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R&D on scintillation materials and photo-sensors for CALIFA. I. Durán on behalf of CWG (IPNO, LUND, IEM/CHALMERSS, USC. Work performed at home laboratories Prototype definition: In-beam tests. Properties of scintillating crystals. Intrinsic energy resolution, density
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R&D on scintillation materials and photo-sensors for CALIFA. I. Durán on behalf of CWG (IPNO, LUND, IEM/CHALMERSS, USC • Work performed at home laboratories • Prototype definition: In-beam tests
Properties of scintillating crystals • Intrinsic energy resolution, density • Maximum light emission • hygroscopic • price !!!! • Long enough to stop and measure high energy p and • High granularity in polar angle due to Lorentz boost.
Matching of scintillators and photo-sensors properties. • Crystal quality, Surface treatment, Wrapping • Election of the adequate photo-sensor • Optical coupling • Light collection uniformity • Shaping time • T and V dependence
R&D program: Crystal + photosensors • Push scintillation materials and photo-sensors producers. • Specify main characteristics for large scale production CsI(Tl), La3Br(Ce), La3Cl(Ce) and PMs, LAAPDs, PinD. In close contact with the Industry St.Gobain, AMCRYS, Lanzhou, SCIONIX,HAMAMATSU, Photonis… - CsI(Tl) has been retained for the Califa Barrel, offering an excellent trade-off performance/price. - LAAPDs provide the best results
Barrel Crystals • Two CsI(Tl) providers have been retained: AMCRYS(Ukraine), Lanzhou (China) AMCRYS Best quality and price. Comercial experience. Lund/Dubna good contact. Lanzhou Very good crystal quality. Interest in NUSTAR/R3B Scientific collaboration?
Wrapping the crystals • To maximise light collection crystals must be wrapped • Best results achieved using polished surfaces and ESR (VM2000)
About Non-Uniformity • (USC) • Light collection depends on the position where the primary energy was deposited. Why non-uniformity is a problem? • (LUND) • (IPNO) mask PM source 137Cs CsI (Tl) crystal dL/L <1 % requested from manufacturers By the time being, we are getting ~ 2 – 4 %
On the crystal's size Tests with realistic sizes following Barrel design Tests with small samples 1cm 13 cm M.Gascón USC
On the crystal's size • (IPNO)
CsI(Tl) with different LAAPD sizes • Different qualities received from Hamamatsu (Si thickness, frames, epoxi windows) PANDA Price 140 € unit (now ~500€) Dimensions: 7x14 mm2 CMS/PANDA Price 110 € unit (now ~500€) Dimensions: 10x10 mm2 R3B prototype Price (now ~2000 €) Dimensions: 10x20 mm2 M.Gascón USC
Energy resolution at Lund with 10x10 LAAPD (S8664) V. Avdeichikov LUND
Two CsI(Tl) with 20 x10 APDs FADC multichannel readout of CsI(Tl) crystals Digital filter avoid pile-up problems Time coincidence allow us add-back analysis M.Gascón USC
APD´s drift problem • The APD's Gain drifts with both Voltage and Temperature G(V,T) = G(Vo,To)(1.03V[volt] – 1.02T[deg]) • T range must be kept low enough to allow V feedback • In any case, both V and T must be slow-controlled (HELP!!!) I.Durán USC
CsI(Tl) with XP1452 at IPN-O • XP1452 green extended bialkali (Quantum efficiency 30% at 420nm, 20% at 550 nm) 9 stages 15 mm 35 mm 30 mm XP1452 • For CsI(Tl): Energy resolution of 5 - 5.5% seams reachable with XP1452 at 1MeV • Cross-Talk around 3 - 5 % (can be improved and easy to correct) • Resolution degrades with magnetic field (main constraint) • (IPNO)
CsI(Tl) with Photodiodes at Lund + PDs do’nt require neither temperature nor voltage stability - Significantly worse energy resolution and higher threshold ~100 keV The gamma energy-resolution depends strongly on the PinD noise level. A low-capacity (15 pF) PD with low current (< 1 nA) can give a resolution close to what an APD can provide. V. Avdeichikov LUND
Lanthanum-based crystals at IEM IEM-CSIC(Madrid)/ Chalmers
Lanthanum-based crystals at IEM IEM-CSIC(Madrid)/ Chalmers
Lanthanum-based crystals at IEM IEM-CSIC(Madrid)/ Chalmers
LUND ProtoZero beam-tests USC IPN-O Different solutions will be tested
CONCLUSIONS on R&D on scintillation materials and photo-sensors for CALIFA. • A lot of satisfactory work has been done • A lot of work remains to be done • Readout electronics and slow-control are open questions I. Durán – Gotenburgo 2008