Energy resolution and linearity of XENON1T in the MeV energy range
Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare...
Ausführliche Beschreibung
Autor*in: |
E. Aprile [verfasserIn] J. Aalbers [verfasserIn] F. Agostini [verfasserIn] M. Alfonsi [verfasserIn] L. Althueser [verfasserIn] F. D. Amaro [verfasserIn] V. C. Antochi [verfasserIn] E. Angelino [verfasserIn] J. Angevaare [verfasserIn] F. Arneodo [verfasserIn] D. Barge [verfasserIn] L. Baudis [verfasserIn] B. Bauermeister [verfasserIn] L. Bellagamba [verfasserIn] M. L. Benabderrahmane [verfasserIn] T. Berger [verfasserIn] P. A. Breur [verfasserIn] A. Brown [verfasserIn] E. Brown [verfasserIn] S. Bruenner [verfasserIn] G. Bruno [verfasserIn] R. Budnik [verfasserIn] C. Capelli [verfasserIn] J. M. R. Cardoso [verfasserIn] D. Cichon [verfasserIn] B. Cimmino [verfasserIn] M. Clark [verfasserIn] D. Coderre [verfasserIn] A. P. Colijn [verfasserIn] J. Conrad [verfasserIn] J. P. Cussonneau [verfasserIn] M. P. Decowski [verfasserIn] A. Depoian [verfasserIn] P. Di Gangi [verfasserIn] A. Di Giovanni [verfasserIn] R. Di Stefano [verfasserIn] S. Diglio [verfasserIn] A. Elykov [verfasserIn] G. Eurin [verfasserIn] A. D. Ferella [verfasserIn] W. Fulgione [verfasserIn] P. Gaemers [verfasserIn] R. Gaior [verfasserIn] A. Gallo Rosso [verfasserIn] M. Galloway [verfasserIn] F. Gao [verfasserIn] M. Garbini [verfasserIn] L. Grandi [verfasserIn] C. Hasterok [verfasserIn] C. Hils [verfasserIn] K. Hiraide [verfasserIn] L. Hoetzsch [verfasserIn] E. Hogenbirk [verfasserIn] J. Howlett [verfasserIn] M. Iacovacci [verfasserIn] Y. Itow [verfasserIn] F. Joerg [verfasserIn] N. Kato [verfasserIn] S. Kazama [verfasserIn] M. Kobayashi [verfasserIn] G. Koltman [verfasserIn] A. Kopec [verfasserIn] H. Landsman [verfasserIn] R. F. Lang [verfasserIn] L. Levinson [verfasserIn] Q. Lin [verfasserIn] S. Lindemann [verfasserIn] M. Lindner [verfasserIn] F. Lombardi [verfasserIn] J. A. M. Lopes [verfasserIn] E. López Fune [verfasserIn] C. Macolino [verfasserIn] J. Mahlstedt [verfasserIn] L. Manenti [verfasserIn] A. Manfredini [verfasserIn] F. Marignetti [verfasserIn] T. Marrodán Undagoitia [verfasserIn] K. Martens [verfasserIn] J. Masbou [verfasserIn] D. Masson [verfasserIn] S. Mastroianni [verfasserIn] M. Messina [verfasserIn] K. Miuchi [verfasserIn] A. Molinario [verfasserIn] K. Morå [verfasserIn] S. Moriyama [verfasserIn] Y. Mosbacher [verfasserIn] M. Murra [verfasserIn] J. Naganoma [verfasserIn] K. Ni [verfasserIn] U. Oberlack [verfasserIn] K. Odgers [verfasserIn] J. Palacio [verfasserIn] B. Pelssers [verfasserIn] R. Peres [verfasserIn] J. Pienaar [verfasserIn] V. Pizzella [verfasserIn] G. Plante [verfasserIn] J. Qin [verfasserIn] H. Qiu [verfasserIn] D. Ramírez García [verfasserIn] S. Reichard [verfasserIn] A. Rocchetti [verfasserIn] N. Rupp [verfasserIn] J. M. F. dos Santos [verfasserIn] G. Sartorelli [verfasserIn] N. Šarčević [verfasserIn] M. Scheibelhut [verfasserIn] S. Schindler [verfasserIn] J. Schreiner [verfasserIn] D. Schulte [verfasserIn] M. Schumann [verfasserIn] L. Scotto Lavina [verfasserIn] M. Selvi [verfasserIn] F. Semeria [verfasserIn] P. Shagin [verfasserIn] E. Shockley [verfasserIn] M. Silva [verfasserIn] H. Simgen [verfasserIn] A. Takeda [verfasserIn] C. Therreau [verfasserIn] D. Thers [verfasserIn] F. Toschi [verfasserIn] G. Trinchero [verfasserIn] C. Tunnell [verfasserIn] M. Vargas [verfasserIn] G. Volta [verfasserIn] O. Wack [verfasserIn] H. Wang [verfasserIn] Y. Wei [verfasserIn] C. Weinheimer [verfasserIn] M. Weiss Xu [verfasserIn] D. Wenz [verfasserIn] C. Wittweg [verfasserIn] J. Wulf [verfasserIn] Z. Xu [verfasserIn] M. Yamashita [verfasserIn] J. Ye [verfasserIn] G. Zavattini [verfasserIn] Y. Zhang [verfasserIn] T. Zhu [verfasserIn] J. P. Zopounidis [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2020 |
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Übergeordnetes Werk: |
In: European Physical Journal C: Particles and Fields - SpringerOpen, 2017, 80(2020), 8, Seite 9 |
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Übergeordnetes Werk: |
volume:80 ; year:2020 ; number:8 ; pages:9 |
Links: |
Link aufrufen |
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DOI / URN: |
10.1140/epjc/s10052-020-8284-0 |
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Katalog-ID: |
DOAJ069971919 |
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100 | 0 | |a E. Aprile |e verfasserin |4 aut | |
245 | 1 | 0 | |a Energy resolution and linearity of XENON1T in the MeV energy range |
264 | 1 | |c 2020 | |
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520 | |a Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. | ||
653 | 0 | |a Astrophysics | |
653 | 0 | |a Nuclear and particle physics. Atomic energy. Radioactivity | |
700 | 0 | |a J. Aalbers |e verfasserin |4 aut | |
700 | 0 | |a F. Agostini |e verfasserin |4 aut | |
700 | 0 | |a M. Alfonsi |e verfasserin |4 aut | |
700 | 0 | |a L. Althueser |e verfasserin |4 aut | |
700 | 0 | |a F. D. Amaro |e verfasserin |4 aut | |
700 | 0 | |a V. C. Antochi |e verfasserin |4 aut | |
700 | 0 | |a E. Angelino |e verfasserin |4 aut | |
700 | 0 | |a J. Angevaare |e verfasserin |4 aut | |
700 | 0 | |a F. Arneodo |e verfasserin |4 aut | |
700 | 0 | |a D. Barge |e verfasserin |4 aut | |
700 | 0 | |a L. Baudis |e verfasserin |4 aut | |
700 | 0 | |a B. Bauermeister |e verfasserin |4 aut | |
700 | 0 | |a L. Bellagamba |e verfasserin |4 aut | |
700 | 0 | |a M. L. Benabderrahmane |e verfasserin |4 aut | |
700 | 0 | |a T. Berger |e verfasserin |4 aut | |
700 | 0 | |a P. A. Breur |e verfasserin |4 aut | |
700 | 0 | |a A. Brown |e verfasserin |4 aut | |
700 | 0 | |a E. Brown |e verfasserin |4 aut | |
700 | 0 | |a S. Bruenner |e verfasserin |4 aut | |
