| author name | recommending | commenting | favorite | papers | recom. | cited | |
|---|---|---|---|---|---|---|---|
| 0 | 0 | 0 | 1296 | 0 | 15026 | [Update] | |
| 0 | 0 | 0 | 3 | 0 | 24 | [Update] | |
| 0 | 0 | 0 | 1 | 0 | 2 | [Update] | |
| 0 | 0 | 0 | 2 | 0 | 1 | [Update] | |
| 0 | 0 | 0 | 5 | 0 | 3 | [Update] | |
| 0 | 0 | 0 | 1 | 0 | 0 | [Update] | |
| 0 | 0 | 0 | 4 | 0 | 2 | [Update] | |
| 0 | 0 | 0 | 14 | 0 | 26 | [Update] | |
| 0 | 0 | 0 | 3 | 0 | 21 | [Update] | |
| 0 | 0 | 0 | 1 | 0 | 0 | [Update] | |
| 0 | 0 | 0 | 1 | 0 | 2 | [Update] | |
| 0 | 0 | 0 | 7 | 0 | 0 | [Update] | |
| 0 | 0 | 0 | 1 | 0 | 9 | [Update] | |
| 0 | 0 | 0 | 7 | 0 | 93 | [Update] | |
| 0 | 0 | 0 | 2 | 0 | 0 | [Update] | |
| 0 | 0 | 0 | 2 | 0 | 0 | [Update] | |
| 0 | 0 | 0 | 5 | 0 | 5 | [Update] | |
| 0 | 0 | 0 | 7 | 0 | 10 | [Update] | |
| 0 | 0 | 0 | 15 | 0 | 148 | [Update] | |
| 0 | 0 | 0 | 2 | 0 | 3 | [Update] | |
| 0 | 0 | 0 | 2 | 0 | 19 | [Update] |
Latest Paper:
G Aad,
B Abbott,
J Abdallah,
A A Abdelalim,
A Abdesselam,
O Abdinov,
B Abi,
M Abolins,
O S Abouzeid,
H Abramowicz,
H Abreu,
E Acerbi,
B S Acharya,
L Adamczyk,
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T N Addy,
J Adelman,
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S Adomeit,
P Adragna,
T Adye,
S Aefsky,
J A Aguilar-Saavedra,
M Aharrouche,
S P Ahlen,
F Ahles,
A Ahmad,
M Ahsan,
G Aielli,
T Akdogan,
T P A Akesson,
G Akimoto,
A V Akimov,
A Akiyama,
M S Alam,
M A Alam,
J Albert,
S Albrand,
M Aleksa,
I N Aleksandrov,
F Alessandria,
C Alexa,
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T Alexopoulos,
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M Aliev,
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J Alison,
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B M M Allbrooke,
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S E Allwood-Spiers,
J Almond,
A Aloisio,
R Alon,
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B Alvarez Gonzalez,
M G Alviggi,
K Amako,
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N Amram,
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H M Braun,
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T Buanes,
Q Buat,
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G A Chelkov,
M A Chelstowska,
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A Cheplakov,
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J T Childers,
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F Corriveau,
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B E Cox,
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M Dosil,
A Dotti,
M T Dova,
J D Dowell,
A D Doxiadis,
A T Doyle,
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J Drees,
N Dressnandt,
H Drevermann,
C Driouichi,
M Dris,
J Dubbert,
S Dube,
E Duchovni,
G Duckeck,
A Dudarev,
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M Dunford,
H Duran Yildiz,
R Duxfield,
M Dwuznik,
F Dydak,
M Düren,
W L Ebenstein,
J Ebke,
S Eckweiler,
K Edmonds,
C A Edwards,
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W Ehrenfeld,
T Ehrich,
T Eifert,
G Eigen,
K Einsweiler,
E Eisenhandler,
T Ekelof,
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K Ellis,
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X Espinal Curull,
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R M Fakhrutdinov,
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Y Fang,
M Fanti,
A Farbin,
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J Farley,
T Farooque,
S M Farrington,
P Farthouat,
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D Fassouliotis,
B Fatholahzadeh,
A Favareto,
L Fayard,
S Fazio,
R Febbraro,
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W Fedorko,
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D Fellmann,
C Feng,
E J Feng,
A B Fenyuk,
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W Fernando,
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A Ferrari,
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R Ferrari,
D E Ferreira de Lima,
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M L Ferrer,
D Ferrere,
C Ferretti,
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M Fiascaris,
F Fiedler,
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L Fiorini,
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G Fischer,
P Fischer,
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M Flechl,
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T Flick,
