Status of sensor R&D in Minsk
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Transcript of Status of sensor R&D in Minsk
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Apr 20, 2023 FCAL collaboration workshop, 2009
. Status of sensor R&D in Minsk
K. Afanaciev, M. Baturitsky, I. Emeliantchik, A. Ignatenko, A. Litomin, V. Shevtsov
FCAL Collaboration Meeting, Zeuthen2009
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Apr 20, 2023 FCAL collaboration workshop, 2009
Availible technology
Synthetic monocrystalline diamonds produced by “ADAMAS” plant near Minsk (www.bsuproduct.by/index.php/.91....1.0.0.html)
The diamond plate size of 5x5 mm area and 200-1000 um thicknessDifferent catalytic environments and synthesis conditions are investigated in order to reduce the impurity content.The detectors could be used in beam monitoring and similar applications.
Our institute have the following facilities CCD measurement setup Absorption spectroscopy setup (optical)
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Apr 20, 2023 FCAL collaboration workshop, 2009
Current work
“Adamas” is working on the optimisation of synthesis processWe are working on establishing the selection criteria to distinguish“detector grade” crystals without cutting and metallisationOptical absorption spectroscopy
CCD ~ 25 um
Lower N content -> edge closer to UV -> better detector properties
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Apr 20, 2023 FCAL collaboration workshop, 2009
Current work
A number of samples were investigated - so far the samples with “good” optical spectrum show CCD above the average ~20 vs < 10 um
Thermobaric treatment seems to improve the detector propertiesAt the moment we are investigateing this.
A few new crystals were selected on the basis of optical spectraand measured. The best have about 25 um CCD. We are going tomake measurements after the thermobaric treatment.
Investigation of different catalytic environments and their influence
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Apr 20, 2023 FCAL collaboration workshop, 2009
Future work
Nitrogen pulse laser will be used for optical fluorescence spectrocopyThis will allow to get more information about impurities and improvethe selection process
A number of newsynthesis thechniqueswill be tried outby ADAMAS
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Apr 20, 2023 FCAL collaboration workshop, 2009
Absorption setup
Xenon pulse lampPX-2
MonochromatorMDR-12
PMT ADC
Stepmot.cont.
Computer
photodiode discriminator
Diamondcrystal
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Apr 20, 2023 FCAL collaboration workshop, 2009
.Gallium Arsenide radiation hardness review
K. Afanaciev
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Apr 20, 2023 FCAL collaboration workshop, 2009
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The material
Gallium arsenide (GaAs)Compound semiconductor, direct bandgapTwo sublattices of face centered cubic lattice(zinc-blende type)
GaAsDensity 5.32 g/cm3
Pair creation E 4.3 eV/pair Band gap 1.42 eV Electron mobility 8500 cm2/Vs
Hole mobility 400 cm2/Vs Dielectric const. 12.85 Radiation length 2.3 cm
Ave. Edep/100 m(by 10 MeV e-) 69.7 keV Ave. pairs/100 m 13000Structure p-n or insul.
GaAs
Semiinsulating - no p-n junction
Doped with shallow donor (Sn)and then compensated with deep acceptor (Cr) resulting in a I-typeconductivity.
Signal charge transport mainlyby electrons
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Apr 20, 2023 FCAL collaboration workshop, 2009
Radiation Tests of Semiconductor Detectors. Valery ChmillPhD Thesis, 2006
Material: Cr and Fe compensated semiinsulating GaAs
Peak position vs dose up to 110 kGy137Cs– gamma rays, E = 661 keV
About 20% drop
23 MeV Neutrons Fluence up to 1.2x1015
Also V.B. Chmill et al. /Nud. Ins&. and Meth. in Phys Res. A 395 (1997) 65-70
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Apr 20, 2023 FCAL collaboration workshop, 2009
Radiation Tests of Semiconductor Detectors. Valery ChmillPhD Thesis
Material: Cr and Fe compensated semiinsulating GaAs
SPS Mixed Beam: 540 GeV protons on beryllium target. Max fluence 7x1014
dose rate ratio 1(red) : 0.32 (green) : 0.16
The dose rate have influence onradiation hardness for hadron irradiation
1012 1015Flux part/cm2*hour
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Apr 20, 2023 FCAL collaboration workshop, 2009
Radiation resistance study of SI GaAs based radiation detectors to extremely high gamma doses
(Nuclear Physics B (Proc. Suppl.) 150 (2006) 402–406)
LEC semiinsulating GaAs undopedIrradiation by 60Co gamma source (1.17 and 1.33 MeV photons)
Low Cr
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Apr 20, 2023 FCAL collaboration workshop, 2009
R.L. Bates et al. Recent results on GaAs detectors(Nuc1. Instr. and Meth. in Phys. Res. A 392 (1997) 269-273)
NIEL - non ionising energy lossLEC undoped GaAs
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Apr 20, 2023 FCAL collaboration workshop, 2009
R.L. Bates at al The effects of radiation on gallium arsenide radiation detectors Nuc1. Instr. and Meth. in Phys. Res. A 395 (1997)54-59
LEC undoped GaAs
neutrons pions
protons