CN101017951A - A compensation method for laser bar thermal lens effect - Google Patents

Abstract

The disclosed thermal-lensing compensation method for laser rod comprises: setting the holophote with a step-motor driving movable mechanism in optical resonator of laser as raised convex mirror toward the laser rod; controlling the step motor by a computer to make the distance from mirror to rod as a = f - R/2 - d/2n. Wherein, R for curvature radius of the mirror, d for rod length, n for refractive index of rod, and f for lens focus. This invention simplifies system structure, affects no energy conversion efficiency, and applies computer to control laser frequency N and pumping energy density Ep for complete automatic compensation.

Description

A kind of compensation method of laser bar thermal lens effect

Technical field

The present invention relates to the laser bar in a kind of solid state laser, especially relate to the compensation method of the laser bar thermal lens effect in a kind of solid state laser.

Background technology

Existing solid state laser absorptive pumping light energy in operation process, except that fraction is exported with laser mode, most of energy change heat into and are deposited on makes it produce temperature rise in the working-laser material, constantly repeating under pumping and the conduction of heat, temperature gradient constantly increases in the operation material, takes away up to heating power and cooling fluid to reach heat balance when heat equates.In the operation material existence of temperature gradient make originally refractive index fully uniformly operation material become the class lens medium, light beam focuses on after by operation material, is commonly called as to be thermal self-focusing.Under the situation of symmetric pump, garden cylindricality laser bar becomes the class globe lens, and its primary flat is called thermal focal length to the distance of focus.Thermal self-focusing not only makes the laser-beam divergence angle increase sharply, and even more serious is can be in the inner real focus that produces of operation material, and it will produce laser damage at material internal.In order to alleviate the influence of thermal lensing effect, extensively adopt at present the operation material end face is worn into concave surface compensating, but can only the specific thermal lensing effect under the particular pump power be compensated Laser Devices.For this reason, people manage to seek the compensation that the ancillary relief device that adds is realized thermal lensing effect, as disclosing a kind of compensation method in No. 02266147.6 Chinese utility model patent specification of bulletin mandate on August 27th, 2003, between solid laser medium (being equivalent to the laser bar among the present invention) and outgoing mirror, an offset lens driven by stepper motors is set, offset lens is moved forward and backward the position of adjusting offset lens according to the size of solid laser medium power by step motor drive.The applied optical principle of this compensation arrangement is to make the distance between laser medium and the offset lens remain thermal focal length and offset lens focal length sum, even thermal lens and offset lens form Kepler telescope, reach the thermal lensing effect of compensation solid laser medium thus, make unstable cavity become stable cavity, high-power laser output has the purpose of stable preferably and beam quality.But also there is following problem in above-mentioned compensation arrangement: the compensation method of this compensation arrangement is that to make the rod and the distance of lens equal " thermal focal length and focal length of lens sum " be thermal lens and lens formation Kepler telescope, this compensation arrangement has only when thermal focal length is very little, " thermal focal length and focal length of lens sum " can be the practical laser device and adopts, when thermal focal length big (as several meters), " thermal focal length and focal length of lens sum " is quite big, is difficult to adopt for the practical laser device; The optical resonator interpolation is gone into the optics element increases laser loss, can be directed at the laser energy conversion efficiency and descend.

Summary of the invention

Technical problem to be solved by this invention provides a kind of optical element that need not add just can realize method that the laser bar thermal lens effect in the solid state laser is compensated.

The present invention solves the problems of the technologies described above the technical scheme that is adopted: a kind of compensation method of laser bar thermal lens effect, the completely reflecting mirror of optical resonator in the laser is arranged to convex mirror to laser bar direction projection, the travel mechanism that is driven by stepper motor is set on described completely reflecting mirror, described stepper motor is by the controlling computer controlling and driving, making the distance between described completely reflecting mirror and the described laser bar is a=f-R/2-d/2n, wherein, R is the radius of curvature of completely reflecting mirror, d is the length of laser bar, n is the refractive index of laser bar, f is a thermal focal length, and it satisfies formula $f=\frac{2\mathrm{\κ}}{N{(\mathrm{\β}+P)}_{\mathrm{\χ}}{E}_{p}d},$ Wherein, κ, β, P, x, d is respectively the coefficient of heat conduction of laser bar material, thermal refractive index coefficient, the stress thermo-optical coeffecient, the length of heating efficiency and laser bar, N is the repetition rate of laser, Ep is the pumping average power of unit volume working-laser material, get the high repetition frequency of laser and the arbitrary value of arbitrary value between the minimum repetition rate and pumping average power, utilize above-mentioned formula to obtain the arbitrary value f of thermal focal length this moment, when f during less than 200cm (for example to the repetition rate neodymium glass laser, high-average power YAG laser), the radius of curvature R of described completely reflecting mirror can be arranged to equal f; As f during more than or equal to 200cm (low average power YAG laser for example), the radius of curvature R of described completely reflecting mirror can be arranged to equal 1.8f.

Above-mentioned compensation method comprises following concrete steps: 1. thermal refractive index coefficient, refractive index, stress thermo-optical coeffecient, heating efficiency, the coefficient of heat conduction and the laser bar length of working-laser material and correlation formula and condition compiled program are sent into computer; 2. utilize computer control laser repetition rate N and pump energy density E _p, and utilize formula $f=\frac{2\mathrm{\κ}}{N{(\mathrm{\β}+P)}_{\mathrm{\χ}}{E}_{p}d}$ Determine the thermal focal length when laser bar reaches heat balance; Distance when 3. utilizing formula a=f-R/2-d/2n to calculate the realization thermal lensing compensation between full transmitting mirror of convex surface and the laser bar by computer, utilize computer to drive stepper motor then and drive the position of the full transmitting mirror of convex surface when optical axis moves to thermal lensing compensation, realize compensation fully automatically.

