12 results on '"R. Hodák"'
Search Results
2. Search for Neutrinoless Quadruple- β Decay of Nd150 with the NEMO-3 Detector
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A. Smetana, A. Žukauskas, V. G. Egorov, R. Saakyan, X. Sarazin, E. Rukhadze, R. Salazar, S. Calvez, Vit Vorobel, F. Nova, D. Waters, O.I. Kochetov, J. J. Evans, D. Lalanne, S. Blot, Vl.I. Tretyak, A.J. Caffrey, B. Morgan, S. Söldner-Rembold, A. Huber, B. Guillon, E. Chauveau, J. Busto, J. C. Thomas, L. Dawson, Masaharu Nomachi, C. L. Riddle, A. Remoto, P. Loaiza, V. I. Tretyak, V. V. Timkin, C. Cerna, C. Augier, R. Arnold, C. Vilela, R. Hodák, A. Basharina-Freshville, H. Ohsumi, C.S. Sutton, T. Le Noblet, Dominique Durand, X.R. Liu, Guillaume Lutter, D. Duchesneau, Hector Gomez, Fedor Šimkovic, Karol Lang, A. S. Barabash, Y. A. Ramachers, Igor Nemchenok, Michele Cascella, Jouni Suhonen, J. Mott, D.V. Filosofov, F. Xie, Karel Smolek, Frédéric Nowacki, Pavel P. Povinec, D. Štefánik, Ch. Marquet, P. Přidal, I. Stekl, X. Garrido, B. Soulé, F. Perrot, J.P. Cesar, A.A. Smolnikov, S. Torre, Yu. Shitov, V.I. Umatov, F. Mamedov, F. Piquemal, V.E. Kovalenko, F. Mauger, D. Boursette, G. Szklarz, G. Eurin, M. Macko, C. Macolino, C. Hugon, R. L. Flack, J. L. Reyss, R. B. Pahlka, S. Blondel, C. Patrick, A. A. Klimenko, M. Bongrand, V.B. Brudanin, I. Vanushin, L. Fajt, P. Guzowski, Y. Lemière, A. Chapon, L. Simard, A. Chopra, Z. J. Liptak, Ph. Hubert, S. Jullian, and S. I. Konovalov
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Physics ,Particle physics ,Electron energy spectrum ,010308 nuclear & particles physics ,Detector ,General Physics and Astronomy ,chemistry.chemical_element ,Electron ,01 natural sciences ,7. Clean energy ,Neodymium ,Lepton number ,Beta decay ,Nuclear physics ,chemistry ,0103 physical sciences ,Underground laboratory ,010306 general physics - Abstract
We report the results of a first experimental search for lepton number violation by four units in the neutrinoless quadruple-β decay of Nd150 using a total exposure of 0.19 kg yr recorded with the NEMO-3 detector at the Modane Underground Laboratory. We find no evidence of this decay and set lower limits on the half-life in the range T1/2>(1.1–3.2)×1021 yr at the 90% C.L., depending on the model used for the kinematic distributions of the emitted electrons.
