2004
DOI: 10.1103/physreva.69.022705
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Calculated total cross sections of electron-impact ionization and excitations in tetrahedral(XY4)andSF

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Cited by 114 publications
(68 citation statements)
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“…The potential terms in V (r, E i ) are derived from the target charge density. The molecular charge density is constructed through a single centre expansion of the atomic charge density at the molecular centre of mass as in [23]. While the (repulsive) static potential V st (r ) is directly calculated from the target charge density, the polarization effects are included through the positron polarization potential V pol (r ) as given by Zhang et al [24].…”
Section: Theorymentioning
confidence: 99%
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“…The potential terms in V (r, E i ) are derived from the target charge density. The molecular charge density is constructed through a single centre expansion of the atomic charge density at the molecular centre of mass as in [23]. While the (repulsive) static potential V st (r ) is directly calculated from the target charge density, the polarization effects are included through the positron polarization potential V pol (r ) as given by Zhang et al [24].…”
Section: Theorymentioning
confidence: 99%
“…Our aim is now to deduce Q ion from our calculated Q inel in the same way as in the electron scattering. Hence to find the contribution of Q ion in Q inel we introduce a method which we have applied previously [1,23,[28][29][30][31] for electron impact on several atomic and molecular targets. To proceed along these lines, we have to first obtain Q inel without Ps-formation cross-section.…”
Section: Theorymentioning
confidence: 99%
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“…The total cross sections such as the total elastic (Q el ) and the total inelastic cross sections (Q inel ) can be derived from the scattering matrix [29]. The sum of these cross sections will then give the total scattering cross section (TCS) Q T [30].…”
Section: High-energy Formalismmentioning
confidence: 99%
“…High-energy electron scattering is modeled using the well-established SCOP formalism [29,30], which employs a partial-wave analysis to solve the Schrödinger equation with various model potentials as its input. The interaction of the incoming electron with the target molecule can be represented by a complex potential comprising real (V R ) and imaginary parts (V I ) as…”
Section: High-energy Formalismmentioning
confidence: 99%