Transit time factor, , characterizes the energy gain of a particle passing through an acceleration gap. The energy change of the particle is given by
where is the charge of the particle, the maximum voltage difference between the gap, the initial phase, defined as the phase of the oscillating field at , compared to the crest. The expression of is given by
Consider a relativistic particle passing through an acceleration gap, and ignore the velocity change of the particle during this acceleration, such that the time is related with its longitudinal position by . The energy change is given by the integration:
where the second integration vanishes because the odd-function of .
as a function of is shown in the figure to the right. To maximize the acceleration efficiency the length of the gap needs to be chose wisely to let be as close to unity as possible. This can be done by choosing to be , for example.
However, if is too small, sparks will appear in the acceleration device as the gradient increases. There is little to be gained by reducing it to less than, say .
The equations above assumed a uniform and constant electric field in the derivation. Realistically, the field is a function of , where is the radius of the particle trajectory w.r.t. the center of acceleration gap, the longitudinal position, and the time.
The modified transit time factor is then
where is the zeroth order modified Bessel function, the zeroth order Bessel function, , and the drift-tube bore radius.