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Liu  J.  Ozygus  B.  Erhard  J.  Ding  A.  Weber  H.  Meng  X. 《Optical and Quantum Electronics》2003,35(8):811-824
A diode-pumped 1.34 m Nd:GdVO4 laser operating in cw and active Q-switching modes has been demonstrated. 4.15 W of cw output power was obtained at the highest attainable pump power of 12.3 W, resulting in an optical conversion efficiency of 33.7%, the slope efficiency was determined to be 37.6%. In Q-switching operation, a maximum average output power of 2.7 W was generated at pulse repetition frequency (PRF) of 50 kHz, with an optical conversion efficiency of 22% and a slope efficiency of 29.2%. The laser pulses with shortest duration, highest energy and peak power were achieved at PRF of 10 kHz, the parameters being 15 ns, 160 J, and 10.7 kW, respectively. By intracavity frequency-doubling with a type II phased-matched KTP crystal, 0.62 W average power at 0.67 m was produced at a PRF of 15 kHz, the resulting pulse energy, peak power, and pulse width being 41.3 J, 2.2 kW, and 19 ns, respectively. A group of analytical formulae, based on rate equations, are presented to evaluate the operational parameters of an actively Q-switched laser. Calculated results were found to be in close consistency with the experimental data.  相似文献   

3.
Diode-pumped passively Q-switched Nd:GdVO4/Cr4+:YAG lasers with a simple flat-flat cavity were demonstrated. The maximum average output power at 1.06 μm was 1.25 W. The highest peak power and pulse energy were 7.56 kW and 75μJ, respectively, with the pulse repetition rate of 11.1 kHz and pulse width of 10 ns at the incident pump power of 8 W.  相似文献   

4.
A high power cryogenic cooling Tm-doped (2%) GdVO4 laser double-end-pumped by fiber-coupled-diode with the center wavelength of 804.5 nm at 21 ℃ is reported. The highest continuous-wave (CW) power of 2.35 W at 1903 nm is attained at pump power of 24 W. The slope efficiency is 12.5% and the threshold is 3.2 W. Single- and double-end-pumped types are investigated.  相似文献   

5.
With a 10-W diode laser to pump Nd:GdVO4 crystal in a folded cavity, we demonstrated Cr4+:YAG passively Q-switched Nd:GdVO4 lasers at 1.06 μm. The maximum average output power of 2.1 W and the highest peak power of 625 W were, respectively, obtained when the initial transmissions of the Cr4+:YAG crystals were 90% and 80%. Received: 8 September 1999 / Revised version: 30 December 1999 / Published online: 8 March 2000  相似文献   

6.
1 Introduction  Inrecentyears ,obviousprogresshasbeenachievedinflashlamppumpingNd∶YAGlaserswithlong pulseandhighaverageoutputpower[1] .ButthereexistsaneedforQ switchedsolid statelasersystemswithhighaverage power .ThismaybeachievedwithNd :YAGoscillator amplif…  相似文献   

7.
In this letter, a diode-pumped continuous-wave and passively Q-switched 1.06 μm laser with a novel composite YVO4/Nd:GdVO4 crystal was demonstrated for the first time. Theoretical calculations showed that the temperature distribution in YVO4/Nd:GdVO4 crystal was lower than that in GdVO4/Nd:GdVO4 and Nd:GdVO4 crystals under the same conditions. After optimizing the mode matching degree, a CW output power of 5.6 W of YVO4/Nd:GdVO4 laser was obtained at the incident pump power of 12 W when the output coupler with transmission of 30% was employed. Using Cr4 +:YAG crystals with initial transmission (T0) of 80% and 90% as saturable absorbers, the pulsed YVO4/Nd:GdVO4 laser characteristics were investigated. At the incident pump power of 12 W, the maximum average output power of 2.76 W and the maximum repetition rate of 189 kHz was achieved when T0 = 90% Cr4 +:YAG was used. The shortest pulse width was 28.1 ns when the initial transmission of the used Cr4 +:YAG was 80%.  相似文献   

8.
We demonstrated a laser-diode pumped Nd-doped yttrium gallium garnet (Nd:YGG) crystal continuous wave (CW) laser at 1.33 μm for the first time to our knowledge. At an incident pump power of 18.5 W, as high as 3.09 W of CW output power at 1.33 μm is achieved. The slope efficiency with respect to the incident pump power was 21.3%, and the fluctuation of the output power was better than 2.8% in the given 4 h. The beam quality factor M2 is 1.14 and 1.16 for tangential direction and sagittal direction, respectively.  相似文献   

9.
With a plano-concave cavity,diode-pumped continuous-wave(CW) and actively Q-switched Nd:YVO4 laser operating at 1.34 μm is demonstrated.Maximum CW output power of 4.76 W and Q-switched average output power of 2.64 W are obtained with output coupler(transmission T = 3.9%).For the Q-switching operation,the theoretically calculated pulse energy and pulse width,with a pulse repetition frequency(PRF) range of 5-40 kHz,coincide with the experimental results.With a T = 11.9% output coupler,the maximum peak power of 24.3 kW and minimum pulse width of 6.5 ns are obtained when the PRF is 10 kHz.To the best of our knowledge,this is the shortest actively Q-switched pulse duration ever obtained in a 1.3-μm Nd-doped vanadate laser.  相似文献   

