Final State Three-Body Coulomb Effects in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">P</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mn>208</mml:mn></mml:mmultiscripts><mml:mo stretchy="false">(</mml:mo><mml:mmultiscripts><mml:mi mathvariant="normal">B</mml:mi><mml:mprescripts/><mml:none/><mml:mn>8</mml:mn></mml:mmultiscripts><mml:mo>,</mml:mo><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">B</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mn>7</mml:mn></mml:mmultiscripts><mml:mi>p</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">P</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mn>208</mml:mn></mml:mmultiscripts></mml:math>Coulomb Breakup Reaction
E. O. AltInstitut für Physik, Universität Mainz, D-55099 Mainz, GermanyB. F. IrgazievCyclotron Institute, Texas A&M University, College Station, Texas 77843A. M. MukhamedzhanovCyclotron Institute, Texas A&M University, College Station, Texas 77843
ABI
Аннотация
We present results of the first calculation of the double differential cross section for the $^{208}\mathrm{P}\mathrm{b}(^{8}\mathrm{B},^{7}\mathrm{B}\mathrm{e}p)^{208}\mathrm{P}\mathrm{b}$ Coulomb breakup reaction which treats the postdecay acceleration of the ejectiles within a genuine three-body approach. From this we conclude that, in order to minimize postdecay Coulomb acceleration effects, experiments should be performed at as small as possible scattering angles, not too low $^{7}\mathrm{B}\mathrm{e}\ensuremath{-}p$ relative energies, and high incident energy.
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