Supersonic diode pumped alkali lasers: Computational fluid dynamics modeling

We report on recent progress on our three-dimensional computational fluid dynamics (3D CFD) modeling of supersonic diode pumped alkali lasers (DPALs), taking into account fluid dynamics and kinetic processes in the lasing medium. For a supersonic Cs DPAL with laser section geometry and resonator parameters similar to those of the 1-kW flowing-gas subsonic Cs DPAL [A.V. Bogachev et al., Quantum Electron. 42, 95 (2012)] the maximum achievable output power, ~ 7 kW, is 25% higher than that achievable in the subsonic case. Comparison between semi-analytical and 3D CFD models for Cs shows that the latter predicts much higher maximum achievable output power than the former. Optimization of the laser parameters using 3D CFD modeling shows that very high power and optical-to-optical efficiency, 35 kW and 82%, respectively, can be achieved in a Cs supersonic device pumped by a collimated cylindrical (0.5 cm diameter) beam. Application of end- or transverse-pumping by collimated rectangular (large cross section ~ 2 - 4 cm2) beam makes it possible to obtain even higher output power, > 250 kW, for ~ 350 kW pumping power. The main processes limiting the power of Cs supersonic DPAL are saturation of the D2 transition and large ~ 40% losses of alkali atoms due to ionization, whereas the influence of gas heating is negligibly small. For supersonic K DPAL both gas heating and ionization effects are shown to be unimportant and the maximum achievable power, ~ 40 kW and 350 kW, for pumping by ~ 100 kW cylindrical and ~ 700 kW rectangular beam, respectively, are higher than those achievable in the Cs supersonic laser. The power achieved in the supersonic K DPAL is two times higher than for the subsonic version with the same resonator and K density at the gas inlet, the maximum optical-to-optical efficiency being 82%.

[1]  V. K. Kanz,et al.  End-pumped continuous-wave alkali vapor lasers: experiment, model, and power scaling , 2004 .

[2]  J. Ciurył,et al.  42P12↔42P32 mixing in potassium induced in collisions with noble gas atoms , 1982 .

[3]  V. A. Eroshenko,et al.  Diode-pumped caesium vapour laser with closed-cycle laser-active medium circulation , 2012 .

[4]  G. Perram,et al.  A three-level analytic model for alkali metal vapor lasers: part I. Narrowband optical pumping , 2010 .

[5]  Boris D. Barmashenko,et al.  Feasibility of supersonic diode pumped alkali lasers: Model calculations , 2013 .

[6]  Xiaojun Xu,et al.  Modeling, numerical approach, and power scaling of alkali vapor lasers in side-pumped configuration with flowing medium , 2011 .

[7]  M. Allegrini,et al.  Energy-pooling collisions in potassium : 4 , 1997 .

[8]  M. K. Shaffer,et al.  Photoionization in alkali lasers. , 2011, Optics express.

[9]  Timothy J. Madden,et al.  Simulation of deleterious processes in a static-cell diode pumped alkali laser , 2014, Photonics West - Lasers and Applications in Science and Engineering.

[10]  Wei Zhang,et al.  Algorithm for evaluation of temperature distribution of a vapor cell in a diode-pumped alkali laser system: part I. , 2014, Optics express.

[11]  K. Waichman,et al.  What can we gain from supersonic operation of diode pumped alkali lasers: model calculations , 2013, Optics/Photonics in Security and Defence.

[12]  B. Barmashenko,et al.  Static diode pumped alkali lasers: Model calculations of the effects of heating, ionization, high electronic excitation and chemical reactions , 2013 .

[13]  A. Shapiro The dynamics and thermodynamics of compressible fluid flow. , 1953 .

[14]  B. Barmashenko,et al.  Analysis of lasing in gas-flow lasers with stable resonators. , 1998, Applied optics.

[15]  P. Gould,et al.  Long-range interaction of the 39K(4s)+39K(4p) asymptote by photoassociative spectroscopy. I. The 0g− pure long-range state and the long-range potential constants , 1997 .

[16]  Boris V. Zhdanov,et al.  Review of alkali laser research and development , 2012 .

[17]  Karol Waichman,et al.  Semi-analytical and 3D CFD DPAL modeling: feasibility of supersonic operation , 2014, Photonics West - Lasers and Applications in Science and Engineering.

[18]  Glen P. Perram,et al.  Transfer between the cesium62P1/2and62P3/2levels induced by collisions with H2, HD, D2, CH4, C2H6, CF4, and C2F6 , 2011 .

[19]  B. Barmashenko,et al.  Analysis of the optical extraction efficiency in gas-flow lasers with different types of resonator. , 1996, Applied optics.

[20]  Weihong Hua,et al.  Theoretical model and novel numerical approach of a broadband optically pumped three-level alkali vapour laser , 2011 .

[21]  A. Shapiro,et al.  The Dynamics And Thermodynamics Of Compressible Fluid Flow, Vol. 2 By Ascher H. Shapiro , 2017 .

[22]  B. Barmashenko,et al.  Modeling of flowing gas diode pumped alkali lasers: dependence of the operation on the gas velocity and on the nature of the buffer gas. , 2012, Optics letters.

[23]  William F. Krupke,et al.  Diode pumped alkali lasers (DPALs)—A review (rev1) , 2012 .

[24]  M. Perrin,et al.  Energy dependence of the total cross sections for K(42Pj1m1 to 42Pj2m2)+He collisions , 1980 .

[25]  Boris D. Barmashenko,et al.  Detailed analysis of kinetic and fluid dynamic processes in diode-pumped alkali lasers , 2013 .

[26]  Qi Zhu,et al.  Analysis of temperature distributions in diode-pumped alkali vapor lasers , 2010 .

[27]  Karol Waichman,et al.  Computational fluid dynamics modeling of subsonic flowing-gas diode-pumped alkali lasers: comparison with semi-analytical model calculations and with experimental results , 2014 .

[28]  J. E. Sansonetti Wavelengths, Transition Probabilities, and Energy Levels for the Spectra of Sodium (NaI–NaXI) , 2008 .

[29]  Alan Gallagher Rubidium and Cesium Excitation Transfer in Nearly Adiabatic Collisions with Inert Gases , 1968 .

[30]  Karol Waichman,et al.  Theoretical studies of the feasibility of supersonic DPALs , 2014, Security and Defence.