10.
A novel design of multimode light power splitter is proposed and fabricated by using secondary asymmetric Y branches.An almost equally divided output among output terminals is obtained experimentally.Maskless laser direct writing technique is applied in the fabrication process to facilitate the formation of power splitters by ultraviolet curable polymer.The analysis of the performances of both four-port and eight-port devices shows that these two dividers obtain a power splitting uniformity of more than 95%.  相似文献   

11.
1 Introduction  Diode pumpedsolid state passive Q switchedsecondharmonicgenerationlaserhashighpowerandhighrepetitionratepulseinnanosecondperiod ,andvariousapplicationsinmicro mechanics ,measurements,film carve ,micro operationsinsurgery ,andsoon[1] .Recent year…  相似文献   

12.
With a non-critically phase-matched KTA crystal, a high-power intracavity optical parametric oscillator (IOPO) driven by a diode-side-pumped acousto-optically Q-switched Nd:YAG laser has been realized. The maximum average output power of 13.6 W at the signal wavelength of 1534 nm and 3 W at the idler wavelength of 3472.7 nm were obtained with the repetition rate of 18 kHz, giving the optical-optical conversion efficiency of about 5.7% from diode-power at 808 nm to OPO signal output, which was the highest conversion efficiency for intracavity KTA OPO with diode-side-pumping configurations to our best knowledge. At the highest output power of 13.6 W, the signal pulse duration of 5.46 ns was obtained, corresponding to the single pulse energy of 756 μJ and peak power of 138 kW, respectively.  相似文献   

13.
We demonstrated a diode-pumped vertical external cavity surface emitting laser with simple plane-concave cavity. When the pump power at a wavelength of 811.6 nm is 1.5 W, the maximum output power is 40.4 mW at the wavelength of 1005.8 nm. The optical-optical conversion efficiency is 2.7%. .  相似文献   

14.
LIUJunhai SHAOZongshu MENGXianlin ZHANGHuaijinZHULi JIANGMinhua(NationalLaboratoryofCrystalMaterials,ShandongUniversity,Jinan250100,China)ReceivedMarch22,1999;RevisedmanuscriptreceivedMarch29,1999DevelopedbyRussianresearchersin1992,Nd∶GDVO4isapotenti…  相似文献   

15.
1 Introduction  Compactgreenlasersareofpotentialinterestformanyapplications ,suchasunderwatercommunication ,opticaldatastorage,display ,andchemicalprocessing[1,2 ] .Atpresent,mostschemesreportedforgeneratinggreenbeamsarebasedonthefrequencyconversionofnear inf…  相似文献   

16.
1 Introduction  Itiseasytoobtainhighharmonic conversionefficiencyby placingthedoublingcrystalintotheresonatorduetothehighfundamental wave powerdensity ,whichisespeciallysuitablefortheharmonicconversionofCWlaserwithmiddleorlowoutputpower.Ifthe passivelyQ s…  相似文献   

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18.
In this paper, the stability of a laser-diode-pumped Cr4+∶YAG passively Nd3+∶YAG Q-switched laser and the influence of the transversal mode structure on the stability are investigated. With the laser operating in TEM00 mode, the pulse energy fluctuation and the repetition rate fluctuation as functions of the repetition rate are measured, and semi-quantitatively and qualitatively analyzed, respectively.  相似文献   

19.
By simultaneously using both V3+:YAG and Co:LMA saturable absorbers in the cavity, a diode-pumped doubly passively Q-switched c-cut Nd:GdVO4 laser at 1.34 μm is demonstrated for the first time. The average output power, the pulse width and the pulse repetition rate have been measured. The experimental results show that the doubly passively Q-switched laser can generate shorter pulse width with higher peak power in comparison to the singly passively Q-switched laser only with V3+:YAG or Co:LMA saturable absorber. At the pump power 13 W, the pulse width has been compressed 83% and the peak power has been improved 15 times, respectively.  相似文献   

20.
The thermal lensing, output characteristics of an end-pumped NYAB laser with high pump power levels and operated at the fundamental wavelength, and the manner of self-frequency-doubling, have been investigated. The thermal lensing in the NYAB crystal was found to be significantly stronger than that in Nd:YVO4 crystal. A maximum output of 3.2 W at 1.06 μm was achieved with an optical conversion efficiency of 29.1% and an average slope efficiency of 37.5%. These results were found to be slightly inferior to those of Nd:YVO4 crystal. When operated in the fashion of selffrequency-doubling, 23 mW green output was obtained at the incident pump power of 5 W, such inefficient operation was attributed to the large mode size in the NYAB crystal.  相似文献   

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