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L R Flores Castillo,
M J Flowerdew,
M Fokitis,
T Fonseca Martin,
D A Forbush,
A Formica,
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T Frank,
M Franklin,
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S T French,
F Friedrich,
R Froeschl,
D Froidevaux,
J A Frost,
C Fukunaga,
E Fullana Torregrosa,
J Fuster,
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O Gabizon,
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G Gagliardi,
P Gagnon,
C Galea,
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V Gallo,
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K K Gan,
Y S Gao,
V A Gapienko,
A Gaponenko,
F Garberson,
M Garcia-Sciveres,
C García,
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R W Gardner,
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H Garitaonandia,
V Garonne,
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C Gatti,
G Gaudio,
B Gaur,
L Gauthier,
I L Gavrilenko,
C Gay,
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J-C Gayde,
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A Gibson,
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D Gillberg,
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F M Giorgi,
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B K Gjelsten,
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G L Glonti,
J R Goddard,
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M Goebel,
T Göpfert,
C Goeringer,
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T Golling,
A Gomes,
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S Gonzalez,
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G Gonzalez Parra,
M L Gonzalez Silva,
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J J Goodson,
L Goossens,
P A Gorbounov,
H A Gordon,
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B Gorini,
E Gorini,
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E Gornicki,
S A Gorokhov,
V N Goryachev,
B Gosdzik,
M Gosselink,
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M Gouighri,
D Goujdami,
M P Goulette,
A G Goussiou,
C Goy,
S Gozpinar,
I Grabowska-Bold,
P Grafström,
K-J Grahn,
F Grancagnolo,
S Grancagnolo,
V Grassi,
V Gratchev,
N Grau,
H M Gray,
J A Gray,
E Graziani,
O G Grebenyuk,
T Greenshaw,
Z D Greenwood,
K Gregersen,
I M Gregor,
P Grenier,
J Griffiths,
N Grigalashvili,
A A Grillo,
S Grinstein,
Y V Grishkevich,
J-F Grivaz,
M Groh,
E Gross,
J Grosse-Knetter,
J Groth-Jensen,
K Grybel,
V J Guarino,
D Guest,
C Guicheney,
A Guida,
S Guindon,
H Guler,
J Gunther,
B Guo,
J Guo,
A Gupta,
Y Gusakov,
V N Gushchin,
P Gutierrez,
N Guttman,
O Gutzwiller,
C Guyot,
C Gwenlan,
C B Gwilliam,
A Haas,
S Haas,
C Haber,
H K Hadavand,
D R Hadley,
P Haefner,
F Hahn,
S Haider,
Z Hajduk,
H Hakobyan,
D Hall,
J Haller,
K Hamacher,
P Hamal,
M Hamer,
A Hamilton,
S Hamilton,
H Han,
L Han,
K Hanagaki,
K Hanawa,
M Hance,
C Handel,
P Hanke,
J R Hansen,
J B Hansen,
J D Hansen,
P H Hansen,
P Hansson,
K Hara,
G A Hare,
T Harenberg,
S Harkusha,
D Harper,
R D Harrington,
O M Harris,
K Harrison,
J Hartert,
F Hartjes,
T Haruyama,
A Harvey,
S Hasegawa,
Y Hasegawa,
S Hassani,
M Hatch,
D Hauff,
S Haug,
M Hauschild,
R Hauser,
M Havranek,
B M Hawes,
C M Hawkes,
R J Hawkings,
A D Hawkins,
D Hawkins,
T Hayakawa,
T Hayashi,
D Hayden,
H S Hayward,
S J Haywood,
E Hazen,
M He,
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V Hedberg,
L Heelan,
S Heim,
B Heinemann,
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L Helary,
C Heller,
M Heller,
S Hellman,
D Hellmich,
C Helsens,
R C W Henderson,
M Henke,
A Henrichs,
A M Henriques Correia,
S Henrot-Versille,
F Henry-Couannier,
C Hensel,
T Henß,
C M Hernandez,
Y Hernández Jiménez,
R Herrberg,
A D Hershenhorn,
G Herten,
R Hertenberger,
L Hervas,
G G Hesketh,
N P Hessey,
E Higón-Rodriguez,
D Hill,
J C Hill,
N Hill,
K H Hiller,
S Hillert,
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A Zemla,
C Zendler,
O Zenin,
T Zeniš,
Z Zinonos,
S Zenz,
D Zerwas,
G Zevi Della Porta,
Z Zhan,
D Zhang,
H Zhang,
J Zhang,
X Zhang,
Z Zhang,
L Zhao,
T Zhao,
Z Zhao,
A Zhemchugov,
S Zheng,
J Zhong,
B Zhou,
N Zhou,
Y Zhou,
C G Zhu,
H Zhu,
J Zhu,
Y Zhu,
X Zhuang,
V Zhuravlov,
D Zieminska,
R Zimmermann,
S Zimmermann,
M Ziolkowski,
R Zitoun,
L Zivković,
V V Zmouchko,
G Zobernig,
A Zoccoli,
Y Zolnierowski,
A Zsenei,
M Zur Nedden,
V Zutshi,
L Zwalinski
Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg i.Br., Germany.
