Spectroscopy of HD+ in high angular momentum states

[1]  R. A. Kennedy,et al.  Vibration-rotation spectroscopy of the HD+ion near the dissociation limit: Part VI. Nuclear hyperfine interactions , 1991 .

[2]  James F. Babb,et al.  Electron-nuclear coupling in the hyperfine structure of the hydrogen molecular ion. , 1991 .

[3]  M. Bawendi,et al.  Laboratory observation of hot bands of H+3 , 1990 .

[4]  R. A. Kennedy,et al.  Relativistic corrections for the ground and first excited states of H+2, HD+ and D+2 , 1990 .

[5]  R. E. Moss,et al.  Variational calculations for high J, low ν levels of HD+ , 1989 .

[6]  J. Tennyson,et al.  Highly excited rovibrational states using a discrete variable representation: The H+3 molecular ion , 1989 .

[7]  R. E. Moss,et al.  Transformed hamiltonian theory for HD , 1989 .

[8]  A. Carrington,et al.  Spectroscopic observation of rotationally quasibound HD+ ions , 1988 .

[9]  A. Carrington,et al.  Vibration-rotation spectroscopy of the HD+ion near the dissociation limit: V. Direct measurement of the asymmetric electron distribution inυ=21 , 1988 .

[10]  A. Carrington,et al.  Vibration-rotation spectroscopy of the HD+ion near the dissociation limit: IV. Nuclear hypedine structure in thev=18–16 band , 1988 .

[11]  R. A. Kennedy,et al.  Vibrational levels of HD+ near dissociation , 1988 .

[12]  R. E. Moss,et al.  A transformed hamiltonian theory for HD+ near dissociation , 1988 .

[13]  J. Poll,et al.  On the higher vibration-rotational levels of HD+ and H2 + , 1986 .

[14]  Bishop,et al.  Breakdown of the Born-Oppenheimer approximation in the calculation of electric hyperpolarizabilities. , 1985, Physical review letters.

[15]  R. A. Kennedy,et al.  Vibration-rotation spectroscopy of the HD+ ion near the dissociation limit: III. Measurements of the ν = 17-15 and 20-17 bands: demonstration of an asymmetric electron distribution , 1985 .

[16]  J. Beynon,et al.  Rotational predissociation of H+.2 ions of different precursor origins , 1983 .

[17]  A. Carrington,et al.  Vibration-rotation spectroscopy of the HD+ ion near the dissociation limit , 1981 .

[18]  D. M. Bishop,et al.  Radiative corrections for the hydrogen molecular ion HD , 1981 .

[19]  A. D. Smith,et al.  Uniform semiclassical calculation of resonance energies and widths near a barrier maximum , 1981 .

[20]  Moshe Shapiro,et al.  A new method for the exact calculation of vibrational–rotational energy levels of triatomic molecules , 1979 .

[21]  R. E. Moss,et al.  On the relativistic corrections for H+2 , 1979 .

[22]  R. McEachran,et al.  Hyperfine structure in the hydrogen molecular ion , 1978 .

[23]  W. Liu,et al.  Energies and widths of quasibound levels (orbiting resonances) for spherical potentials , 1978 .

[24]  Maurice Cohen,et al.  The hyperfine structure of H + 2 , 1977 .

[25]  D. M. Bishop.  Relativistic corrections for H2+ and its isotopes , 1977 .

[26]  R. Ray,et al.  HYPERFINE STRUCTURE IN THE INFRARED SPECTRUM OF $HD^{+}$ , 1977 .

[27]  J. Maas,et al.  Unimolecular dissociation of H+2 and D+2 , 1975 .

[28]  J. Peek,et al.  Metastable states observable in the mass spectrum of H2 , 1975 .

[29]  B. R. Johnson,et al.  The multichannel log-derivative method for scattering calculations , 1973 .

[30]  M. Shapiro.  Dynamics of Dissociation. I. Computational Investigation of Unimolecular Breakdown Processes , 1972 .

[31]  Michael V Berry,et al.  Semiclassical approximations in wave mechanics , 1972 .

[32]  J. W. Cooley,et al.  An improved eigenvalue corrector formula for solving the Schrödinger equation for central fields , 1961 .

[33]  A. Riviere,et al.  Dissociation of H_{2}^{+} and He^{-} by Electric Fields , 1960 .