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Charge exchange between bare beryllium and boron with metastable hydrogen atoms at low energies

Theoretical results for [sup 9]Be[sup 4+]-H(2[ital s]) and [sup 11]B[sup 5+]-H(2[ital s]) partial and total charge-exchange cross sections at low relative velocities (0.027--0.32 a.u.) are given, using the Landau-Zener method. The necessary molecular parameters for this method are obtained from the...

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Published in:Physical review. A, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 1993-11, Vol.48 (5A), p.3680-3683
Main Author: CASAUBON, J. I
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description Theoretical results for [sup 9]Be[sup 4+]-H(2[ital s]) and [sup 11]B[sup 5+]-H(2[ital s]) partial and total charge-exchange cross sections at low relative velocities (0.027--0.32 a.u.) are given, using the Landau-Zener method. The necessary molecular parameters for this method are obtained from the exact one-electron diatomic molecule (OEDM) molecular energies. The partial cross sections which are mainly populated are those corresponding to the principal quantum number of separated atoms [ital n]=5 for Be[sup 3+] and [ital n]=6 for B[sup 4+]. The total cross sections show a rather strong increase with increasing collision energies and a quite large maximum. They lie between the cross sections corresponding to the neighbor reactions for the incident nuclei with [ital Z]=3 (Li), [ital Z]=6 (C), and [ital Z]=7 (N). The atomic collisions with beryllium are very important in plasma tokamaks.
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A, Atomic, molecular, and optical physics</jtitle><addtitle>Phys Rev A</addtitle><date>1993-11-01</date><risdate>1993</risdate><volume>48</volume><issue>5A</issue><spage>3680</spage><epage>3683</epage><pages>3680-3683</pages><issn>1050-2947</issn><eissn>1094-1622</eissn><coden>PLRAAN</coden><abstract>Theoretical results for [sup 9]Be[sup 4+]-H(2[ital s]) and [sup 11]B[sup 5+]-H(2[ital s]) partial and total charge-exchange cross sections at low relative velocities (0.027--0.32 a.u.) are given, using the Landau-Zener method. The necessary molecular parameters for this method are obtained from the exact one-electron diatomic molecule (OEDM) molecular energies. The partial cross sections which are mainly populated are those corresponding to the principal quantum number of separated atoms [ital n]=5 for Be[sup 3+] and [ital n]=6 for B[sup 4+]. The total cross sections show a rather strong increase with increasing collision energies and a quite large maximum. They lie between the cross sections corresponding to the neighbor reactions for the incident nuclei with [ital Z]=3 (Li), [ital Z]=6 (C), and [ital Z]=7 (N). The atomic collisions with beryllium are very important in plasma tokamaks.</abstract><cop>College Park, MD</cop><pub>American Physical Society</pub><pmid>9910036</pmid><doi>10.1103/PhysRevA.48.3680</doi><tpages>4</tpages></addata></record>
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ispartof Physical review. A, Atomic, molecular, and optical physics, 1993-11, Vol.48 (5A), p.3680-3683
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language eng
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source American Physical Society:Jisc Collections:APS Read and Publish 2023-2025 (reading list)
subjects ALKALINE EARTH ISOTOPES
ATOM COLLISIONS
Atomic and molecular collision processes and interactions
ATOMIC AND MOLECULAR PHYSICS
BERYLLIUM 9
BERYLLIUM IONS
BERYLLIUM ISOTOPES
BORON 11
BORON IONS
BORON ISOTOPES
CATIONS
CHARGE EXCHANGE
Charge transfer
CHARGED PARTICLES
COLLISIONS
ELEMENTS
ENERGY LEVELS
ENERGY RANGE
EVEN-ODD NUCLEI
Exact sciences and technology
EXCITED STATES
HYDROGEN
ION COLLISIONS
ION-ATOM COLLISIONS
IONS
ISOTOPES
LANDAU-ZENER FORMULA
LIGHT NUCLEI
METASTABLE STATES
MULTICHARGED IONS
NONMETALS
NUCLEI
ODD-EVEN NUCLEI
Physics
STABLE ISOTOPES 664300 -- Atomic & Molecular Physics-- Collision Phenomena-- (1992-)
title Charge exchange between bare beryllium and boron with metastable hydrogen atoms at low energies
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