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- 2017
- Full Text
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3. The BiPo-3 detector for the measurement of ultra low natural radioactivities of thin materials
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A.S. Barabash, A. Basharina-Freshville, E. Birdsall, S. Blondel, S. Blot, M. Bongrand, D. Boursette, V. Brudanin, J. Busto, A.J. Caffrey, S. Calvez, M. Cascella, S. Cebrián, C. Cerna, J.P Cesar, E. Chauveau, A. Chopra, T. Dafní, S. De Capua, D. Duchesneau, D. Durand, V. Egorov, G. Eurin, J.J. Evans, L. Fajt, D. Filosofov, R. Flack, X. Garrido, H. Gómez, B. Guillon, P. Guzowski, K. Holý, R. Hodák, A. Huber, C. Hugon, F.J. Iguaz, I.G. Irastorza, A. Jeremie, S. Jullian, M. Kauer, A. Klimenko, O. Kochetov, S.I. Konovalov, V. Kovalenko, K. Lang, Y. Lemière, T. Le Noblet, Z. Liptak, X.R. Liu, P. Loaiza, G. Lutter, G. Luzón, M. Macko, F. Mamedov, C. Marquet, F. Mauger, B. Morgan, J. Mott, I. Nemchenok, M. Nomachi, F. Nova, H. Ohsumi, G. Oliviéro, A. Ortiz de Solórzano, R.B. Pahlka, J. Pater, F. Perrot, F. Piquemal, P. Povinec, P. Přidal, Y.A. Ramachers, A. Remoto, B. Richards, C.L. Riddle, E. Rukhadze, R. Saakyan, R. Salazar, X. Sarazin, Yu. Shitov, L. Simard, F. Šimkovic, A. Smetana, K. Smolek, A. Smolnikov, S. Söldner-Rembold, B. Soulé, I. Štekl, J. Thomas, V. Timkin, S. Torre, Vl.I. Tretyak, V.I. Tretyak, V.I. Umatov, C. Vilela, V. Vorobel, D. Waters, A. Žukauskas, Laboratoire de l'Accélérateur Linéaire (LAL), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Laboratoire Souterrain de Modane (LSM - UMR 6417), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut Universitaire de France (IUF), Ministère de l'Education nationale, de l’Enseignement supérieur et de la Recherche (M.E.N.E.S.R.), SuperNEMO, Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])
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Physics ,Physics - Instrumentation and Detectors ,010308 nuclear & particles physics ,Canfranc Underground Laboratory ,Detector ,FOS: Physical sciences ,Instrumentation and Detectors (physics.ins-det) ,010403 inorganic & nuclear chemistry ,01 natural sciences ,3. Good health ,0104 chemical sciences ,Nuclear physics ,Activity measurements ,0103 physical sciences ,Sensitivity (control systems) ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,Instrumentation ,Mathematical Physics - Abstract
The BiPo-3 detector, running in the Canfranc Underground Laboratory (Laboratorio Subterr\'aneo de Canfranc, LSC, Spain) since 2013, is a low-radioactivity detector dedicated to measuring ultra low natural radionuclide contaminations of $^{208}$Tl ($^{232}$Th chain) and $^{214}$Bi ($^{238}$U chain) in thin materials. The total sensitive surface area of the detector is 3.6 m$^2$. The detector has been developed to measure radiopurity of the selenium double $\beta$-decay source foils of the SuperNEMO experiment. In this paper the design and performance of the detector, and results of the background measurements in $^{208}$Tl and $^{214}$Bi, are presented, and validation of the BiPo-3 measurement with a calibrated aluminium foil is discussed. Results of the $^{208}$Tl and $^{214}$Bi activity measurements of the first enriched $^{82}$Se foils of the double $\beta$-decay SuperNEMO experiment are reported. The sensitivity of the BiPo-3 detector for the measurement of the SuperNEMO $^{82}$Se foils is $\mathcal{A}$($^{208}$Tl) $, Comment: 37 pages, 29 figures
