212 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.
- Ershaidat N.
- 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.
- Franklin M.
- Freeman J. C.
- Frisch B
- Frueboes T
- Funakoshi Y.
- Funk W
- Furic I.
- Gaddi A
- Gallinaro M
- Gallinaro M.
- Garcia J. E.
- 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.
- Giokaris N.
- Giordano D
- Giromini P.
- Giurgiu G.
- Glagolev V.
- Glege F
- Glenzinski D.
- Gninenko S
- Goh J
- Gokieli R
- Gold M.
- Goldin D.
- Goldschmidt N.
- Golossanov A.
- Golovtsov V
- Golubev N
- Golutvin I
- Gomez G
- Gomez G.
- Gomez JP
- Gomez-Ceballos G.
- 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.
- Henderson C
- 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.
- Joo K. K.
- 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
- Kim H
- 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
- Seo E
- Seo H
- Sforza F.
- Shalhout S. Z.
- Shears T.
- Shekhar R.
- Shepard P. F.
- Shigirev A
- Shimojima M.
- Shin S
- Shmatov S
- Shochet M.
- Shreyber-Tecker I.
- Silva P
- Silverwood H
- Sim KS
- Simonenko A.
- Sinervo P.
- Slabospitsky S
- Sliwa K.
- Smirnov I
- Smirnov V
- Smith J. R.
- Snider F. D.
- Sobol A
- Soha A.
- Song H.
- Sorin V.
- Squillacioti P.
- St Denis R.
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- Stelzer B.
- Stelzer-Chilton O.
- Stentz D.
- 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.
- Tecchio M.
- Teng P. K.
- Thom J.
- Thome J.
- Thompson D. S.
- Thompson G. A.
- Thomson E.
- Toback D.
- Tokar S.
- Tollefson K.
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- Torre S.
- Torretta D.
- Totaro P.
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- Troitsky S
- Troshin S
- Trovato M.
- Tyurin N
- Ukegawa F.
- Uozumi S.
- Uvarov L
- Uzunian A
- Valdez HC
- Valencia FV
- Varela J
- Varganov A.
- Vavilov S
- Vazquez DD
- Vazquez F.
- Velev G.
- Vellidis C.
- Vidal M.
- Vila I
- Vila I.
- Vilar R.
- Villasenor-Cendejas LM
- Vinogradov A
- Virto AL
- Vizan J.
- Vlasov E
- Vogel M.
- Volkov A
- Volodko A
- Volpi G.
- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alexander J
- Aliev T
- Allfrey P
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Asaadi J
- Asghar MI
- Askew A
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avery P
- Avetisyan A
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ballin J
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
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- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauer J
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Bedoya CF
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Bell AJ
- Bell KW
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- Bellan R
- Bellinger JN
- Belotelov I
- Belyaev A
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- Bendavid J
- Bender W
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- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Bergholz M
- Beri SB
- Bernardini J
- Bernet C
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- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Besson A
- Betchart B
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
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- Bhatti A
- Bialas W
- Bian JG
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
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- Bodek A
- Bodin D
- Boeriu O
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- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondar N
- Bondu O
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- Boos E
- Borcherding F
- Borgia MA
- Bornheim A
- Borras K
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- Bortignon P
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- Bose S
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- Bostock F
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- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Broccolo G
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmuller O
- Buege V
- Buehler M
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burelo ED
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Caballero IG
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon A
- Cali IA
- Callner J
- Calvo E
- Camanzi B
- Caminada L
- Campagnari C
- Campbell A
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- Yilmaz Y
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- Ziebarth EB
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- Zorbilmez C
- Zotto P
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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 the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Chatrchyan S
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- Choudhury RK
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- Yagil A
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- Yun JC
- Yuste C
- Zabi A
- Zabolotny W
- Zachariadou A
- Zalewski P
- Zampieri A
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
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- Zheng Y
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- Zhukov V
- Zhukova V
- Ziebarth EB
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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
CMS Data Processing Workflows during an Extended Cosmic Ray Run
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anisimov A
- Antillon E
- Antipov P
- Antonelli L
- Anttila E
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arnold B
- Arora S
- Artamonov A
- Asaadi J
- Asghar MI
- Ashby S
- Askew A
- Atac M
- Atramentov O
- Auffray E