The χ_{b}(nP) quarkonium states are produced in proton-proton collisions at the Large Hadron Collider at sqrt[s]=7 TeV and recorded by the ATLAS detector. Using a data sample corresponding to an integrated luminosity of 4.4 fb^{-1}, these states are reconstructed through their radiative decays to Υ(1S,2S) with Υ→μ^{+}μ^{-}. In addition to the mass peaks corresponding to the decay modes χ_{b}(1P,2P)→Υ(1S)γ, a new structure centered at a mass of 10.530±0.005(stat)±0.009(syst) GeV is also observed, in both the Υ(1S)γ and Υ(2S)γ decay modes. This structure is interpreted as the χ_{b}(3P) system.
T Aaltonen,
B Alvarez González,
S Amerio,
D Amidei,
A Anastassov,
A Annovi,
J Antos,
G Apollinari,
J A Appel,
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A Barbaro-Galtieri,
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F Chlebana,
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W H Chung,
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P de Barbaro,
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M d'Errico,
A Di Canto,
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A Golossanov,
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M Goncharov,
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I Gorelov,
A T Goshaw,
K Goulianos,
S Grinstein,
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S R Hahn,
E Halkiadakis,
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J Y Han,
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R F Harr,
K Hatakeyama,
C Hays,
M Heck,
J Heinrich,
M Herndon,
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S Hou,
R E Hughes,
M Hurwitz,
U Husemann,
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D Jang,
B Jayatilaka,
E J Jeon,
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M Jones,
K K Joo,
S Y Jun,
T R Junk,
T Kamon,
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N Kimura,
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J Konigsberg,
A V Kotwal,
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S Kwang,
A T Laasanen,
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R L Lander,
K Lannon,
A Lath,
G Latino,
T Lecompte,
E Lee,
H S Lee,
J S Lee,
S W Lee,
S Leo,
S Leone,
J D Lewis,
A Limosani,
C-J Lin,
M Lindgren,
E Lipeles,
A Lister,
D O Litvintsev,
C Liu,
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Q Liu,
T Liu,
S Lockwitz,
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D Lucchesi,
J Lueck,
P Lujan,
P Lukens,
G Lungu,
J Lys,
R Lysak,
R Madrak,
K Maeshima,
P Maestro,
S Malik,
G Manca,
A Manousakis-Katsikakis,
F Margaroli,
C Marino,
M Martínez,
P Mastrandrea,
K Matera,
M E Mattson,
A Mazzacane,
P Mazzanti,
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P McIntyre,
R McNulty,
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C Mesropian,
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N Moggi,
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C S Moon,
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M Trovato,
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C Vellidis,
M Vidal,
I Vila,
R Vilar,
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M Vogel,
G Volpi,
P Wagner,
R L Wagner,
T Wakisaka,
R Wallny,
S M Wang,
A Warburton,
D Waters,
W C Wester 3rd,
D Whiteson,
A B Wicklund,
E Wicklund,
S Wilbur,
F Wick,
H H Williams,
J S Wilson,
P Wilson,
B L Winer,
P Wittich,
S Wolbers,
H Wolfe,
T Wright,
X Wu,
Z Wu,
K Yamamoto,
D Yamato,
T Yang,
U K Yang,
Y C Yang,
W-M Yao,
G P Yeh,
K Yi,
J Yoh,
K Yorita,
T Yoshida,
G B Yu,
I Yu,
S S Yu,
J C Yun,
A Zanetti,
Y Zeng,
C Zhou,
S Zucchelli
Division of High Energy Physics, Department of Physics, University of Helsinki and Helsinki Institute of Physics, FIN-00014, Helsinki, Finland.
We have measured the W-boson mass M_{W} using data corresponding to 2.2 fb^{-1} of integrated luminosity collected in pp[over ¯] collisions at sqrt[s]=1.96 TeV with the CDF II detector at the Fermilab Tevatron collider. Samples consisting of 470 126 W→eν candidates and 624 708 W→μν candidates yield the measurement M_{W}=80 387±12_{stat.}±15_{syst.}=80 387±19 MeV/c^{2}. This is the most precise measurement of the W-boson mass to date and significantly exceeds the precision of all previous measurements combined.