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- 2017
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4. The BiPo-3 detector
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L. Simard, S. Blot, M. Bongrand, H. Gómez, A. Chopra, Z. J. Liptak, Jose Busto, P. Guzowski, Y. Lemière, Y. A. Ramachers, S. I. Konovalov, E. Chauveau, F. Perrot, B. Richards, V. V. Timkin, V.I. Umatov, X. Garrido, E. Birdsall, Pavel P. Povinec, Masaharu Nomachi, L. Fajt, Vit Vorobel, S. Torre, P. Přidal, V. Brudanin, G. Eurin, F. Mamedov, A.J. Caffrey, S. Söldner-Rembold, D. Boursette, Ruben Saakyan, O.I. Kochetov, C. Vilela, X.R. Liu, F. Piquemal, C. Hugon, Guillaume Lutter, J. Mott, M. Macko, Karol Lang, A. Jeremie, A. Žukauskas, Karol Holý, Yu. Shitov, S. De Capua, Michele Cascella, V. G. Egorov, A.A. Smolnikov, E. Rukhadze, P. Loaiza, S. Calvez, D. Waters, X. Sarazin, Joleen Pater, A. Smetana, J. J. Evans, D. Duchesneau, A. S. Barabash, Juergen Thomas, S. Blondel, I. Stekl, A. Huber, C. Cerna, D.V. Filosofov, V. I. Tretyak, V.E. Kovalenko, F. Mauger, G. Oliviéro, Fedor Šimkovic, R. L. Flack, Igor Nemchenok, B. Guillon, H. Ohsumi, M. Kauer, T. Le Noblet, R. B. Pahlka, Dominique Durand, Vl.I. Tretyak, F. Nova, S. Jullian, B. Morgan, A. A. Klimenko, C. L. Riddle, A. Remoto, A. Basharina-Freshville, R. Hodák, Karel Smolek, B. Soulé, Ch. Marquet, Laboratoire de l'Accélérateur Linéaire (LAL), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Laboratoire Souterrain de Modane (LSM - UMR 6417), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut Universitaire de France (IUF), Ministère de l'Education nationale, de l’Enseignement supérieur et de la Recherche (M.E.N.E.S.R.), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Aix Marseille Université (AMU), Laboratoire d'Annecy de Physique des Particules (LAPP/Laboratoire d'Annecy-le-Vieux de Physique des Particules), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), and Centre National de la Recherche Scientifique (CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
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Photomultiplier ,measurement methods ,chemistry.chemical_element ,Scintillator ,010403 inorganic & nuclear chemistry ,01 natural sciences ,Bismuth ,Nuclear physics ,thallium ,Optics ,Neutrino Ettore Majorana Observatory ,Double beta decay ,Double beta-decay detectors ,0103 physical sciences ,bismuth ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,background: radioactivity ,FOIL method ,scintillation counter ,Physics ,Radiation ,photomultiplier ,010308 nuclear & particles physics ,business.industry ,Detector ,double-beta decay ,0104 chemical sciences ,chemistry ,Scintillation counter ,admixture ,Low-radioactivity measurements ,business - Abstract
The BiPo-3 detector is a low radioactive detector dedicated to measuring ultra-low natural contaminations of 208Tl and 214Bi in thin materials, initially developed to measure the radiopurity of the double β decay source foils of the SuperNEMO experiment at the μBq/kg level. The BiPo-3 technique consists in installing the foil of interest between two thin ultra-radiopure scintillators coupled to low radioactive photomultipliers. The design and performances of the detector are presented. In this paper, the final results of the 208Tl and 214Bi activity measurements of the first enriched 82Se foils are reported for the first time, showing the capability of the detector to reach sensitivities in the range of some μBq/kg.
