{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,8,6]],"date-time":"2025-08-06T12:11:15Z","timestamp":1754482275864,"version":"3.37.3"},"reference-count":31,"publisher":"Springer Science and Business Media LLC","issue":"5","license":[{"start":{"date-parts":[[2024,5,21]],"date-time":"2024-05-21T00:00:00Z","timestamp":1716249600000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"},{"start":{"date-parts":[[2024,5,21]],"date-time":"2024-05-21T00:00:00Z","timestamp":1716249600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["link.springer.com"],"crossmark-restriction":false},"short-container-title":["Eur. Phys. J. C"],"abstract":"<jats:title>Abstract<\/jats:title><jats:p>Noble element time projection chambers are a leading technology for rare event detection in physics, such as for dark matter and neutrinoless double beta decay searches. Time projection chambers typically assign event position in the drift direction using the relative timing of prompt scintillation and delayed charge collection signals, allowing for reconstruction of an absolute position in the drift direction. In this paper, alternate methods for assigning event drift distance via quantification of electron diffusion in a pure high pressure xenon gas time projection chamber are explored. Data from the NEXT-White detector demonstrate the ability to achieve good position assignment accuracy for both high- and low-energy events. Using point-like energy deposits from <jats:inline-formula><jats:alternatives><jats:tex-math>$$^{83\\textrm{m}}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msup>\n                    <mml:mrow\/>\n                    <mml:mrow>\n                      <mml:mn>83<\/mml:mn>\n                      <mml:mtext>m<\/mml:mtext>\n                    <\/mml:mrow>\n                  <\/mml:msup>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>Kr calibration electron captures (<jats:inline-formula><jats:alternatives><jats:tex-math>$$E\\sim 45$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>E<\/mml:mi>\n                    <mml:mo>\u223c<\/mml:mo>\n                    <mml:mn>45<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>\u00a0keV), the position of origin of low-energy events is determined to 2\u00a0cm precision with bias <jats:inline-formula><jats:alternatives><jats:tex-math>$$&lt; 1~$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mo>&lt;<\/mml:mo>\n                    <mml:mn>1<\/mml:mn>\n                    <mml:mspace\/>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>mm. A convolutional neural network approach is then used to quantify diffusion for longer tracks (<jats:inline-formula><jats:alternatives><jats:tex-math>$$E\\ge ~1.5$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>E<\/mml:mi>\n                    <mml:mo>\u2265<\/mml:mo>\n                    <mml:mspace\/>\n                    <mml:mn>1.5<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula>\u00a0MeV), from radiogenic electrons, yielding a precision of 3\u00a0cm on the event barycenter. The precision achieved with these methods indicates the feasibility energy calibrations of better than 1%\u00a0FWHM at Q<jats:inline-formula><jats:alternatives><jats:tex-math>$$_{\\beta \\beta }$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mrow\/>\n                    <mml:mrow>\n                      <mml:mi>\u03b2<\/mml:mi>\n                      <mml:mi>\u03b2<\/mml:mi>\n                    <\/mml:mrow>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> in pure xenon, as well as the potential for event fiducialization in large future detectors using an alternate method that does not rely on primary scintillation.