903 research outputs found
Precise measurement of the W-boson mass with the CDF II detector
- Author
- Aaltonen T.
- Abbaneo D
- Adzic P
- Aguilar-Benitez M
- Ahmad M
- Ahmed I
- Albajar C
- Allfrey P
- Almeida N
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Andreev V
- Andreev Y
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Arce P
- Arisawa T.
- Artikov A.
- Asaadi J.
- Asghar MI
- Ashmanskas W.
- Auerbach B.
- Auffray E
- Aurisano A.
- Auzinger G
- Azarkin M
- Azfar F.
- Azhgirey I
- Badgett W.
- Bae T.
- Baillon P
- Ball AH
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barney D
- Barria P.
- Bartos P.
- Battilana C
- Bauce M.
- Bedeschi F.
- Bedoya CF
- Beecher D.
- Behari S.
- Bell AJ
- Bellettini G.
- Bellinger J.
- Belotelov I
- Benedetti D
- Benjamin D.
- Beretvas A.
- Bernet C
- Bhatti A.
- Bialas W
- Bilinskas MJ
- Binkley M.
- Bisello D.
- Bitioukov S
- Bizjak I.
- Bland K. R.
- Bloch P
- Blumenfeld B.
- Bocci A
- Bocci A.
- Bodek A.
- Bolognesi S
- Bondar N
- Boos E
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Breuker H
- Brigliadori L.
- Bromberg C.
- Brona G
- Brucken E.
- Budagov J.
- Budd H. S.
- Bunin P
- Bunkowski K
- Burelo ED
- Burkett K.
- Busetto G.
- Bussey P.
- Butler PH
- Buzatu A.
- Caballero IG
- Cabrillo IJ
- Calamba A.
- Calancha C.
- Calderon A
- Calvo E
- Camarda S.
- Campanelli M.
- Campbell M.
- Campderros JD
- Camporesi T
- Canelli F.
- Cano E
- Carls B.
- Carlsmith D.
- Carosi R.
- Carrillo S.
- Carron S.
- Casal B.
- Casarsa M.
- Castro A.
- Catastini P.
- Cauz D.
- Cavaliere V.
- Cavalli-Sforza M.
- Cepeda M
- Cerminara G
- Cerrada M
- Cerri A.
- Cerrito L.
- Chen Y. C.
- Chertok M.
- Chiarelli G.
- Chlachidze G.
- Chlebana F.
- Cho K.
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chokheli D.
- Christiansen T
- Chuang SH
- Chung W. H.
- Chung Y. S.
- Cifuentes JAB
- Ciocci M. A.
- Clark A.
- Clarke C.
- Codispoti G
- Colino N
- Compostella G.
- Convery M. E.
- Conway J.
- Corbo M.
- Cordelli M.
- Cortabitarte RV
- Cox C. A.
- Cox D. J.
- Crescioli F.
- Cuevas J
- Cuevas J.
- Culbertson R.
- Cure B
- Cwiok M
- d'Ascenzo N.
- D'Enterria D
- d'Errico M.
- D'Onofrio M.
- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
- David A
- de Barbaro P.
- De La Cruz B
- De Roeck A
- de Troconiz JF
- Dell'Orso M
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Djordjevic M
- Doesburg R
- Dominik W
- Donati S.
- Dong P.
- Dorigo M.
- Dorigo T.
- Doroba K
- Dremin I
- Dubinin M
- Dudko L
- Ebina K.
- Elagin A.
- Elliott-Peisert A
- Eppig A.
- Epshteyn V
- Erbacher R.
- Errede S.
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- Ershov A
- Eusebi R.
- Faccioli P
- Farrington S.
- Feindt M.
- Felcini M
- Fernandez J. P.
- Fernandez M
- Fernandez P. Movilla
- Ferrando A
- Field R.
- Finger M
- Finger M
- Flanagan G.
- Flix J
- Folgueras S
- Forrest R.
- Fouz MC
- Frank M. J.
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- Frueboes T
- Funakoshi Y.
- Funk W
- Furic I.
- Gaddi A
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- Garcia JMV
- Garcia-Abia P
- Garfinkel A. F.
- Garosi P.
- Garrido RGR
- Gavrilov V
- Gennai S
- Georgiou G
- Gerberich H.
- Gerchtein E.
- Gerwig H
- Giagu S.
- Giakoumopoulou V.
- Giannetti P.
- Gibson K.
- Gigi D
- Gill K
- Ginsburg C. M.
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- Giurgiu G.
- Glagolev V.
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- Gninenko S
- Goh J
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- Golossanov A.
- Golovtsov V
- Golubev N
- Golutvin I
- Gomez G
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- Goncharov M.
