A comparative nearside-farside analysis of the He–N2+ and He–N2 inelastic collisions

[1]  T. Stoecklin,et al.  Strong isotope effect in ultracold collision of N{sub 2}{sup +} ({nu}=1, j=0) with He: A case study of virtual-state scattering , 2005 .

[2]  A. Voronin,et al.  Rotational excitation and de-excitation of HF molecules by He atoms , 2005 .

[3]  R. Krems Molecules near absolute zero and external field control of atomic and molecular dynamics , 2005, physics/0504156.

[4]  J. Black,et al.  An atomic and molecular database for analysis of submillimetre line observations , 2004, astro-ph/0411110.

[5]  R. Krems,et al.  Editorial: Quo vadis, cold molecules? , 2004 .

[6]  J. Rayez,et al.  Vibrational deactivation of F2(ν=1,j=0) by 1H at very low energy , 2004 .

[7]  J. Rayez,et al.  Vibrational deactivation of F{sub 2}({nu}=1, j=0) by {sup 3}He at very low energy: A comparative study with the He-N{sub 2} collision , 2003 .

[8]  B. Martínez-Haya,et al.  Low temperature rotational relaxation of N2 in collisions with He , 2003 .

[9]  J. Rayez,et al.  Vibrational quenching of N 2 ( ν = 1 , j rot = j ) by 3 He : Surface and close-coupling calculations at very low energy , 2002 .

[10]  J. Connor,et al.  Nearside–farside analysis of differential cross sections using Jacobi functions of the first and second kinds: Application to Ar+N2 rotationally inelastic scattering , 2001 .

[11]  J. Connor,et al.  Nearside−Farside Analysis of Differential Cross Sections: Ar + HF Rotationally Inelastic Scattering† , 2001 .

[12]  J. Connor,et al.  Semiclassical nearside–farside theory for inelastic and reactive atom–diatom collisions , 1999 .

[13]  J. Connor,et al.  Nearside–farside analysis of differential cross sections: Ar+N2 rotationally inelastic scattering using associated Legendre functions of the first and second kinds , 1998 .

[14]  A. S. Dickinson,et al.  Semi-classical and quantal calculation of state-to-state generalized cross-sections for N+2-He mixtures , 1998 .

[15]  J. Connor,et al.  Nearside–farside analysis of differential cross sections: Diffraction and rainbow scattering in atom–atom and atom–molecule rotationally inelastic sudden collisions , 1996 .

[16]  H. Rabitz,et al.  A general method for constructing multidimensional molecular potential energy surfaces from ab initio calculations , 1996 .

[17]  D. Colbert,et al.  A novel discrete variable representation for quantum mechanical reactive scattering via the S-matrix Kohn method , 1992 .

[18]  Hatchell Pj Evaluation of semiclassical trajectory contributions to the cross section. , 1989 .

[19]  F. Gianturco,et al.  Computed rotational rainbows from realistic potential energy surfaces , 1985 .

[20]  M. Raimondi Valence body study of the potential energy surface for the system He … HF , 1984 .

[21]  A. Sapse Ab initio studies of weakly bound complexes between some nonpolar molecules and hydrogen fluoride , 1983 .

[22]  R. Anderson Solution of vibrational excitation problems with constant step size Magnus propagators: Convergence, perturbation analysis, and approximate decoupling , 1982 .

[23]  R. Watts,et al.  The helium-hydrogen fluoride potential surface , 1981 .

[24]  J. Connor,et al.  Complex angular momentum analysis of diffraction scattering in atomic collisions , 1981 .

[25]  J. Launay Molecular collision processes. I. Body-fixed theory of collisions between two systems with arbitrary angular momenta , 1977 .

[26]  R. C. Fuller Qualitative behavior of heavy-ion elastic scattering angular distributions , 1975 .

[27]  G. C. Wick,et al.  On the general theory of collisions for particles with spin , 1959 .