<\/jats:p>","DOI":"10.1140\/epjc\/s10052-024-12865-9","type":"journal-article","created":{"date-parts":[[2024,5,21]],"date-time":"2024-05-21T18:03:53Z","timestamp":1716314633000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":1,"title":["Demonstration of event position reconstruction based on diffusion in the NEXT-white detector"],"prefix":"10.1140","volume":"84","author":[{"given":"J.","family":"Haefner","sequence":"first","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0009-0009-0971-5559","authenticated-orcid":false,"given":"K. E.","family":"Navarro","sequence":"additional","affiliation":[]},{"given":"R.","family":"Guenette","sequence":"additional","affiliation":[]},{"given":"B. J. P.","family":"Jones","sequence":"additional","affiliation":[]},{"given":"A.","family":"Tripathi","sequence":"additional","affiliation":[]},{"given":"C.","family":"Adams","sequence":"additional","affiliation":[]},{"given":"H.","family":"Almaz\u00e1n","sequence":"additional","affiliation":[]},{"given":"V.","family":"\u00c1lvarez","sequence":"additional","affiliation":[]},{"given":"B.","family":"Aparicio","sequence":"additional","affiliation":[]},{"given":"A. I.","family":"Aranburu","sequence":"additional","affiliation":[]},{"given":"L.","family":"Arazi","sequence":"additional","affiliation":[]},{"given":"I. J.","family":"Arnquist","sequence":"additional","affiliation":[]},{"given":"F.","family":"Auria-Luna","sequence":"additional","affiliation":[]},{"given":"S.","family":"Ayet","sequence":"additional","affiliation":[]},{"given":"C. D. R.","family":"Azevedo","sequence":"additional","affiliation":[]},{"given":"K.","family":"Bailey","sequence":"additional","affiliation":[]},{"given":"F.","family":"Ballester","sequence":"additional","affiliation":[]},{"given":"M. del","family":"Barrio-Torregrosa","sequence":"additional","affiliation":[]},{"given":"A.","family":"Bayo","sequence":"additional","affiliation":[]},{"given":"J. M.","family":"Benlloch-Rodr\u00edguez","sequence":"additional","affiliation":[]},{"given":"F. I. G. M.","family":"Borges","sequence":"additional","affiliation":[]},{"given":"A.","family":"Brodolin","sequence":"additional","affiliation":[]},{"given":"N.","family":"Byrnes","sequence":"additional","affiliation":[]},{"given":"S.","family":"C\u00e1rcel","sequence":"additional","affiliation":[]},{"given":"J. V.","family":"Carri\u00f3n","sequence":"additional","affiliation":[]},{"given":"S.","family":"Cebri\u00e1n","sequence":"additional","affiliation":[]},{"given":"E.","family":"Church","sequence":"additional","affiliation":[]},{"given":"L.","family":"Cid","sequence":"additional","affiliation":[]},{"given":"C. A. N.","family":"Conde","sequence":"additional","affiliation":[]},{"given":"T.","family":"Contreras","sequence":"additional","affiliation":[]},{"given":"F. P.","family":"Coss\u00edo","sequence":"additional","affiliation":[]},{"given":"E.","family":"Dey","sequence":"additional","affiliation":[]},{"given":"G.","family":"D\u00edaz","sequence":"additional","affiliation":[]},{"given":"T.","family":"Dickel","sequence":"additional","affiliation":[]},{"given":"M.","family":"Elorza","sequence":"additional","affiliation":[]},{"given":"J.","family":"Escada","sequence":"additional","affiliation":[]},{"given":"R.","family":"Esteve","sequence":"additional","affiliation":[]},{"given":"R.","family":"Felkai","sequence":"additional","affiliation":[]},{"given":"L. M. P.","family":"Fernandes","sequence":"additional","affiliation":[]},{"given":"P.","family":"Ferrario","sequence":"additional","affiliation":[]},{"given":"A. L.","family":"Ferreira","sequence":"additional","affiliation":[]},{"given":"F. W.","family":"Foss","sequence":"additional","affiliation":[]},{"given":"E. D. C.","family":"Freitas","sequence":"additional","affiliation":[]},{"given":"Z.","family":"Freixa","sequence":"additional","affiliation":[]},{"given":"J.","family":"Generowicz","sequence":"additional","affiliation":[]},{"given":"A.","family":"Goldschmidt","sequence":"additional","affiliation":[]},{"given":"J. J.","family":"G\u00f3mez-Cadenas","sequence":"additional","affiliation