- Gonzalez O.
- Gorelov I.
- Gorski M
- Goshaw A. T.
- Goulianos K.
- Gouzevitch M
- Govoni P
- Gowdy S
- Gribushin A
- Grigelionis I
- Grinstein S.
- Grishin V
- Griso S. Pagan
- Grosso-Pilcher C.
- Group R. C.
- Guiducci L
- Hahn S. R.
- Halkiadakis E.
- Hamaguchi A.
- Han J. Y.
- Hansen M
- Happacher F.
- Hara K.
- Hare D.
- Hare M.
- Harr R. F.
- Harvey J
- Hatakeyama K.
- Hays C.
- Heck M.
- Hegeman J
- Hegner B
- Heinrich J.
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- Hernandez AS
- Hernandez JM
- Herndon M.
- Hesketh G
- Hewamanage S.
- Hocker A.
- Hoffmann HF
- Hong B
- Honma A
- Hoorani HR
- Hopkins W.
- Horn D.
- Hou S.
- Hughes R. E.
- Hurwitz M.
- Husemann U.
- Hussain N.
- Hussein M.
- Huston J.
- Ibarguen HAS
- Iglesias LL
- Innocente V
- Introzzi G.
- Iori M.
- Ivanov A.
- Ivanov Y
- James E.
- Jang D.
- Janot P
- Janulis M
- Jayatilaka B.
- Jeon E. J.
- Jimeno AR
- Jindariani S.
- Jo M
- Jones M.
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- Jorda C
- Josa MI
- Jun S. Y.
- Junk T. R.
- Kachanov V
- Kaftanov V
- Kalinowski A
- Kamenev A
- Kamon T.
- Kang S
- Karavakis E
- Karchin P. E.
- Karjavin V
- Kasmi A.
- Kato Y.
- Kazana M
- Ketchum W.
- Keung J.
- Khan WA
- Khotilovich V.
- Khurshid T
- Kilminster B.
- Kim D. H.
- Kim H
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- Kim H. S.
- Kim J. E.
- Kim JH
- Kim M. J.
- Kim S. B.
- Kim S. H.
- Kim TJ
- Kim V
- Kim Y. J.
- Kim Y. K.
- Kimura N.
- Kirakosyan M
- Kirby M.
- Kirsanov M
- Klimenko S.
- Knoepfel K.
- Kodolova O
- Kondo K.
- Konecki M
- Kong D. J.
- Konigsberg J.
- Konstantinov D
- Korablev A
- Kossov M
- Kotwal A. V.
- Kozlov G
- Krasnikov N
- Kreps M.
- Krofcheck D
- Krokhotin A
- Krolikowski J
- Kroll J.
- Krop D.
- Krpic D
- Kruse M.
- Krutelyov V.
- Krychkine V
- Kuhr T.
- Kurata M.
- Kwang S.
- Laasanen A. T.
- Lami S.
- Lammel S.
- Lancaster M.
- Lander R. L.
- Lanev A
- Lannon K.
- Lath A.
- Latino G.
- LeCompte T.
- Lecoq P
- Lee E.
- Lee H. S.
- Lee J
- Lee J. S.
- Lee KS
- Lee S
- Lee S. W.
- Leo S.
- Leone S.
- Leonidopoulos C
- Levchenko P
- Lewis J. D.
- Limosani A.
- Lin C. -J.
- Linares EC
- Lindgren M.
- Lipeles E.
- Lister A.
- Litvintsev D. O.
- Liu C.
- Liu H.
- Liu Q.
- Liu T.
- Llatas MC
- Lockwitz S.
- Loginov A.
- Lokhtin I
- Lopez OG
- Lopez SG
- Lopez-Fernandez R
- Lourenco C
- Lucchesi D.
- Lueck J.
- Lujan P.
- Lukens P.
- Lungu G.
- Lychkovskaya N
- Lys J.
- Lysak R.
- Macpherson A
- Madrak R.
- Maeshima K.
- Maestre JA
- Maestro P.
- Maki T
- Malgeri L
- Malik S.
- Manca G.
- Mannelli M
- Manousakis-Katsikakis A.
- Marco J
- Marco R
- Margaroli F.
- Marino C.
- Martinez M.
- Martins P
- Martisiute D
- Masetti L
- Mastrandrea P.
- Matera K.
- Matorras F
- Mattson M. E.
- Matveev V
- Mazzacane A.
- Mazzanti P.
- McFarland K. S.
- McIntyre P.
- McNulty R.
- Mehta A.
- Mehtala P.
- Meijers F
- Menendez JF
- Merino G
- Mersi S
- Meschi E
- Mesropian C.
- Miao T.
- Mietlicki D.
- Milosevic J
- Mitra A.
