Abstract

Short-lived \(\alpha \) emitters with N = 128–131 and Z = 91–93 were studied in the fusion reaction ^40Ar + ^187Re using the digital pulse processing technique at the gas-filled recoil separator Spectrometer for Heavy Atom and Nuclear Structure (SHANS). Two new isotopes ^223,224Np were identified and the decay of 220 Pa was re-investigated through temporal and spatial correlations. The pileup signals were resolved by using the digital pulse processing technique. An \(\alpha \) decay with half-life of \(T_{1/2} = 2.15(_{52}^{100})\) μs and energy of \(E_{\alpha } = 9477(44)\) keV was attributed to ^223Np. Two \(\alpha \)-decay branches with half-life of \(T_{1/2} = 38(_{11}^{26})\) μs, \(\alpha \) energies of 9137(21) and 8868(60) keV were assigned to ^224Np, decaying to two excited states in ^220Pa. The results of ^223Np disprove the existence of a Z = 92 subshell closure.

Highlights

  • The evolution of proton shell structure beyond 208 Pb is of decisive importance for the shell stabilization of superheavy elements

  • This is at variance with large-scale shell-model calculations [6], which show no sign of a shell gap at Z = 92 for N = 126 isotones and are in overall agreement with spectroscopic data on these isotones up to U [6,7,8,9,10]

  • In order to identify decay chains belonging to 223 Np, all digital traces correlated to the subsequent α decay of 215 Ac (Eα = 7600(4) keV, T1/2 = 0.17(1) s) [25], which are the third members of the α-decay chain originating from 223 Np, were checked event by event for the presence of multiple pulses

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Summary

Introduction

The evolution of proton shell structure beyond 208 Pb is of decisive importance for the shell stabilization of superheavy elements. 52 ) μs and energy of Eα = 9477(44) keV was attributed to 223 Np. Two α-decay branches with half-life of T1/2 = 38(26 The proton separation energy, ground-state spin and parity of odd-Z isotopes beyond

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