700 | 0 | |a G. Bruno |e verfasserin |4 aut | |
700 | 0 | |a R. Budnik |e verfasserin |4 aut | |
700 | 0 | |a C. Capelli |e verfasserin |4 aut | |
700 | 0 | |a J. M. R. Cardoso |e verfasserin |4 aut | |
700 | 0 | |a D. Cichon |e verfasserin |4 aut | |
700 | 0 | |a B. Cimmino |e verfasserin |4 aut | |
700 | 0 | |a M. Clark |e verfasserin |4 aut | |
700 | 0 | |a D. Coderre |e verfasserin |4 aut | |
700 | 0 | |a A. P. Colijn |e verfasserin |4 aut | |
700 | 0 | |a J. Conrad |e verfasserin |4 aut | |
700 | 0 | |a J. P. Cussonneau |e verfasserin |4 aut | |
700 | 0 | |a M. P. Decowski |e verfasserin |4 aut | |
700 | 0 | |a A. Depoian |e verfasserin |4 aut | |
700 | 0 | |a P. Di Gangi |e verfasserin |4 aut | |
700 | 0 | |a A. Di Giovanni |e verfasserin |4 aut | |
700 | 0 | |a R. Di Stefano |e verfasserin |4 aut | |
700 | 0 | |a S. Diglio |e verfasserin |4 aut | |
700 | 0 | |a A. Elykov |e verfasserin |4 aut | |
700 | 0 | |a G. Eurin |e verfasserin |4 aut | |
700 | 0 | |a A. D. Ferella |e verfasserin |4 aut | |
700 | 0 | |a W. Fulgione |e verfasserin |4 aut | |
700 | 0 | |a P. Gaemers |e verfasserin |4 aut | |
700 | 0 | |a R. Gaior |e verfasserin |4 aut | |
700 | 0 | |a A. Gallo Rosso |e verfasserin |4 aut | |
700 | 0 | |a M. Galloway |e verfasserin |4 aut | |
700 | 0 | |a F. Gao |e verfasserin |4 aut | |
700 | 0 | |a M. Garbini |e verfasserin |4 aut | |
700 | 0 | |a L. Grandi |e verfasserin |4 aut | |
700 | 0 | |a C. Hasterok |e verfasserin |4 aut | |
700 | 0 | |a C. Hils |e verfasserin |4 aut | |
700 | 0 | |a K. Hiraide |e verfasserin |4 aut | |
700 | 0 | |a L. Hoetzsch |e verfasserin |4 aut | |
700 | 0 | |a E. Hogenbirk |e verfasserin |4 aut | |
700 | 0 | |a J. Howlett |e verfasserin |4 aut | |
700 | 0 | |a M. Iacovacci |e verfasserin |4 aut | |
700 | 0 | |a Y. Itow |e verfasserin |4 aut | |
700 | 0 | |a F. Joerg |e verfasserin |4 aut | |
700 | 0 | |a N. Kato |e verfasserin |4 aut | |
700 | 0 | |a S. Kazama |e verfasserin |4 aut | |
700 | 0 | |a M. Kobayashi |e verfasserin |4 aut | |
700 | 0 | |a G. Koltman |e verfasserin |4 aut | |
700 | 0 | |a A. Kopec |e verfasserin |4 aut | |
700 | 0 | |a H. Landsman |e verfasserin |4 aut | |
700 | 0 | |a R. F. Lang |e verfasserin |4 aut | |
700 | 0 | |a L. Levinson |e verfasserin |4 aut | |
700 | 0 | |a Q. Lin |e verfasserin |4 aut | |
700 | 0 | |a S. Lindemann |e verfasserin |4 aut | |
700 | 0 | |a M. Lindner |e verfasserin |4 aut | |
700 | 0 | |a F. Lombardi |e verfasserin |4 aut | |
700 | 0 | |a J. A. M. Lopes |e verfasserin |4 aut | |
700 | 0 | |a E. López Fune |e verfasserin |4 aut | |
700 | 0 | |a C. Macolino |e verfasserin |4 aut | |
700 | 0 | |a J. Mahlstedt |e verfasserin |4 aut | |
700 | 0 | |a L. Manenti |e verfasserin |4 aut | |
700 | 0 | |a A. Manfredini |e verfasserin |4 aut | |
700 | 0 | |a F. Marignetti |e verfasserin |4 aut | |
700 | 0 | |a T. Marrodán Undagoitia |e verfasserin |4 aut | |
700 | 0 | |a K. Martens |e verfasserin |4 aut | |
700 | 0 | |a J. Masbou |e verfasserin |4 aut | |
700 | 0 | |a D. Masson |e verfasserin |4 aut | |
700 | 0 | |a S. Mastroianni |e verfasserin |4 aut | |
700 | 0 | |a M. Messina |e verfasserin |4 aut | |
700 | 0 | |a K. Miuchi |e verfasserin |4 aut | |
700 | 0 | |a A. Molinario |e verfasserin |4 aut | |
700 | 0 | |a K. Morå |e verfasserin |4 aut | |
700 | 0 | |a S. Moriyama |e verfasserin |4 aut | |
700 | 0 | |a Y. Mosbacher |e verfasserin |4 aut | |
700 | 0 | |a M. Murra |e verfasserin |4 aut | |
700 | 0 | |a J. Naganoma |e verfasserin |4 aut | |
700 | 0 | |a K. Ni |e verfasserin |4 aut | |
700 | 0 | |a U. Oberlack |e verfasserin |4 aut | |
700 | 0 | |a K. Odgers |e verfasserin |4 aut | |
700 | 0 | |a J. Palacio |e verfasserin |4 aut | |
700 | 0 | |a B. Pelssers |e verfasserin |4 aut | |
700 | 0 | |a R. Peres |e verfasserin |4 aut | |
700 | 0 | |a J. Pienaar |e verfasserin |4 aut | |
700 | 0 | |a V. Pizzella |e verfasserin |4 aut | |
700 | 0 | |a G. Plante |e verfasserin |4 aut | |
700 | 0 | |a J. Qin |e verfasserin |4 aut | |
700 | 0 | |a H. Qiu |e verfasserin |4 aut | |
700 | 0 | |a D. Ramírez García |e verfasserin |4 aut | |
700 | 0 | |a S. Reichard |e verfasserin |4 aut | |
700 | 0 | |a A. Rocchetti |e verfasserin |4 aut | |
700 | 0 | |a N. Rupp |e verfasserin |4 aut | |
700 | 0 | |a J. M. F. dos Santos |e verfasserin |4 aut | |
700 | 0 | |a G. Sartorelli |e verfasserin |4 aut | |
700 | 0 | |a N. Šarčević |e verfasserin |4 aut | |
700 | 0 | |a M. Scheibelhut |e verfasserin |4 aut | |
700 | 0 | |a S. Schindler |e verfasserin |4 aut | |
700 | 0 | |a J. Schreiner |e verfasserin |4 aut | |
700 | 0 | |a D. Schulte |e verfasserin |4 aut | |
700 | 0 | |a M. Schumann |e verfasserin |4 aut | |
700 | 0 | |a L. Scotto Lavina |e verfasserin |4 aut | |
700 | 0 | |a M. Selvi |e verfasserin |4 aut | |
700 | 0 | |a F. Semeria |e verfasserin |4 aut | |
700 | 0 | |a P. Shagin |e verfasserin |4 aut | |
700 | 0 | |a E. Shockley |e verfasserin |4 aut | |
700 | 0 | |a M. Silva |e verfasserin |4 aut | |
700 | 0 | |a H. Simgen |e verfasserin |4 aut | |
700 | 0 | |a A. Takeda |e verfasserin |4 aut | |
700 | 0 | |a C. Therreau |e verfasserin |4 aut | |
700 | 0 | |a D. Thers |e verfasserin |4 aut | |
700 | 0 | |a F. Toschi |e verfasserin |4 aut | |
700 | 0 | |a G. Trinchero |e verfasserin |4 aut | |
700 | 0 | |a C. Tunnell |e verfasserin |4 aut | |
700 | 0 | |a M. Vargas |e verfasserin |4 aut | |
700 | 0 | |a G. Volta |e verfasserin |4 aut | |
700 | 0 | |a O. Wack |e verfasserin |4 aut | |
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700 | 0 | |a C. Weinheimer |e verfasserin |4 aut | |
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700 | 0 | |a Z. Xu |e verfasserin |4 aut | |
700 | 0 | |a M. Yamashita |e verfasserin |4 aut | |
