Journal of High Energy Physics (Jul 2025)
Reconstructing neutrinoless double beta decay event kinematics in a xenon gas detector with vertex tagging
- The NEXT collaboration,
- 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
Affiliations
- The NEXT collaboration
- M. Martínez-Vara
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- K. Mistry
- Department of Physics, University of Texas at Arlington
- F. Pompa
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- B. J. P. Jones
- Department of Physics, University of Texas at Arlington
- J. Martín-Albo
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- M. Sorel
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- C. Adams
- Argonne National Laboratory
- H. Almazán
- Department of Physics and Astronomy, Manchester University
- V. Álvarez
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- B. Aparicio
- Department of Organic Chemistry I, Universidad del Pais Vasco (UPV/EHU), Centro de Innovación en Química Avanzada (ORFEO-CINQA)
- A. I. Aranburu
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- L. Arazi
- Unit of Nuclear Engineering, Faculty of Engineering Sciences, Ben-Gurion University of the Negev
- I. J. Arnquist
- Pacific Northwest National Laboratory (PNNL)
- F. Auria-Luna
- Department of Organic Chemistry I, Universidad del Pais Vasco (UPV/EHU), Centro de Innovación en Química Avanzada (ORFEO-CINQA)
- S. Ayet
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- C. D. R. Azevedo
- Institute of Nanostructures, Nanomodelling and Nanofabrication (i3N), Universidade de Aveiro
- K. Bailey
- Argonne National Laboratory
- F. Ballester
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- M. del Barrio-Torregrosa
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- A. Bayo
- Laboratorio Subterráneo de Canfranc
- J. M. Benlloch-Rodríguez
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- F. I. G. M. Borges
- LIP, Department of Physics, University of Coimbra
- A. Brodolin
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- N. Byrnes
- Department of Physics, University of Texas at Arlington
- S. Cárcel
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- A. Castillo
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- E. Church
- Pacific Northwest National Laboratory (PNNL)
- L. Cid
- Laboratorio Subterráneo de Canfranc
- C. A. N. Conde
- LIP, Department of Physics, University of Coimbra
- T. Contreras
- Department of Physics, Harvard University
- F. P. Cossío
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- R. Coupe
- Department of Physics and Astronomy, Manchester University
- E. Dey
- Department of Physics, University of Texas at Arlington
- G. Díaz
- Instituto Gallego de Física de Altas Energías, Univ. de Santiago de Compostela
- C. Echevarria
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- M. Elorza
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. Escada
- LIP, Department of Physics, University of Coimbra
- R. Esteve
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- R. Felkai
- Unit of Nuclear Engineering, Faculty of Engineering Sciences, Ben-Gurion University of the Negev
- L. M. P. Fernandes
- LIBPhys, Physics Department, University of Coimbra
- P. Ferrario
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- A. L. Ferreira
- Institute of Nanostructures, Nanomodelling and Nanofabrication (i3N), Universidade de Aveiro
- F. W. Foss
- Department of Chemistry and Biochemistry, University of Texas at Arlington
- Z. Freixa
- Department of Applied Chemistry, Universidad del Pais Vasco (UPV/EHU)
- J. García-Barrena
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- J. J. Gómez-Cadenas
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. W. R. Grocott
- Department of Physics and Astronomy, Manchester University
- R. Guenette
- Department of Physics and Astronomy, Manchester University
- J. Hauptman
- Department of Physics and Astronomy, Iowa State University
- C. A. O. Henriques
- LIBPhys, Physics Department, University of Coimbra
- J. A. Hernando Morata
- Instituto Gallego de Física de Altas Energías, Univ. de Santiago de Compostela
- P. Herrero-Gómez
- Racah Institute of Physics, The Hebrew University of Jerusalem
- V. Herrero
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- C. Hervés Carrete
- Instituto Gallego de Física de Altas Energías, Univ. de Santiago de Compostela
- Y. Ifergan
- Unit of Nuclear Engineering, Faculty of Engineering Sciences, Ben-Gurion University of the Negev
