2018
DOI: 10.1063/1.5029533
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The paradox of characteristics of silicon detectors operated at temperature close to liquid helium

Abstract: The aim of this study is to give characterization of silicon p+/n/n+ detectors for the monitoring systems of the Large Hadron Collider machine at CERN with the focus on justifying the choice of silicon resistivity for the detector operation at the temperature of 1.9–10 K. The detectors from n-type silicon with the resistivity of 10, 4.5, and 0.5 kΩ cm were investigated at the temperature from 293 up to 7 K by the Transient Current Technique with a 660 nm pulse laser and alpha-particles. The shapes of the detec… Show more

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Cited by 7 publications
(3 citation statements)
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“…Both carrier–carrier and lattice scattering increase. Compared to Si photodetectors, the conductivity change rate per unit temperature for the PSD is 1.625 × 10 −9 A V −1 K −1 , which is much smaller than that of Si PSD, in which the conductance sensitivity is 6.67 × 10 −7 A V −1 K −1 . This PSD based on CdS branched nanostructures is not much sensitive to temperature, shows good performance, and can work well at low temperatures.…”
Section: Resultsmentioning
confidence: 92%
“…Both carrier–carrier and lattice scattering increase. Compared to Si photodetectors, the conductivity change rate per unit temperature for the PSD is 1.625 × 10 −9 A V −1 K −1 , which is much smaller than that of Si PSD, in which the conductance sensitivity is 6.67 × 10 −7 A V −1 K −1 . This PSD based on CdS branched nanostructures is not much sensitive to temperature, shows good performance, and can work well at low temperatures.…”
Section: Resultsmentioning
confidence: 92%
“…In the presence of doping profiles, carrier freezeout effects that occur at temperatures < 100 K become an important factor to control. Recent tests on non-irradiated 𝑝 + -𝑛-𝑛 + silicon sensors for possible high-luminosity LHC beam loss monitor designs [40] show only small differences in current pulses at temperatures between 100 K and 7.6 K for 4.5 and 10 kΩ cm silicon sensors with a bias voltage of 100 V (above depletion voltage). The pulse shapes at these temperatures are narrower as a function of time…”
Section: Jinst 18 P12005mentioning
confidence: 99%
“…Thus, the time resolution of the TCT was limited mainly by the RC product of the installation (50 Ω input resistance of oscilloscope and the capacitance of the sample under study) and by the analog response of the coaxial cable line. The experimental setup was described in detail in [21].…”
Section: Samples and Experimental Setupmentioning
confidence: 99%