Introduction

BIRKS, J.B.

doi:10.1016/b978-0-08-010472-0.50006-9

Cited by 24 publications

(34 citation statements)

References 22 publications

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“…This result is in agreement with that reported in [11]. Such a behaviour of the α/β ratio can be explained by the energy dependence of ionization density of α particles [40]. It should be also noted, that α/β ratio is not actually a property of a crystal, but more likely a certain characteristics of the detector depending on the shape and surface quality of a crystal, shaping time of electronics, etc.…”

Section: α/β Ratiosupporting

confidence: 81%

Further study of CdWO4 crystal scintillators as detectors for high sensitivity experiments: Scintillation properties and pulse-shape discrimination

Bardelli

Bini

Bizzeti

et al. 2006

Nuclear Instruments and Methods in Physics Research Section A:

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Energy resolution, light yield, non-proportionality in the scintillation response, α/β ratio, pulse shape for γ rays and α particles were studied with CdWO 4 crystal scintillators. Some indication for a difference in the emission spectra for γ rays and α particles was observed. No dependence of CdWO 4 pulse shape on emission spectrum wavelengths under laser, α particles and γ ray excitation was observed. Dependence of scintillation pulse shape for γ quanta and α particles and pulse-shape discrimination ability on temperature was measured in the range of 0 − 24 • C.

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Section: α/β Ratiosupporting

confidence: 81%

Further study of CdWO4 crystal scintillators as detectors for high sensitivity experiments: Scintillation properties and pulse-shape discrimination

Bardelli

Bini

Bizzeti

et al. 2006

Nuclear Instruments and Methods in Physics Research Section A:

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“…The energy deposit is converted into the number of photons. Quenching effects of the scintillation are modeled based on Birks' law [41,42]. The effect of collection and attenuation of the light in the scintillator and the WLS fiber is modeled based on the results of electron beam irradiation tests.…”

Section: Ingrid Detector Response Simulationmentioning

confidence: 99%

Measurement of the inclusiveνμcharged current cross section on iron and hydrocarbon in the T2K on-axis neutrino beam

Abe¹,

Adam²,

Aihara³

et al. 2014

Phys. Rev. D

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Measurement of the inclusive ν µ charged current cross section on iron and hydrocarbon in the T2K on-axis neutrino beam We report a measurement of the νµ inclusive charged current cross sections on iron and hydrocarbon in the T2K on-axis neutrino beam. The measured inclusive charged current cross sections on iron and hydrocarbon averaged over the T2K on-axis flux with a mean neutrino energy of 1.51 GeV are (1.444 ± 0.002(stat.) +0.189 −0.157 (syst.)) × 10 −38 cm 2 /nucleon, and (1.379 ± 0.009(stat.) +0.178 −0.147 (syst.)) × 10 −38 cm 2 /nucleon, respectively, and their cross section ratio is 1.047 ± 0.007(stat.) ± 0.035(syst.). These results agree well with the predictions of neutrino interaction model and thus we checked the correct treatment of the nuclear effect for iron and hydrocarbon targets in the model within the measurement precisions.

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“…Neutrons transmit their energy to the host hydrogen nuclei characterized by a high electronic stopping power. Mainly via π-electron ionization followed by recombination, these protons cause a high density of excited molecules decaying by fluorescence, delayed fluorescence or phosphorescence [3]. Consequently, the scintillation signal following the interaction of a neutron, will contain, besides the "prompt" decay associated to fluorescence, a slow component, especially connected to delayed fluorescence.…”

Section: Neutron Identification In Liquid Scintillatorsmentioning

confidence: 99%

“…The emission of light accompanying the relaxation between singlet states is the fuorescence (≈ 10 −9 s in liquid scintillators) while phosphorescence (> 10 −6 s) means the radiative de-excitation, of low probability, from a triplet to the singlet ground state. Between, delayed fluorescence (10 to 100 times slower than fluorescence) also occurs at high densities of molecules excited in triplet states [3].…”

Section: Neutron Identification In Liquid Scintillatorsmentioning

confidence: 99%

“…We have recently used it to measure the neutron cross talk yield between two liquid cells. Neutrons of 1.5 MeV were produced via the 3 H(p, n) 3 He reaction by means of a proton pulsed beam characterized by a period of 400 ns and a bunch width of a few ns. The detectors were placed at two different distances and angles (both of them larger for the second cell) with respect to the target and the beam direction, respectively.…”

Section: Neutron Identification In Liquid Scintillatorsmentioning

confidence: 99%

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