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Projected WIMP sensitivity of the LUX-ZEPLIN dark matter experiment
- Author
- Akerib DS
- Akerlof CW
- Alsum SK
- AraĂşjo HM
- Arthurs M
- Bai X
- Bailey AJ
- Balajthy J
- Balashov S
- Bauer D
- Belle J
- Beltrame P
- Benson T
- Bernard EP
- Biesiadzinski TP
- Boast KE
- Boxer B
- BrĂĄs P
- Buckley JH
- Bugaev VV
- Burdin S
- Busenitz JK
- Carels C
- Carlsmith DL
- Carlson B
- Carmona-Benitez MC
- Chan C
- Cherwinka JJ
- Cole A
- Cottle A
- Craddock WW
- Currie A
- Cutter JE
- Dahl CE
- De Viveiros L
- Dobi A
- Dobson JEY
- Druszkiewicz E
- Edberg TK
- Edwards WR
- Fan A
- Fayer S
- Fiorucci S
- Fruth T
- Gaitskell RJ
- Genovesi J
- Ghag C
- Gilchriese MGD
- Hall CR
- Hans S
- Hanzel K
- Haselschwardt SJ
- Hertel SA
- Hillbrand S
- Hjemfelt C
- Hoff MD
- Hor JYK
- Huang DQ
- Ignarra CM
- Ji W
- Kaboth AC
- Kamdin K
- Keefner J
- Khaitan D
- Khazov A
- Kim YD
- Kocher CD
- Korolkova EV
- Kraus H
- Krebs HJ
- Kreczko L
- Krikler B
- Kudryavtsev VA
- Kyre S
- Lee J
- Lenardo BG
- Leonard DS
- Lesko KT
- Levy C
- Li J
- Liao FT
- Liao J
- Lin J
- Lindote A
- Linehan R
- Lippincott WH
- Liu X
- Lopes MI
- Lorenzon W
- Luitz S
- Lyle JM
- LĂłpez Paredes B
- Majewski P
- Manalaysay A
- Mannino RL
- Maupin C
- McKinsey DN
- Meng Y
- Miller EH
- Van Der Grinten MGD
- Publication venue
- eScholarship, University of California
- Publication date
- 01/03/2020
- Field of study
LUX-ZEPLIN (LZ) is a next-generation dark matter direct detection experiment that will operate 4850 feet underground at the Sanford Underground Research Facility (SURF) in Lead, South Dakota, USA. Using a two-phase xenon detector with an active mass of 7 tonnes, LZ will search primarily for low-energy interactions with weakly interacting massive particles (WIMPs), which are hypothesized to make up the dark matter in our galactic halo. In this paper, the projected WIMP sensitivity of LZ is presented based on the latest background estimates and simulations of the detector. For a 1000 live day run using a 5.6-tonne fiducial mass, LZ is projected to exclude at 90% confidence level spin-independent WIMP-nucleon cross sections above 1.4Ă10-48 cm2 for a 40 GeV/c2 mass WIMP. Additionally, a 5Ď discovery potential is projected, reaching cross sections below the exclusion limits of recent experiments. For spin-dependent WIMP-neutron(-proton) scattering, a sensitivity of 2.3Ă10-43 cm2 (7.1Ă10-42 cm2) for a 40 GeV/c2 mass WIMP is expected. With underground installation well underway, LZ is on track for commissioning at SURF in 2020
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
- Author
- Aaltonen T
- Ahmed S
- Alam MS
- Albert J
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Azzolini V
- Badgett W
- Bae T
- Band HR
- Banerjee S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bedeschi F
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Bhuyan B
- Bianchi F
- Bisello D
- Bizjak I
- Bland KR
- Blumenfeld B
- Bocci A
- Bodek A
- Bomben M
- Bortoletto D
- Bosisio L
- Boudreau J
- Boveia A
- Brigliadori L
- Bromberg C
- Brucken E
- Budagov J
- Budd HS
- Bula R
- Burchat PR
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Calamba A
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Cartaro C
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen X
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chung WH
- Chung YS
- Ciocci MA
- Clark A
- Clarke C
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cossutti F
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- Datta M
- de Barbaro P
- Dell'Orso M
- Della Ricca G
- Demortier L
- Deninno M
- Devoto F
- Di Canto A
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo M
- Dorigo T
- Ebina K
- Eckmann R
- Edwards AJ
- Elagin A
- Eppig A
- Erbacher R
- Ernst JA
- Errede S
- Ershaidat N
- Eusebi R
- Farrington S
- Feindt M
- Fernandez JP
- Fernandez PM
- Field R
- Flanagan G
- Flood KT
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Funakoshi Y
- Furic I
- Gallinaro M
- Gallo F
- Gamba D
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldin D
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Hamano K
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Harrison PF
- Hatakeyama K
- Hays C
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- Heinrich J
- Herndon M
- Hewamanage S
- Hocker A
- Hollar JJ