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- 2017
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5. Measurement of the double-beta decay half-life and search for the neutrinoless double-beta decay ofCa48with the NEMO-3 detector
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F. Nova, X.R. Liu, B. Morgan, C. L. Riddle, A. Remoto, Hector Gomez, Jouni Suhonen, S. Calvez, S. V. Zhukov, M. Bongrand, Masaharu Nomachi, A. Basharina-Freshville, F. Piquemal, O.I. Kochetov, J. Baker, Karol Lang, D. Waters, V. I. Tretyak, R. Salazar, Vl.I. Tretyak, Jose Busto, V. G. Egorov, S. Blondel, V. V. Timkin, Y. A. Ramachers, X. Sarazin, E. Rukhadze, B. Richards, P. Guzowski, Y. Lemière, V. I. Lebedev, Guillaume Lutter, A. M. Bakalyarov, J. L. Reyss, J.P. Cesar, S. Torre, F. Mamedov, V.E. Kovalenko, F. Mauger, Frédéric Nowacki, A. Chapon, Fedor Šimkovic, G. Szklarz, R. Arnold, Igor Nemchenok, A. Smetana, A. Chopra, Z. J. Liptak, C. Hugon, V. B. Brudanin, J. Mott, P. Loaiza, Michele Cascella, R. Saakyan, G. Eurin, F. Perrot, V. I. Umatov, R. B. Pahlka, I. Stekl, S. Söldner-Rembold, A. S. Barabash, S. Blot, D.V. Filosofov, L. Simard, Ch. Marquet, N.I. Rukhadze, A. Žukauskas, Ph. Hubert, Vit Vorobel, E. Chauveau, A.A. Smolnikov, R. L. Flack, J. J. Evans, A. A. Klimenko, S. Jullian, D. Lalanne, Yu. Shitov, A. Huber, J. C. Thomas, C. Cerna, Lukas Fajt, I. Vanushin, Pavel P. Povinec, C.S. Sutton, H. Ohsumi, T. Le Noblet, Dominique Durand, S. I. Konovalov, P. Přidal, A. J. Caffrey, R. Hodák, Karel Smolek, X. Garrido, B. Soulé, D. Duchesneau, C. Vilela, B. Guillon, and C. Augier
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Physics ,Particle physics ,010308 nuclear & particles physics ,Half-life ,01 natural sciences ,Lower limit ,Nuclear physics ,MAJORANA ,Double beta decay ,0103 physical sciences ,Underground laboratory ,Neutrino ,010306 general physics ,Majoron - Abstract
The NEMO-3 experiment at the Modane Underground Laboratory has investigated the double-$\beta$ decay of $^{48}{\rm Ca}$. Using $5.25$ yr of data recorded with a $6.99\,{\rm g}$ sample of $^{48}{\rm Ca}$, approximately $150$ double-$\beta$ decay candidate events have been selected with a signal-to-background ratio greater than $3$. The half-life for the two-neutrino double-$\beta$ decay of $^{48}{\rm Ca}$ has been measured to be $T^{2\nu}_{1/2}\,=\,[6.4\, ^{+0.7}_{-0.6}{\rm (stat.)} \, ^{+1.2}_{-0.9}{\rm (syst.)}] \times 10^{19}\,{\rm yr}$. A search for neutrinoless double-$\beta$ decay of $^{48}{\rm Ca}$ yields a null result and a corresponding lower limit on the half-life is found to be $T^{0\nu}_{1/2} > 2.0 \times 10^{22}\,{\rm yr}$ at $90\%$ confidence level, translating into an upper limit on the effective Majorana neutrino mass of $ < 6.0 - 26$ ${\rm eV}$, with the range reflecting different nuclear matrix element calculations. Limits are also set on models involving Majoron emission and right-handed currents.
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- 2016
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6. Results of the search for neutrinoless double-βdecay inMo100with the NEMO-3 experiment
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B. Morgan, C. L. Riddle, A. Remoto, A. Basharina-Freshville, J. Baker, Fedor Šimkovic, Igor Nemchenok, F. Piquemal, S. Söldner-Rembold, S. Calvez, V. Egorov, D. Duchesneau, V. V. Timkin, A. S. Barabash, E. Rukhadze, V.I. Tretyak, A. Huber, A. A. Klimenko, D.V. Filosofov, Jouni Suhonen, L. Simard, A. Smetana, J. L. Reyss, F. Perrot, Ruben Saakyan, V. Vorobel, Stijn Blot, R. B. Pahlka, Frédéric Nowacki, Guillaume Lutter, J. J. Evans, D. Lalanne, Yu. Shitov, C. Augier, Ph. Hubert, Karel Smolek, B. Soulé, C. Cerna, Jose Busto, P. Guzowski, Y. Lemière, A. J. Caffrey, V. I. Umatov, A. Chapon, F. Nova, V.E. Kovalenko, Haley Louise Gomez, M. Bongrand, D. Waters, F. Mauger, R. Arnold, S. I. Konovalov, E. Chauveau, Pavel P. Povinec, O.I. Kochetov, C. Vilela, I. Vanushin, S. Jullian, Catherine Marquet, S. Blondel, G. Eurin, Lukas Fajt, J. Mott, Z. J. Liptak, V.B. Brudanin, C. Hugon, Y. A. Ramachers, B. Richards, J.P. Cesar, S. Torre, F. Mamedov, K. Lang, P. Loaiza, C. S. Sutton, G. Szklarz, X. Sarazin, Juergen Thomas, R. Hodák, Masaharu Nomachi, R. Flack, B. Guillon, P. Přidal, A.A. Smolnikov, I. Stekl, A. Žukauskas, Vl.I. Tretyak, H. Ohsumi, T. Le Noblet, Dominique Durand, and Xavier Garrido