T Aaltonen,
B Alvarez González,
S Amerio,
D Amidei,
A Anastassov,
A Annovi,
J Antos,
G Apollinari,
J A Appel,
T Arisawa,
A Artikov,
J Asaadi,
W Ashmanskas,
B Auerbach,
A Aurisano,
F Azfar,
W Badgett,
T Bae,
A Barbaro-Galtieri,
V E Barnes,
B A Barnett,
P Barria,
P Bartos,
M Bauce,
F Bedeschi,
S Behari,
G Bellettini,
J Bellinger,
D Benjamin,
A Beretvas,
A Bhatti,
D Bisello,
I Bizjak,
K R Bland,
B Blumenfeld,
A Bocci,
A Bodek,
D Bortoletto,
J Boudreau,
A Boveia,
L Brigliadori,
C Bromberg,
E Brucken,
J Budagov,
H S Budd,
K Burkett,
G Busetto,
P Bussey,
A Buzatu,
A Calamba,
C Calancha,
S Camarda,
M Campanelli,
M Campbell,
F Canelli,
B Carls,
D Carlsmith,
R Carosi,
S Carrillo,
S Carron,
B Casal,
M Casarsa,
A Castro,
P Catastini,
D Cauz,
V Cavaliere,
M Cavalli-Sforza,
A Cerri,
L Cerrito,
Y C Chen,
M Chertok,
G Chiarelli,
G Chlachidze,
F Chlebana,
K Cho,
D Chokheli,
W H Chung,
Y S Chung,
M A Ciocci,
A Clark,
C Clarke,
G Compostella,
M E Convery,
J Conway,
M Corbo,
M Cordelli,
C A Cox,
D J Cox,
F Crescioli,
J Cuevas,
R Culbertson,
D Dagenhart,
N d'Ascenzo,
M Datta,
P de Barbaro,
M Dell'orso,
L Demortier,
M Deninno,
F Devoto,
M d'Errico,
A Di Canto,
B Di Ruzza,
J R Dittmann,
M D'Onofrio,
S Donati,
P Dong,
M Dorigo,
T Dorigo,
K Ebina,
A Elagin,
A Eppig,
R Erbacher,
S Errede,
N Ershaidat,
R Eusebi,
S Farrington,
M Feindt,
J P Fernandez,
R Field,
G Flanagan,
R Forrest,
M J Frank,
M Franklin,
J C Freeman,
Y Funakoshi,
I Furic,
M Gallinaro,
J E Garcia,
A F Garfinkel,
P Garosi,
H Gerberich,
E Gerchtein,
S Giagu,
V Giakoumopoulou,
P Giannetti,
K Gibson,
C M Ginsburg,
N Giokaris,
P Giromini,
G Giurgiu,
V Glagolev,
D Glenzinski,
M Gold,
D Goldin,
N Goldschmidt,
A Golossanov,
G Gomez,
G Gomez-Ceballos,
M Goncharov,
O González,
I Gorelov,
A T Goshaw,
K Goulianos,
S Grinstein,
C Grosso-Pilcher,
R C Group,
J Guimaraes da Costa,
S R Hahn,
E Halkiadakis,
A Hamaguchi,
J Y Han,
F Happacher,
K Hara,
D Hare,
M Hare,
R F Harr,
K Hatakeyama,
C Hays,
M Heck,
J Heinrich,
M Herndon,
S Hewamanage,
A Hocker,
W Hopkins,
D Horn,
S Hou,
R E Hughes,
M Hurwitz,
U Husemann,
N Hussain,
M Hussein,
J Huston,
G Introzzi,
M Iori,
A Ivanov,
E James,
D Jang,
B Jayatilaka,
E J Jeon,
S Jindariani,
M Jones,
K K Joo,
S Y Jun,
T R Junk,
T Kamon,
P E Karchin,
A Kasmi,
Y Kato,
W Ketchum,
J Keung,
V Khotilovich,
B Kilminster,
D H Kim,
H S Kim,
J E Kim,
M J Kim,
S B Kim,
S H Kim,
Y K Kim,
Y J Kim,
N Kimura,
M Kirby,
S Klimenko,
K Knoepfel,
K Kondo,
D J Kong,
J Konigsberg,
A V Kotwal,
M Kreps,
J Kroll,
D Krop,
M Kruse,
V Krutelyov,
T Kuhr,
M Kurata,
S Kwang,
A T Laasanen,
S Lami,
S Lammel,
M Lancaster,
R L Lander,
K Lannon,
A Lath,
G Latino,
T Lecompte,
E Lee,
H S Lee,
J S Lee,
S W Lee,
S Leo,
S Leone,
J D Lewis,
A Limosani,
C-J Lin,
M Lindgren,
E Lipeles,
A Lister,
D O Litvintsev,
C Liu,
H Liu,
Q Liu,
T Liu,
S Lockwitz,
A Loginov,
D Lucchesi,
J Lueck,
P Lujan,
P Lukens,
G Lungu,
J Lys,
R Lysak,
R Madrak,
K Maeshima,
P Maestro,
S Malik,
G Manca,
A Manousakis-Katsikakis,
F Margaroli,
C Marino,
M Martínez,
P Mastrandrea,
K Matera,
M E Mattson,
A Mazzacane,
P Mazzanti,
K S McFarland,
P McIntyre,
R McNulty,
A Mehta,
P Mehtala,
C Mesropian,
T Miao,
D Mietlicki,
A Mitra,
H Miyake,
S Moed,
N Moggi,
M N Mondragon,
C S Moon,
R Moore,
M J Morello,
J Morlock,
P Movilla Fernandez,
A Mukherjee,
Th Muller,
P Murat,
M Mussini,
J Nachtman,
Y Nagai,
J Naganoma,
I Nakano,
A Napier,
J Nett,
C Neu,
M S Neubauer,
J Nielsen,
L Nodulman,
S Y Noh,
O Norniella,
L Oakes,
S H Oh,
Y D Oh,
I Oksuzian,
T Okusawa,
R Orava,
L Ortolan,
S Pagan Griso,
C Pagliarone,
E Palencia,
V Papadimitriou,
A A Paramonov,
J Patrick,
G Pauletta,
M Paulini,
C Paus,
D E Pellett,
A Penzo,
T J Phillips,
G Piacentino,
E Pianori,
J Pilot,
K Pitts,
C Plager,
L Pondrom,
S Poprocki,
K Potamianos,
F Prokoshin,
A Pranko,
F Ptohos,
G Punzi,
A Rahaman,
