Difference between revisions of "K Long and muon Detection"
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*Geometry (scintillator-Fe) optimization beyond Belle/II | *Geometry (scintillator-Fe) optimization beyond Belle/II | ||
*Simulation questions and needs | *Simulation questions and needs | ||
| − | ** implement a KLM-type structure and detector readout/response (Fun4All, | + | ** implement a KLM-type structure and detector readout/response (Fun4All, etc.) |
| − | ** study above issues: nominal and then performance vs. tradeoffs | + | ** study above issues: nominal and then any focused performance vs. tradeoffs |
== (Hadronic) calorimetry references == | == (Hadronic) calorimetry references == | ||
Revision as of 10:05, 4 July 2021
- K_Long and muon Detection (-4 < η < 1)
- Modest granularity Fe/Scintillator sampling, based on Belle-II KLM detector
Current design and implementation issues (in progress)
- K_L identification; neutrals measurement limitations
- Geometry (scintillator-Fe) optimization beyond Belle/II
- Simulation questions and needs
- implement a KLM-type structure and detector readout/response (Fun4All, etc.)
- study above issues: nominal and then any focused performance vs. tradeoffs
(Hadronic) calorimetry references
- Richard Wigman's Annual Review article (the bible) [1]
- NuTeV Fe-scintillator sampling calorimeter and "thin" HCAL implications [2]
- Example of a Fe-scintillator hodoscopic hadron calorimeter [3]
- Belle superconducting solenoid magnet development paper [4] (url="https://doi.org/10.1007/978-1-4757-9047-4_25")
- Endcap scintillator KLM for Belle II [5]
- 3 May 2018. Leo Piilonen, BNL Focused KLM-Readout Review (slides) [6]
- Belle II detector drawing (top view) [7]
