Abstract

A novel method for direct electronic “fast-timing” lifetime measurements of nuclear excited states via γ-γ coincidences using an array equipped with N very fast high-resolution LaBr3(Ce) scintillator detectors is presented. The generalized centroid difference method provides two independent “start” and “stop” time spectra obtained without any correction by a superposition of the N(N – 1)/2 calibrated γ-γ time difference spectra of the N detector fast-timing system. The two fast-timing array time spectra correspond to a forward and reverse gating of a specific γ-γ cascade and the centroid difference as the time shift between the centroids of the two time spectra provides a picosecond-sensitive mirror-symmetric observable of the set-up. The energydependent mean prompt response difference between the start and stop events is calibrated and used as a single correction for lifetime determination. These combined fast-timing array mean γ-γ zero-time responses can be determined for 40 keV < Eγ < 1.4 MeV with a precision better than 10 ps using a 152Eu γ-ray source. The new method is described with examples of (n,γ) and (n,f,γ) experiments performed at the intense cold-neutron beam facility PF1B of the Institut Laue-Langevin in Grenoble, France, using 16 LaBr3(Ce) detectors within the EXILL&FATIMA campaign in 2013. The results are discussed with respect to possible systematic errors induced by background contributions.

Highlights

  • A novel method for direct electronic "fast-timing" lifetime measurements of nuclear excited states via γ-γ coincidences using an array equipped with N very fast high-resolution LaBr3(Ce) scintillator detectors is presented

  • The generalized centroid difference method provides two independent “start” and “stop” time spectra obtained without any correction by a superposition of the N(N − 1)/2 calibrated γ-γ time difference spectra of the N detector fast-timing system

  • The new method is described with examples of (n,γ) and (n,f,γ) experiments performed at the intense cold-neutron beam facility PF1B of the Institut Laue-Langevin in Grenoble, France, using 16 LaBr3(Ce) detectors within the EXILL&FATIMA campaign in 2013

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Summary

Introduction

EPJ Web of Conferences with an exponential decay as: D(t) = nλ t P(t − t0)e−λ(t − t )dt −∞. Where n is the total number of detected γ-γ events in the time difference spectrum, λ the transition (decay) probability and τ the mean lifetime of the nuclear excited state interconnected by the γ-γ cascade and t0 is the position (centroid) of the PRF P(t). The experimental PRF provides important information on timing characteristics and is obtained for lifetimes which are smaller than 1 ps (systematic errors are expected to be larger). For lifetimes which are larger than the FWHM of the PRF, the mean lifetime is obtained directly using the slope method [1]. Lifetimes which are smaller than the FWHM of the PRF can be determined using the centroid-shift method [6].

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