V Ramakrishnan,
N Ranjan,
I Redondo,
P Renton,
M Rescigno,
T Riddick,
F Rimondi,
L Ristori,
A Robson,
T Rodrigo,
T Rodriguez,
E Rogers,
S Rolli,
R Roser,
F Ruffini,
A Ruiz,
J Russ,
V Rusu,
A Safonov,
W K Sakumoto,
Y Sakurai,
L Santi,
K Sato,
V Saveliev,
A Savoy-Navarro,
P Schlabach,
A Schmidt,
E E Schmidt,
T Schwarz,
L Scodellaro,
A Scribano,
F Scuri,
S Seidel,
Y Seiya,
A Semenov,
F Sforza,
S Z Shalhout,
T Shears,
P F Shepard,
M Shimojima,
M Shochet,
I Shreyber-Tecker,
A Simonenko,
P Sinervo,
K Sliwa,
J R Smith,
F D Snider,
A Soha,
V Sorin,
H Song,
P Squillacioti,
M Stancari,
R St Denis,
B Stelzer,
O Stelzer-Chilton,
D Stentz,
J Strologas,
G L Strycker,
Y Sudo,
A Sukhanov,
I Suslov,
K Takemasa,
Y Takeuchi,
J Tang,
M Tecchio,
P K Teng,
J Thom,
J Thome,
G A Thompson,
E Thomson,
D Toback,
S Tokar,
K Tollefson,
T Tomura,
D Tonelli,
S Torre,
D Torretta,
P Totaro,
M Trovato,
F Ukegawa,
S Uozumi,
A Varganov,
F Vázquez,
G Velev,
C Vellidis,
M Vidal,
I Vila,
R Vilar,
J Vizán,
M Vogel,
G Volpi,
P Wagner,
R L Wagner,
T Wakisaka,
R Wallny,
S M Wang,
A Warburton,
D Waters,
W C Wester 3rd,
D Whiteson,
A B Wicklund,
E Wicklund,
S Wilbur,
F Wick,
H H Williams,
J S Wilson,
P Wilson,
B L Winer,
P Wittich,
S Wolbers,
H Wolfe,
T Wright,
X Wu,
Z Wu,
K Yamamoto,
D Yamato,
T Yang,
U K Yang,
Y C Yang,
W-M Yao,
G P Yeh,
K Yi,
J Yoh,
K Yorita,
T Yoshida,
G B Yu,
I Yu,
S S Yu,
J C Yun,
A Zanetti,
Y Zeng,
C Zhou,
S Zucchelli
Division of High Energy Physics, Department of Physics, University of Helsinki and Helsinki Institute of Physics, FIN-00014, Helsinki, Finland.
The angular distributions of muons from Υ(1S,2S,3S)→μ^{+}μ^{-} decays are measured using data from pp[over ¯] collisions at sqrt[s]=1.96 TeV corresponding to an integrated luminosity of 6.7 fb^{-1} and collected with the CDF II detector at the Fermilab Tevatron. This analysis is the first to report the full angular distributions as functions of transverse momentum p_{T} for Υ mesons in both the Collins-Soper and s-channel helicity frames. This is also the first measurement of the spin alignment of Υ(3S) mesons. Within the kinematic range of Υ rapidity |y|<0.6 and p_{T} up to 40 GeV/c, the angular distributions are found to be nearly isotropic.
IEEE Trans Biomed Eng. 2012 May 7;:
22581127
This paper presents a novel solution of a handheld external controller to a miniaturized capsule endoscope in the gastrointestinal (GI) tract. Traditional capsule endoscopes move passively by peristaltic wave generated in the GI tract and the gravity, which makes it impossible for endoscopists to manipulate the capsule endoscope to the diagnostic disease areas. In this study, the main objective is to present an endoscopic capsule and a magnetic field navigator (MFN) that allows endoscopists to remotely control the locomotion and viewing angle of an endoscopic capsule. The attractive merits of this study are that the maneuvering of the endoscopic capsule can be achieved by the external MFN with effectiveness, low-cost, and operation safety, both from a theoretical and an experimental point of view. In order to study the magnetic interactions between the endoscopic capsule and the external MFN, a magnetic-analysis model is established for computer-based finite-element simulations. In addition, experiments are conducted to show the control effectiveness of the MFN to the endoscopic capsule. Finally, several prototype endoscopic capsules and a prototype MFN are fabricated, and their actual capabilities are experimentally assessed via in vitro and ex vivo tests using a stomach model and a resected porcine stomach, respectively. Both in vitro and ex vivo test results demonstrate great potential and practicability of achieving high-precision rotation and controllable movement of the capsule using the developed MFN.
