Documents
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Publications
- Ho-San Ko, Neutral Pion Electroproduction and development of a Neutral Particle Spectrometer, tel-02927155, 2020UPASS129 (2020)
- T. Horn, V.V. Berdnikov, et al., Scintillating crystals for the Neutral Particle Spectrometer in Hall C at JLab, Nucl. Inst. Meth. A, Volume 956, 11 March 2020, 163375
- T. Horn, A PbWO4-based Neutral Particle Spectrometer in Hall C at 12 GeV JLab, J.Phys.Conf.Ser. 587 (2015) 1, 012048 (CALOR2014 Proceedings)
PAC Presentations and NPS Physics Notes
PAC46: TCS
PAC45: WACS polarization observables
PAC43: WACS polarization observables, TCS LOI
PAC42: WACS, pi0 photoproduction
PAC40: DVCS/pi0 cross sections, SIDIS pi0, WACS
Physics Notes
DVCS/pi0 Cross Sections and SIDIS pi0
Wide-Angle Compton Scattering (WACS)
WACS Neutral Pion Photoproduction
Magnet
Calorimeter
NPS Geant4 simulation for Hall C DVCS
- GitHub: use DVCS_evt_gen/.
- Information for 2023 update to Ho San KO GEANT4 model: NPS_GEANT.pdf
NPS Beamline Technical Drawings
NPS software and calibration
- Energy Calibration of NPS Calorimeter, June 2020 == [jroche] There is a mistake in the evaluation of match between the vertical coverage of the HMS and of the calorimeter. This 2020 document will be updated shortly, but for now, it is better to read this document.
Crystal characterization
- Table of results of SICCAS crystals produced in 2014 and 2015 - measurements carried out at CUA
- Results of tests of subsets of the 10+5 SICCAS produced crystals (2014) at Giessen, BNL, and Caltech
- Results of crystals 2, 3, 6, 8, and 9 from Giessen:
- Absorption coefficient
- Transmittance
- Light Yields: LY_2, LY_3, LY_6, LY_8, LY_9
- PbWO4 references:
- P. Adzic et al., "Radiation Hardness qualification of PbWO4 scintillation crystals for the CMS Electromagnetic Calorimeter", CMS Note 2009/016
- A.A. Annenkov et al., "Lead Tungstate scintillation material", NIM A 490 (2002) 30-50
- P. Yang et al., "Growth of large-size crystal of PbWO4 by vertical Brigdman method with multi-crucibles
- R. W. Novotny, "The Electromagnetic Calorimetry of the PANDA Detector at FAIR", J. Phys. Conf. Serv. 404 012063 (2012)
PMTs
- PMT specs: Hamamatsu R4125, 19mm diameter, gain is about 8.7E+5 at 1.5kV max. anode voltage and rise time 2.5ns. This PMT was also used in Primex and we have designed a new active voltage divider that improves the performance of the PMT by a factor of 25. See the report at the 2012 IEEE NSS/MIC/RTSD conference by V. Popov and H. Mkrtchyan.
Hamamatsu PMT Specs 11 Oct 2013, C.E.Hyde
- specs on standard 1" PMTs:
- R8619 10 stage PMT
- R9800 8 stage PMT
- Low profile (short) 29mm R7111 PMT Media:R7111.pdf
- Mesh Dynode PMT (30x30 mm2) Media:R11187_data_sheet_0911.pdf R11187=replacement for Hall A DVCS R7877
- Magnetic Field Response Media:R7877_Magnetic_Field_Characteristics.pdf
- Cathode Lifetime data Media:QG1369A_R7877_Life.pdf
- R7525 29mmφ PMT Media:R7525-TPMH1244E02.pdf
- R4125 19mmφ (Standard for PbWO4)
- Magnetic Field Response Media:R4125_Effects_of_Magnetic_Fields.pdf
- Cathode Lifetime data Media:R4125_(100_uA_&_1000_h)_QG0016B.pdf
NPS Dose Rate Estimates
Scattering Chamber Information:
- outer diameter = 45 inches
- inner diameter = 43.125 inches
- distance beam line to SHMS window = 1.25 inches
So for a point target, the minimum angle is 58 mr or 3.4 degrees. For an extended target you will need to adjust, it becomes about 4 degree for a 15 cm target. So assume 3.5 degrees as rough number.
Study of possibilities for larger beam pipe assemblies
Energy spectra for electrons, photons, positrons including fits
Rates and rates per crystal vs. angle relative to beam for: 4 m from target, 6.6 GeV beam energy, 1uA beam current, and 10-cm LH2 target for:
History of the NPS (2012)
Light monitoring and Curing System
Notes on Light Monitoring System from Hamlet
Notes on Curing System from Hamlet
Electronics
- Experimental requirements on hardware: