- Record: found
- Abstract: not found
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Indication of Reactor\({\overline{\nu }}_{e}\)Disappearance in the Double Chooz Experiment
Y. Abe ,
C. Aberle ,
T. Akiri ,
J. C. dos Anjos ,
F. Ardellier ,
A. F. Barbosa ,
A. Baxter ,
M. Bergevin ,
A. Bernstein ,
T. J. C. Bezerra ,
L. Bezrukhov ,
E. Blucher ,
M. Bongrand ,
N. S. Bowden ,
C. Buck ,
J. Busenitz ,
A. Cabrera ,
E. Caden ,
L. Camilleri ,
R. Carr ,
M. Cerrada ,
P.-J. Chang ,
P. Chimenti ,
T. Classen ,
A. P. Collin ,
E. Conover ,
J. M. Conrad ,
S. Cormon ,
J. I. Crespo-Anadón ,
M. Cribier ,
K. Crum ,
A. Cucoanes ,
M. V. D’Agostino ,
E. Damon ,
J. V. Dawson ,
S. Dazeley ,
M. Dierckxsens ,
D. Dietrich ,
Z. Djurcic ,
M. Dracos ,
V. Durand ,
Y. Efremenko ,
M. Elnimr ,
Y. Endo ,
A. Etenko ,
E. Falk ,
M. Fallot ,
M. Fechner ,
F. von Feilitzsch ,
J. Felde ,
S. M. Fernandes ,
D. Franco ,
A. J. Franke ,
M. Franke ,
H. Furuta ,
R. Gama ,
I. Gil-Botella ,
L. Giot ,
M. Göger-Neff ,
L. F. G. Gonzalez ,
M. C. Goodman ,
J. TM. Goon ,
D. Greiner ,
B. Guillon ,
N. Haag ,
C. Hagner ,
T. Hara ,
F. X. Hartmann ,
J. Hartnell ,
T. Haruna ,
J. Haser ,
A. Hatzikoutelis ,
T. Hayakawa ,
M. Hofmann ,
G. A. Horton-Smith ,
M. Ishitsuka ,
J. Jochum ,
C. Jollet ,
C. L. Jones ,
F. Kaether ,
L. Kalousis ,
Y. Kamyshkov ,
D. M. Kaplan ,
T. Kawasaki ,
G. Keefer ,
E. Kemp ,
H. de Kerret ,
Y. Kibe ,
T. Konno ,
D. Kryn ,
M. Kuze ,
T. Lachenmaier ,
C. E. Lane ,
C. Langbrandtner ,
T. Lasserre ,
A. Letourneau ,
D. Lhuillier ,
H. P. Lima ,
M. Lindner ,
Y. Liu ,
J. M. López-Castanõ ,
J. M. LoSecco ,
B. K. Lubsandorzhiev ,
S. Lucht ,
D. McKee ,
J. Maeda ,
C. N. Maesano ,
C. Mariani ,
J. Maricic ,
J. Martino ,
T. Matsubara ,
G. Mention ,
A. Meregaglia ,
T. Miletic ,
R. Milincic ,
A. Milzstajn ,
H. Miyata ,
D. Motta ,
Th. A. Mueller ,
Y. Nagasaka ,
K. Nakajima ,
P. Novella ,
M. Obolensky ,
L. Oberauer ,
A. Onillon ,
A. Osborn ,
I. Ostrovskiy ,
C. Palomares ,
S. J. M. Peeters ,
I. M. Pepe ,
S. Perasso ,
P. Perrin ,
P. Pfahler ,
A. Porta ,
W. Potzel ,
R. Queval ,
J. Reichenbacher ,
B. Reinhold ,
A. Remoto ,
D. Reyna ,
M. Röhling ,
S. Roth ,
H. A. Rubin ,
Y. Sakamoto ,
R. Santorelli ,
F. Sato ,
S. Schönert ,
S. Schoppmann ,
U. Schwan ,
T. Schwetz ,
M. H. Shaevitz ,
D. Shrestha ,
J-L. Sida ,
V. Sinev ,
M. Skorokhvatov ,
E. Smith ,
J. Spitz ,
A. Stahl ,
I. Stancu ,
M. Strait ,
A. Stüken ,
F. Suekane ,
S. Sukhotin ,
T. Sumiyoshi ,
Y. Sun ,
Z. Sun ,
R. Svoboda ,
H. Tabata ,
N. Tamura ,
K. Terao ,
A. Tonazzo ,
M. Toups ,
H. H. Trinh Thi ,
C. Veyssiere ,
S. Wagner ,
H. Watanabe ,
B. White ,
C. Wiebusch ,
L. Winslow ,
M. Worcester ,
M. Wurm ,
E. Yanovitch ,
F. Yermia ,
K. Zbiri ,
V. Zimmer ,
Double Chooz Collaboration
March 28 2012
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Abstract
The Double Chooz experiment presents an indication of reactor electron antineutrino
disappearance consistent with neutrino oscillations. An observed-to-predicted ratio
of events of 0.944±0.016(stat)±0.040(syst) was obtained in 101 days of running at
the Chooz nuclear power plant in France, with two 4.25 GW(th) reactors. The results
were obtained from a single 10 m(3) fiducial volume detector located 1050 m from the
two reactor cores. The reactor antineutrino flux prediction used the Bugey4 flux measurement
after correction for differences in core composition. The deficit can be interpreted
as an indication of a nonzero value of the still unmeasured neutrino mixing parameter
sin(2)2θ(13). Analyzing both the rate of the prompt positrons and their energy spectrum,
we find sin(2)2θ(13)=0.086±0.041(stat)±0.030(syst), or, at 90% C.L., 0.017<sin(2)2θ(13)<0.16.
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