Rotational energy transfer in collisions of CH A2Δ, v=0 with Ar, N2 and CO2
暂无分享,去创建一个
[1] F. Stuhl,et al. State-to-state rate constants for the rotational relaxation of NH(A 3Π,v=0) radicals in inelastic collisions with NH3 , 2002 .
[2] F. Stuhl,et al. Rotationally resolved quenching and relaxation of CH(A2Δ,v=0,N) in the presence of CO , 2002 .
[3] R. Marsh,et al. Collisional Properties of the OH Molecule , 2001 .
[4] A. Kaledin,et al. Potential energy surfaces for CH(A 2Δ)–Ar and analysis of the A 2Δ–X 2Π band system , 2001 .
[5] M. Alexander,et al. Experimental and theoretical study of Λ-doublet resolved rotationally inelastic collisions of highly rotationally excited CH(A 2Δ,v=0) with Ar , 2001 .
[6] F. Stuhl,et al. State-to-state rate constants for the rotational relaxation of CH(B 2Σ−,v=0,J) in inelastic collisions with Ar , 2001 .
[7] F. Stuhl,et al. Fine-structure state resolved rotationally inelastic collisions of CH(A 2Δ,v=0) with Ar: A combined experimental and theoretical study , 2001 .
[8] R. Marsh,et al. Rotational transfer in diatom–diatom collisions , 2001 .
[9] J. Jeffries,et al. Collisional processes near the CH B 2Σ- v′=0,1 predissociation limit in laser-induced fluorescence flame diagnostics , 2000 .
[10] King‐Chuen Lin,et al. Rotational energy transfer within CH A 2Δ(v=0) and B 2Σ−(v=0) states by collisions with He, Ar, N2, CO, N2O, and CHBr3 using a time-resolved Fourier transform spectrometer , 2000 .
[11] C. Murray,et al. State-specific collisional coupling of the CH A 2Δ and B 2Σ− states , 2000 .
[12] C. Murray,et al. Rotational-state resolved coupling of CH A2Δ and B2Σ− in collisions with CO2 , 2000 .
[13] D. Crosley,et al. Radiative, collisional, and predissociative effects in CH laser-induced-fluorescence flame thermometry. , 1999, Applied optics.
[14] R. Farrow,et al. Measurements of ground-state OH rotational energy-transfer rates , 1999 .
[15] J. Lindner,et al. Multi-photon dissociation of CHBr3 at 248 and 193 nm: observation of the electronically excited CH() product , 1998 .
[16] M. Osborne,et al. Quantized momentum mechanics of inelastic and reactive collisions: the role of energy and angular momentum constraints , 1998 .
[17] P. Beaud,et al. Picosecond investigation of the collisional deactivation of OH A 2Sigma+(v' = 1, N' = 4, 12) in an atmospheric-pressure flame. , 1998, Applied optics.
[18] T. Nielsen,et al. Picosecond laser-induced fluorescence measurement of rotational energy transfer of OH A (2)?(+) (v? = 2) in atmospheric pressure flames. , 1997, Applied optics.
[19] K. Kohse-Höinghaus,et al. A scaling formalism for the representation of rotational energy transfer in OH (A2Σ+) in combustion experiments , 1996 .
[20] D. Crosley,et al. Electronic transition moment and rotational transition probabilities in CH. I. A 2Δ–X 2Π system , 1996 .
[21] F. Stuhl,et al. State‐resolved inelastic collisions of single rotational, fine‐structure, and Λ doublet levels of NH(A 3Π) with helium: A combined experimental and theoretical study , 1996 .
[22] M. Zachwieja. New Investigations of the A2Δ-X2Π Band System in the CH Radical and a New Reduction of the Vibration-Rotation Spectrum of CH from the ATMOS Spectra , 1995 .
[23] M. Osborne,et al. A fitting law for rotational transfer rates: An angular momentum model with predictive power , 1994 .
[24] J. Whitehead,et al. Rotational and Vibrational Energy Transfer in CH (B 2.SIGMA. , 1994 .
[25] C. Fotakis,et al. Rotational dependence of the quenching of electronically excited CH(A 2Δ) and CH (B 2Σ−) produced by laser photolysis of acetone at 193 nm , 1994 .
