Fundamental bound on scintillation timing
In plain words
Light arrives at the sensor at random times, which sets a floor on how precisely the arrival can be timed. The exact floor for realistic detectors is not established.
Precise statement
Derive the Cramer-Rao lower bound (the minimum variance any unbiased estimator can reach) on timing precision for a scintillation detector including non-exponential rise and decay, position-dependent light transport inside the crystal, photodetector single-photon time response and dark counts, and construct an estimator reaching it. An answer is the bound as a function of photon yield, rise time, decay time and transit-time spread, plus a realizable estimator.
What would settle it
A derivation with an estimator demonstrated in simulation and on bench data to approach the bound.
Status in the literature
Unverified note: it names recent work and was partly written without a live literature search; it awaits a check by an editor.
Bounds exist for simplified emission models since Seifert, van Dam and Schaart (2012); the realistic transport case was not closed as of 2025.
Parent problems
- Special case of Is 10 ps coincidence time resolution reachable? · open · from revision 1
Results
No results have been posted on this problem yet.
Post a result · how results are checked
Sign in to follow or save this problem
Comments (0)
Comments are not records: they are not signed, stamped or logged. How comments work
No comments yet.
Sign in to comment.