- Hopkins W
- Horn D
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- Hurwitz M
- Husemann U
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- Izen JM
- Jain V
- James E
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- Jayatilaka B
- Jeon EJ
- Jindariani S
- Jones M
- Joo KK
- Jun SY
- Junk TR
- Kamon T
- Karchin PE
- Kasmi A
- Kato Y
- Ketchum W
- Keung J
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- Kilminster B
- Kim DH
- Kim HS
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- Kim SH
- Kim YJ
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- Kirby M
- Klimenko S
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- Kocian ML
- Kondo K
- Kong DJ
- Konigsberg J
- Kotwal AV
- Kowalewski R
- Kreps M
- Krishnamurthy M
- Kroll J
- Krop D
- Kruse M
- Krutelyov V
- Kuhr T
- Kurata M
- Kutter PE
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lanceri L
- Lander RL
- Lannon K
- Lath A
- Latham TE
- Latino G
- LeCompte T
- Lee E
- Lee HS
- Lee JS
- Lee SW
- Leith DWGS
- Leo S
- Leone S
- Lewis JD
- Li S
- Limosani A
- Lin CJ
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu H
- Liu Q
- Liu T
- Lockwitz S
- Loginov A
- Lopez-March N
- Lou XC
- Lucchesi D
- Lueck J
- Luitz S
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- Luth V
- Lynch HL
- Lys J
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- Madrak R
- Maeshima K
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- Margaroli F
- Marino C
- Marsiske H
- Martinez M
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- Mastrandrea P
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- Mattson ME
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- McFarland KS
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- Mesropian C
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- Mietlicki D
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- Moggi N
- Mohanty GB
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Mukherjee A
- Muller DR
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- Nakano I
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- Oksuzian I
- Okusawa T
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- Rahaman A
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- Redondo I
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- Rodrigo T
- Rodriguez T
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- Roodman A
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- Sakumoto WK
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- Schindler RH
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- Scribano A
- Scuri F
- Seidel S
- Seiya Y
- Semenov A
- Sforza F
- Shalhout SZ
- Shears T
- Shepard PF
- Shimojima M
- Shochet M
- Shreyber-Tecker I
- Simonenko A
- Sinervo P
- Sliwa K
- Smith JR
- Snider FD
- Snyder A
- Sobie RJ
- Soha A
- Song H
- Sorin V
- Spanier SM
- Squillacioti P
- St Denis R
- Stancari M
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Strycker GL
- Su D
- Sudo Y
- Sukhanov A
- Sullivan MK
- Suslov I
- Suzuki K
- Swain SK
- Takemasa K
- Takeuchi Y
- Tang J
- Tecchio M
- Teng PK
- Thom J
- Thome J
- Thompson GA
- Thompson JM
- Thomson E
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Totaro P
- Trovato M
- Ukegawa F
- Uozumi S
- Va'vra J
- Varganov A
- Vazquez F
- Velev G
- Vellidis C
- Vidal M
- Vila I
- Vilar R
- Vitale L
- Vizan J
- Vogel M
- Volpi G
- Wagner AP
- Wagner P
- Wagner RL
- Wakisaka T
- Wallny R
- Wang SM
- Wappler FR
- Warburton A
- Waters D
- Weaver M
- Wester WC
- Whiteson D
- Wick F
- Wicklund AB
- Wicklund E
- Wilbur S
- Wilden L
- Williams HH
- Wilson JS
- Wilson P
- Winer BL
- Wisniewski WJ
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wright DH
- Wright T
- Wu SL
- Wu X
- Wu Z
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Ye S
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zain SB
- Zanetti A
- Zeng Y
- Zhou C
- Ziegler V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of time-integrated CP-violation asymmetries in the
resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II
data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar
collisions at sqrt(s) = 1.96 TeV. The charm mesons used in this analysis come
from D*+(2010) to D0 pi+ and D*-(2010) to D0bar pi-, where the production
flavor of the charm meson is determined by the charge of the accompanying pion.