[26] A. Marks. A multiple hard-ellipsoid model for rotationally inelastic collisions , 1994 .
[27] K. Kohse-Höinghaus,et al. State-to-state rotational energy transfer in OH (A2Σ+, υ′=1) , 1993 .
[28] Colin J. Williams,et al. Rotational transfer, an angular momentum model , 1993 .
[29] J. Whitehead,et al. Rotational and vibrational energy transfer in CH(A2Δ) , 1993 .
[30] F. Stuhl,et al. Spectroscopic study of Λ‐doublet, spin, and rotational relaxation in the NH(A 3Π,v=0) state , 1992 .
[31] U. Meier,et al. State-specific rotational energy transfer in OH (A2Σ+, v′=0) by some combustion-relevant collision partners , 1992 .
[32] J. Whitehead,et al. Collisional removal rates for electronically excited CH radicals (B) and (C) , 1992 .
[33] M. Alexander,et al. Quantum scattering studies of inelastic collisions of NH(A 3Π) with helium: Fine‐structure and Λ‐doublet propensities , 1991 .
[34] F. Stuhl,et al. Electronic quenching of methylidyne(A2.DELTA.), imidogen(A3.PI.), imidogen(c1.PI.), and phosphinidene(A3.PI.) between 240 and 420 K , 1991 .
[35] K. Kohse-Höinghaus. Laser techniques for the quantitative detection of reactive intermediates in combustion systems , 1991 .
[36] H. Werner,et al. Quantum scattering study of rotational energy transfer in OH(A 2Σ+, v’=0) in collisions with He(1S) , 1990 .
[37] U. Meier,et al. Rotational energy transfer in OH (A 2Σ+, v’=0): A method for the direct determination of state‐to‐state transfer coefficients , 1990 .
[38] Hans-Joachim Werner,et al. Ab initio calculation of the OH (X 2Π, A 2Σ+)+Ar potential energy surfaces and quantum scattering studies of rotational energy transfer in the OH (A 2Σ+) state , 1990 .
[39] Deborah G. Sauder,et al. Rotationally inelastic collisions of a molecule in a 1Δ electronic state: NH(a 1Δ) , 1989 .
[40] D. Crosley. Rotational and translational effects in collisions of electronically excited diatomic hydrides , 1989 .
[41] M. J. Dyer,et al. Time-resolved CH (A(2)Delta and B(2)Sigma(-)) laser-induced fluorescence in low pressure hydrocarbon flames. , 1988, Applied optics.
[42] J. L. Kinsey,et al. A nomenclature for Λ‐doublet levels in rotating linear molecules , 1988 .
[43] William A. Wakeham,et al. The Forces Between Molecules , 1987 .
[44] D. Crosley,et al. Collisional quenching of CH A 2Δ, v' = 0 at 1300 K , 1987 .
[45] H. Rieley,et al. Collisionally induced rotational energy transfer within the A2Δ state of CH , 1987 .
[46] D. Crosley,et al. Energy transfer processes in CH A 2 Δ and B 2 Σ − in an atmospheric pressure flame , 1985 .
[47] M. Alexander,et al. Symmetry selection rules in inelastic collisions of diatomic molecules in 3Π electronic states , 1983 .
[48] M. Alexander. Rotationally inelastic collisions between a diatomic molecule in a2Pi electronic state and a structureless target , 1982 .
[49] I. Snook,et al. Solvation forces in simple dense fluids. II. Effect of chemical potential , 1981 .
[50] H. Rabitz,et al. Quantum number and energy scaling for nonreactive collisions , 1979 .
[51] D. Pritchard,et al. Simple scaling law for rotational-energy transfer in Na/sub 2/*-Xe collisions , 1978 .
[52] N. Elander,et al. Predissociation effects in the A, B, and C states of CH and the interstellar formation rate of CH via inverse predissociation. [Lifetime measurements, rotation-vibration levels] , 1976 .
[53] R. Levine,et al. Cross sections for rotational energy transfer: An information‐theoretic synthesis , 1976 .
[54] Bowen Liu,et al. Valence Excited States of CH. 111. Radiative Lifetimes , 1975 .
[55] John C. Polanyi,et al. Mechanism of Rotational Relaxation , 1972 .