":[]},{"given":"R.","family":"Gonz\u00e1lez","sequence":"additional","affiliation":[]},{"given":"J.","family":"Grocott","sequence":"additional","affiliation":[]},{"given":"K.","family":"Hafidi","sequence":"additional","affiliation":[]},{"given":"J.","family":"Hauptman","sequence":"additional","affiliation":[]},{"given":"C. A. O.","family":"Henriques","sequence":"additional","affiliation":[]},{"given":"J. A. Hernando","family":"Morata","sequence":"additional","affiliation":[]},{"given":"P.","family":"Herrero-G\u00f3mez","sequence":"additional","affiliation":[]},{"given":"V.","family":"Herrero","sequence":"additional","affiliation":[]},{"given":"C.","family":"Herv\u00e9s Carrete","sequence":"additional","affiliation":[]},{"given":"Y.","family":"Ifergan","sequence":"additional","affiliation":[]},{"given":"L.","family":"Labarga","sequence":"additional","affiliation":[]},{"given":"L.","family":"Larizgoitia","sequence":"additional","affiliation":[]},{"given":"A.","family":"Larumbe","sequence":"additional","affiliation":[]},{"given":"P.","family":"Lebrun","sequence":"additional","affiliation":[]},{"given":"F.","family":"Lopez","sequence":"additional","affiliation":[]},{"given":"N.","family":"L\u00f3pez-March","sequence":"additional","affiliation":[]},{"given":"R.","family":"Madigan","sequence":"additional","affiliation":[]},{"given":"R. D. P.","family":"Mano","sequence":"additional","affiliation":[]},{"given":"A. P.","family":"Marques","sequence":"additional","affiliation":[]},{"given":"J.","family":"Mart\u00edn-Albo","sequence":"additional","affiliation":[]},{"given":"G.","family":"Mart\u00ednez-Lema","sequence":"additional","affiliation":[]},{"given":"M.","family":"Mart\u00ednez-Vara","sequence":"additional","affiliation":[]},{"given":"Z. E.","family":"Meziani","sequence":"additional","affiliation":[]},{"given":"R. L.","family":"Miller","sequence":"additional","affiliation":[]},{"given":"K.","family":"Mistry","sequence":"additional","affiliation":[]},{"given":"J.","family":"Molina-Canteras","sequence":"additional","affiliation":[]},{"given":"F.","family":"Monrabal","sequence":"additional","affiliation":[]},{"given":"C. M. B.","family":"Monteiro","sequence":"additional","affiliation":[]},{"given":"F. J.","family":"Mora","sequence":"additional","affiliation":[]},{"given":"J.","family":"Mu\u00f1oz Vidal","sequence":"additional","affiliation":[]},{"given":"P.","family":"Novella","sequence":"additional","affiliation":[]},{"given":"A.","family":"Nu\u00f1ez","sequence":"additional","affiliation":[]},{"given":"D. R.","family":"Nygren","sequence":"additional","affiliation":[]},{"given":"E.","family":"Oblak","sequence":"additional","affiliation":[]},{"given":"J.","family":"Palacio","sequence":"additional","affiliation":[]},{"given":"B.","family":"Palmeiro","sequence":"additional","affiliation":[]},{"given":"A.","family":"Para","sequence":"additional","affiliation":[]},{"given":"I.","family":"Parmaksiz","sequence":"additional","affiliation":[]},{"given":"J.","family":"Pelegrin","sequence":"additional","affiliation":[]},{"given":"M.","family":"P\u00e9rez Maneiro","sequence":"additional","affiliation":[]},{"given":"M.","family":"Querol","sequence":"additional","affiliation":[]},{"given":"A. B.","family":"Redwine","sequence":"additional","affiliation":[]},{"given":"J.","family":"Renner","sequence":"additional","affiliation":[]},{"given":"I.","family":"Rivilla","sequence":"additional","affiliation":[]},{"given":"J.","family":"Rodr\u00edguez","sequence":"additional","affiliation":[]},{"given":"C.","family":"Rogero","sequence":"additional","affiliation":[]},{"given":"L.","family":"Rogers","sequence":"additional","affiliation":[]},{"given":"B.","family":"Romeo","sequence":"additional","affiliation":[]},{"given":"C.","family":"Romo-Luque","sequence":"additional","affiliation":[]},{"given":"F. P.","family":"Santos","sequence":"additional","affiliation":[]},{"given":"J. M. F.","family":"dos