- Aurisano A
- Autermann C
- Avery P
- Avetisyan A
- Avila C
- Awan MIM
- Ayan AS
- Ayhan A
- Azhgirey I
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- Wyslouch B
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- Yohay R
- Yoo HD
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- Yun JC
- Yuste C
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- Zachariadou A
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- Zanetti M
- Zang SL
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- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
- Zhang J
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- Zhang Y
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- Zheng Y
- Zhiltsov V
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- Zhukov V
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- Publication venue
- INSTITUTE OF PHYSICS PUBLISHING
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
Aligning the CMS Muon Chambers with the Muon Alignment System during an Extended Cosmic Ray Run
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anh T. Vu
- Anisimov A
- Antillon E
- Antipov P
- Antonelli L
- Anttila E
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arnold B
- Arora S
- Artamonov A
- Asaadi J
- Asghar MI
- Ashby S
- Askew A
- Atac M
- Atramentov O
- Auffray E
- Aurisano A
- Autermann C
- Avery P
- Avetisyan A
- Avila C
- Awan MIM
- Ayan AS
- Ayhan A
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babb J
- Babucci E
- Baccaro S
- Bacchetta N
- Bacchi W
- Bachtis M
- Baden D
- Badgett W
- Baechler J
- Baer H
- Baesso P
- Baffioni S
- Bagby L
- Bagliesi G
- Bahk SY
- Bailleux D
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Baldin B
- Ball AH
- Ball G
- Ballin J
- Bally SL
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Banicz K
- Bansal S
- Banzuzi K
- Barashko V
- Barbagli G
- Barberis E
- Barbone L
- Barcala JM
- Barcellan L
- Bard R
- Bargassa P
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- Publication venue
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
The population of merging compact binaries inferred using gravitational waves through GWTC-3
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- Publication venue
- Publication date
- 23/02/2022
- Field of study
We report on the population properties of 76 compact binary mergers detected with gravitational waves below a false alarm rate of 1 per year through GWTC-3. The catalog contains three classes of binary mergers: BBH, BNS, and NSBH mergers. We infer the BNS merger rate to be between 10 Gpc−3yr−1 and 1700 Gpc−3yr−1 and the NSBH merger rate to be between 7.8 Gpc−3yr−1 and 140 Gpc−3yr−1 , assuming a constant rate density versus comoving volume and taking the union of 90% credible intervals for methods used in this work. Accounting for the BBH merger rate to evolve with redshift, we find the BBH merger rate to be between 17.9 Gpc−3yr−1 and 44 Gpc−3yr−1 at a fiducial redshift (z=0.2). We obtain a broad neutron star mass distribution extending from 1.2−0.2+0.1M⊙ to 2.0−0.3+0.3M⊙. We can confidently identify a rapid decrease in merger rate versus component mass between neutron star-like masses and black-hole-like masses, but there is no evidence that the merger rate increases again before 10 M⊙. We also find the BBH mass distribution has localized over- and under-densities relative to a power law distribution. While we continue to find the mass distribution of a binary's more massive component strongly decreases as a function of primary mass, we observe no evidence of a strongly suppressed merger rate above ∼60M⊙. The rate of BBH mergers is observed to increase with redshift at a rate proportional to (1+z)κ with κ=2.9−1.8+1.7 for z≲1. Observed black hole spins are small, with half of spin magnitudes below χi≃0.25. We observe evidence of negative aligned spins in the population, and an increase in spin magnitude for systems with more unequal mass ratio
Diving below the spin-down limit:constraints on gravitational waves from the energetic young pulsar PSR J0537-6910
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 23/12/2020
- Field of study
We present a search for continuous gravitational-wave signals from the young, energetic X-ray pulsar PSR J0537-6910 using data from the second and third observing runs of LIGO and Virgo. The search is enabled by a contemporaneous timing ephemeris obtained using NICER data. The NICER ephemeris has also been extended through 2020 October and includes three new glitches. PSR J0537-6910 has the largest spin-down luminosity of any pulsar and is highly active with regards to glitches. Analyses of its long-term and inter-glitch braking indices provided intriguing evidence that its spin-down energy budget may include gravitational-wave emission from a time-varying mass quadrupole moment. Its 62 Hz rotation frequency also puts its possible gravitational-wave emission in the most sensitive band of LIGO/Virgo detectors. Motivated by these considerations, we search for gravitational-wave emission at both once and twice the rotation frequency. We find no signal, however, and report our upper limits. Assuming a rigidly rotating triaxial star, our constraints reach below the gravitational-wave spin-down limit for this star for the first time by more than a factor of two and limit gravitational waves from the l = m = 2 mode to account for less than 14% of the spin-down energy budget. The fiducial equatorial ellipticity is limited to less than about 3 x 10⁻⁵, which is the third best constraint for any young pulsar
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