- Miyake H.
- Moed S.
- Moggi N.
- Moisenz P
- Mondragon M. N.
- Moon C. S.
- Moon DH
- Moore R.
- Morello M. J.
- Moreno SC
- Morlock J.
- Moser R
- Mozer MU
- Mukherjee A.
- Mulders M
- Muller Th.
- Murat P.
- Murzin V
- Musella P
- Mussini M.
- Nachtman J.
- Nagai Y.
- Naganoma J.
- Nakano I.
- Napier A.
- Nawrocki K
- Nayak A
- Nesvold E
- Nett J.
- Neu C.
- Neubauer M. S.
- Nguyen M
- Nielsen J.
- Nodulman L.
- Noh S. Y.
- Norniella O.
- Nurse E.
- Oakes L.
- Obraztsov S
- Oh S. H.
- Oh Y. D.
- Oksuzian I.
- Okusawa T.
- Orava R.
- Oreshkin V
- Orimoto T
- Orsini L
- Ortolan L.
- Pagliarone C.
- Palencia E.
- Palichik V
- Papadimitriou V.
- Paramonov A. A.
- Pardo PL
- Pardos CD
- Park C
- Park IC
- Park S
- Park SK
- Parracho PGF
- Pashenkov A
- Patrick J.
- Pauletta G.
- Paulini M.
- Paus C.
- Pelayo JP
- Pellett D. E.
- Penzo A.
- Perelygin V
- Perez E
- Perez JAC
- Petrilli A
- Petrov P
- Petrov V
- Petrushanko S
- Pfeiffer A
- Phillips T. J.
- Piacentino G.
- Pianori E.
- Pierini M
- Pilot J.
- Pimia M
- Pineda AM
- Pitts K.
- Plager C.
- Polese G
- Pondrom L.
- Poprocki S.
- Potamianos K.
- Pranko A.
- Prokoshin F.
- Ptohos F.
- Punzi G.
- Qazi S
- Racz A
- Rahaman A.
- Ramakrishnan V.
- Ramos FD
- Ramos JPF
- Ranjan N.
- Redondo I
- Redondo I.
- Renton P.
- Rescigno M.
- Reyes-Santos MA
- Rhee HB
- Ribeiro PQ
- Riddick T.
- Rimondi F.
- Ristori L.
- Rivero CM
- Robson A.
- Rodrigo T
- Rodrigo T.
- Rodriguez T.
- Rogers E.
- Rolandi G
- Rolli S.
- Romanowska-Rybinska K
- Romero L
- Rommerskirchen T
- Roser R.
- Rovelli
- Ruffini F.
- Ruiz A.
- Rusakov SV
- Russ J.
- Rusu V.
- Ryu G
- Ryutin R
- Sabonis T
- Safonov A.
- Safronov G
- Sakumoto W. K.
- Sakurai Y.
- Sanchez FJM
- Sanchez JG
- Santaolalla J
- Santi L.
- Sanudo MS
- Sarycheva L
- Sato K.
- Saveliev V.
- Savoy-Navarro A.
- Savrin V
- Schlabach P.
- Schmidt A.
- Schmidt E. E.
- Schwarz T.
- Scodellaro L
- Scodellaro L.
- Scribano A.
- Scuri F.
- Seidel S.
- Seixas J
- Seiya Y.
- Semenov A.
- Semenov S
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- Sforza F.
- Shalhout S. Z.
- Shears T.
- Shekhar R.
- Shepard P. F.
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- Shin S
- Shmatov S
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- Silva P
- Silverwood H
- Sim KS
- Simonenko A.
- Sinervo P.
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- Smirnov I
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- Sobol A
- Soha A.
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- Stolin V
- Strologas J.
- Strycker G. L.
- Sudo Y.
- Sukhanov A.
- Sulimov V
- Sun S.
- Suslov I.
- Szleper M
- Takemasa K.
- Takeuchi Y.
- Tang J.
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- Tollefson K.
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- Trovato M.
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- Uzunian A
- Valdez HC
- Valencia FV
- Varela J
- Varganov A.
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- Vila I
- Vila I.
- Vilar R.
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- Vinogradov A
- Virto AL
- Vizan J.
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- Vorobyev A
- Wagner P.
- Wagner R. L.
- Wakisaka T.
- Wallny R.
- Wallny R.
- Wang S. M.
- Wang S. M.
- Warburton A.
- Warburton A.
- Waters D.
- Waters D.
- Weinberger M.
- Wester W. C. III
- Wester W. C. III
- Whitehouse B.
- Whiteson D.
- Whiteson D.
- Wick F.
- Wick F.
- Wicklund A. B.
- Wicklund A. B.