Santos","sequence":"additional","affiliation":[]},{"given":"I.","family":"Shomroni","sequence":"additional","affiliation":[]},{"given":"A.","family":"Sim\u00f3n","sequence":"additional","affiliation":[]},{"given":"S. R.","family":"Soleti","sequence":"additional","affiliation":[]},{"given":"M.","family":"Sorel","sequence":"additional","affiliation":[]},{"given":"J.","family":"Soto-Oton","sequence":"additional","affiliation":[]},{"given":"J. M. R.","family":"Teixeira","sequence":"additional","affiliation":[]},{"given":"J. F.","family":"Toledo","sequence":"additional","affiliation":[]},{"given":"J.","family":"Torrent","sequence":"additional","affiliation":[]},{"given":"A.","family":"Trettin","sequence":"additional","affiliation":[]},{"given":"A.","family":"Us\u00f3n","sequence":"additional","affiliation":[]},{"given":"J. F. C. A.","family":"Veloso","sequence":"additional","affiliation":[]},{"given":"J.","family":"Waiton","sequence":"additional","affiliation":[]},{"given":"J. T.","family":"White","sequence":"additional","affiliation":[]}],"member":"297","published-online":{"date-parts":[[2024,5,21]]},"reference":[{"unstructured":"NEXT Collaboration, P. Novella et al., Measurement of the $${}^{136}$$Xe two-neutrino double beta decay half-life via direct background subtraction in NEXT. arXiv:2111.11091","key":"12865_CR1"},{"unstructured":"EXO Collaboration, G. Anton et al., Search for neutrinoless double-$$\\beta $$ decay with the complete EXO-200 dataset. Phys. Rev. Lett. 123 (2019). arXiv:1906.02723","key":"12865_CR2"},{"unstructured":"nEXO Collaboration, G. Adhikari et al., nEXO: neutrinoless double beta decay search beyond $$10^{28}$$ year half-life sensitivity. J. Phys. G Nucl. Part. Phys. 49: 015104 (2021). arXiv:2106.16243","key":"12865_CR3"},{"unstructured":"PandaX Collaboration, Y. Meng et al., Dark matter search results from the PandaX-4T commissioning run. Phys. Rev. Lett. 127 (2021). arXiv:2107.13438","key":"12865_CR4"},{"issue":"12","key":"12865_CR5","first-page":"1","volume":"77","author":"E Aprile","year":"2017","unstructured":"E. Aprile, J. Aalbers, F. Agostini, M. Alfonsi, F. Amaro, M. Anthony, B. Antunes, F. Arneodo, M. Balata, P. Barrow et al., The xenon1t dark matter experiment. Eur. Phys. J. C 77(12), 1\u201323 (2017)","journal-title":"Eur. Phys. J. C"},{"unstructured":"LUX-Zeplin Collaboration, D.S. Akerib et al., The LUX-ZEPLIN (LZ) experiment. Nucl. Instrum. Methods Phys. Res. Sect. A Accel. Spectrom. Detect. Assoc. Equip. 953, 163047 (2020). arXiv:1910.09124","key":"12865_CR6"},{"unstructured":"DarkSide Collaboration, P. Agnes et al., Low-mass dark matter search with the DarkSide-50 experiment. Phys. Rev. Lett. 121 (2018). arXiv:1802.06994","key":"12865_CR7"},{"issue":"07","key":"12865_CR8","doi-asserted-by":"publisher","first-page":"P07013","DOI":"10.1088\/1748-0221\/13\/07\/P07013","volume":"13","author":"A Sim\u00f3n","year":"2018","unstructured":"A. Sim\u00f3n, R. Felkai, G. Mart\u00ednez-Lema, F. Monrabal, D. Gonz\u00e1lez-D\u00edaz, M. Sorel, J.H. Morata, J. G\u00f3mez-Cadenas, C. Adams, V. \u00c1lvarez et al., Electron drift properties in high pressure gaseous xenon. J. Instrum. 13(07), P07013 (2018)","journal-title":"J. Instrum."},{"unstructured":"NEXT Collaboration, A.D. McDonald\u00a0et al., Electron drift and longitudinal diffusion in high pressure xenon-helium gas mixtures. J. Instrum. 