An ab initio study of singlet and triplet Rydberg states of N2
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[1] S. Kotochigova. Controlling interactions between highly magnetic atoms with Feshbach resonances , 2014, Reports on progress in physics. Physical Society.
[2] Nadia Balucani,et al. CRITICAL REVIEW OF N, N+, N+2, N++, And N++2 MAIN PRODUCTION PROCESSES AND REACTIONS OF RELEVANCE TO TITAN'S ATMOSPHERE , 2013 .
[3] S. Guberman. Spectroscopy above the ionization threshold: dissociative recombination of the ground vibrational level of N2+. , 2012, The Journal of chemical physics.
[4] Jonathan Tennyson,et al. UKRmol: a low-energy electron- and positron-molecule scattering suite , 2012, The European Physical Journal D.
[5] J. Tennyson,et al. Positron collisions with molecular hydrogen: cross sections and annihilation parameters calculated using the R-matrix with pseudo-states method , 2011 .
[6] M. Hochlaf,et al. Valence–Rydberg electronic states of N2: spectroscopy and spin–orbit couplings , 2010 .
[7] Jonathan Tennyson,et al. Electron–molecule collision calculations using the R-matrix method , 2010 .
[8] M. Hochlaf,et al. Quintet electronic states of N2. , 2010, The Journal of chemical physics.
[9] Jonathan Tennyson,et al. R-matrix calculation of low-energy electron collisions with uracil. , 2009, The Journal of chemical physics.
[10] J. P. Sprengers,et al. Structure and predissociation of the 3psigma(u)D (3)Sigma(u) (+) Rydberg state of N(2): first extreme-ultraviolet and new near-infrared observations, with coupled-channels analysis. , 2008, Journal of Chemical Physics.
[11] S. Gibson,et al. A coupled-channel model of the 3Pi(u) states of N2: structure and interactions of the 3ssigma(g)F3 3Pi(u) and 3ppi(u)G3 3Pi(u) Rydberg states. , 2008, The Journal of chemical physics.
[12] M. Hochlaf,et al. Sign reversal of the spin-orbit constant for the C 3Pi(u) state of N2. , 2008, The Journal of chemical physics.
[13] S. Guberman. Role of excited core Rydberg states in dissociative recombination. , 2007, The journal of physical chemistry. A.
[14] H. Michels. ELECTRONIC STRUCTURE OF EXCITED STATES OF SELECTED ATMOSPHERIC SYSTEMS , 2007 .
[15] J. Tennyson,et al. R-matrix calculation of the potential energy curves for Rydberg states of carbon monoxide , 2006 .
[16] T. Hashimoto,et al. A predissociative triplet Rydberg state of the nitrogen molecule studied by near-infrared diode laser kinetic spectroscopy , 2006 .
[17] C. Cossart-Magos,et al. New Rydberg-Rydberg transitions in N2. Identification of the d3 1Σg+ state , 2004 .
[18] J. P. Sprengers,et al. Pump-probe lifetime measurements on singlet ungerade states in molecular nitrogen , 2004 .
[19] J. Tennyson. Partitioned R-matrix theory for molecules , 2004 .
[20] J. Tennyson,et al. Program Summary , 2000 .
[21] W. Meyer,et al. Dipole-allowed excited states of N2: Potential energy curves, vibrational analysis, and absorption intensities , 2001 .
[22] J. Tennyson,et al. Dissociative recombination of NO+: calculations and comparison with experiment , 2000 .
[23] W. Ubachs,et al. Observation of the gamma(IIg)-I-1-c '(1)(4)Sigma(+)(u) and k(1)II(g)-c '(1)(4)Sigma(+)(u) systems of N-2 , 1999 .
[24] J. Tennyson,et al. Comment on `Potential energy surfaces of excited states of H2−' (Chem. Phys. Lett. 285 (1998) 114–120) , 1999 .
[25] J. Dormand,et al. Continuous approximation with embedded Runge-Kutta-Nyström methods , 1999 .
[26] J. Tennyson,et al. The UK molecular R-matrix codes , 1998 .
[27] Launay,et al. The High-Resolution Vacuum Ultraviolet Emission Spectrum of Molecular Nitrogen from 82.6 to 124.2 nm: Level Energies of 10 Excited Singlet Electronic States , 1998, Journal of molecular spectroscopy.
[28] M. Fujitake,et al. Near-Infrared Diode Laser Spectroscopy of the Nitrogen Molecule in Rydberg State: Analysis of thec1Πu−a″1Σg+,v= 1–0 Band , 1997 .
[29] J. Tennyson,et al. R-matrix calculations for polyatomic molecules: electron scattering by , 1997 .
[30] J. Tennyson,et al. CORRIGENDUM: Ab initio potential energy curves of Rydberg, valence and continuum states of NO , 1997 .
[31] J. Tennyson. R-matrix calculation of Rydberg states of CO , 1996 .
[32] J. Tennyson,et al. R-matrix calculation of the bound and continuum states of the - system , 1996 .
[33] J. Tennyson. A new algorithm for Hamiltonian matrix construction in electron - molecule collision calculations , 1996 .
[34] Jonathan Tennyson,et al. The UK Molecular R-Matrix Scattering Package: a Computational Perspective , 1995 .
[35] P. Cosby,et al. Charge-transfer production of predissociated N2 states. I. The n = 3 Rydberg state region (12.8–14 eV) , 1994 .
[36] F. Rostas,et al. The Electronic Ground State of Molecular Nitrogen , 1993 .
[37] P. Levelt,et al. XUV-laser spectroscopy on the c′41∑+u, v = 0 and c31Πu, v = 0 Rydberg states of N2 , 1992 .
[38] J. Tennyson,et al. Bound states using the R-matrix method: Rydberg states of HeH , 1991 .
[39] J. Subtil,et al. New emission bands in the high resolution spectrum of molecular nitrogen between 107.7 and 124.2nm , 1991 .
[40] C. Jungen,et al. High‐resolution jet absorption study of nitrogen near 800 Å , 1990 .
[41] F. Launay,et al. Vacuum ultraviolet emission from highly excited states of molecular nitrogen , 1989 .
[42] M. Seaton. Use of the R matrix method for bound-state calculations. I. General theory , 1985 .
[43] R. D. Verma,et al. Absorption spectrum of the b'1Σu+ from X1Σg+ transition of the N2 molecule excited by the flash discharge technique , 1984 .
[44] F. Launay,et al. Evidence for Predissociation of N 2 into N( 2 D)+N( 2 D) from New High-Resolution Vacuum-Ultraviolet Emission Bands , 1984 .
[45] K. Dressler,et al. Nonadiabatic representations of the 1Σ+u and 1Πu states of the N2 molecule , 1983 .
[46] M. Kakimoto,et al. High-resolution optogalvanic study of the c4(0)1Πu, c′5(0)1Σu+, and a″(0)1Σg+ Rydberg states of N2 , 1982 .
[47] A. D. McLean,et al. Ab initio study of valence-state potential energy curves of nitrogen , 1982 .
[48] Paul H. Krupenie,et al. The spectrum of molecular nitrogen , 1977 .
[49] R. Singh,et al. Potential-energy curves for O2+, N2+, and CO+ , 1966 .