We apply a Dalitz-amplitude analysis for the description of the dynamic decay
structure and use two complementary approaches, namely a full Dalitz-plot fit
employing the isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D0bar Dalitz plots. We
find no CP-violation effects and measure an asymmetry of ACP = (-0.05 +- 0.57
(stat) +- 0.54 (syst))% for the overall integrated CP-violation asymmetry,
consistent with the standard model prediction.Comment: 15 page
Diffractive Dijet Production at sqrt(s)=630 and 1800 GeV at the Fermilab Tevatron
- Author
- Acosta D
- Affolder T
- Akimoto H
- Albrow MG
- Amaral P
- Ambrose D
- Amidei D
- Anikeev K
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Bailey S
- Band HR
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berge JP
- Berryhill J
- Bhatti A
- Bianchi F
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bolla G
- Bona M
- Bonushkin Y
- Borras K
- Bortoletto D
- Bosisio L
- Boudreau J
- Brandl A
- Bromberg C
- Brown CM
- Brozovic M
- Brubaker E
- Bruner N
- Buckley-Geer E
- Budagov J
- Budd HS
- Bugg W
- Burchat PR
- Burkett K
- Busetto G
- Byon-Wagner A
- Byrum KL
- Cabrera S
- Calafiura P
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Charles E
- Chen C
- Chen YC
- Cheng CH
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung JY
- Chung YS
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- Clark AG
- Cohn H
- Colijn AP
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- Cordelli M
- Coward DH
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- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
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- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Della Ricca G
- Demers S
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- Derwent PF
- Devlin T
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- Dorigo T
- Dunwoodie W
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- Eichenbaum AM
- Einsweiler K
- Elias JE
- Engels E
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- Errede S
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- Pagliarone C
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- St Denis R
- Steele J
- Stefanini A
- Stelzer J
- Strologas J
- Strumia F
- Stuart D
- Su D
- Sullivan MK
- Sumorok K
- Suzuki T
- Takano T
- Takashima R
- Takikawa K
- Tamburello P
- Tanaka HA
- Tanaka M
- Tannenbaum B
- Tecchio M
- Teng PK
- Terashi K
- Tesarek RJ
- Tether S
- Thompson AS
- Thomson E
- Thurman-Keup R
- Tipton P
- Tkaczyk S
- Toback D
- Tollefson K
- Tollestrup A
- Tonelli D
- Toyoda H
- Trischuk W
- Tseng J
- Tsybychev D
- Turini N
- Ukegawa F
- Va'vra J
- Vaiciulis T
- Valls J
- van den Brink S
- Vejcik S
- Velev G
- Veramendi G
- Vidal R
- Vila I
- Vilar R
- Volobouev I
- von der Mey M
- von Wimmersperg-Toeller JH
- Vuagnin G
- Vucinic D
- Wagner RG
- Wagner RL
- Wagner SR
- Wallace NB
- Wan Z
- Wang C
- Wang MJ
- Wang SM
- Ward B
- Waschke S
- Watanabe T
- Waters D
- Watts T
- Webb R
- Weinstein AJR
- Wenzel H
- Wester WC
- Wicklund AB
- Wicklund E
- Wilkes T
- Williams HH
- Wilson P
- Winer BL
- Winn D
- Wisniewski WJ
- Wolbers S
- Wolinski D
- Wolinski J
- Wolinski S
- Worm S
- Wright DH
- Wu SL
- Wu X
- Wyss J
- Yao W
- Yeh GP
- Yeh P
- Yoh J
- Yosef C
- Yoshida T
- Young CC
- Yu I
- Yu S
- Yu Z
- Yu Z
- Zanetti A
- Zetti F
- Zucchelli S DP
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 17/09/2001
- Field of study
We report a measurement of the diffractive structure function FjjDâ of
the antiproton obtained from a study of dijet events produced in association
with a leading antiproton in pËâp collisions at sâ=630 GeV at the
Fermilab Tevatron. The ratio of FjjDâ at sâ=630 GeV to FjjDâ
