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Note that the detection sensitivity is less for measuring a loss signal, as in the case of the synchrotron, as opposed to a signal coming from the population of a new state. However, this can be (at least partly) compensated for by the fact that in a synchrotron elastic collisions contribute to the loss signal, and the elastic collision cross-sections are commonly larger than those for inelastic collisions
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Note that the detection sensitivity is less for measuring a loss signal, as in the case of the synchrotron, as opposed to a signal coming from the population of a new state. However, this can be (at least partly) compensated for by the fact that in a synchrotron elastic collisions contribute to the loss signal, and the elastic collision cross-sections are commonly larger than those for inelastic collisions.
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syn), i.e., when the molecules pass many gaps (bunchers) before completing one longitudinal oscillation. This condition is not strictly fulfilled in our case as the molecules pass only four gaps before completing an oscillation. This implies that the shape of the packet in phase-space changes as a function of the position in the ring; the position spread is larger at the gaps and smaller at the quarter-ring positions. Note that for molecules moving slower than 50 m/s the model breaks down completely, and the buncher is no longer stable.
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syn), i.e., when the molecules pass many gaps (bunchers) before completing one longitudinal oscillation. This condition is not strictly fulfilled in our case as the molecules pass only four gaps before completing an oscillation. This implies that the shape of the packet in phase-space changes as a function of the position in the ring; the position spread is larger at the gaps and smaller at the quarter-ring positions. Note that for molecules moving slower than 50 m/s the model breaks down completely, and the buncher is no longer stable.
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