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To a certain extent the larger vacancy island density island is also caused by the flux larger by a factor of 2 for =82-83° in comparison to that of =86°.
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We feel that this presentation of the channel has advantages over the usual plots of equipotential lines of the continuum potential, since our presentation includes the effect of atom shadowing, which is important at small perpendicular energies and for heavy projectiles.
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These values are obtained using χ (0) =πn d3 ψ22, where the acceptance angle ψ2 is given by Eq. 8, n is the atomic number density of the crystal, and d is the interatomic distance along the atomic string (Refs.).
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These values are obtained using χ (0) =πn d3 ψ22, where the acceptance angle ψ2 is given by Eq. 8, n is the atomic number density of the crystal, and d is the interatomic distance along the atomic string (Refs.).
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|