Abstract

The lifetimes of the low-lying excited states 2+ and 4+ have been directly measured in the neutron-deficient 106,108Sn isotopes. The nuclei were populated via a deep-inelastic reaction and the lifetime measurement was performed employing a differential plunger device. The emitted γ rays were detected by the AGATA array, while the reaction products were uniquely identified by the VAMOS++ magnetic spectrometer. Large-Scale Shell-Model calculations with realistic forces indicate that, independently of the pairing content of the interaction, the quadrupole force is dominant in the B(E2;21+→0g.s.+) values and it describes well the experimental pattern for 104−114Sn; the B(E2;41+→21+) values, measured here for the first time, depend critically on a delicate pairing-quadrupole balance, disclosed by the very precise results in 108Sn.

Highlights

  • A little over a decade ago, the Sn isotopes were considered the paradigms of pairing dominance: low-lying states of good seniority, nearly constant J π = 2+1 excitation energies and parabolic B(E2; 2+1 → 0+g.s.) behavior

  • The emitted γ rays were detected by the AGATA array, while the reaction products were uniquely identified by the VAMOS++ magnetic spectrometer

  • Thanks to the precise determination of the ion velocity vector and the identification of the first interaction point of each γ ray inside AGATA, Doppler correction was applied on an eventby-event basis

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Summary

Introduction

A little over a decade ago, the Sn isotopes were considered the paradigms of pairing dominance: low-lying states of good seniority, nearly constant J π = 2+1 excitation energies and parabolic B(E2; 2+1 → 0+g.s.) behavior. From Coulomb-excitation measurements with radioactive ion beams only the reduced transition probability between the first excited 2+ state and the ground state could be determined [1,2,3,4,5,6,7,8] Within experimental uncertainties, they suggest a rather-constant behavior for 106 ≤ A ≤ 110, instead of the parabolic trend expected when isovector T = 1 pairing dominates. The B(E2; 4+1 → 2+1 ) values were completely absent in the neutron-deficient Sn isotopes

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