English
Related papers

Related papers: Reactor Rate Modulation oscillation analysis with …

200 papers

The CHOOZ experiment measured the antineutrino flux at a distance of about 1 Km from two nuclear reactors in order to detect possible neutrino oscillations with squared mass differences as low as 10**-3 eV**2 for full mixing. We show that…

Sterile neutrinos are one candidate to explain anomalies in neutrino oscillations. The mass-difference-driving oscillation between flavors can be probed only within specific combinations of baseline and flight energy. For a neutrino whose…

High Energy Physics - Phenomenology · Physics 2013-03-26 S. K. Kang , Y. D. Kim , Y. Ko , K. Siyeon

The analysis and results are presented from the complete data set recorded at Palo Verde between September 1998 and July 2000. In the experiment, the $\nuebar$ interaction rate has been measured at a distance of 750 and 890 m from the…

High Energy Physics - Experiment · Physics 2008-11-26 F. Boehm , J. Busenitz , B. Cook , G. Gratta , H. Henrikson , J. Kornis , D. Lawrence , K. B. Lee , K. McKinney , L. Miller , V. Novikov , A. Piepke , B. Ritchie , D. Tracy , P. Vogel , Y-F. Wang , J. Wolf

We study the optimization of a green-field, two-baseline reactor experiment with respect to the sensitivity for electron antineutrino disappearance in search of a light sterile neutrino. We consider both commercial and research reactors and…

High Energy Physics - Phenomenology · Physics 2022-02-16 Jeffrey M. Berryman , Luis A. Delgadillo , Patrick Huber

Estimation of the signal amplitudes and counting rates for coherent scattering of reactor antineutrino off atomic nuclei in two-phase xenon and argon detectors has been done. A conceptual design of detector based on the existing…

Nuclear Experiment · Physics 2009-06-23 Dmitri Akimov , Alexander Bondar , Alexander Burenkov , Alexei Buzulutskov

Reactor experiments are well suited to probe the possible loss of coherence of neutrino oscillations due to wave-packets separation. We combine data from the short-baseline experiments Daya Bay and the Reactor Experiment for Neutrino…

High Energy Physics - Phenomenology · Physics 2021-06-10 André de Gouvêa , Valentina De Romeri , Christoph A. Ternes

Recently, three reactor neutrino experiments, Daya Bay, Double Chooz and RENO have directly measured the neutrino mixing angle $\theta_{13}$. In this paper, another important oscillation parameter, effective $\Delta m_{31}^2$ (= $\Delta…

High Energy Physics - Experiment · Physics 2013-08-21 T. J. C. Bezerra , H. Furuta , F. Suekane , T. Matsubara

In this work, we present a realistic analysis of the potential of the present-day reactor experiments Double Chooz, Daya Bay and RENO for probing the existence of sterile neutrinos. We present exclusion regions for sterile oscillation…

High Energy Physics - Phenomenology · Physics 2015-03-20 Kalpana Bora , Debajyoti Dutta , Pomita Ghoshal

SNO+ is a multipurpose liquid-scintillator neutrino detector located 2 km underground at SNOLAB, Canada. Three large nuclear reactors at baselines of 240-350 km allow a precise measurement of the neutrino oscillation parameter $\Delta…

High Energy Physics - Experiment · Physics 2026-04-08 William Parker

A three-neutrino analysis of oscillation data is performed using the recent, more finely binned Super-K oscillation data, together with the CHOOZ, K2K, and MINOS data. The solar parameters, $\Delta_{21}$ and $\theta_{12}$, are fixed from a…

Nuclear Theory · Physics 2010-04-06 J. E. Roa , D. C. Latimer , D. J. Ernst

The Daya Bay experiment was the first to report simultaneous measurements of reactor antineutrinos at multiple baselines leading to the discovery of $\bar{\nu}_e$ oscillations over km-baselines. Subsequent data has provided the world's most…

