Far-infrared amplified spontaneous emission and collisional energy transfer between the E 0(g)⁺ (³P₂) and D 0(u)⁺ (³P₂) ion-pair states of I₂.
暂无分享,去创建一个
[1] K. Tsukiyama,et al. Far infrared stimulated emission from the ns and nf Rydberg states of NO. , 2013, The Journal of chemical physics.
[2] K. Tsukiyama,et al. Laser induced amplified spontaneous emission from the f 0(g)(+) (3P0) ion-pair state of I2. , 2013, The Journal of chemical physics.
[3] T. Ridley,et al. Amplified spontaneous emission and collisional transfer from the f0(g)+ ((3)P0) ion-pair state of I2. , 2009, The Journal of chemical physics.
[4] T. Ridley,et al. The influence of amplified spontaneous emission in collisional energy transfer studies exemplified by E0g+(3P2) to D0u+(3P2) transfer in I2 , 2008, CP 2008.
[5] M. Fukushima,et al. UV emission of I2 from the ion-pair state following amplified spontaneous emission. , 2008, The Journal of chemical physics.
[6] V. A. Alekseev,et al. Characterization of a shallow-bound 0g+ valence state of I2 using emission from the D 0u+(3P2) and F' 0u+(1D2) ion-pair states populated by amplified spontaneous emission. , 2007, Physical chemistry chemical physics : PCCP.
[7] V. A. Alekseev,et al. Evidence for amplified spontaneous emission from the E0g+(3P2) and γ1u(3P2) ion-pair states of I2 excited by optical–optical double resonance , 2007 .
[8] K. Tsukiyama,et al. The band of ND3 studied by laser-induced amplified spontaneous emission and transient gain spectroscopy , 2004 .
[9] V. A. Alekseev. Amplified spontaneous emission and its application for population of resonant states of the Xe and Kr atoms , 2002 .
[10] T. Ishiwata,et al. Absolute Position of the D′2g(3P2) Ion-Pair State of I2 Determined by Perturbation-Facilitated Optical–Optical Double Resonance , 2002 .
[11] T. Yotsumoto,et al. Optical–Optical Double Resonance Spectroscopy of I2 through the Parity Mixed Valence States , 2001 .
[12] C. J. Fecko,et al. Collision-induced electronic energy transfer from v=0 of the E(0g+) ion-pair state in I2: Collisions with I2(X) , 2001 .
[13] M. Fukushima,et al. Optical-Optical Double-Resonance Spectroscopy of the 1u(3P2) and 2u(3P2) States of I2 Through the A3Π(1u) State , 2000 .
[14] W. Ubachs,et al. Collision-induced E(0g+)- D(0 u+) state-to-state energy transfer in I2 , 1999 .
[15] T. Ichimura,et al. Parametric four-wave mixing in the H2Σ+,H′2Π(v′=0) states of NO , 1997 .
[16] K. Uehara,et al. Cascading amplified spontaneous emission of NO Rydberg states , 1996 .
[17] H. Hasegawa,et al. The C1Σ+-B1-Σ+ amplified spontaneous emission in CO , 1996 .
[18] Czarnetzki,et al. Generation of vacuum-ultraviolet radiation in H2 by nonlinear optical processes near the EF- and B-state resonances. , 1991, Physical Review A. Atomic, Molecular, and Optical Physics.
[19] H. Hertz,et al. Properties of laser-induced stimulated emission for diagnostic purposes , 1990 .
[20] I. Tanaka,et al. A Spectroscopic Study of the D(0u , 1987 .
[21] M. Broyer,et al. Extensive study of the 1g(3P2) ion pair state of I2 , 1983 .
[22] J. Brand,et al. The E-B band system of diatomic iodine , 1982 .
[23] W. Cooke,et al. Effects of blackbody radiation on highly excited atoms , 1980 .
[24] L. Allen,et al. Amplified spontaneous emission I. The threshold condition , 1971 .