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Study of radiation damage in silicon detectors for high ... - F9

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30 2. Operation and Radiation Damage <strong>of</strong> Silicon Detectorsdefect complexes. It is well proven by experiments that deep level acceptor-like statesare generated dur<strong>in</strong>g ir<strong>radiation</strong>. Accord<strong>in</strong>g to equations 2.10 and 2.13 the full depletionvoltage is proportional to jN eff j. It means that, <strong>for</strong> an <strong>in</strong>itially n type bulk, at low uencesFDV is decreas<strong>in</strong>g with uence until the <strong>in</strong>version po<strong>in</strong>t is reached and then it starts to<strong>in</strong>crease with uence. Thus at <strong>high</strong> total uences full depletion voltage may grow too<strong>high</strong> <strong>for</strong> a normal operation <strong>of</strong> the device. This <strong>in</strong>crease <strong>of</strong> depletion voltage is the ma<strong>in</strong>problem <strong>for</strong> operation <strong>of</strong> <strong>silicon</strong> <strong>detectors</strong> <strong>in</strong> a <strong>high</strong> <strong>radiation</strong> environment.The uence dependence <strong>of</strong> the <strong>in</strong>itially present shallow level dopants is however notwell understood yet. Dierent models have been proposed to expla<strong>in</strong> experimental results.R. Wunstorf et al. [29] reports on measurements <strong>of</strong> removal <strong>of</strong> both <strong>in</strong>itial shallowdonors and acceptors, together with deep level acceptor creation. Development <strong>of</strong> theeective dopant concentration with uence can thus be parametrised asN eff () = N 0 De ;c D ; N 0 Ae ;c A ; g (2.51)Donor removal constant has been determ<strong>in</strong>ed to be c D 2:5 10 ;13 cm 2 and acceptorremoval constant c A 1:98 10 ;13 cm 2 .F. Lemeilleur [30] however reports l<strong>in</strong>ear dependence <strong>of</strong> the <strong>in</strong>version uence on<strong>in</strong>itial dopant concentration with <strong>in</strong>v = (18 0:6cm) N eff (0). At the same time uencedependence <strong>of</strong> N eff is parametrised bywith c D 2:5 10 ;14 cm 2 and g 1:1 10 ;2 cm 2 .N eff () = N 0 De ;c D ; N 0 A ; g (2.52)H. Feick [20] assumes low level <strong>of</strong> compensation <strong>of</strong> his <strong>in</strong>itial material (N 0 A N O D )and is thus not sensitive to changes <strong>in</strong> concentration <strong>of</strong> <strong>in</strong>itial acceptors. Exponentialdependence <strong>of</strong> the donor concentration on uence is reported with removal rate equal toc D =(2:4 1:4) 10 ;13 cm 2 , but with only about a third <strong>of</strong> <strong>in</strong>itial donors be<strong>in</strong>g subjectto the removal. Reduced donor removal was also reported <strong>in</strong> [50].Watts [31] used numerical modell<strong>in</strong>g <strong>of</strong> deep acceptor creation to generate N effversus neutron uence <strong>for</strong> p and n type diodes. No <strong>in</strong>itial dopant removal was used <strong>in</strong>the calculations and good agreement with the data is reported. It is thus claimed that no<strong>in</strong>itial dopant removal is required to successfully expla<strong>in</strong> the uence dependence <strong>of</strong> N eff .Similarly, compensation <strong>of</strong> <strong>in</strong>itial donors by deep acceptors <strong>in</strong>stead <strong>of</strong> donor removal isalso suggested by [32].Due to lack <strong>of</strong> <strong>in</strong><strong>for</strong>mation about <strong>in</strong>itial donor and acceptor concentration, lowcompensation 15 has been assumed throughout this work. Initial donor concentration is15Assum<strong>in</strong>g low compensation N 0 A N 0 D , and with <strong>in</strong>itial donor concentration N 0 D < 4 1011 cm ;3 ,<strong>in</strong>itial acceptor concentration can be neglected.

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