Department of Hepatobiliary Surgery, the Second Affiliated Hospital of Chongqing Medical University, Chongqing, People's Republic of China.
AIMS To investigate the protective role of nitric oxide (NO) induced by ischemic preconditioning (IP) on cold ischemic-reperfusion (IR) injury of rat liver grafts. METHODS One hundred twenty-eight male Sprague Dawley rats used for orthotopic liver transplantation were randomly divided into four groups (n = 32): administering heparin before ischemic reperfusion (control group); IP with 10-minute ischemia and 10-minute reperfusion before IR (IP group); adenosine before IR (Ade group); and L-NAME (NG-nitro-L-arginine methyl ester)+ IP before IR (NAME group). Half of each group were used to investigate 1-week recipient survival rate, and another to obtain blood and hepatic tissue samples after 2-hour reperfusion. RESULTS One-week survival bile production, serum NO, and antioxidase activity were higher but serum alanine aminotransferase, tumor necrosis factor-α, and superoxide levels in hepatic tissue were lower in the IP group and Ade group versus the control group or NAME group. Liver sinusoidal endothelial cells in the IP and Ade groups showed less injury than the other groups. CONCLUSION NO induced by IP can improve 1-week survival and rat liver function as well as protect liver sinusoidal endothelial cells.
Sci Rep. 2012 ;2 :388
22563522
Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education, and School of Physics and Technology, Wuhan University , Wuhan 430072, China.
The spin current, orbit angular momentum current and total angular momentum current in a tensor form have been universally defined according to the quantum electrodynamics. Their conservation quantities and the continuity equations have been discussed in different cases. Non-relativistic approximation forms are deduced in order to explain their physical meanings, and to analyze some experimental results. The spin current of helical edge states in HgTe/CdTe quantum wells is calculated to demonstrate the properties of the spin current of the two dimensional quantum spin-Hall system. A generalized spin-orbit coupling term in the semiconducting media is deduced based on the theory of the electrodynamics in the moving media. It is recommended to use the effective total angular momentum current instead of the pure spin current to describe the distribution of polarization and the transport properties in spintronics.
Br J Radiol. 2012 May 2;:
22553290
Department of Medical Ultrasound, Medical Imaging Center, Tenth People's Hospital of Tongji University, Shanghai Tenth People's Hospital, Shanghai, China.
Objectives: To assess the value of contrast-enhanced ultrasound (CEUS) in differentiating hepatocellular carcinoma (HCC) from non-neoplastic lesion in cirrhotic liver in comparison with baseline ultrasound.Methods: A total of 147 nodules (diameter ≤5.0 cm) in 133 cirrhotic patients (mean age ± standard deviation: 52±13 years, range 20-82 years; gender: 111 men and 22 women) were examined with CEUS. They were 116 HCCs, 26 macroregenerative nodules and 5 high-grade dysplastic nodules. CEUS was performed with a real-time contrast-specific mode and a sulphur hexafluoride-filled microbubble contrast agent.Results: Hyper-vascularity was observed in 94.8%(110/116) HCCs, 3.8%(1/26) macroregenerative nodules and 60.0%(3/5) high-grade dysplastic nodules during arterial phase on CEUS. Detection rates of typical vascular pattern (i.e. hyper-vascularity during arterial phase and subsequent washout) in HCCs with diameter of ≤2.0 cm, 2.1-3.0 cm and 3.1-5.0 cm were 69.2%(27/39), 97.1%(33/34) and 100.0%(43/43), respectively. CEUS significantly improved the sensitivity [88.8%(103/116) vs 37.1%(43/116), p<0.001], negative predictive value [70.5%(31/44) vs 31.5%(29/92), p<0.001], and accuracy [91.2%(134/147) vs 49.0%(72/147), p<0.001] in differentiating HCCs from non-neoplastic lesions when compared with baseline ultrasound. However, the sensitivity and accuracy of CEUS for HCCs ≤2.0 cm diameter were significantly lower than those for HCCs of 2.1-3.0 cm and 3.1-5.0 cm diameter.Conclusions: CEUS improves diagnostic performance in differentiating HCCs from non-neoplastic nodules in cirrhotic patients compared with baseline ultrasound. Diagnosis of HCCs ≤2.0 cm diameter by CEUS is still a clinical concern, and thus needs further investigation.
Am J Clin Oncol. 2012 Apr 27;:
22547011
Department of Oncology, First Affiliated Hospital of China Medical University, Shenyang, Liaoning Province, China.