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Signal region ,01 natural sciences ,Beta decay ,Lower limit ,Nuclear physics ,MAJORANA ,Double beta decay ,0103 physical sciences ,Underground laboratory ,Beta (velocity) ,Neutrino ,010306 general physics - Abstract
The NEMO-3 detector, which had been operating in the Modane Underground Laboratory from 2003 to 2010, was designed to search for neutrinoless double $\beta$ ($0\nu\beta\beta$) decay. We report final results of a search for $0\nu\beta\beta$ decays with $6.914$ kg of $^{100}$Mo using the entire NEMO-3 data set with a detector live time of $4.96$ yr, which corresponds to an exposure of 34.3 kg$\cdot$yr. We perform a detailed study of the expected background in the $0\nu\beta\beta$ signal region and find no evidence of $0\nu\beta\beta$ decays in the data. The level of observed background in the $0\nu\beta\beta$ signal region $[2.8-3.2]$ MeV is $0.44 \pm 0.13$ counts/yr/kg, and no events are observed in the interval $[3.2-10]$ MeV. We therefore derive a lower limit on the half-life of $0\nu\beta\beta$ decays in $^{100}$Mo of $T_{1/2}(0\nu\beta\beta)> 1.1 \times 10^{24}$ yr at the $90\%$ Confidence Level, under the hypothesis of light Majorana neutrino exchange. Depending on the model used for calculating nuclear matrix elements, the limit for the effective Majorana neutrino mass lies in the range $\langle m_{\nu} \rangle < 0.33$--$0.62$ eV. We also report constraints on other lepton-number violating mechanisms for $0\nu\beta\beta$ decays.
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- 2015
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7. New search for double electron capture in Cd-106 decay with the TGV-2 spectrometer
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Lukas Fajt, V. B. Brudanin, V. G. Egorov, E. Rukhadze, A.V. Salamatin, J. M. Jose, R. Hodák, S. V. Rosov, Yu. Shitov, A. A. Klimenko, N. I. Rukhadze, A. Kovalík, Ch. Briançon, V. V. Timkin, M. Špavorova, E. A. Yakushev, F. Šimkovic, I. Stekl, CSNSM SNO, Centre de Spectrométrie Nucléaire et de Spectrométrie de Masse (CSNSM), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)-Centre de Sciences Nucléaires et de Sciences de la Matière (CSNSM), and Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,[PHYS]Physics [physics] ,Nuclear and High Energy Physics ,Isotope ,Spectrometer ,010308 nuclear & particles physics ,Stable isotope ratio ,Electron capture ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,7. Clean energy ,Atomic and Molecular Physics, and Optics ,Nuclear physics ,Double beta decay ,Isotopes of cadmium ,0103 physical sciences ,Gamma spectroscopy ,DOUBLE-BETA DECAY ,010306 general physics ,Radioactive decay - Abstract
International audience; A new experiment devoted to searches for double electron capture in Cd-106 decay is being performed at the Modane underground laboratory (4800 mwe) with the 32-detector TGV-2 spectrometer. The limit T (1/2)(2 nu EC/EC) > 2.0x10(20) yr at a 90%confidence level (C.L.) was obtained from a preliminary analysis of data obtained over 2250 h of measurements with about 23.2 g sample enriched in the isotope Cd-106 to 99.57%. The limits T (1/2)(KL, 2741 keV) > 0.9 x 10(20) yr and T (1/2)(KK, 2718 keV) a parts per thousand << 1.4 x 10(20) yr at a 90% C.L. on the neutrinoless decay of Cd-106 were obtained from measurements performed with the Obelix low-background spectrometer from high-purity germanium (HPGe spectrometer) for a sample of mass about 23.2 g enriched in the isotope Cd-106.
