Far-infrared laser-emission spectroscopy on ammonia isotopomers

In this paper we report the investigation of the isotopic ammonia gases14NH3,14NH2D,14NHD2,15NH3 and15ND3 optically pumped by a continuously tunable 20 atm CO2-laser. We found 267 far-infrared emission lines, produced by both inversion and Raman processes, in the frequency range from 15 cm−1 to about 250 cm−1. 200 of these were observed for the first time. We obtained far-infrared Raman tuning ranges exceeding 3 cm−1, photon conversion coefficients up to 12% and maximum output energies of 0.9 mJ. Furthermore, the optimum gas pressure, the polarization and the transient behavior of optically pumped ammonia have been investigated.

[1]  S. Marchetti,et al.  A tunable NH3 Raman laser in the 60–150 μm wavelength region by pumping with a continuously tunable multiatmosphere CO2 laser , 1987 .

[2]  J. Henningsen Assignment of laser lines in optically pumped CH3OH , 1977, IEEE Journal of Quantum Electronics.

[3]  G. Herzberg,et al.  Molecular Spectra and Molecular Structure , 1992 .

[4]  K. Gullberg,et al.  Submillimeter Emission from Optically Pumped 14NH3 , 1973 .

[5]  Koichi M. T. Yamada,et al.  Simultaneous analysis of the microwave and infrared spectra of 14ND3 and 15ND3 for the ν2 excited state , 1984 .

[6]  K. Renk,et al.  100 ps far-infrared laser pulses from optically pumped D2O , 1993 .

[7]  K. F. Renk,et al.  Tuning characteristics of a high pressure CO2 laser pumped CH3F Raman laser , 1986 .

[8]  Wen-sen Zhu,et al.  Optically pumped 15NH3 Raman FIR laser , 1989 .

[9]  A. F. Krupnov,et al.  A simultaneous analysis of the microwave, submillimeterwave, far infrared, and infrared-microwave two-photon transitions between the ground and ν2 inversion-rotation levels of 14NH3 , 1981 .

[10]  M. Redon,et al.  New CW far-infrared lasing in 14 NH 3 using Stark tuning , 1979 .

[11]  D. P. Scherrer,et al.  Generation of ultrashort far-infrared pulses optically pumped with truncated hybrid 10 μm CO2-laser pulses , 1992 .

[12]  J. Johns,et al.  The ν2 and ν4 bands of 14ND3 , 1986 .

[13]  V. Kartha,et al.  Inversion-rotation interaction in NH 2 D: intensity perturbations in the ν 2 band , 1987 .

[14]  F. Shimizu Stark Spectroscopy of NH3 ν2 Band by 10‐μ CO2 and N2O Lasers , 1970 .

[15]  B. Lax,et al.  Laser pumped molecular lasers - Part I: Theory , 1979, IEEE Journal of Quantum Electronics.

[16]  L. Coudert,et al.  Inversion doubling in the ν2 vibration-rotation band of NH2D and ND2H , 1986 .

[17]  K. Rao,et al.  The Δk = ±2 perturbation-allowed ν4 band and inversion-rotation energy levels of 15NH3 , 1985 .

[18]  Y. Nishi,et al.  Fir laser emissions from population inversion transition by TEA-CO2 laser pumping , 1990 .

[19]  H. Statz,et al.  Phase Locking of Modes in Lasers , 1965 .

[20]  K. Renk,et al.  Determination of the spectral width of Raman gain regions for different far infrared laser gases using a metal mesh Fabry Pérot interferometer , 1992 .

[21]  S. Marchetti,et al.  Pure MW Raman laser emission in superradiant mode in ammonia by pumping with 9P20 CO2 laser line , 1984 .