2012-02-29 | 2012-07-11 | 中国科学院上海光学精密机械研究所 | Hollow ring-shaped light beam output solid laser and using method therefor |
CN103572341A (en) * | 2013-09-23 | 2014-02-12 | 江苏大学 | Electrochemical composite decomposition manufacturing method and device of laser light tube electrode |
CN104942435A (en) * | 2015-07-14 | 2015-09-30 | 中国工程物理研究院激光聚变研究中心 | Laser machining head and laser machining method thereof |
CN105071206B (en) * | 2015-09-17 | 2018-04-13 | 江苏师范大学 | A kind of vortex laser based on laser medium center zero gain structure |
CN105071206A (en) * | 2015-09-17 | 2015-11-18 | 江苏师范大学 | Vortex laser based on laser medium center zero gain structure |
CN105958311B (en) * | 2016-06-24 | 2019-01-04 | 长春理工大学 | Spherical aberration regulates and controls the area Re Wen and the laser sizing amplification hollow laser of double square |
CN105958311A (en) * | 2016-06-24 | 2016-09-21 | 长春理工大学 | Dual-rectangular hollow laser based on spherical aberration regulation-control thermal-stability region and laser shaping and amplification |
CN109217077A (en) * | 2018-11-15 | 2019-01-15 | 云南大学 | A kind of tunable hollow laser of self-mixing |
CN109217096A (en) * | 2018-11-15 | 2019-01-15 | 云南大学 | A kind of double half anti-gauss hollow Q-switched lasers of the adjustable polarization based on electro-optic crystal |
CN109217096B (en) * | 2018-11-15 | 2019-08-27 | 云南大学 | A kind of double half anti-gauss hollow Q-switched lasers of the adjustable polarization based on electro-optic crystal |
CN109217077B (en) * | 2018-11-15 | 2019-08-27 | 云南大学 | A kind of tunable hollow laser of self-mixing |
CN114498272A (en) * | 2021-12-16 | 2022-05-13 | 深圳大学 | Intermediate infrared vector vortex optical rotation generating device and method |
CN114336241A (en) * | 2021-12-30 | 2022-04-12 | 云南大学 | Tunable hollow laser based on electro-optic crystal axial cone |
CN114336241B (en) * | 2021-12-30 | 2024-01-05 | 云南大学 | Tunable hollow laser based on electro-optic crystal axicon |
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