Instrumentation and Detectors · Physics 2016-02-02 F. P. An , J. Z. Bai , A. B. Balantekin , H. R. Band , D. Beavis , W. Beriguete , M. Bishai , S. Blyth , R. L. Brown , I. Butorov , D. Cao , G. F. Cao , J. Cao , R. Carr , W. R. Cen , W. T. Chan , Y. L. Chan , J. F. Chang , L. C. Chang , Y. Chang , C. Chasman , H. Y. Chen , H. S. Chen , M. J. Chen , Q. Y. Chen , S. J. Chen , S. M. Chen , X. C. Chen , X. H. Chen , X. S. Chen , Y. X. Chen , Y. Chen , J. H. Cheng , J. Cheng , Y. P. Cheng , J. J. Cherwinka , S. Chidzik , K. Chow , M. C. Chu , J. P. Cummings , J. de Arcos , Z. Y. Deng , X. F. Ding , Y. Y. Ding , M. V. Diwan , L. Dong , J. Dove , E. Draeger , X. F. Du , D. A. Dwyer , W. R. Edwards , S. R. Ely , S. D. Fang , J. Y. Fu , Z. W. Fu , L. Q. Ge , V. Ghazikhanian , R. Gill , J. Goett , M. Gonchar , G. H. Gong , H. Gong , Y. A. Gornushkin , M. Grassi , L. S. Greenler , W. Q. Gu , M. Y. Guan , R. P. Guo , X. H. Guo , R. W. Hackenburg , R. L. Hahn , R. Han , S. Hans , M. He , Q. He , W. S. He , K. M. Heeger , Y. K. Heng , A. Higuera , P. Hinrichs , T. H. Ho , M. Hoff , Y. K. Hor , Y. B. Hsiung , B. Z. Hu , L. M. Hu , L. J. Hu , T. Hu , W. Hu , E. C. Huang , H. Z. Huang , H. X. Huang , P. W. Huang , X. Huang , X. T. Huang , P. Huber , G. Hussain , Z. Isvan , D. E. Jaffe , P. Jaffke , K. L. Jen , S. Jetter , X. P. Ji , X. L. Ji , H. J. Jiang , W. Q. Jiang , J. B. Jiao , R. A. Johnson , J. Joseph , L. Kang , S. H. Kettell , S. Kohn , M. Kramer , K. K. Kwan , M. W. Kwok , T. Kwok , C. Y. Lai , W. C. Lai , W. H. Lai , T. J. Langford , K. Lau , L. Lebanowski , J. Lee , M. K. P. Lee , R. T. Lei , R. Leitner , J. K. C. Leung , K. Y. Leung , C. A. Lewis , B. Li , C. Li , D. J. Li , F. Li , G. S. Li , J. Li , N. Y. Li , Q. J. Li , S. F. Li , S. C. Li , W. D. Li , X. B. Li , X. N. Li , X. Q. Li , Y. Li , Y. F. Li , Z. B. Li , H. Liang , J. Liang , C. J. Lin , G. L. Lin , P. Y. Lin , S. X. Lin , S. K. Lin , Y. C. Lin , J. J. Ling , J. M. Link , L. Littenberg , B. R. Littlejohn , B. J. Liu , C. Liu , D. W. Liu , H. Liu , J. L. Liu , J. C. Liu , S. Liu , S. S. Liu , X. Liu , Y. B. Liu , C. Lu , H. Q. Lu , J. S. Lu , A. Luk , K. B. Luk , T. Luo , X. L. Luo , L. H. Ma , Q. M. Ma , X. Y. Ma , X. B. Ma , Y. Q. Ma , B. Mayes , K. T. McDonald , M. C. McFarlane , R. D. McKeown , Y. Meng , I. Mitchell , D. Mohapatra , J. Monari Kebwaro , J. E. Morgan , Y. Nakajima , J. Napolitano , D. Naumov , E. Naumova , C. Newsom , H. Y. Ngai , W. K. Ngai , Y. B. Nie , Z. Ning , J. P. Ochoa-Ricoux , A. Olshevskiy , A. Pagac , H. -R. Pan , S. Patton , C. Pearson , V. Pec , J. C. Peng , L. E. Piilonen , L. Pinsky , C. S. J. Pun , F. Z. Qi , M. Qi , X. Qian , N. Raper , B. Ren , J. Ren , R. Rosero , B. Roskovec , X. C. Ruan , W. R. Sands , B. Seilhan , B. B. Shao , K. Shih , W. Y. Song , H. Steiner , P. Stoler , M. Stuart , G. X. Sun , J. L. Sun , N. Tagg , Y. H. Tam , H. K. Tanaka , W. Tang , X. Tang , D. Taychenachev , H. Themann , Y. Torun , S. Trentalange , O. Tsai , K. V. Tsang , R. H. M. Tsang , C. E. Tull , Y. C. Tung , N. Viaux , B. Viren , S. Virostek , V. Vorobel , C. H. Wang , L. S. Wang , L. Y. Wang , L. Z. Wang , M. Wang , N. Y. Wang , R. G. Wang , T. Wang , W. Wang , W. W. Wang , X. T. Wang , X. Wang , Y. F. Wang , Z. Wang , Z. Wang , Z. M. Wang , D. M. Webber , H. Y. Wei , Y. D. Wei , L. J. Wen , D. L. Wenman , K. Whisnant , C. G. White , L. Whitehead , C. A. Whitten , J. Wilhelmi , T. Wise , H. C. Wong , H. L. H. Wong , J. Wong , S. C. F. Wong , E. Worcester , F. F. Wu , Q. Wu , D. M. Xia , J. K. Xia , S. T. Xiang , Q. Xiao , Z. Z. Xing , G. Xu , J. Y. Xu , J. L. Xu , J. Xu , W. Xu , Y. Xu , T. Xue , J. Yan , C. G. Yang , L. Yang , M. S. Yang , M. T. Yang , M. Ye , M. Yeh , Y. S. Yeh , K. Yip , B. L. Young , G. Y. Yu , Z. Y. Yu , S. Zeng , L. Zhan , C. Zhang , F. H. Zhang , H. H. Zhang , J. W. Zhang , K. Zhang , Q. X. Zhang , Q. M. Zhang , S. H. Zhang , X. T. Zhang , Y. C. Zhang , Y. H. Zhang , Y. M. Zhang , Y. X. Zhang , Y. M. Zhang , Z. J. Zhang , Z. Y. Zhang , Z. P. Zhang , J. Zhao , Q. W. Zhao , Y. F. Zhao , Y. B. Zhao , L. Zheng , W. L. Zhong , L. Zhou , N. Zhou , Z. Y. Zhou , H. L. Zhuang , S. Zimmerman , J. H. Zou

