Dynamic Radiation Effects Induced by Short-Pulsed GeV U-Ion Beams in Graphite and h-BN Targets

<table class="table-group" id="tab3"><tr><td><table class="table"><tr><td class="thead-hr" colspan="3"><hr/></td></tr><tr class="thead"><td class="align_left"> </td><td class="align_center">SGL R6650</td><td class="align_center">HeBoSint D100</td></tr><tr><td class="thead-hr" colspan="3"><hr/></td></tr><tr><td class="align_left"><i>f</i><sub><i>b1</i>, fixed</sub> (kHz)</td><td class="align_center">7.69</td><td class="align_center">10.07</td></tr><tr><td class="align_left"><i>f</i><sub><i>b1,</i> free</sub> (kHz)</td><td class="align_center">5.32</td><td class="align_center">7.04</td></tr><tr><td class="align_left"><i>f</i><sub><i>tr</i></sub> (MHz)</td><td class="align_center">2.73</td><td class="align_center">3.62</td></tr><tr class="table-tr"><td colspan="3"><hr class="tbody-hr"/></td></tr></table></td></tr></table>

<div>Calculated first-order frequencies for bending and transversal elastic stress waves of isotropic graphite grade SIGRAFINE R6650 and h-BN grade HeBoSint D100.</div>

Shock and Vibration

tab3

Table 3

Table 3: Dynamic Radiation Effects Induced by Short-Pulsed GeV U-Ion Beams in Graphite and h-BN Targets 