- F. Kellerer
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- L. Larizgoitia
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- A. Larumbe
- Department of Organic Chemistry I, Universidad del Pais Vasco (UPV/EHU), Centro de Innovación en Química Avanzada (ORFEO-CINQA)
- P. Lebrun
- Fermi National Accelerator Laboratory
- F. Lopez
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- N. López-March
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- R. Madigan
- Department of Chemistry and Biochemistry, University of Texas at Arlington
- R. D. P. Mano
- LIBPhys, Physics Department, University of Coimbra
- A. P. Marques
- LIP, Department of Physics, University of Coimbra
- G. Martínez-Lema
- Unit of Nuclear Engineering, Faculty of Engineering Sciences, Ben-Gurion University of the Negev
- R. L. Miller
- Department of Chemistry and Biochemistry, University of Texas at Arlington
- J. Molina-Canteras
- Department of Organic Chemistry I, Universidad del Pais Vasco (UPV/EHU), Centro de Innovación en Química Avanzada (ORFEO-CINQA)
- F. Monrabal
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- C. M. B. Monteiro
- LIBPhys, Physics Department, University of Coimbra
- F. J. Mora
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- K. E. Navarro
- Department of Physics, University of Texas at Arlington
- P. Novella
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- A. Nuñez
- Laboratorio Subterráneo de Canfranc
- D. R. Nygren
- Department of Physics, University of Texas at Arlington
- E. Oblak
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. Palacio
- Laboratorio Subterráneo de Canfranc
- B. Palmeiro
- Department of Physics and Astronomy, Manchester University
- A. Para
- Fermi National Accelerator Laboratory
- I. Parmaksiz
- Department of Physics, University of Texas at Arlington
- A. Pazos
- Department of Applied Chemistry, Universidad del Pais Vasco (UPV/EHU)
- J. Pelegrin
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- M. Pérez Maneiro
- Instituto Gallego de Física de Altas Energías, Univ. de Santiago de Compostela
- M. Querol
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- J. Renner
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- I. Rivilla
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- C. Rogero
- Centro de Física de Materiales (CFM), CSIC & Universidad del Pais Vasco (UPV/EHU)
- L. Rogers
- Argonne National Laboratory
- B. Romeo
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- C. Romo-Luque
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- V. San Nacienciano
- Department of Organic Chemistry I, Universidad del Pais Vasco (UPV/EHU), Centro de Innovación en Química Avanzada (ORFEO-CINQA)
- F. P. Santos
- LIP, Department of Physics, University of Coimbra
- J. M. F. dos Santos
- LIBPhys, Physics Department, University of Coimbra
- M. Seemann
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- I. Shomroni
- Racah Institute of Physics, The Hebrew University of Jerusalem
- P. A. O. C. Silva
- LIBPhys, Physics Department, University of Coimbra
- A. Simón
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- S. R. Soleti
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. Soto-Oton
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- J. M. R. Teixeira
- LIBPhys, Physics Department, University of Coimbra
- S. Teruel-Pardo
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- J. F. Toledo
- Instituto de Instrumentación para Imagen Molecular (I3M), Centro Mixto CSIC - Universitat Politècnica de València
- C. Tonnelé
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- S. Torelli
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. Torrent
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- A. Trettin
- Department of Physics and Astronomy, Manchester University
- A. Usón
- Instituto de Física Corpuscular (IFIC), CSIC & Universitat de València
- P. R. G. Valle
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- J. F. C. A. Veloso
- Institute of Nanostructures, Nanomodelling and Nanofabrication (i3N), Universidade de Aveiro
- J. Waiton
- Department of Physics and Astronomy, Manchester University
- A. Yubero-Navarro
- Donostia International Physics Center, BERC Basque Excellence Research Centre
- DOI
- https://doi.org/10.1007/jhep07(2025)170
- Journal volume & issue
-
Vol. 2025,
no. 7
pp. 1 – 22
Abstract
Abstract 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, T 1 and T 2. 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.
Keywords