700 | 0 | |a J. Ye |e verfasserin |4 aut | |
700 | 0 | |a G. Zavattini |e verfasserin |4 aut | |
700 | 0 | |a Y. Zhang |e verfasserin |4 aut | |
700 | 0 | |a T. Zhu |e verfasserin |4 aut | |
700 | 0 | |a J. P. Zopounidis |e verfasserin |4 aut | |
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2020 |
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10.1140/epjc/s10052-020-8284-0 doi (DE-627)DOAJ069971919 (DE-599)DOAJ061f56a5441044009b681378a41c3033 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Aprile verfasserin aut Energy resolution and linearity of XENON1T in the MeV energy range 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity J. Aalbers verfasserin aut F. Agostini verfasserin aut M. Alfonsi verfasserin aut L. Althueser verfasserin aut F. D. Amaro verfasserin aut V. C. Antochi verfasserin aut E. Angelino verfasserin aut J. Angevaare verfasserin aut F. Arneodo verfasserin aut D. Barge verfasserin aut L. Baudis verfasserin aut B. Bauermeister verfasserin aut L. Bellagamba verfasserin aut M. L. Benabderrahmane verfasserin aut T. Berger verfasserin aut P. A. Breur verfasserin aut A. Brown verfasserin aut E. Brown verfasserin aut S. Bruenner verfasserin aut G. Bruno verfasserin aut R. Budnik verfasserin aut C. Capelli verfasserin aut J. M. R. Cardoso verfasserin aut D. Cichon verfasserin aut B. Cimmino verfasserin aut M. Clark verfasserin aut D. Coderre verfasserin aut A. P. Colijn verfasserin aut J. Conrad verfasserin aut J. P. Cussonneau verfasserin aut M. P. Decowski verfasserin aut A. Depoian verfasserin aut P. Di Gangi verfasserin aut A. Di Giovanni verfasserin aut R. Di Stefano verfasserin aut S. Diglio verfasserin aut A. Elykov verfasserin aut G. Eurin verfasserin aut A. D. Ferella verfasserin aut W. Fulgione verfasserin aut P. Gaemers verfasserin aut R. Gaior verfasserin aut A. Gallo Rosso verfasserin aut M. Galloway verfasserin aut F. Gao verfasserin aut M. Garbini verfasserin aut L. Grandi verfasserin aut C. Hasterok verfasserin aut C. Hils verfasserin aut K. Hiraide verfasserin aut L. Hoetzsch verfasserin aut E. Hogenbirk verfasserin aut J. Howlett verfasserin aut M. Iacovacci verfasserin aut Y. Itow verfasserin aut F. Joerg verfasserin aut N. Kato verfasserin aut S. Kazama verfasserin aut M. Kobayashi verfasserin aut G. Koltman verfasserin aut A. Kopec verfasserin aut H. Landsman verfasserin aut R. F. Lang verfasserin aut L. Levinson verfasserin aut Q. Lin verfasserin aut S. Lindemann verfasserin aut M. Lindner verfasserin aut F. Lombardi verfasserin aut J. A. M. Lopes verfasserin aut E. López Fune verfasserin aut C. Macolino verfasserin aut J. Mahlstedt verfasserin aut L. Manenti verfasserin aut A. Manfredini verfasserin aut F. Marignetti verfasserin aut T. Marrodán Undagoitia verfasserin aut K. Martens verfasserin aut J. Masbou verfasserin aut D. Masson verfasserin aut S. Mastroianni verfasserin aut M. Messina verfasserin aut K. Miuchi verfasserin aut A. Molinario verfasserin aut K. Morå verfasserin aut S. Moriyama verfasserin aut Y. Mosbacher verfasserin aut M. Murra verfasserin aut J. Naganoma verfasserin aut K. Ni verfasserin aut U. Oberlack verfasserin aut K. Odgers verfasserin aut J. Palacio verfasserin aut B. Pelssers verfasserin aut R. Peres verfasserin aut J. Pienaar verfasserin aut V. Pizzella verfasserin aut G. Plante verfasserin aut J. Qin verfasserin aut H. Qiu verfasserin aut D. Ramírez García verfasserin aut S. Reichard verfasserin aut A. Rocchetti verfasserin aut N. Rupp verfasserin aut J. M. F. dos Santos verfasserin aut G. Sartorelli verfasserin aut N. Šarčević verfasserin aut M. Scheibelhut verfasserin aut S. Schindler verfasserin aut J. Schreiner verfasserin aut D. Schulte verfasserin aut M. Schumann verfasserin aut L. Scotto Lavina verfasserin aut M. Selvi verfasserin aut F. Semeria verfasserin aut P. Shagin verfasserin aut E. Shockley verfasserin aut M. Silva verfasserin aut H. Simgen verfasserin aut A. Takeda verfasserin aut C. Therreau verfasserin aut D. Thers verfasserin aut F. Toschi verfasserin aut G. Trinchero verfasserin aut C. Tunnell verfasserin aut M. Vargas verfasserin aut G. Volta verfasserin aut O. Wack verfasserin aut H. Wang verfasserin aut Y. Wei verfasserin aut C. Weinheimer verfasserin aut M. Weiss Xu verfasserin aut D. Wenz verfasserin aut C. Wittweg verfasserin aut J. Wulf verfasserin aut Z. Xu verfasserin aut M. Yamashita verfasserin aut J. Ye verfasserin aut G. Zavattini verfasserin aut Y. Zhang verfasserin aut T. Zhu verfasserin aut J. P. Zopounidis verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 8, Seite 9 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:8 pages:9 https://doi.org/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/article/061f56a5441044009b681378a41c3033 kostenfrei http://link.springer.com/article/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 8 9 |