Several efforts are ongoing for the development of spherical gaseous time projection chamber detectors for the observation of rare phenomena such as weakly interacting massive particles or neutrino interactions. The proposed detector,…

We estimate the dependence of $\nu_{\mu}$ to $\nu_{e}$ conversion on parameters $\theta_{13}$ and $\delta_{CP}$ for several experimental facilities studying neutrino oscillations. We use the S-Matrix theory to estimate $\bar{\nu_e}$…

High Energy Physics - Phenomenology · Physics 2012-10-08 Leonard S. Kisslinger , Ernest M. Henley , Mikkel B. Johnson

Hints for sizable $\sin^2 \theta_{13}$ have been reported in earlier global neutrino oscillation data analyses as well as will be reported in this work, and quite recently by the Double Chooz experiment. However, as we enter the era of…

High Energy Physics - Phenomenology · Physics 2011-11-15 Melin Huang , S. D. Reitzner , Wei-Chun Tsai , Huitzu Tu

Random coincidences of nuclear events can be one of the main background sources in low-temperature calorimetric experiments looking for neutrinoless double-beta decay, especially in those searches based on scintillating bolometers embedding…

In this paper we do a three-generation oscillation analysis of the latest (848 days) Super-Kamiokande (SK) atmospheric neutrino data going beyond the one mass scale dominance (OMSD) approximation. We fix $\Delta_{12} = \Delta_{13}$…

High Energy Physics - Phenomenology · Physics 2011-05-23 Sandhya Choubey , Srubabati Goswami , Kamales Kar

