2013
DOI: 10.1016/j.astropartphys.2013.06.010
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Ionization efficiency study for low energy nuclear recoils in germanium

Abstract: We used the internal conversion (E 0 transition) of germanium-72 to indirectly measure the low energy nuclear recoils of germanium. Together with a reliable Monte Carlo package, in which we implement the internal conversion process, the data was compared to the Lindhard (k=0.159) and Barker-Mei models. A shape analysis indicates that both models agree well with data in the region of interest within 4%. The most probable value (MPV) of the nuclear recoils obtained from the shape analysis is 17.5 ± 0.12 (sys) ± … Show more

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Cited by 14 publications
(22 citation statements)
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“…Experimental measurements in Ge are consistent with Lindhard theory down to at least a recoil energy of 254 eV [38][39][40]. We choose the cutoff E y 0 to be at 40 eV, roughly a factor of 2-3 times higher than the minimum energy required for dislocating a Ge atom from its lattice site [41].…”
Section: Ionization Yield In Gementioning
confidence: 67%
“…Experimental measurements in Ge are consistent with Lindhard theory down to at least a recoil energy of 254 eV [38][39][40]. We choose the cutoff E y 0 to be at 40 eV, roughly a factor of 2-3 times higher than the minimum energy required for dislocating a Ge atom from its lattice site [41].…”
Section: Ionization Yield In Gementioning
confidence: 67%
“…Some of them try to describe the electronic and nuclear stopping power at low energies as in [239] for ionisation in germanium. This model is verified by a dedicated data-MC comparison of neutron scattering off germanium [255]. In [256][257] and [258], the scintillation and ionisation for liquid noble-gas detector are modelled.…”
Section: Calibration Of the Recoil-energiesmentioning
confidence: 89%
“…For the last decade, DM experiments have been rejecting irreducible electron recoil backgrounds using the differing yield between nuclear and electronic recoils, often called the quenching factor, utilizing simultaneous measurements of energy in complementary detection channels (see e.g., Refs. [32,33] and Appendix B). For solid-state experiments, the readout typically comprises both a heat (E det ) and charge or light (E e ) signal.…”
Section: Determining Signal Originmentioning
confidence: 99%