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10.1140/epjc/s10052-020-8284-0 doi (DE-627)DOAJ069971919 (DE-599)DOAJ061f56a5441044009b681378a41c3033 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Aprile verfasserin aut Energy resolution and linearity of XENON1T in the MeV energy range 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity J. Aalbers verfasserin aut F. Agostini verfasserin aut M. Alfonsi verfasserin aut L. Althueser verfasserin aut F. D. Amaro verfasserin aut V. C. Antochi verfasserin aut E. Angelino verfasserin aut J. Angevaare verfasserin aut F. Arneodo verfasserin aut D. Barge verfasserin aut L. Baudis verfasserin aut B. Bauermeister verfasserin aut L. Bellagamba verfasserin aut M. L. Benabderrahmane verfasserin aut T. Berger verfasserin aut P. A. Breur verfasserin aut A. Brown verfasserin aut E. Brown verfasserin aut S. Bruenner verfasserin aut G. Bruno verfasserin aut R. Budnik verfasserin aut C. Capelli verfasserin aut J. M. R. Cardoso verfasserin aut D. Cichon verfasserin aut B. Cimmino verfasserin aut M. Clark verfasserin aut D. Coderre verfasserin aut A. P. Colijn verfasserin aut J. Conrad verfasserin aut J. P. Cussonneau verfasserin aut M. P. Decowski verfasserin aut A. Depoian verfasserin aut P. Di Gangi verfasserin aut A. Di Giovanni verfasserin aut R. Di Stefano verfasserin aut S. Diglio verfasserin aut A. Elykov verfasserin aut G. Eurin verfasserin aut A. D. Ferella verfasserin aut W. Fulgione verfasserin aut P. Gaemers verfasserin aut R. Gaior verfasserin aut A. Gallo Rosso verfasserin aut M. Galloway verfasserin aut F. Gao verfasserin aut M. Garbini verfasserin aut L. Grandi verfasserin aut C. Hasterok verfasserin aut C. Hils verfasserin aut K. Hiraide verfasserin aut L. Hoetzsch verfasserin aut E. Hogenbirk verfasserin aut J. Howlett verfasserin aut M. Iacovacci verfasserin aut Y. Itow verfasserin aut F. Joerg verfasserin aut N. Kato verfasserin aut S. Kazama verfasserin aut M. Kobayashi verfasserin aut G. Koltman verfasserin aut A. Kopec verfasserin aut H. Landsman verfasserin aut R. F. Lang verfasserin aut L. Levinson verfasserin aut Q. Lin verfasserin aut S. Lindemann verfasserin aut M. Lindner verfasserin aut F. Lombardi verfasserin aut J. A. M. Lopes verfasserin aut E. López Fune verfasserin aut C. Macolino verfasserin aut J. Mahlstedt verfasserin aut L. Manenti verfasserin aut A. Manfredini verfasserin aut F. Marignetti verfasserin aut T. Marrodán Undagoitia verfasserin aut K. Martens verfasserin aut J. Masbou verfasserin aut D. Masson verfasserin aut S. Mastroianni verfasserin aut M. Messina verfasserin aut K. Miuchi verfasserin aut A. Molinario verfasserin aut K. Morå verfasserin aut S. Moriyama verfasserin aut Y. Mosbacher verfasserin aut M. Murra verfasserin aut J. Naganoma verfasserin aut K. Ni verfasserin aut U. Oberlack verfasserin aut K. Odgers verfasserin aut J. Palacio verfasserin aut B. Pelssers verfasserin aut R. Peres verfasserin aut J. Pienaar verfasserin aut V. Pizzella verfasserin aut G. Plante verfasserin aut J. Qin verfasserin aut H. Qiu verfasserin aut D. Ramírez García verfasserin aut S. Reichard verfasserin aut A. Rocchetti verfasserin aut N. Rupp verfasserin aut J. M. F. dos Santos verfasserin aut G. Sartorelli verfasserin aut N. Šarčević verfasserin aut M. Scheibelhut verfasserin aut S. Schindler verfasserin aut J. Schreiner verfasserin aut D. Schulte verfasserin aut M. Schumann verfasserin aut L. Scotto Lavina verfasserin aut M. Selvi verfasserin aut F. Semeria verfasserin aut P. Shagin verfasserin aut E. Shockley verfasserin aut M. Silva verfasserin aut H. Simgen verfasserin aut A. Takeda verfasserin aut C. Therreau verfasserin aut D. Thers verfasserin aut F. Toschi verfasserin aut G. Trinchero verfasserin aut C. Tunnell verfasserin aut M. Vargas verfasserin aut G. Volta verfasserin aut O. Wack verfasserin aut H. Wang verfasserin aut Y. Wei verfasserin aut C. Weinheimer verfasserin aut M. Weiss Xu verfasserin aut D. Wenz verfasserin aut C. Wittweg verfasserin aut J. Wulf verfasserin aut Z. Xu verfasserin aut M. Yamashita verfasserin aut J. Ye verfasserin aut G. Zavattini verfasserin aut Y. Zhang verfasserin aut T. Zhu verfasserin aut J. P. Zopounidis verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 8, Seite 9 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:8 pages:9 https://doi.org/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/article/061f56a5441044009b681378a41c3033 kostenfrei http://link.springer.com/article/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 8 9 |
allfields_unstemmed |
10.1140/epjc/s10052-020-8284-0 doi (DE-627)DOAJ069971919 (DE-599)DOAJ061f56a5441044009b681378a41c3033 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Aprile verfasserin aut Energy resolution and linearity of XENON1T in the MeV energy range 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity J. Aalbers verfasserin aut F. Agostini verfasserin aut M. Alfonsi verfasserin aut L. Althueser verfasserin aut F. D. Amaro verfasserin aut V. C. Antochi verfasserin aut E. Angelino verfasserin aut J. Angevaare verfasserin aut F. Arneodo verfasserin aut D. Barge verfasserin aut L. Baudis verfasserin aut B. Bauermeister verfasserin aut L. Bellagamba verfasserin aut M. L. Benabderrahmane verfasserin aut T. Berger verfasserin aut P. A. Breur verfasserin aut A. Brown verfasserin aut E. Brown verfasserin aut S. Bruenner verfasserin aut G. Bruno verfasserin aut R. Budnik verfasserin aut C. Capelli verfasserin aut J. M. R. Cardoso verfasserin aut D. Cichon verfasserin aut B. Cimmino verfasserin aut M. Clark verfasserin aut D. Coderre verfasserin aut A. P. Colijn verfasserin aut J. Conrad verfasserin aut J. P. Cussonneau verfasserin aut M. P. Decowski verfasserin aut A. Depoian verfasserin aut P. Di Gangi verfasserin aut A. Di Giovanni verfasserin aut R. Di Stefano verfasserin aut S. Diglio verfasserin aut A. Elykov verfasserin aut G. Eurin verfasserin aut A. D. Ferella verfasserin aut W. Fulgione verfasserin aut P. Gaemers verfasserin aut R. Gaior verfasserin aut A. Gallo Rosso verfasserin aut M. Galloway verfasserin aut F. Gao verfasserin aut M. Garbini verfasserin aut L. Grandi verfasserin aut C. Hasterok verfasserin aut C. Hils verfasserin aut K. Hiraide verfasserin aut L. Hoetzsch verfasserin aut E. Hogenbirk verfasserin aut J. Howlett verfasserin aut M. Iacovacci verfasserin aut Y. Itow verfasserin aut F. Joerg verfasserin aut N. Kato verfasserin aut S. Kazama verfasserin aut M. Kobayashi verfasserin aut G. Koltman verfasserin aut A. Kopec verfasserin aut H. Landsman verfasserin