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- 2015
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8. Double electron capture of 106Cd in the TGV-2 experiment
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A.V. Salamatin, N. I. Rukhadze, V. B. Brudanin, P. Kouba, Fedor Šimkovic, E. A. Yakushev, V. G. Egorov, V. V. Timkin, E. Rukhadze, F. Rychnovský, Lukas Fajt, Ch. Briançon, I. Stekl, R. Hodák, Yu. Shitov, A. Kovalík, A. A. Klimenko, F. Piquemal, S. V. Rozov, CSNSM SNO, Centre de Sciences Nucléaires et de Sciences de la Matière (CSNSM), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)-Centre de Spectrométrie Nucléaire et de Spectrométrie de Masse (CSNSM), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), and Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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[PHYS]Physics [physics] ,Physics ,Electron spectrometer ,Spectrometer ,010308 nuclear & particles physics ,Electron capture ,double beta decay ,Resonance ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,7. Clean energy ,01 natural sciences ,Beta decay ,Nuclear physics ,neutrino ,Double beta decay ,Isotopes of cadmium ,0103 physical sciences ,010306 general physics ,Radioactive decay - Abstract
International audience; A new experimental run of searching for EC/EC decay of Cd-106 was performed at the Modane underground laboratory (4800 m w.e.) using the TGV-2 spectrometer and similar to 23.2 g Cd-106 with enrichment of 99.57%. The limit on 2 nu EC/EC decay of Cd-106 -T-1/2(2 nu EC/EC) > 3.1x10(20) y, at 90% C. L was obtained from the preliminary calculation of experimental data accumulated for 7018 h of measurement. The limits on the resonance neutrino-less double electron capture decay of Cd-106 were obtained from the measurement of similar to 23.2 g of Cd-106 with the low-background HPGe spectrometer OBELIX lasted 395 h -T-1/2(KL, 2741 keV) > 0.9x10(20) y and T-1/2(KK, 2718 keV) > 1.4x10(20) y at 90% C.L.
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- 2015
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9. Investigations of 2β decay of 106Cd and 58Ni with HPGe spectrometer OBELIX
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Yu. Shitov, M. Špavorova, A. A. Klimenko, R. Hodák, E. Rukhadze, F. Piquemal, I. Stekl, Lukas Fajt, E. A. Yakushev, P. Loaiza, V. B. Brudanin, O.I. Kochetov, N. I. Rukhadze, M. Zampaolo, and S. V. Rozov
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Physics ,Nuclear physics ,Spectrometer ,Isotopes of palladium ,Electron capture ,Isotopes of cadmium ,Double beta decay ,Beta decay ,Radioactive decay ,Particle detector - Abstract
Investigations of double beta decay processes to excited states of daughter nuclei were performed at the Modane underground laboratory (LSM, France, 4800 m w.e.) using the high sensitivity spectrometer OBELIX [1], which is a common activity of JINR Dubna, IEAP CTU in Prague and LSM. The spectrometer is based on the HPGe detector with the sensitive volume of 600 cm3 and relative efficiency of 160%. Investigation of resonant neutrino-less double electron capture of 106Cd was performed with ∼23.2 g of 106Cd (enrichment of 99.57%) during ∼17 days. The experiment with natural Ni (∼21.7 kg of mass) was also carried out during ∼47 days. The preliminary experimental limits for 0νEC/EC resonant decay to the excited states of 106Pd and different modes of β β decay 58Ni are presented.
