<p>If neutrinoless double beta decay is discovered, the next natural step would be understanding the lepton number violating physics responsible for it. Several alternatives exist beyond the exchange of light neutrinos. Some of these mechanisms can be distinguished by measuring phase-space observables, namely the opening angle cos <i>θ</i> among the two decay electrons, and the electron energy spectra, <i>T</i><sub>1</sub> and <i>T</i><sub>2</sub>. In this work, we study the statistical accuracy and precision in measuring these kinematic observables in a future xenon gas detector with the added capability to precisely locate the decay vertex. For realistic detector conditions (a gas pressure of 10 bar and spatial resolution of 4 mm), we find that the average <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mrow> <mo>cos</mo> <mspace width="0.25em" /> <mi>θ</mi> </mrow> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{\cos\ \theta } \)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <msub> <mi>T</mi> <mn>1</mn> </msub> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{T_1} \)</EquationSource> </InlineEquation> values can be reconstructed with a precision of 0.19 and 110 keV, respectively, assuming that only 10 neutrinoless double beta decay events are detected.</p>

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Reconstructing neutrinoless double beta decay event kinematics in a xenon gas detector with vertex tagging

  • M. Martínez-Vara,
  • K. Mistry,
  • F. Pompa,
  • B. J. P. Jones,
  • J. Martín-Albo,
  • M. Sorel,
  • C. Adams,
  • H. Almazán,
  • V. Álvarez,
  • B. Aparicio,
  • A. I. Aranburu,
  • L. Arazi,
  • I. J. Arnquist,
  • F. Auria-Luna,
  • S. Ayet,
  • C. D. R. Azevedo,
  • K. Bailey,
  • F. Ballester,
  • M. del Barrio-Torregrosa,
  • A. Bayo,
  • J. M. Benlloch-Rodríguez,
  • F. I. G. M. Borges,
  • A. Brodolin,
  • N. Byrnes,
  • S. Cárcel,
  • A. Castillo,
  • E. Church,
  • L. Cid,
  • C. A. N. Conde,
  • T. Contreras,
  • F. P. Cossío,
  • R. Coupe,
  • E. Dey,
  • G. Díaz,
  • C. Echevarria,
  • M. Elorza,
  • J. Escada,
  • R. Esteve,
  • R. Felkai,
  • L. M. P. Fernandes,
  • P. Ferrario,
  • A. L. Ferreira,
  • F. W. Foss,
  • Z. Freixa,
  • J. García-Barrena,
  • J. J. Gómez-Cadenas,
  • J. W. R. Grocott,
  • R. Guenette,
  • J. Hauptman,
  • C. A. O. Henriques,
  • J. A. Hernando Morata,
  • P. Herrero-Gómez,
  • V. Herrero,
  • C. Hervés Carrete,
  • Y. Ifergan,
  • F. Kellerer,
  • L. Larizgoitia,
  • A. Larumbe,
  • P. Lebrun,
  • F. Lopez,
  • N. López-March,
  • R. Madigan,
  • R. D. P. Mano,
  • A. P. Marques,
  • G. Martínez-Lema,
  • R. L. Miller,
  • J. Molina-Canteras,
  • F. Monrabal,
  • C. M. B. Monteiro,
  • F. J. Mora,
  • K. E. Navarro,
  • P. Novella,
  • A. Nuñez,
  • D. R. Nygren,
  • E. Oblak,
  • J. Palacio,
  • B. Palmeiro,
  • A. Para,
  • I. Parmaksiz,
  • A. Pazos,
  • J. Pelegrin,
  • M. Pérez Maneiro,
  • M. Querol,
  • J. Renner,
  • I. Rivilla,
  • C. Rogero,
  • L. Rogers,
  • B. Romeo,
  • C. Romo-Luque,
  • V. San Nacienciano,
  • F. P. Santos,
  • J. M. F. dos Santos,
  • M. Seemann,
  • I. Shomroni,
  • P. A. O. C. Silva,
  • A. Simón,
  • S. R. Soleti,
  • J. Soto-Oton,
  • J. M. R. Teixeira,
  • S. Teruel-Pardo,
  • J. F. Toledo,
  • C. Tonnelé,
  • S. Torelli,
  • J. Torrent,
  • A. Trettin,
  • A. Usón,
  • P. R. G. Valle,
  • J. F. C. A. Veloso,
  • J. Waiton,
  • A. Yubero-Navarro

摘要

If neutrinoless double beta decay is discovered, the next natural step would be understanding the lepton number violating physics responsible for it. Several alternatives exist beyond the exchange of light neutrinos. Some of these mechanisms can be distinguished by measuring phase-space observables, namely the opening angle cos θ among the two decay electrons, and the electron energy spectra, T1 and T2. In this work, we study the statistical accuracy and precision in measuring these kinematic observables in a future xenon gas detector with the added capability to precisely locate the decay vertex. For realistic detector conditions (a gas pressure of 10 bar and spatial resolution of 4 mm), we find that the average cos θ ¯ \( \overline{\cos\ \theta } \) and T 1 ¯ \( \overline{T_1} \) values can be reconstructed with a precision of 0.19 and 110 keV, respectively, assuming that only 10 neutrinoless double beta decay events are detected.