14(08), P08009 (2019). arXiv:1902.05544","key":"12865_CR9"},{"unstructured":"NEXT Collaboration, C. Adams et al., Sensitivity of a tonne-scale NEXT detector for neutrinoless double-beta decay searches. J. High Energy Phys. 2021(8), 1\u201324 (2021). arXiv:2005.06467","key":"12865_CR10"},{"issue":"11","key":"12865_CR11","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.104.112007","volume":"104","author":"A Avasthi","year":"2021","unstructured":"A. Avasthi, T. Bowyer, C. Bray, T. Brunner, N. Catarineu, E. Church, R. Guenette, S. Haselschwardt, J. Hayes, M. Heffner et al., Kiloton-scale xenon detectors for neutrinoless double beta decay and other new physics searches. Phys. Rev. D 104(11), 112007 (2021)","journal-title":"Phys. Rev. D"},{"issue":"08","key":"12865_CR12","doi-asserted-by":"publisher","first-page":"P08006","DOI":"10.1088\/1748-0221\/18\/08\/P08006","volume":"18","author":"N Byrnes","year":"2023","unstructured":"N. Byrnes, I. Parmaksiz, C. Adams, J. Asaadi, J. Baeza-Rubio, K. Bailey, E. Church, D. Gonz\u00e1lez-D\u00edaz, A. Higley, B. Jones et al., Next-crab-0: a high pressure gaseous xenon time projection chamber with a direct VUV camera based readout. J. Instrum. 18(08), P08006 (2023)","journal-title":"J. Instrum."},{"issue":"13","key":"12865_CR13","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.120.132504","volume":"120","author":"A McDonald","year":"2018","unstructured":"A. McDonald, B. Jones, D. Nygren, C. Adams, V. \u00c1lvarez, C. Azevedo, J. Benlloch-Rodr\u00edguez, F. Borges, A. Botas, S. C\u00e1rcel et al., Demonstration of single-barium-ion sensitivity for neutrinoless double-beta decay using single-molecule fluorescence imaging. Phys. Rev. Lett. 120(13), 132504 (2018)","journal-title":"Phys. Rev. Lett."},{"issue":"7814","key":"12865_CR14","doi-asserted-by":"publisher","first-page":"48","DOI":"10.1038\/s41586-020-2431-5","volume":"583","author":"I Rivilla","year":"2020","unstructured":"I. Rivilla, B. Aparicio, J.M. Bueno, D. Casanova, C. Tonnel\u00e9, Z. Freixa, P. Herrero, C. Rogero, J.I. Miranda, R.M. Mart\u00ednez-Ojeda et al., Fluorescent bicolour sensor for low-background neutrinoless double $$\\beta $$ decay experiments. Nature 583(7814), 48\u201354 (2020)","journal-title":"Nature"},{"issue":"11","key":"12865_CR15","doi-asserted-by":"publisher","first-page":"P11021","DOI":"10.1088\/1748-0221\/15\/11\/P11021","volume":"15","author":"AL Villalpando","year":"2020","unstructured":"A.L. Villalpando, J. Mart\u00edn-Albo, W. Chen, R. Guenette, C. Lego, J. Park, F. Capasso, Improving the light collection efficiency of silicon photomultipliers through the use of metalenses. J. Instrum. 15(11), P11021 (2020)","journal-title":"J. Instrum."},{"doi-asserted-by":"crossref","unstructured":"D. Nygren, High-pressure xenon gas electroluminescent TPC for $$0 \\nu \\beta \\beta $$-decay search. Nucl. Instrum. Meth. A 603, 337\u2013348 (2009)","key":"12865_CR16","DOI":"10.1016\/j.nima.2009.01.222"},{"unstructured":"NEXT Collaboration, V. \u00c1lvarez et al., Operation and first results of the NEXT-DEMO prototype using a silicon photomultiplier tracking array. J. Instrum. 8, P09011 (2013). arXiv:1306.0471","key":"12865_CR17"},{"unstructured":"NEXT Collaboration, P. Ferrario et al., First proof of topological signature in the high pressure xenon gas TPC with electroluminescence amplification for the NEXT experiment. J. High Energy Phys. (Online) 2016 (2016). arXiv:1507.05902","key":"12865_CR18"},{"unstructured":"NEXT Collaboration, P. Novella et al., Radiogenic backgrounds in the NEXT double beta decay experiment. J. High Energy Phys. 2019 (2019). arXiv:1905.13625","key":"12865_CR19"},{"unstructured":"NEXT Collaboration, J. Renner\u00a0et al., Energy calibration of the NEXT-White detector with 1% resolution near Q$$\\beta \\beta $$ of 136Xe. J. High Energy Phys. 2019 (2019). arXiv:1905.13110","key":"12865_CR20"},{"unstructured":"NEXT Collaboration, P. Ferrario\u00a0et al., Demonstration of the event identification capabilities of the NEXT-White detector. J. High Energy Phys. 2019 (2019). arXiv:1905.13141","key":"12865_CR21"},{"unstructured":"NEXT Collaboration, F. Monrabal\u00a0et al., The NEXT White (NEW) detector. J. Instrum. 