M. Adinolfi et al.
Published in: Nucl. Instrum. Meth. A494 (2002) 326-331
Notes:
“Dual” readout: measure time on both sides of fiber ($t_{A,B}$); use average of $t_{A,B}$ as timing measurement, and $v*(t_A - t_B)$ as longitudinal position
N. Cartiglia et al.
Published in: arXiv:2603.10841 [hep-ex]
Notes:
MIP deposits charge non-uniformly along the track
Coulomb replusion between clusters make high (low) charge-density clusters experience stronger (weaker) repulsive force. smearing out the initial non-uniformity
Large deposits are amplified less because of gain saturation (high density lowers the bias field), regularizing the signal