2013
DOI: 10.1103/physreva.88.013415
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Breakup ofH2+by photon impact

Abstract: Total and partial cross sections for breakup of ground rovibronic state of H + 2 by photon impact are calculated using the exact nonadiabatic nonrelativistic Hamiltonian without approximation. The converged results span six orders of magnitude. The breakup cross section is divided into dissociative excitation and dissociative ionization. The dissociative excitation channels are divided into contributions from principal quantum numbers 1 through 4. For dissociative ionization the fully differential cross sectio… Show more

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Cited by 12 publications
(12 citation statements)
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References 67 publications
(96 reference statements)
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“…In this figure the present results are compared with an exact numerical treatment using the full grid in the electronic coordinates and bond length, and with the Born-Oppenheimer approximation at the equilibrium bond length of 2a 0 . As already mentioned, such exact results have previously been reported by us [61] and more recently in Ref. [62].…”
Section: H + 2 Photoionization Cross Sectionssupporting
confidence: 80%
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“…In this figure the present results are compared with an exact numerical treatment using the full grid in the electronic coordinates and bond length, and with the Born-Oppenheimer approximation at the equilibrium bond length of 2a 0 . As already mentioned, such exact results have previously been reported by us [61] and more recently in Ref. [62].…”
Section: H + 2 Photoionization Cross Sectionssupporting
confidence: 80%
“…As in Ref. [61], we additionally compare the results of the Chase approximation [69] which entails a convolution of the Born-Oppenheimer result over the wave packets of the initial and final vibrational states,…”
Section: H + 2 Photoionization Cross Sectionsmentioning
confidence: 99%
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“…We use atomic units unless otherwise stated. The theoretical description of the hydrogen molecular ion has been achieved in previous works employing cylindrical [28,29] or prolate spheroidal coordinates [30][31][32][33][34]. For the numerical respresentation of the molecular wave function, we here employ a single-center expansion using spherical harmonics, Y r l m ( ) to treat the angular degrees of freedom of the electron and a discrete variable representation combined with a finite element method (DVR) for the radial part of both the electronic (f i (r)) and nuclear (χ j (R)) components of the wave packet.…”
Section: Time-dependent Schrödinger Equation (Tdse)mentioning
confidence: 99%