- Wicklund E.
- Wicklund E.
- Wilbur S.
- Wilbur S.
- Williams H. H.
- Williams H. H.
- Willmott C
- Wilson J. S.
- Wilson J. S.
- Wilson P.
- Wilson P.
- Winer B. L.
- Winer B. L.
- Wittich P.
- Wittich P.
- Wohri HK
- Wolbers S.
- Wolbers S.
- Wolfe H.
- Wolfe H.
- Wright T.
- Wright T.
- Wrochna G
- Wu X.
- Wu X.
- Wu Z.
- Wu Z.
- Yamamoto K.
- Yamamoto K.
- Yamaoka J.
- Yamato D.
- Yang T.
- Yang T.
- Yang U. K.
- Yang U. K.
- Yang Y. C.
- Yang Y. C.
- Yao W. -M.
- Yao W. -M.
- Yeh G. P.
- Yeh G. P.
- Yi K.
- Yi K.
- Yoh J.
- Yoh J.
- Yorita K.
- Yorita K.
- Yoshida T.
- Yoshida T.
- Yu G. B.
- Yu G. B.
- Yu I
- Yu I.
- Yu I.
- Yu S. S.
- Yu S. S.
- Yun J. C.
- Yun J. C.
- Zalewski R
- Zanetti A.
- Zanetti A.
- Zarubin A
- Zeng Y.
- Zeng Y.
- Zhokin A
- Zhou C.
- Zucchelli S..
- Zucchelli S..ng S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We have measured the W-boson mass MW using data corresponding to 2.2/fb of
integrated luminosity collected in proton-antiproton collisions at 1.96 TeV
with the CDF II detector at the Fermilab Tevatron collider. Samples consisting
of 470126 W->enu candidates and 624708 W->munu candidates yield the measurement
MW = 80387 +- 12 (stat) +- 15 (syst) = 80387 +- 19 MeV. This is the most
precise measurement of the W-boson mass to date and significantly exceeds the
precision of all previous measurements combined
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anielski J
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche L
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bach M
- Badala A
- Baek YW
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Bari DD
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barros GOVD
- Barroso VC
- Bartke J
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bjelogrlic S
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
- Bornec YL
- Bose S
- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
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- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camerini P
- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
- Catanescu V
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- Cervantes IM
- Chang B
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- Chattopadhyay S
- Chattopadhyay S
- Chawla I
- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chinellato DD
- Chochula P
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Coccetti F
- Colamaria F
- Colella D
- Collaboration ALICE
- Constantin P
- Contin G
- Contreras JG
- Corchero MAD
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cuveland JD
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash A
- Dash S
- Davalos AM
- De S
- Delagrange H
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- Demanov V
- Denes E
- Deppman A
- Diaz AC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
- Dubey AK
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Engel H
- Erasmo GD
- Erdal HA
- Espagnon B
- Estienne M
- Esumi S
- Evans D
- Eyyubova G
- Fabris D
- Faivre J
- Falchieri D
- Falco AD
- Fantoni A
- Fasel M
- Fearick R
- Fedunov A
- Fehlker D
- Feldkamp L
- Felea D
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo MAS
- Filchagin S
- Filho EPDO
- Filho NC
- Finogeev D
- Fionda FM
- Fiore EM
- Floris M
- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
- Fuchs U
- Furget C
- Gaardhoje JJ
- Gagliardi M
- Gago A
- Gallio M
- Gangadharan DR
- Ganoti P
- Garabatos C
- Garcia GM
- Garcia-Solis E
- Garishvili I
- Gerhard J
- Germain M
- Geuna C
- Gheata A
- Gheata M
- Ghidini B
- Ghosh P
- Gianotti P
- Giglio CD
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- Zavada P
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- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zoeller MH
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Civinini C
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- CMS Collaboration
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- Cripps N
- Cuevas J
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- Cumalat JP
- Cuplov V
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- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
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- Das S
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- Daubie E
- David A
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- de Barbaro P
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- de Cassagnac RG
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- de Monchenault GH
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- Eugster J
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
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- Zhu RY
- Zhukov V
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- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Adiguzel A
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- Afanasiev S
- Agostino L
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Abbaneo D
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- Xaplanteris L.
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- Zachariadou A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Compressed representation of a partially defined integer function over multiple arguments
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
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- Sguazzoni G
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- Shoaib M
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- Ujvari B
- Ulmer KA
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- Ungaro D
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- Uzunian A
- Vaandering EW
- Valls N
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- Villella I
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- Virto AL
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- Volkov A
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- Volodko A
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- Wehrli L
- Weiler T
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- Wickramage N
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- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
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- Wood JS
- Worm SD
- Wright D
- Wrochna G
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
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