Compared with prior art, the invention has the advantages that simple in structure, do not need the compensation arrangement that adds, laser loss in the optical resonator is increased, do not influence the laser energy conversion efficiency, after the radius of curvature of having determined completely reflecting mirror, just can utilize computer control laser repetition rate N and pump energy density E _p, utilize computer to drive stepper motor and drive spherical mirror along the optical axis translation, CD-ROM drive motor realizes compensation fully automatically automatically.

Description of drawings

Fig. 1 is the structural representation of the laser of use compensation method of the present invention.

Embodiment

Embodiment describes in further detail the present invention below in conjunction with accompanying drawing.

Embodiment one: as shown in the figure, wherein 1 for plating the film spherical mirror that is all-trans of 1053nm wavelength, and 2 is the N3122 phosphate nd glass laser rod of φ 8 * 200, and 3 is the laser output coupling mirror.The glass laser rod volume is 10cm ³, establish pump energy density E _p=20J/cm ³, repetition rate is N=5Hz, with heating efficiency χ=0.08, thermal refractive index coefficient β=-4.3 * 10 of N3122 glass ^-6/ ℃, stress thermo-optical coeffecient P=5.8 * 10 ^-6/ ℃, coefficient of heat conduction κ=0.0056W/cm ℃, the long d=20cm substitution formula of rod $f=\frac{2\mathrm{\κ}}{N{(\mathrm{\β}+P)}_{\mathrm{\χ}}{E}_{p}d}$ The thermal focal length that obtains glass bar 2 is f=47cm, gets the radius of curvature R=47cm of spherical mirror 1, and f, d value and laser glass refractive index n=1.53 substitution a=0.5f-d/2n are obtained the thermal lensing compensation of glass bar 2 apart from a=17cm.To different pump energy density E _pOr different repetition rate N, use a computer and can calculate corresponding thermal focal length f respectively, and utilize formula a=f-R/2-d/2n to calculate corresponding compensation position a.

Embodiment two: as shown in the figure, wherein 1 is the be all-trans spherical mirror of film of plating 1064nm, and 2 is the YAG laser bar of φ 6 * 100, and 3 is the laser output coupling mirror.Set pump energy density E _p=15J/cm ³, repetition rate is N=10Hz, with YAG heating efficiency χ=0.05, thermal refractive index coefficient β=7.3 * 10 ^-6/ ℃, stress thermo-optical coeffecient P=8 * 10 ^-6/ ℃, coefficient of heat conduction κ=0.13W/cm ℃, the long d=10cm substitution formula of rod $f=\frac{2\mathrm{\κ}}{N{(\mathrm{\β}+P)}_{\mathrm{\χ}}{E}_{p}d}$ The thermal focal length that obtains described glass bar is f=227cm, gets radius of curvature R=1.8 f=409cm of spherical mirror 1, and f, d value and laser glass refractive index n=1.82 substitution a=0.1f-d/2n are compensated position a=20cm.To different pump energy density E _pOr different repetition rate N, use a computer and can calculate corresponding thermal focal length f respectively, and utilize formula a=f-R/2-d/2n to calculate corresponding compensation position a.

Claims (2)

1. the compensation method of a laser bar thermal lens effect, it is characterized in that the completely reflecting mirror of optical resonator in the laser is arranged to convex mirror to laser bar direction projection, the travel mechanism that is driven by stepper motor is set on described completely reflecting mirror, described stepper motor is by the controlling computer controlling and driving, making the distance between described completely reflecting mirror and the described laser bar is a=f-R/2-d/2n, wherein, R is the radius of curvature of completely reflecting mirror, d is the length of laser bar, n is the refractive index of laser bar, f is a thermal focal length, and it satisfies formula $f=\frac{2\mathrm{\κ}}{N(\mathrm{\β}+P)\mathrm{\χ}{E}_{p}d},$ Wherein, κ, β, P, χ, d is respectively the coefficient of heat conduction of laser bar material, thermal refractive index coefficient, the stress thermo-optical coeffecient, the length of heating efficiency and laser bar, N is the repetition rate of laser, Ep is the pumping average power of unit volume working-laser material, get the high repetition frequency of laser and the arbitrary value of arbitrary value between the minimum repetition rate and pumping average power, utilize above-mentioned formula to obtain the arbitrary value f of thermal focal length this moment, as f during less than 200cm, the radius of curvature R of described completely reflecting mirror is arranged to equal f, as f during more than or equal to 200cm, the radius of curvature R of described completely reflecting mirror is arranged to equal 1.8f.

2. the compensation method of a kind of laser bar thermal lens effect according to claim 1 and 2 is characterized in that it comprises following concrete steps: 1. thermal refractive index coefficient, refractive index, stress thermo-optical coeffecient, heating efficiency, the coefficient of heat conduction and the laser bar length of working-laser material and correlation formula and condition compiled program are sent into computer; 2. utilize computer control laser repetition rate N and pump energy density E _p, and utilize formula $f=\frac{2\mathrm{\κ}}{N(\mathrm{\β}+P)\mathrm{\χ}{E}_{p}d}$ Determine the thermal focal length when laser bar reaches heat balance; Distance when 3. utilizing formula a=f-R/2-d/2n to calculate the realization thermal lensing compensation between full transmitting mirror of convex surface and the laser bar by computer, utilize computer to drive stepper motor then and drive the position of the full transmitting mirror of convex surface when optical axis moves to thermal lensing compensation, realize compensation fully automatically.

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