Chebyshev solution of large linear systems.
Solution of linear system of equations with singularity and stabile with respect to small changes in matrix elements
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Solution of linear system of equations with singularity and stabile with respect to small changes in matrix elements
S matrix elements for diatomic molecule rotational excitation by scattered atom computed by Amplitude Density Functions method
Additional matrix elements necessary for third approximation to viscosity of multicomponent gas mixtures
Report presents the finite difference equations in time and finite element matrix equations in space for general linear thermovisoelastic problems. The equations are derived for a general three-dimensional body but are applicable to one- and two-dimensional configurations with minor changes.
Finite difference and finite element matrix equations for linear thermoviscoelastic material
Direct Coulomb interaction matrix elements between hydrogen atoms in ground states calculated, presenting interaction potential
Full wave calculation of gravity waves for thermospheric model, describing wave type reflection, transmission, conversion and coupling by scattering matrix elements
Lumped and distributed parameter systems, discussing transfer matrix elements, connecting lines, etc
Off-diagonal matrix elements of Breit interaction between singlet-triplet transitions for helium isoelectronic sequences
Matrix elements of nonadiabatic perturbation emphasized in semiempirical theory for evaluating polyatomic molecules radiationless rate constants in terms of electronic-vibrational state
Time dependent matrix elements for multistate impact-parameter calculations for atom-atom inelastic cross sections
Polarized light scattering angle relationship with Mueller matrix elements for polydisperse systems of irregular randomly oriented particles
Nucleus energy spectra projection from Hartree- Fock intrinsic wave functions model space, using coupled orbital matrix elements
Inelastic scattering transition densities in single particle operator reduced matrix elements between initial and final nuclear states for nucleon angular momentum calculations
Computer program for solving attitude error equations related to gimballed platform is described. Program generates matrix elements of attitude error equations when initial matrices and trigonometric identities have been defined. Program is written for IBM 360 computer.
For the first time the Brueckner-Hartree-Fock (BHF) method was applied to nuclei whose intrinsic structure is nonspherical. One aim was to investigate whether the energy dependent reaction matrix calculated from a realistic nucleon-nucleon interaction leads to deformations similar to, or different from, those obtained from energy independent interactions in Hartree-Fock (HF) calculations. Reaction matrix elements were calculated as a function of starting energy for the Hamada-Johnston interaction, using a Pauli operator appropriate to O-16 and a shifted oscillator spectrum for virtual excited states. Binding energies, single-particle energies, radii, and shape deformations of the intrinsic state in unrenormalized as well as renormalized BHF are discussed and compared with previous HF studies. Results are presented for C-12, O-16, and Ne-20.
The Brueckner-Hartree-Fock (BHF) method has been applied to nuclei whose intrinsic structure is nonspherical. Reaction matrix elements were calculated as functions of starting energy for the Hamada-Johnston interaction using the Pauli operator appropriate to O-16 and a shifted oscillator spectrum for virtual excited states. Binding energies, single particle energies, radii, and shape deformations of the intrinsic state, in ordinary as well as renormalized BHF, are discussed and compared with previous HF studies and with experiment when possible. Results are presented for C-12, 0-16 and Ne-20. It is found that the binding energies and radii are too small, but that separation energies are well reproduced when the renormalized theory is used.
Cross sections and kinematic distributions for the trident production process plus or negative muon plus charge yields plus or minus muon plus electron plus positron plus charge (with charge = dipion moment and Fe) are given for beam energies of 100 to 300 GeV at fixed (electron positron) masses from 5 to 15 GeV. This process is interesting as a test of quantum electrodynamics at high energies, and in particular as a test of the form of the photon propagator at large timelike (four-momentum) squared. For this purpose, it is desirable to impose kinematic cuts that favor those Bethe-Heitler graphs which contain a timelike photon propagator. It is found that there are substantial differences between the kinematic distributions for the full Bethe-Heitler matrix element and the distributions for the two timelike-photon graphs alone; these differences can be exploited in the selection of appropriate kinematic cuts.