Electron scattering from the fine structure levels within the 1s22s22p2 3Pe ground state of C I

The authors have calculated cross sections for elastic and inelastic scattering from the fine structure levels within the 1s22s22p2 3Pe ground state of C I using the R-matrix method. They include the states 1s22s22p2 3Pe, 1De, 1Se in the expansion of the total wavefunction, plus 3So, 3Po and 3Do polarisation pseudostates to allow for the ground state polarisability. The fine structure energy splittings are included explicitly. The authors present collision strengths for the inelastic transitions, averaged over a Maxwellian electron velocity distribution, for electron temperatures from 7.5 to 10000 K.

[1]  M. Silber,et al.  Detection of the 370 micron 3P2-3P1 fine-structure forbidden line of C I , 1985 .

[2]  J. Croskery,et al.  VPM — A new asymptotic package , 1982 .

[3]  P. Burke,et al.  Electron scattering by atoms and ions using the Breit-Pauli Hamiltonian: An R-matrix approach , 1980 .

[4]  Thomas G. Phillips,et al.  Detection of the 610 micron /492 GHz/ line of interstellar atomic carbon , 1980 .

[5]  R. Nesbet Atomic polarizabilities for ground and excited states of C, N, and O , 1977 .

[6]  A. Hibbert,et al.  Atomic polarizabilities and polarized pseudo-states in the multiconfigurational approach. II. First row atoms and ions , 1977 .

[7]  M. L. Dourneuf,et al.  Ab initio calculation of atomic negative-ion states in the polarized frozen-core approximation. I. The attachment energies for O-(2P0) and C-(4S0) , 1977 .

[8]  M Le Dourneuf,et al.  Electron impact excitation of fine-structure levels of atomic oxygen , 1976 .

[9]  P. Burke,et al.  Atomic polarizabilities and polarized pseudo-states in the multiconfigurational approach. I. Theory and application to C, N and O , 1976 .

[10]  M. Gailitis New forms of asymptotic expansions for wavefunctions of charged-particle scattering , 1976 .

[11]  R. Nesbet,et al.  Low-energy electron scattering by atomic carbon , 1975 .

[12]  W. C. Lineberger,et al.  Binding energies in atomic negative ions , 1975 .

[13]  R. Nesbet,et al.  Matrix variational calculations of electron scattering by C, N, and O atoms , 1974 .

[14]  M. Krauss,et al.  COUPLED MULTICONFIGURATIONAL SELF-CONSISTENT-FIELD METHOD FOR ATOMIC DIPOLE POLARIZABILITIES. I. THEORY AND APPLICATION TO CARBON. , 1972 .

[15]  Norman Scott,et al.  A general program to calculate atomic continuum processes incorporating model potentials and the Breit-Pauli Hamiltonian within the R-matrix method , 1984 .

[16]  M. Seaton,et al.  Impact, a program for the solution of the coupled integro-differential equations of electron-atom collision theory , 1984 .

[17]  H. Werner,et al.  Finite perturbation calculations for the static dipole polarizabilities of the first-row atoms , 1976 .

[18]  W. D. Robb,et al.  R-matrix theory of atomic processes , 1975 .