aut R. F. Lang verfasserin aut L. Levinson verfasserin aut Q. Lin verfasserin aut S. Lindemann verfasserin aut M. Lindner verfasserin aut F. Lombardi verfasserin aut J. A. M. Lopes verfasserin aut E. López Fune verfasserin aut C. Macolino verfasserin aut J. Mahlstedt verfasserin aut L. Manenti verfasserin aut A. Manfredini verfasserin aut F. Marignetti verfasserin aut T. Marrodán Undagoitia verfasserin aut K. Martens verfasserin aut J. Masbou verfasserin aut D. Masson verfasserin aut S. Mastroianni verfasserin aut M. Messina verfasserin aut K. Miuchi verfasserin aut A. Molinario verfasserin aut K. Morå verfasserin aut S. Moriyama verfasserin aut Y. Mosbacher verfasserin aut M. Murra verfasserin aut J. Naganoma verfasserin aut K. Ni verfasserin aut U. Oberlack verfasserin aut K. Odgers verfasserin aut J. Palacio verfasserin aut B. Pelssers verfasserin aut R. Peres verfasserin aut J. Pienaar verfasserin aut V. Pizzella verfasserin aut G. Plante verfasserin aut J. Qin verfasserin aut H. Qiu verfasserin aut D. Ramírez García verfasserin aut S. Reichard verfasserin aut A. Rocchetti verfasserin aut N. Rupp verfasserin aut J. M. F. dos Santos verfasserin aut G. Sartorelli verfasserin aut N. Šarčević verfasserin aut M. Scheibelhut verfasserin aut S. Schindler verfasserin aut J. Schreiner verfasserin aut D. Schulte verfasserin aut M. Schumann verfasserin aut L. Scotto Lavina verfasserin aut M. Selvi verfasserin aut F. Semeria verfasserin aut P. Shagin verfasserin aut E. Shockley verfasserin aut M. Silva verfasserin aut H. Simgen verfasserin aut A. Takeda verfasserin aut C. Therreau verfasserin aut D. Thers verfasserin aut F. Toschi verfasserin aut G. Trinchero verfasserin aut C. Tunnell verfasserin aut M. Vargas verfasserin aut G. Volta verfasserin aut O. Wack verfasserin aut H. Wang verfasserin aut Y. Wei verfasserin aut C. Weinheimer verfasserin aut M. Weiss Xu verfasserin aut D. Wenz verfasserin aut C. Wittweg verfasserin aut J. Wulf verfasserin aut Z. Xu verfasserin aut M. Yamashita verfasserin aut J. Ye verfasserin aut G. Zavattini verfasserin aut Y. Zhang verfasserin aut T. Zhu verfasserin aut J. P. Zopounidis verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 8, Seite 9 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:8 pages:9 https://doi.org/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/article/061f56a5441044009b681378a41c3033 kostenfrei http://link.springer.com/article/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 8 9 |
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10.1140/epjc/s10052-020-8284-0 doi (DE-627)DOAJ069971919 (DE-599)DOAJ061f56a5441044009b681378a41c3033 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Aprile verfasserin aut Energy resolution and linearity of XENON1T in the MeV energy range 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity J. Aalbers verfasserin aut F. Agostini verfasserin aut M. Alfonsi verfasserin aut L. Althueser verfasserin aut F. D. Amaro verfasserin aut V. C. Antochi verfasserin aut E. Angelino verfasserin aut J. Angevaare verfasserin aut F. Arneodo verfasserin aut D. Barge verfasserin aut L. Baudis verfasserin aut B. Bauermeister verfasserin aut L. Bellagamba verfasserin aut M. L. Benabderrahmane verfasserin aut T. Berger verfasserin aut P. A. Breur verfasserin aut A. Brown verfasserin aut E. Brown verfasserin aut S. Bruenner verfasserin aut G. Bruno verfasserin aut R. Budnik verfasserin aut C. Capelli verfasserin aut J. M. R. Cardoso verfasserin aut D. Cichon verfasserin aut B. Cimmino verfasserin aut M. Clark verfasserin aut D. Coderre verfasserin aut A. P. Colijn verfasserin aut J. Conrad verfasserin aut J. P. Cussonneau verfasserin aut M. P. Decowski verfasserin aut A. Depoian verfasserin aut P. Di Gangi verfasserin aut A. Di Giovanni verfasserin aut R. Di Stefano verfasserin aut S. Diglio verfasserin aut A. Elykov verfasserin aut G. Eurin verfasserin aut A. D. Ferella verfasserin aut W. Fulgione verfasserin aut P. Gaemers verfasserin aut R. Gaior verfasserin aut A. Gallo Rosso verfasserin aut M. Galloway verfasserin aut F. Gao verfasserin aut M. Garbini verfasserin aut L. Grandi verfasserin aut C. Hasterok verfasserin aut C. Hils verfasserin aut K. Hiraide verfasserin aut L. Hoetzsch verfasserin aut E. Hogenbirk verfasserin aut J. Howlett verfasserin aut M. Iacovacci verfasserin aut Y. Itow verfasserin aut F. Joerg verfasserin aut N. Kato verfasserin aut S. Kazama verfasserin aut M. Kobayashi verfasserin aut G. Koltman verfasserin aut A. Kopec verfasserin aut H. Landsman verfasserin aut R. F. Lang verfasserin aut L. Levinson verfasserin aut Q. Lin verfasserin aut S. Lindemann verfasserin aut M. Lindner verfasserin aut F. Lombardi verfasserin aut J. A. M. Lopes verfasserin aut E. López Fune verfasserin aut C. Macolino verfasserin aut J. Mahlstedt verfasserin aut L. Manenti verfasserin aut A. Manfredini verfasserin aut F. Marignetti verfasserin aut T. Marrodán Undagoitia verfasserin aut K. Martens verfasserin aut J. Masbou verfasserin aut D. Masson verfasserin aut S. Mastroianni verfasserin aut M. Messina verfasserin aut K. Miuchi verfasserin aut A. Molinario verfasserin aut K. Morå verfasserin aut S. Moriyama verfasserin aut Y. Mosbacher verfasserin aut M. Murra verfasserin aut J. Naganoma verfasserin aut K. Ni verfasserin aut U. Oberlack verfasserin aut K. Odgers verfasserin aut J. Palacio verfasserin aut B. Pelssers verfasserin aut R. Peres verfasserin aut J. Pienaar verfasserin aut V. Pizzella verfasserin aut G. Plante verfasserin aut J. Qin verfasserin aut H. Qiu verfasserin aut D. Ramírez García verfasserin aut S. Reichard verfasserin aut A. Rocchetti verfasserin aut N. Rupp verfasserin aut J. M. F. dos Santos verfasserin