Temperature dependence of the quenching of N2 (C 3Πu) by N2 (X) and O2 (X)
暂无分享,去创建一个
M. Fraga | J. Wieser | R. Krücken | L. Pereira | T. Heindl | A. Ulrich | A. Morozov
[1] M. Fraga,et al. Temperature-dependent quenching of UV fluorescence of N2 , 2008 .
[2] T. Waldenmaier,et al. Measurement of the air fluorescence yield with the airlight experiment , 2008 .
[3] B. Keilhauer,et al. Air fluorescence relevant for cosmic-ray detection---Review of pioneering measurements , 2008, 0807.3844.
[4] B. Keilhauer,et al. Air fluorescence relevant for cosmic-ray detection---Summary of the 5th fluorescence workshop, El Escorial 2007 , 2008, 0807.3760.
[5] E. al.,et al. Temperature and Humidity Dependence of Air Fluorescence Yield measured by AIRFLY , 2007, 0711.4583.
[6] J. Wieser,et al. Influence of pressure on the relative population of the two lowest vibrational levels of the C 3 Πu state of nitrogen for electron beam excitation , 2008 .
[7] P. Ambrico,et al. On N2(C3Πu, v = 0) state lifetime and collisional deactivation rate by N2 , 2007 .
[8] P. Ambrico,et al. OODR-LIF direct measurement of N2(C 3Πu, v = 0–4) electronic quenching and vibrational relaxation rate coefficients by N2 collision , 2006 .
[9] J. Wieser,et al. Spatial distribution of fluorescent light emitted from neon and nitrogen excited by low energy electron beams , 2006 .
[10] J. Wieser,et al. Gas kinetic studies using a table-top set-up with electron beam excitation: quenching of molecular nitrogen emission by water vapour , 2005 .
[11] M. Nagano,et al. New measurement on photon yields from air and the application to the energy estimation of primary cosmic rays , 2004, astro-ph/0406474.
[12] Marko Zavrtanik,et al. Properties and performance of the prototype instrument for the Pierre Auger Observatory , 2004, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.
[13] D. Camin. The Southern Pierre Auger observatory: status and prospectives , 2004 .
[14] S. Pszona,et al. The track structure of α-particles from the point of view of ionization-cluster formation in "nanometric" volumes of nitrogen , 2002, Radiation and environmental biophysics.
[15] S. Starikovskaia,et al. Collisional deactivation of N2(C , v=0, 1, 2, 3) states by N2, O2, H2 and H2O molecules , 2000 .
[16] Yousfi,et al. Monte Carlo simulation of electron swarms at low reduced electric fields. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.
[17] Phelps,et al. Anisotropic scattering of electrons by N2 and its effect on electron transport. , 1985, Physical review. A, General physics.
[18] J. Galy,et al. De‐excitation of N2 (C 3Πu ; ν′ = 0 and 1) levels in mixtures of oxygen and nitrogen , 1973 .
[19] W.K. (Bill) Peterson,et al. Tables of secondary-electron-production cross sections , 1972 .