OBJECTIVES:: The purpose of this study was to evaluate the outcome of the ratio between metastatic and examined lymph nodes (N ratio) in gastric cancer patients with <15 examined lymph nodes after curative resection. METHODS:: A retrospective study of 710 patients who underwent radical gastrectomy (R0) for gastric cancer from January 1980 to December 2000 was analyzed statistically to identify the N ratio. Patients with <15 examined lymph nodes (group 1, n=327) and those with ≥15 examined lymph nodes (group 2, n=383) were analyzed separately. N ratio categories were identified as follows: N ratio 0, 0%; N ratio 1, 1% to 9%; N ratio 2, 10% to 25%; and N ratio 3,>25%. All the enrolled categories were evaluated by the best cutoff approach. RESULTS:: The univariate analysis showed that age, tumor site, tumor size, surgery, T categories, number of metastatic nodes, and N ratio significantly affected prognosis in groups 1 and 2. By multivariate analysis, the N ratio (but not the TNM N category) classification was retained as an independent prognostic factor in groups 1 and 2 compared with the N category system. However, patients with N1 disease in group 1 obtained a better postoperative prognosis than those with N1 disease in group 2 according to the N stage classification (P=0.003). When the N ratio classification was applied, no significant differences were found for N ratios 0, 1, 2, or 3 between the 2 groups (P>0.05). CONCLUSIONS:: The metastatic lymph node ratio is an independent prognostic factor regardless of the examined number of lymph nodes. In predicting the prognosis of gastric cancer, the staging system based on the metastatic lymph node ratio is more reliable than the system based on the number of metastatic lymph nodes regardless of the examined number of lymph nodes. This can help improve the TNM staging classification of gastric cancer and reduce the International Union Against Cancer N categories of stage migration.
A Bondar,
A Garmash,
R Mizuk,
D Santel,
K Kinoshita,
I Adachi,
H Aihara,
K Arinstein,
D M Asner,
T Aushev,
T Aziz,
A M Bakich,
E Barberio,
K Belous,
V Bhardwaj,
M Bischofberger,
A Bozek,
M Bračko,
T E Browder,
M-C Chang,
P Chang,
A Chen,
B G Cheon,
K Chilikin,
R Chistov,
I-S Cho,
K Cho,
S-K Choi,
Y Choi,
J Dalseno,
M Danilov,
Z Doležal,
A Drutskoy,
S Eidelman,
D Epifanov,
J E Fast,
V Gaur,
N Gabyshev,
Y M Goh,
B Golob,
J Haba,
T Hara,
K Hayasaka,
Y Hoshi,
H J Hyun,
T Iijima,
K Inami,
A Ishikawa,
M Iwabuchi,
Y Iwasaki,
T Iwashita,
T Julius,
J H Kang,
T Kawasaki,
H Kichimi,
C Kiesling,
J B Kim,
J H Kim,
K T Kim,
M J Kim,
Y J Kim,
B R Ko,
N Kobayashi,
S Koblitz,
P Kodyš,
S Korpar,
P Križan,
T Kuhr,
R Kumar,
T Kumita,
A Kuzmin,
J S Lange,
S-H Lee,
J Li,
Y Li,
J Libby,
C Liu,
Z Q Liu,
D Liventsev,
R Louvot,
D Matvienko,
S McOnie,
H Miyata,
Y Miyazaki,
G B Mohanty,
A Moll,
N Muramatsu,
R Mussa,
M Nakao,
Z Natkaniec,
S Neubauer,
M Niiyama,
S Nishida,
K Nishimura,
O Nitoh,
T Nozaki,
S L Olsen,
Y Onuki,
P Pakhlov,
G Pakhlova,
H Park,
H K Park,
T K Pedlar,
M Petrič,
L E Piilonen,
A Poluektov,
M Prim,
M Ritter,
M Röhrken,
S Ryu,
H Sahoo,
Y Sakai,
T Sanuki,
O Schneider,
C Schwanda,
K Senyo,
M E Sevior,
M Shapkin,
V Shebalin,
T-A Shibata,
J-G Shiu,
B Shwartz,
F Simon,
P Smerkol,
Y-S Sohn,
A Sokolov,
E Solovieva,
M Starič,
M Sumihama,
T Sumiyoshi,
S Tanaka,
G Tatishvili,
Y Teramoto,
I Tikhomirov,
M Uchida,
S Uehara,
T Uglov,
Y Ushiroda,
S E Vahsen,
G Varner,
A Vinokurova,
C H Wang,
M-Z Wang,
P Wang,
X L Wang,
Y Watanabe,
K M Williams,
E Won,
B D Yabsley,
Y Yamashita,
M Yamauchi,
C Z Yuan,
Y Yusa,
Z P Zhang,
V Zhilich,
V Zhulanov,
A Zupanc,
O Zyukova
Budker Institute of Nuclear Physics SB RAS and Novosibirsk State University, Novosibirsk 630090.
We report the observation of two narrow structures in the mass spectra of the π^{±}Υ(nS)(n=1, 2, 3) and π^{±}h_{b}(mP)(m=1, 2) pairs that are produced in association with a single charged pion in Υ(5S) decays. The measured masses and widths of the two structures averaged over the five final states are M_{1}=(10 607.2±2.0) MeV/c^{2}, Γ_{1}=(18.4±2.4) MeV, and M_{2}=(10 652.2±1.5) MeV/c^{2}, Γ_{2}=(11.5±2.2) MeV. The results are obtained with a 121.4 fb^{-1} data sample collected with the Belle detector in the vicinity of the Υ(5S) resonance at the KEKB asymmetric-energy e^{+}e^{-} collider.
