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Direct determination of the atomic mass difference of the pairs <math><mrow><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts><mtext>-</mtext><mmultiscripts><mi>Se</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></mrow></math> and <math><mrow><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts><mtext>-</mtext><mmultiscripts><mi>Gd</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></mrow></math> rules out <math><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></math> and <math><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></math> as possible candidates for electron (anti)neutrino mass measurements
dc.contributor.author | GE, Z. | |
dc.contributor.author | ERONEN, T. | |
hal.structure.identifier | Centre d'Etudes Nucléaires de Bordeaux Gradignan [CENBG] | |
dc.contributor.author | DE ROUBIN, A. | |
dc.contributor.author | KOSTENSALO, J. | |
dc.contributor.author | SUHONEN, J. | |
dc.contributor.author | NESTERENKO, D.A. | |
dc.contributor.author | BELIUSKINA, O. | |
dc.contributor.author | DE GROOTE, R. | |
dc.contributor.author | DELAFOSSE, C. | |
dc.contributor.author | GELDHOF, S. | |
dc.contributor.author | GINS, W. | |
hal.structure.identifier | Centre d'Etudes Nucléaires de Bordeaux Gradignan [CENBG] | |
dc.contributor.author | HUKKANEN, M. | |
dc.contributor.author | JOKINEN, A. | |
dc.contributor.author | KANKAINEN, A. | |
dc.contributor.author | KOTILA, J. | |
dc.contributor.author | KOSZORÚS, Á. | |
dc.contributor.author | MOORE, I.D. | |
dc.contributor.author | RAGGIO, A. | |
dc.contributor.author | RINTA-ANTILA, S. | |
dc.contributor.author | VIRTANEN, V. | |
dc.contributor.author | WEAVER, A.P. | |
dc.contributor.author | ZADVORNAYA, A. | |
dc.date.issued | 2022 | |
dc.description.abstractEn | The first direct determination of the ground-state–to–ground-state <math><mi>Q</mi></math> values of the <math><msup><mi>β</mi><mo>−</mo></msup></math> decay <math><mrow><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts><mspace width="4pt"/><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Se</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></mrow></math> and the electron-capture decay <math><mrow><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts><mspace width="4pt"/><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Gd</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></mrow></math> was performed utilizing the double Penning trap mass spectrometer JYFLTRAP. By measuring the atomic mass difference of the decay pairs via the phase-imaging ion-cyclotron-resonance technique, the <math><mi>Q</mi></math> values of <math><mrow><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts><mspace width="4pt"/><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Se</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></mrow></math> and <math><mrow><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts><mspace width="4pt"/><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Gd</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></mrow></math> were determined to be 2959.265(74) keV and 814.94(18) keV, respectively. The precision was increased relative to earlier measurements by factors of 12 and 57, respectively. The new <math><mi>Q</mi></math> values are 1.33 keV and 5 keV lower compared to the values adopted in the most recent Atomic Mass Evaluation 2020. With the newly determined ground-state–to–ground-state <math><mi>Q</mi></math> values combined with the excitation energy from <math><mi>γ</mi></math>-ray spectroscopy, the <math><mi>Q</mi></math> values for ground-state–to–excited-state transitions <math><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></math> (ground state) <math><mrow><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Se</mi><none/><mo>*</mo><mprescripts/><none/><mn>76</mn></mmultiscripts></mrow></math> (2968.4(7) keV) and <math><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></math> (ground state) <math><mrow><mo>→</mo><mspace width="4pt"/><mmultiscripts><mi>Gd</mi><none/><mo>*</mo><mprescripts/><none/><mn>155</mn></mmultiscripts></mrow></math> (815.731(3) keV) were derived to be <math><mrow><mo>−</mo><mn>9.13</mn><mo>(</mo><mn>70</mn><mo>)</mo></mrow></math> keV and <math><mrow><mo>−</mo><mn>0.79</mn><mo>(</mo><mn>18</mn><mo>)</mo></mrow></math> keV. Thus we have confirmed that both of the <math><msup><mi>β</mi><mo>−</mo></msup></math>-decay and EC-decay candidate transitions are energetically forbidden at a level of at least <math><mrow><mn>4</mn><mi>σ</mi></mrow></math>, thus definitely excluding these two cases from the list of potential candidates for the search of low-<math><mi>Q</mi></math>-value <math><msup><mi>β</mi><mo>−</mo></msup></math> or EC decays to determine the electron-(anti)neutrino mass. | |
dc.language.iso | en | |
dc.subject.en | neutrino: mass | |
dc.subject.en | excited state: energy | |
dc.subject.en | mass: spectrometer | |
dc.subject.en | ground state | |
dc.subject.en | mass difference | |
dc.subject.en | radio wave | |
dc.subject.en | ion: acceleration | |
dc.subject.en | Penning trap | |
dc.subject.en | electron | |
dc.subject.en | antineutrino electron | |
dc.subject.en | semileptonic decay | |
dc.title.en | Direct determination of the atomic mass difference of the pairs <math><mrow><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts><mtext>-</mtext><mmultiscripts><mi>Se</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></mrow></math> and <math><mrow><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts><mtext>-</mtext><mmultiscripts><mi>Gd</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></mrow></math> rules out <math><mmultiscripts><mi>As</mi><mprescripts/><none/><mn>76</mn></mmultiscripts></math> and <math><mmultiscripts><mi>Tb</mi><mprescripts/><none/><mn>155</mn></mmultiscripts></math> as possible candidates for electron (anti)neutrino mass measurements | |
dc.type | Article de revue | |
dc.identifier.doi | 10.1103/PhysRevC.106.015502 | |
dc.subject.hal | Physique [physics]/Physique Nucléaire Expérimentale [nucl-ex] | |
dc.identifier.arxiv | 2202.07656 | |
bordeaux.journal | Phys.Rev.C | |
bordeaux.page | 015502 | |
bordeaux.volume | 106 | |
bordeaux.issue | 1 | |
bordeaux.peerReviewed | oui | |
hal.identifier | hal-03594135 | |
hal.version | 1 | |
hal.popular | non | |
hal.audience | Internationale | |
hal.origin.link | https://hal.archives-ouvertes.fr//hal-03594135v1 | |
bordeaux.COinS | ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Phys.Rev.C&rft.date=2022&rft.volume=106&rft.issue=1&rft.spage=015502&rft.epage=015502&rft.au=GE,%20Z.&ERONEN,%20T.&DE%20ROUBIN,%20A.&KOSTENSALO,%20J.&SUHONEN,%20J.&rft.genre=article |
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