1975
DOI: 10.1109/tns.1975.4327632
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Comparitive Ionization Energies for Protons, Deuterons and Alpha Particles in High Purity Germanium and Si(Li) Nuclear Radiation Detectors

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Cited by 17 publications
(3 citation statements)
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“…The result of this fitting procedure is summarized in Fig. 4b and provides the dead layer thickness d=(1.00.2) m; the sensitivity of the electronic chain is (2.300  0.002) keV/channel corresponding to 640 electrons/channel as evaluated assuming an average energy to create one electron/hole pair (eh) in silicon of 3.6 eV [25].…”
Section: Calibration and Dead Layer Measurementmentioning
confidence: 99%
“…The result of this fitting procedure is summarized in Fig. 4b and provides the dead layer thickness d=(1.00.2) m; the sensitivity of the electronic chain is (2.300  0.002) keV/channel corresponding to 640 electrons/channel as evaluated assuming an average energy to create one electron/hole pair (eh) in silicon of 3.6 eV [25].…”
Section: Calibration and Dead Layer Measurementmentioning
confidence: 99%
“…where ε np is the average energy required to create electron/hole pairs (in silicon 3.6 eV, [71]), E I is the energy of the ion probe, and dx dE I is the relevant ionization energy loss that can be extracted from SRIM simulations, as shown in Fig. 25 for the ions used.…”
Section: Ibic Characterization Of a Partly Damaged Sc Diode -A New Mo...mentioning
confidence: 99%
“…Experimental techniques like Deep Level Transient Spectroscopy (DLTS) are limited to characterisation of the single carrier traps and determination of the single carrier capture coefficient (either electron or hole; c n = c p or vice versa). In this case relation(71) simplifies to:…”
mentioning
confidence: 99%