13, P12010 (2018). arXiv:1804.02409","key":"12865_CR22"},{"issue":"5","key":"12865_CR23","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.105.055501","volume":"105","author":"P Novella","year":"2022","unstructured":"P. Novella, M. Sorel, A. Us\u00f3n, C. Adams, H. Almaz\u00e1n, V. \u00c1lvarez, B. Aparicio, A. Aranburu, L. Arazi, I. Arnquist et al., Measurement of the Xe 136 two-neutrino double-$$\\beta $$-decay half-life via direct background subtraction in next. Phys. Rev. C 105(5), 055501 (2022)","journal-title":"Phys. Rev. C"},{"unstructured":"P.\u00a0Novella, M.\u00a0Sorel, A.\u00a0Us\u00f3n, C.\u00a0Adams, H.\u00a0Almaz\u00e1n, V.\u00a0\u00c1lvarez, B.\u00a0Aparicio, A.\u00a0Aranburu, L.\u00a0Arazi, I.\u00a0Arnquist et\u00a0al., Demonstration of neutrinoless double beta decay searches in gaseous xenon with next, arXiv preprint arXiv:2305.09435 (2023)","key":"12865_CR24"},{"doi-asserted-by":"crossref","unstructured":"V.\u00a0Alvarez, F.I. Borges, S.\u00a0C\u00e1rcel, J.\u00a0Carmona, J.\u00a0Castel, J.\u00a0Catal\u00e1, S.\u00a0Cebri\u00e1n, A.\u00a0Cervera, D.\u00a0Chan, C.A. Conde et\u00a0al., Next-100 technical design report (tdr). Executive summary. J. Instrum. 7(06), T06001 (2012)","key":"12865_CR25","DOI":"10.1088\/1748-0221\/7\/06\/T06001"},{"doi-asserted-by":"crossref","unstructured":"NEXT Collaboration, G. Mart\u00ednez-Lema\u00a0et al., Calibration of the NEXT-White detector using $$^{83m}$$Kr decays. J. Instrum. 13, P10014 (2018). arXiv:1804.01780","key":"12865_CR26","DOI":"10.1088\/1748-0221\/13\/10\/P10014"},{"unstructured":"NEXT Collaboration, J. Mart\u00edn-Albo et al., Sensitivity of NEXT-100 to neutrinoless double beta decay. JHEP 05, 159 (2016). arXiv:1511.09246","key":"12865_CR27"},{"unstructured":"NEXT Collaboration, A. Sim\u00f3n\u00a0et al., Electron drift properties in high pressure gaseous xenon. J. Instrum. 13, P07013 (2018). arXiv:1804.01680","key":"12865_CR28"},{"unstructured":"NEXT Collaboration, J. Renner\u00a0et al., Background rejection in NEXT using deep neural networks. J. Instrum. 12, T01004 (2017). arXiv:1609.06202","key":"12865_CR29"},{"unstructured":"NEXT Collaboration, M. Kekic\u00a0et al., Demonstration of background rejection using deep convolutional neural networks in the NEXT experiment. J. High Energy Phys. 2021 (2021). arXiv:2009.10783","key":"12865_CR30"},{"unstructured":"F.\u00a0Chollet et\u00a0al., Keras. https:\/\/keras.io (2015)","key":"12865_CR31"}],"container-title":["The European Physical Journal C"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/link.springer.com\/content\/pdf\/10.1140\/epjc\/s10052-024-12865-9.pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/link.springer.com\/article\/10.1140\/epjc\/s10052-024-12865-9\/fulltext.html","content-type":"text\/html","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/link.springer.com\/content\/pdf\/10.1140\/epjc\/s10052-024-12865-9.pdf","content-type":"application\/pdf","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2024,6,17]],"date-time":"2024-06-17T19:24:05Z","timestamp":1718652245000},"score":1,"resource":{"primary":{"URL":"https:\/\/link.springer.com\/10.1140\/epjc\/s10052-024-12865-9"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2024,5,21]]},"references-count":31,"journal-issue":{"issue":"5","published-online":{"date-parts":[[2024,5]]}},"alternative-id":["12865"],"URL":"https:\/\/doi.org\/10.1140\/epjc\/s10052-024-12865-9","relation":{},"ISSN":["1434-6052"],"issn-type":[{"type":"electronic","value":"1434-6052"}],"subject":[],"published":{"date-parts":[[2024,5,21]]},"assertion":[{"value":"19 February 2024","order":1,"name":"received","label":"Received","group":{"name":"ArticleHistory","label":"Article History"}},{"value":"29 April 2024","order":2,"name":"accepted","label":"Accepted","group":{"name":"ArticleHistory","label":"Article History"}},{"value":"21 May 2024","order":3,"name":"first_online","label":"First Online","group":{"name":"ArticleHistory","label":"Article History"}}],"article-number":"518"}}