aut G. Sartorelli verfasserin aut N. Šarčević verfasserin aut M. Scheibelhut verfasserin aut S. Schindler verfasserin aut J. Schreiner verfasserin aut D. Schulte verfasserin aut M. Schumann verfasserin aut L. Scotto Lavina verfasserin aut M. Selvi verfasserin aut F. Semeria verfasserin aut P. Shagin verfasserin aut E. Shockley verfasserin aut M. Silva verfasserin aut H. Simgen verfasserin aut A. Takeda verfasserin aut C. Therreau verfasserin aut D. Thers verfasserin aut F. Toschi verfasserin aut G. Trinchero verfasserin aut C. Tunnell verfasserin aut M. Vargas verfasserin aut G. Volta verfasserin aut O. Wack verfasserin aut H. Wang verfasserin aut Y. Wei verfasserin aut C. Weinheimer verfasserin aut M. Weiss Xu verfasserin aut D. Wenz verfasserin aut C. Wittweg verfasserin aut J. Wulf verfasserin aut Z. Xu verfasserin aut M. Yamashita verfasserin aut J. Ye verfasserin aut G. Zavattini verfasserin aut Y. Zhang verfasserin aut T. Zhu verfasserin aut J. P. Zopounidis verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 8, Seite 9 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:8 pages:9 https://doi.org/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/article/061f56a5441044009b681378a41c3033 kostenfrei http://link.springer.com/article/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 8 9 |
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10.1140/epjc/s10052-020-8284-0 doi (DE-627)DOAJ069971919 (DE-599)DOAJ061f56a5441044009b681378a41c3033 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Aprile verfasserin aut Energy resolution and linearity of XENON1T in the MeV energy range 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity J. Aalbers verfasserin aut F. Agostini verfasserin aut M. Alfonsi verfasserin aut L. Althueser verfasserin aut F. D. Amaro verfasserin aut V. C. Antochi verfasserin aut E. Angelino verfasserin aut J. Angevaare verfasserin aut F. Arneodo verfasserin aut D. Barge verfasserin aut L. Baudis verfasserin aut B. Bauermeister verfasserin aut L. Bellagamba verfasserin aut M. L. Benabderrahmane verfasserin aut T. Berger verfasserin aut P. A. Breur verfasserin aut A. Brown verfasserin aut E. Brown verfasserin aut S. Bruenner verfasserin aut G. Bruno verfasserin aut R. Budnik verfasserin aut C. Capelli verfasserin aut J. M. R. Cardoso verfasserin aut D. Cichon verfasserin aut B. Cimmino verfasserin aut M. Clark verfasserin aut D. Coderre verfasserin aut A. P. Colijn verfasserin aut J. Conrad verfasserin aut J. P. Cussonneau verfasserin aut M. P. Decowski verfasserin aut A. Depoian verfasserin aut P. Di Gangi verfasserin aut A. Di Giovanni verfasserin aut R. Di Stefano verfasserin aut S. Diglio verfasserin aut A. Elykov verfasserin aut G. Eurin verfasserin aut A. D. Ferella verfasserin aut W. Fulgione verfasserin aut P. Gaemers verfasserin aut R. Gaior verfasserin aut A. Gallo Rosso verfasserin aut M. Galloway verfasserin aut F. Gao verfasserin aut M. Garbini verfasserin aut L. Grandi verfasserin aut C. Hasterok verfasserin aut C. Hils verfasserin aut K. Hiraide verfasserin aut L. Hoetzsch verfasserin aut E. Hogenbirk verfasserin aut J. Howlett verfasserin aut M. Iacovacci verfasserin aut Y. Itow verfasserin aut F. Joerg verfasserin aut N. Kato verfasserin aut S. Kazama verfasserin aut M. Kobayashi verfasserin aut G. Koltman verfasserin aut A. Kopec verfasserin aut H. Landsman verfasserin aut R. F. Lang verfasserin aut L. Levinson verfasserin aut Q. Lin verfasserin aut S. Lindemann verfasserin aut M. Lindner verfasserin aut F. Lombardi verfasserin aut J. A. M. Lopes verfasserin aut E. López Fune verfasserin aut C. Macolino verfasserin aut J. Mahlstedt verfasserin aut L. Manenti verfasserin aut A. Manfredini verfasserin aut F. Marignetti verfasserin aut T. Marrodán Undagoitia verfasserin aut K. Martens verfasserin aut J. Masbou verfasserin aut D. Masson verfasserin aut S. Mastroianni verfasserin aut M. Messina verfasserin aut K. Miuchi verfasserin aut A. Molinario verfasserin aut K. Morå verfasserin aut S. Moriyama verfasserin aut Y. Mosbacher verfasserin aut M. Murra verfasserin aut J. Naganoma verfasserin aut K. Ni verfasserin aut U. Oberlack verfasserin aut K. Odgers verfasserin aut J. Palacio verfasserin aut B. Pelssers verfasserin aut R. Peres verfasserin aut J. Pienaar verfasserin aut V. Pizzella verfasserin aut G. Plante verfasserin aut J. Qin verfasserin aut H. Qiu verfasserin aut D. Ramírez García verfasserin aut S. Reichard verfasserin aut A. Rocchetti verfasserin aut N. Rupp verfasserin aut J. M. F. dos Santos verfasserin aut G. Sartorelli verfasserin aut N. Šarčević verfasserin aut M. Scheibelhut verfasserin aut S. Schindler verfasserin aut J. Schreiner verfasserin aut D. Schulte verfasserin aut M. Schumann verfasserin aut L. Scotto Lavina verfasserin aut M. Selvi verfasserin aut F. Semeria verfasserin aut P. Shagin verfasserin aut E. Shockley verfasserin aut M. Silva verfasserin aut H. Simgen verfasserin aut A. Takeda verfasserin aut C. Therreau verfasserin aut D. Thers verfasserin aut F. Toschi verfasserin aut G. Trinchero verfasserin aut C. Tunnell verfasserin aut M. Vargas verfasserin aut G. Volta verfasserin aut O. Wack verfasserin aut H. Wang verfasserin aut Y. Wei verfasserin aut C. Weinheimer verfasserin aut M. Weiss Xu verfasserin aut D. Wenz verfasserin aut C. Wittweg verfasserin aut J. Wulf verfasserin aut Z. Xu verfasserin aut M. Yamashita verfasserin aut J. Ye verfasserin aut G. Zavattini verfasserin aut Y. Zhang verfasserin aut T. Zhu verfasserin aut J. P. Zopounidis verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 8, Seite 9 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:8 pages:9 https://doi.org/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/article/061f56a5441044009b681378a41c3033 kostenfrei http://link.springer.com/article/10.1140/epjc/s10052-020-8284-0 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 8 9 |