G Aad,
B Abbott,
J Abdallah,
S Abdel Khalek,
A A Abdelalim,
A Abdesselam,
O Abdinov,
B Abi,
M Abolins,
O S Abouzeid,
H Abramowicz,
H Abreu,
E Acerbi,
B S Acharya,
L Adamczyk,
D L Adams,
T N Addy,
J Adelman,
M Aderholz,
S Adomeit,
P Adragna,
T Adye,
S Aefsky,
J A Aguilar-Saavedra,
M Aharrouche,
S P Ahlen,
F Ahles,
A Ahmad,
M Ahsan,
G Aielli,
T Akdogan,
T P A Akesson,
G Akimoto,
A V Akimov,
A Akiyama,
M S Alam,
M A Alam,
J Albert,
S Albrand,
M Aleksa,
I N Aleksandrov,
F Alessandria,
C Alexa,
G Alexander,
G Alexandre,
T Alexopoulos,
M Alhroob,
M Aliev,
G Alimonti,
J Alison,
M Aliyev,
B M M Allbrooke,
P P Allport,
S E Allwood-Spiers,
J Almond,
A Aloisio,
R Alon,
A Alonso,
B Alvarez Gonzalez,
M G Alviggi,
K Amako,
P Amaral,
C Amelung,
V V Ammosov,
A Amorim,
G Amorós,
N Amram,
C Anastopoulos,
L S Ancu,
N Andari,
T Andeen,
C F Anders,
G Anders,
K J Anderson,
A Andreazza,
V Andrei,
M-L Andrieux,
X S Anduaga,
A Angerami,
F Anghinolfi,
A Anisenkov,
N Anjos,
A Annovi,
A Antonaki,
M Antonelli,
A Antonov,
J Antos,
F Anulli,
S Aoun,
L Aperio Bella,
R Apolle,
G Arabidze,
I Aracena,
Y Arai,
A T H Arce,
S Arfaoui,
J-F Arguin,
E Arik,
M Arik,
A J Armbruster,
O Arnaez,
V Arnal,
C Arnault,
A Artamonov,
G Artoni,
D Arutinov,
S Asai,
R Asfandiyarov,
S Ask,
B Asman,
L Asquith,
K Assamagan,
A Astbury,
A Astvatsatourov,
B Aubert,
E Auge,
K Augsten,
M Aurousseau,
G Avolio,
R Avramidou,
D Axen,
C Ay,
G Azuelos,
Y Azuma,
M A Baak,
G Baccaglioni,
C Bacci,
A M Bach,
H Bachacou,
K Bachas,
M Backes,
M Backhaus,
E Badescu,
P Bagnaia,
S Bahinipati,
Y Bai,
D C Bailey,
T Bain,
J T Baines,
O K Baker,
M D Baker,
S Baker,
E Banas,
P Banerjee,
Sw Banerjee,
D Banfi,
A Bangert,
V Bansal,
H S Bansil,
L Barak,
S P Baranov,
A Barashkou,
A Barbaro Galtieri,
T Barber,
E L Barberio,
D Barberis,
M Barbero,
D Y Bardin,
T Barillari,
M Barisonzi,
T Barklow,
N Barlow,
B M Barnett,
R M Barnett,
A Baroncelli,
G Barone,
A J Barr,
F Barreiro,
J Barreiro Guimarães da Costa,
P Barrillon,
R Bartoldus,
A E Barton,
V Bartsch,
R L Bates,
L Batkova,
J R Batley,
A Battaglia,
M Battistin,
F Bauer,
H S Bawa,
S Beale,
T Beau,
P H Beauchemin,
R Beccherle,
P Bechtle,
H P Beck,
S Becker,
M Beckingham,
K H Becks,
A J Beddall,
A Beddall,
S Bedikian,
V A Bednyakov,
C P Bee,
M Begel,
S Behar Harpaz,
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A I Kononov,
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E Strauss,
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Yu M Sviridov,
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T Sykora,
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J Sánchez,
D Ta,
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H Takai,
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X Zhuang,
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D Zieminska,
R Zimmermann,
S Zimmermann,
M Ziolkowski,
R Zitoun,
L Zivković,
V V Zmouchko,
G Zobernig,
A Zoccoli,
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A Zsenei,
M Zur Nedden,
V Zutshi,
L Zwalinski
Fakultät für Mathematik und Physik, Albert-Ludwigs-Universität, Freiburg i.Br., Germany.
A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9 fb^{-1} collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of sqrt[s]=7 TeV. In the diphoton mass range 110-150 GeV, the largest excess with respect to the background-only hypothesis is observed at 126.5 GeV, with a local significance of 2.8 standard deviations. Taking the look-elsewhere effect into account in the range 110-150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113-115 GeV and 134.5-136 GeV.
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