“…In addition, the electronic stopping of slow channelled ions has been predicted to oscillate with the projectile atomic number Z 1 by many theoretical and experimental studies [30][31][32]. This oscillation has also been observed specifically in single-crystalline Si [33][34][35][36], even though only one of these works is experimental, and employed samples are not well-defined. For amorphous targets, Z 1 oscillations have been observed e.g.…”
We present experiments demonstrating trajectory-dependent electronic excitations at low ion velocities, where ions are expected to primarily interact with delocalized valence electrons. The energy loss of H
“…In addition, the electronic stopping of slow channelled ions has been predicted to oscillate with the projectile atomic number Z 1 by many theoretical and experimental studies [30][31][32]. This oscillation has also been observed specifically in single-crystalline Si [33][34][35][36], even though only one of these works is experimental, and employed samples are not well-defined. For amorphous targets, Z 1 oscillations have been observed e.g.…”
We present experiments demonstrating trajectory-dependent electronic excitations at low ion velocities, where ions are expected to primarily interact with delocalized valence electrons. The energy loss of H
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