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E. Aprile @@aut@@ J. Aalbers @@aut@@ F. Agostini @@aut@@ M. Alfonsi @@aut@@ L. Althueser @@aut@@ F. D. Amaro @@aut@@ V. C. Antochi @@aut@@ E. Angelino @@aut@@ J. Angevaare @@aut@@ F. Arneodo @@aut@@ D. Barge @@aut@@ L. Baudis @@aut@@ B. Bauermeister @@aut@@ L. Bellagamba @@aut@@ M. L. Benabderrahmane @@aut@@ T. Berger @@aut@@ P. A. Breur @@aut@@ A. Brown @@aut@@ E. Brown @@aut@@ S. Bruenner @@aut@@ G. Bruno @@aut@@ R. Budnik @@aut@@ C. Capelli @@aut@@ J. M. R. Cardoso @@aut@@ D. Cichon @@aut@@ B. Cimmino @@aut@@ M. Clark @@aut@@ D. Coderre @@aut@@ A. P. Colijn @@aut@@ J. Conrad @@aut@@ J. P. Cussonneau @@aut@@ M. P. Decowski @@aut@@ A. Depoian @@aut@@ P. Di Gangi @@aut@@ A. Di Giovanni @@aut@@ R. Di Stefano @@aut@@ S. Diglio @@aut@@ A. Elykov @@aut@@ G. Eurin @@aut@@ A. D. Ferella @@aut@@ W. Fulgione @@aut@@ P. Gaemers @@aut@@ R. Gaior @@aut@@ A. Gallo Rosso @@aut@@ M. Galloway @@aut@@ F. Gao @@aut@@ M. Garbini @@aut@@ L. Grandi @@aut@@ C. Hasterok @@aut@@ C. Hils @@aut@@ K. Hiraide @@aut@@ L. Hoetzsch @@aut@@ E. Hogenbirk @@aut@@ J. Howlett @@aut@@ M. Iacovacci @@aut@@ Y. Itow @@aut@@ F. Joerg @@aut@@ N. Kato @@aut@@ S. Kazama @@aut@@ M. Kobayashi @@aut@@ G. Koltman @@aut@@ A. Kopec @@aut@@ H. Landsman @@aut@@ R. F. Lang @@aut@@ L. Levinson @@aut@@ Q. Lin @@aut@@ S. Lindemann @@aut@@ M. Lindner @@aut@@ F. Lombardi @@aut@@ J. A. M. Lopes @@aut@@ E. López Fune @@aut@@ C. Macolino @@aut@@ J. Mahlstedt @@aut@@ L. Manenti @@aut@@ A. Manfredini @@aut@@ F. Marignetti @@aut@@ T. Marrodán Undagoitia @@aut@@ K. Martens @@aut@@ J. Masbou @@aut@@ D. Masson @@aut@@ S. Mastroianni @@aut@@ M. Messina @@aut@@ K. Miuchi @@aut@@ A. Molinario @@aut@@ K. Morå @@aut@@ S. Moriyama @@aut@@ Y. Mosbacher @@aut@@ M. Murra @@aut@@ J. Naganoma @@aut@@ K. Ni @@aut@@ U. Oberlack @@aut@@ K. Odgers @@aut@@ J. Palacio @@aut@@ B. Pelssers @@aut@@ R. Peres @@aut@@ J. Pienaar @@aut@@ V. Pizzella @@aut@@ G. Plante @@aut@@ J. Qin @@aut@@ H. Qiu @@aut@@ D. Ramírez García @@aut@@ S. Reichard @@aut@@ A. Rocchetti @@aut@@ N. Rupp @@aut@@ J. M. F. dos Santos @@aut@@ G. Sartorelli @@aut@@ N. Šarčević @@aut@@ M. Scheibelhut @@aut@@ S. Schindler @@aut@@ J. Schreiner @@aut@@ D. Schulte @@aut@@ M. Schumann @@aut@@ L. Scotto Lavina @@aut@@ M. Selvi @@aut@@ F. Semeria @@aut@@ P. Shagin @@aut@@ E. Shockley @@aut@@ M. Silva @@aut@@ H. Simgen @@aut@@ A. Takeda @@aut@@ C. Therreau @@aut@@ D. Thers @@aut@@ F. Toschi @@aut@@ G. Trinchero @@aut@@ C. Tunnell @@aut@@ M. Vargas @@aut@@ G. Volta @@aut@@ O. Wack @@aut@@ H. Wang @@aut@@ Y. Wei @@aut@@ C. Weinheimer @@aut@@ M. Weiss Xu @@aut@@ D. Wenz @@aut@@ C. Wittweg @@aut@@ J. Wulf @@aut@@ Z. Xu @@aut@@ M. Yamashita @@aut@@ J. Ye @@aut@@ G. Zavattini @@aut@@ Y. Zhang @@aut@@ T. Zhu @@aut@@ J. P. Zopounidis @@aut@@ |
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This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. 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Coderre</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">A. P. Colijn</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">J. Conrad</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">J. P. Cussonneau</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">M. P. Decowski</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">A. 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Joerg</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">N. Kato</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">S. Kazama</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">M. Kobayashi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">G. Koltman</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">A. Kopec</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">H. 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QB460-466 QC770-798 Energy resolution and linearity of XENON1T in the MeV energy range |
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Energy resolution and linearity of XENON1T in the MeV energy range |
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E. Aprile J. Aalbers F. Agostini M. Alfonsi L. Althueser F. D. Amaro V. C. Antochi E. Angelino J. Angevaare F. Arneodo D. Barge L. Baudis B. Bauermeister L. Bellagamba M. L. Benabderrahmane T. Berger P. A. Breur A. Brown E. Brown S. Bruenner G. Bruno R. Budnik C. Capelli J. M. R. Cardoso D. Cichon B. Cimmino M. Clark D. Coderre A. P. Colijn J. Conrad J. P. Cussonneau M. P. Decowski A. Depoian P. Di Gangi A. Di Giovanni R. Di Stefano S. Diglio A. Elykov G. Eurin A. D. Ferella W. Fulgione P. Gaemers R. Gaior A. Gallo Rosso M. Galloway F. Gao M. Garbini L. Grandi C. Hasterok C. Hils K. Hiraide L. Hoetzsch E. Hogenbirk J. Howlett M. Iacovacci Y. Itow F. Joerg N. Kato S. Kazama M. Kobayashi G. Koltman A. Kopec H. Landsman R. F. Lang L. Levinson Q. Lin S. Lindemann M. Lindner F. Lombardi J. A. M. Lopes E. López Fune C. Macolino J. Mahlstedt L. Manenti A. Manfredini F. Marignetti T. Marrodán Undagoitia K. Martens J. Masbou D. Masson S. Mastroianni M. Messina K. Miuchi A. Molinario K. Morå S. Moriyama Y. Mosbacher M. Murra J. Naganoma K. Ni U. Oberlack K. Odgers J. Palacio B. Pelssers R. Peres J. Pienaar V. Pizzella G. Plante J. Qin H. Qiu D. Ramírez García S. Reichard A. Rocchetti N. Rupp J. M. F. dos Santos G. Sartorelli N. Šarčević M. Scheibelhut S. Schindler J. Schreiner D. Schulte M. Schumann L. Scotto Lavina M. Selvi F. Semeria P. Shagin E. Shockley M. Silva H. Simgen A. Takeda C. Therreau D. Thers F. Toschi G. Trinchero C. Tunnell M. Vargas G. Volta O. Wack H. Wang Y. Wei C. Weinheimer M. Weiss Xu D. Wenz C. Wittweg J. Wulf Z. Xu M. Yamashita J. Ye G. Zavattini Y. Zhang T. Zhu J. P. Zopounidis |