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- 2015
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10. Status of the SuperNEMO demonstrator
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R. Hodák
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Nuclear physics ,Physics ,Particle physics ,Double beta decay ,Physics beyond the Standard Model ,Neutrino Ettore Majorana Observatory ,Neutrino ,Neutrino oscillation - Abstract
The hunt for the neutrino mass in the process of the neutrinoless double beta decay (0νβ β) belongs to a crucial task in the field of physics beyond the Standard model. The next generation experiment SuperNEMO, based on the NEMO-3 calo-tracko detection technique is devoted to measure this extremely rare nuclear process within the half-life sensitivity T1/20v of 1 × 1026 years, which correspond to the sensitivity on the effective neutrino mass 〈mν〉 of 40 – 110 meV. In this contribution, a progress in the construction and commissioning of the first SuperNEMO module - demonstrator, is reported.
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- 2015
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11. Search for neutrinoless double-beta decay ofMo100with the NEMO-3 detector
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C. Hugon, I. Vanushin, Pavel P. Povinec, E. Rukhadze, V. Egorov, A.J. Caffrey, F. Nova, Karol Lang, X. Sarazin, B. Morgan, A. Smetana, D. Waters, Guillaume Lutter, Catherine Marquet, C. L. Riddle, A. Remoto, P. Loaiza, C. Augier, F. Piquemal, V.I. Tretyak, D. Lalanne, D. Durand, Juergen Thomas, A. Basharina-Freshville, J. Busto, R. Saakyan, J. Mott, A. S. Barabash, Y. Lemière, V. I. Umatov, J. J. Evans, A.A. Smolnikov, A. A. Klimenko, L. Simard, Fedor Šimkovic, Hector Gomez, V.B. Brudanin, R. Hodák, J. L. Reyss, Masaharu Nomachi, Igor Nemchenok, C. Cerna, S. Blot, Z. J. Liptak, A. Chapon, R. B. Pahlka, Ph. Hubert, P. Guzowski, D. Duchesneau, S. Jullian, C.S. Sutton, F. Nowacki, Karel Smolek, X. Garrido, B. Soulé, R. Arnold, Jouni Suhonen, R. L. Flack, G. Eurin, V. V. Timkin, A. Žukauskas, F. Mauger, J. Baker, V. Kovalenko, B. Guillon, S. I. Konovalov, Yu. Shitov, O.I. Kochetov, C. Vilela, F. Perrot, B. Richards, S. Torre, F. Mamedov, G. Szklarz, Y. A. Ramachers, S. Söldner-Rembold, M. Bongrand, S. Blondel, Vit Vorobel, E. Chauveau, I. Stekl, Vl.I. Tretyak, and H. Ohsumi
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Electron ,01 natural sciences ,Beta decay ,Lepton number ,Nuclear physics ,MAJORANA ,Double beta decay ,0103 physical sciences ,Beta (velocity) ,Neutrino ,010306 general physics ,Energy (signal processing) - Abstract
We report the results of a search for the neutrinoless double-$\beta$ decay (0$\nu\beta\beta$) of $^{100}$Mo, using the NEMO-3 detector to reconstruct the full topology of the final state events. With an exposure of 34.7 kg.y, no evidence for the 0$\nu\beta\beta$ signal has been found, yielding a limit for the light Majorana neutrino mass mechanism of $T_{1/2}(0\nu\beta\beta)>1.1 \times 10^{24}$ years (90% C.L.) once both statistical and systematic uncertainties are taken into account. Depending on the Nuclear Matrix Elements this corresponds to an upper limit on the Majorana effective neutrino mass of $ < 0.3-0.8$ eV (90% C.L.). Constraints on other lepton number violating mechanisms of 0$\nu\beta\beta$ decays are also given. Searching for high-energy double electron events in all suitable sources of the detector, no event in the energy region [3.2-10] MeV is observed for an exposure of 47 kg.y.