Two neutrino double $\beta$ decay can create irremovable background even in high energy resolution detectors searching for neutrinoless double $\beta$ decay due to random coincidence of $2\nu2\beta$ events in case of poor time resolution.…

Instrumentation and Detectors · Physics 2013-01-21 D. M. Chernyak , F. A. Danevich , A. Giuliani , E. Olivieri , M. Tenconi , V. I. Tretyak

Reactor antineutrinos are used to study neutrino oscillation, search for signatures of non-standard neutrino interactions, and to monitor reactor operation for safeguard applications. The flux and energy spectrum of reactor antineutrinos…

High Energy Physics - Experiment · Physics 2013-05-01 K. M. Heeger , B. R. Littlejohn , H. P. Mumm , M. N. Tobin

Liquid scintillators are a common choice for neutrino physics experiments, but their capabilities to perform background rejection by scintillation pulse shape discrimination is generally limited in large detectors. This paper describes a…

Xenon dual-phase time projections chambers (TPCs) have proven to be a successful technology in studying physical phenomena that require low-background conditions. With 40t of liquid xenon (LXe) in the TPC baseline design, DARWIN will have a…

Instrumentation and Detectors · Physics 2024-07-26 M. Adrover , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , B. Antunovic , E. Aprile , M. Babicz , D. Bajpai , E. Barberio , L. Baudis , M. Bazyk , N. Bell , L. Bellagamba , R. Biondi , Y. Biondi , A. Bismark , C. Boehm , A. Breskin , E. J. Brookes , A. Brown , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , A. Chauvin , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , M. P. Decowski , A. Deisting , P. Di Gangi , S. Diglio , M. Doerenkamp , G. Drexlin , K. Eitel , A. Elykov , R. Engel , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , W. Fulgione , P. Gaemers , R. Gaior , M. Galloway , N. Garroum , S. Ghosh , F. Girard , R. Glade-Beucke , F. Glück , L. Grandi , J. Grigat , R. Größle , H. Guan , M. Guida , R. Hammann , V. Hannen , S. Hansmann-Menzemer , N. Hargittai , T. Hasegawa , C. Hils , A. Higuera , K. Hiraoka , L. Hoetzsch , M. Iacovacci , Y. Itow , J. Jakob , F. Jörg , M. Kara , P. Kavrigin , S. Kazama , M. Keller , B. Kilminster , M. Kleifges , M. Kobayashi , A. Kopec , B. von Krosigk , F. Kuger , H. Landsman , R. F. Lang , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , F. Lombardi , J. Loizeau , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , T. Marrodán Undagoitia , J. A. M. Lopes , F. Marignetti , K. Martens , J. Masbou , S. Mastroianni , S. Milutinovic , K. Miuchi , R. Miyata , A. Molinario , C. M. B. Monteiro , K. Morå , E. Morteau , Y. Mosbacher , J. Müller , M. Murra , J. L. Newstead , K. Ni , U. G. Oberlack , I. Ostrovskiy , B. Paetsch , M. Pandurovic , Q. Pellegrini , R. Peres , J. Pienaar , M. Pierre , M. Piotter , G. Plante , T. R. Pollmann , L. Principe , J. Qi , J. Qin , M. Rajado Silva , D. Ramírez García , A. Razeto , S. Sakamoto , L. Sanchez , P. Sanchez-Lucas , J. M. F. dos Santos , G. Sartorelli , A. Scaffidi , P. Schulte , H. -C. Schultz-Coulon , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Sharma , W. Shen , M. Silva , H. Simgen , R. Singh , M. Solmaz , O. Stanley , M. Steidl , P. L. Tan , A. Terliuk , D. Thers , T. Thümmler , F. Tönnies , F. Toschi , G. Trinchero , R. Trotta , C. Tunnell , P. Urquijo , K. Valerius , S. Vecchi , S. Vetter , G. Volta , D. Vorkapic , W. Wang , K. M. Weerman , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , J. Wolf , T. Wolf , V. H. S. Wu , M. Wurm , Y. Xing , M. Yamashita , J. Ye , G. Zavattini , K. Zuber
‹ Prev 1 8 9 10 Next ›