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energy resolution and linearity of xenon1t in the mev energy range |
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Energy resolution and linearity of XENON1T in the MeV energy range |
abstract |
Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. |
abstractGer |
Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. |
abstract_unstemmed |
Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. The very good result achieved in XENON1T opens up new windows for the xenon dual-phase dark matter detectors to simultaneously search for other rare events. |
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Energy resolution and linearity of XENON1T in the MeV energy range |
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J. Aalbers F. Agostini M. Alfonsi L. Althueser F. D. Amaro V. C. Antochi E. Angelino J. Angevaare F. Arneodo D. Barge L. Baudis B. Bauermeister L. Bellagamba M. L. Benabderrahmane T. Berger P. A. Breur A. Brown E. Brown S. Bruenner G. Bruno R. Budnik C. Capelli J. M. R. Cardoso D. Cichon B. Cimmino M. Clark D. Coderre A. P. Colijn J. Conrad J. P. Cussonneau M. P. Decowski A. Depoian P. Di Gangi A. Di Giovanni R. Di Stefano S. Diglio A. Elykov G. Eurin A. D. Ferella W. Fulgione P. Gaemers R. Gaior A. Gallo Rosso M. Galloway F. Gao M. Garbini L. Grandi C. Hasterok C. Hils K. Hiraide L. Hoetzsch E. Hogenbirk J. Howlett M. Iacovacci Y. Itow F. Joerg N. Kato S. Kazama M. Kobayashi G. Koltman A. Kopec H. Landsman R. F. Lang L. Levinson Q. Lin S. Lindemann M. Lindner F. Lombardi J. A. M. Lopes E. López Fune C. Macolino J. Mahlstedt L. Manenti A. Manfredini F. Marignetti T. Marrodán Undagoitia K. Martens J. Masbou D. Masson S. Mastroianni M. Messina K. Miuchi A. Molinario K. Morå S. Moriyama Y. Mosbacher M. Murra J. Naganoma K. Ni U. Oberlack K. Odgers J. Palacio B. Pelssers R. Peres J. Pienaar V. Pizzella G. Plante J. Qin H. Qiu D. Ramírez García S. Reichard A. Rocchetti N. Rupp J. M. F. dos Santos G. Sartorelli N. Šarčević M. Scheibelhut S. Schindler J. Schreiner D. Schulte M. Schumann L. Scotto Lavina M. Selvi F. Semeria P. Shagin E. Shockley M. Silva H. Simgen A. Takeda C. Therreau D. Thers F. Toschi G. Trinchero C. Tunnell M. Vargas G. Volta O. Wack H. Wang Y. Wei C. Weinheimer M. Weiss Xu D. Wenz C. Wittweg J. Wulf Z. Xu M. Yamashita J. Ye G. Zavattini Y. Zhang T. Zhu J. P. Zopounidis |
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J. Aalbers F. Agostini M. Alfonsi L. Althueser F. D. Amaro V. C. Antochi E. Angelino J. Angevaare F. Arneodo D. Barge L. Baudis B. Bauermeister L. Bellagamba M. L. Benabderrahmane T. Berger P. A. Breur A. Brown E. Brown S. Bruenner G. Bruno R. Budnik C. Capelli J. M. R. Cardoso D. Cichon B. Cimmino M. Clark D. Coderre A. P. Colijn J. Conrad J. P. Cussonneau M. P. Decowski A. Depoian P. Di Gangi A. Di Giovanni R. Di Stefano S. Diglio A. Elykov G. Eurin A. D. Ferella W. Fulgione P. Gaemers R. Gaior A. Gallo Rosso M. Galloway F. Gao M. Garbini L. Grandi C. Hasterok C. Hils K. Hiraide L. Hoetzsch E. Hogenbirk J. Howlett M. Iacovacci Y. Itow F. Joerg N. Kato S. Kazama M. Kobayashi G. Koltman A. Kopec H. Landsman R. F. Lang L. Levinson Q. Lin S. Lindemann M. Lindner F. Lombardi J. A. M. Lopes E. López Fune C. Macolino J. Mahlstedt L. Manenti A. Manfredini F. Marignetti T. Marrodán Undagoitia K. Martens J. Masbou D. Masson S. Mastroianni M. Messina K. Miuchi A. Molinario K. Morå S. Moriyama Y. Mosbacher M. Murra J. Naganoma K. Ni U. Oberlack K. Odgers J. Palacio B. Pelssers R. Peres J. Pienaar V. Pizzella G. Plante J. Qin H. Qiu D. Ramírez García S. Reichard A. Rocchetti N. Rupp J. M. F. dos Santos G. Sartorelli N. Šarčević M. Scheibelhut S. Schindler J. Schreiner D. Schulte M. Schumann L. Scotto Lavina M. Selvi F. Semeria P. Shagin E. Shockley M. Silva H. Simgen A. Takeda C. Therreau D. Thers F. Toschi G. Trinchero C. Tunnell M. Vargas G. Volta O. Wack H. Wang Y. Wei C. Weinheimer M. Weiss Xu D. Wenz C. Wittweg J. Wulf Z. Xu M. Yamashita J. Ye G. Zavattini Y. Zhang T. Zhu J. P. Zopounidis |
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10.1140/epjc/s10052-020-8284-0 |
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up_date |
2024-07-04T01:20:52.997Z |
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Aprile</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Energy resolution and linearity of XENON1T in the MeV energy range</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2020</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Xenon dual-phase time projection chambers designed to search for weakly interacting massive particles have so far shown a relative energy resolution which degrades with energy above $$\sim $$ ∼ 200 keV due to the saturation effects. This has limited their sensitivity in the search for rare events like the neutrinoless double-beta decay of $$^{136} \hbox {Xe}$$ 136Xe at its Q value, $$Q_{\beta \beta }\simeq 2.46\,\hbox {MeV}$$ Qββ≃2.46MeV . For the XENON1T dual-phase time projection chamber, we demonstrate that the relative energy resolution at $$1\,\sigma /\mu $$ 1σ/μ is as low as ($$0.80 \pm 0.02$$ 0.80±0.02 ) % in its one-ton fiducial mass, and for single-site interactions at $$Q_{\beta \beta }$$ Qββ . We also present a new signal correction method to rectify the saturation effects of the signal readout system, resulting in more accurate position reconstruction and indirectly improving the energy resolution. 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score |
7.399913 |