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- 2014
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12. Investigation of double beta decay of 100Mo to excited states of 100Ru
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Frédéric Nowacki, C. Cerna, Pavel P. Povinec, J. Mott, Karel Smolek, Ph. Hubert, S. Blondel, O.I. Kochetov, C. Vilela, A. Žukauskas, B. Soulé, Vl.I. Tretyak, Fedor Šimkovic, C.S. Sutton, S. Jullian, J. J. Evans, V.B. Brudanin, L. Dragounová, Masaharu Nomachi, H. Gómez, V. Egorov, G. Eurin, A.A. Smolnikov, I. Stekl, Igor Nemchenok, A.J. Caffrey, Vit Vorobel, E. Chauveau, A. A. Klimenko, R. Hodák, S. Blot, V. I. Umatov, A. Smetana, R. Arnold, P. Guzowski, V. Kovalenko, Y. Lemière, R. Saakyan, F. Perrot, C. Augier, A. Chapon, S. I. Konovalov, X. Garrido, J. L. Reyss, P. Čermák, V. V. Timkin, S. Söldner-Rembold, R. B. Pahlka, A. S. Barabash, D. Duchesneau, M. Bongrand, Guillaume Lutter, J. Hůlka, Z. J. Liptak, Catherine Marquet, F. Nova, Karol Lang, E. Rukhadze, F. Mauger, B. Morgan, V.I. Tretyak, C. L. Riddle, A. Remoto, P. Loaiza, H. Ohsumi, Dominique Durand, A. Basharina-Freshville, Jouni Suhonen, D. Lalanne, Yu. Shitov, Juergen Thomas, G. Szklarz, L. Simard, F. Piquemal, Y. A. Ramachers, B. Richards, S. Torre, F. Mamedov, C. Hugon, X. Sarazin, D. Waters, G. Warot, N.I. Rukhadze, R. L. Flack, J. Busto, B. Guillon, Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de l'Accélérateur Linéaire (LAL), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Neutrino et Faibles Radioactivités (NEMO), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Souterrain de Modane (LSM - UMR 6417), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Laboratoire des Sciences du Climat et de l'Environnement [Gif-sur-Yvette] (LSCE), Université de Versailles Saint-Quentin-en-Yvelines (UVSQ)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Océan et Interfaces (OCEANIS), Université de Versailles Saint-Quentin-en-Yvelines (UVSQ)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Université de Versailles Saint-Quentin-en-Yvelines (UVSQ)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), NEMO-3, Université de Strasbourg (UNISTRA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université de Versailles Saint-Quentin-en-Yvelines (UVSQ), and Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université de Versailles Saint-Quentin-en-Yvelines (UVSQ)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université de Versailles Saint-Quentin-en-Yvelines (UVSQ)
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Physics ,Nuclear and High Energy Physics ,Decay scheme ,ta114 ,FOS: Physical sciences ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,External source ,7. Clean energy ,3. Good health ,Nuclear physics ,Excited state ,Excited nucleus ,Double beta decay ,Nuclear Experiment (nucl-ex) ,Atomic physics ,Hpge detector ,Nuclear Experiment - Abstract
Double beta decay of $^{100}$Mo to the excited states of daughter nuclei has been studied using a 600 cm$^3$ low-background HPGe detector and an external source consisting of 2588 g of 97.5% enriched metallic $^{100}$Mo, which was formerly inside the NEMO-3 detector and used for the NEMO-3 measurements of $^{100}$Mo. The half-life for the two-neutrino double beta decay of $^{100}$Mo to the excited 0$^+_1$ state in $^{100}$Ru is measured to be $T_{1/2}=[7.5 \pm{0.6}(stat) \pm {0.6}(syst)]\cdot 10^{20}$ yr. For other $(0\nu + 2\nu)$ transitions to the 2$^+_1$, 2$^+_2$, 0$^+_2$, 2$^+_3$ and 0$^+_3$ levels in $^{100}$Ru, limits are obtained at the level of $\sim (0.25-1.1)\cdot 10^{22}$ yr., Comment: 19 pages, 4 figures. arXiv admin note: text overlap with arXiv:0904.1924
- Published
- 2014
- Full Text
- View/download PDF
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