obtained from a similar measurement at sâ=1800 GeV is compared with
expectations from QCD factorization and with theoretical predictions. We also
report a measurement of the Ξ (x-Pomeron) and β (x of parton in
Pomeron) dependence of FjjDâ at sâ=1800 GeV. In the region
0.035<Ξ<0.095, âŁtâŁ<1 GeV2 and β<0.5, FjjDâ(β,Ξ) is
found to be of the form βâ1.0Âą0.1Ξâ0.9Âą0.1, which obeys
β-Ξ factorization.Comment: LaTeX, 9 pages, Submitted to Phys. Rev. Letter
A Study of B0 -> J/psi K(*)0 pi+ pi- Decays with the Collider Detector at Fermilab
- Author
- Affolder T
- Akimoto H
- Akopian A
- Albrow MG
- Amaral P
- Amidei D
- Anikeev K
- Anthony PL
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Aston D
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Bailey S
- Baird K
- Band HR
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berge JP
- Berryhill J
- Bhatti A
- Bianchi F
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom E
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bokhari W
- Bolla G
- Bona M
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Boyarski AM
- Brandl A
- Bromberg C
- Brown CM
- Brozovic M
- Brubaker E
- Bruner N
- Buckley-Geer E
- Budagov J
- Budd HS
- Bugg W
- Bulos F
- Burchat PR
- Burkett K
- Busetto G
- Byon-Wagner A
- Byrum KL
- Cabrera S
- Calafiura P
- Calderini G
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Charles E
- Chen C
- Chen YC
- Cheng CH
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung YS
- Ciobanu CI
- Clark AG
- Claus R
- Cohn H
- Colijn AP
- Connolly A
- Convery MR
- Conway J
- Cordelli M
- Coupal DP
- Coward DH
- Cranshaw J
- Cropp R
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- de Barbaro P
- De Silva A
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demortier L
- Deninno M
- Derwent PF
- Devlin T
- Di Girolamo B
- Di Lodovico F
- Dittmann JR
- Dominguez A
- Donati S
- Done J
- Dorfan J
- Dorigo T
- Doser M
- Dunwoodie W
- Eddy N
- Eichenbaum AM
- Einsweiler K
- Elias JE
- Engels E
- Erbacher R
- Errede D
- Errede S
- Fan Q
- Fang HC
- Feild RG
- Fernandez JP
- Ferretti C
- Field RC
- Field RD
- Fiori I
- Flaugher B
- Foster GW
- Franklin M
- Freeman J
- Friedman J
- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gamba D
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Giannetti P
- Giromini P
- Glagolev V
- Glanzman T
- Glenzinski D
- Godfrey L
- Gold M
- Goldstein J
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Gowdy SJ
- Green C
- Grim G
- Gris P
- Groer L
- Grosso P
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
- Hahn SR
- Hall C
- Handa T
- Handler R
- Hao W
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
- Henderson R
- Herndon M
- Hill C
- Himel T
- Hoffman KD
- Holck C
- Hollebeek R
- Holloway L
- Hu H
- Huffer ME
- Huffman BT
- Hughes R
- Huston J
- Huth J
- Ikeda H
- Incandela J
- Innes WR
- Introzzi G
- Iwai J
- Iwata Y
- Izen JM
- James E
- Jessop CP
- Johnson JR
- Jones M
- Joshi U
- Kambara H
- Kamon T
- Kaneko T
- Karr K
- Kasha H
- Kato Y
- Keaffaber TA
- Kelley K
- Kelly M
- Kelsey MH
- Kennedy RD
- Kephart R
- Khazins D
- Kikuchi T
- Kilminster B
- Kim BJ
- Kim DH
- Kim HS
- Kim MJ
- Kim P
- Kim SB
- Kim SH
- Kim YK
- Kirby M
- Kirk M
- Kirkby D
- Kirsch L
- Kitayama I
- Klimenko S
- Kocian ML
- Koehn P
- Kondo K
- Konigsberg J
- Kordich TMB
- Korn A
- Korytov A
- Kovacs E
- Kowalewski R
- Kroll J
- Kruse M
- Kuhlmann SE
- Kurino K
- Kuwabara T
- Laasanen AT
- Lai N
- Lami S
- Lammel S
- Lancaster J
- Lancaster M
- Lanceri L
- Lander R
- Langenegger U
- Lath A
- Latino G
- LeCompte T
- Lee AM
- Lee K
- Leith DWGS
- Leone S
- Lewis JD
- Lindgren M
- Liss TM
- Litvintsev DO
- Liu JB
- Liu R
- Liu YC
- Lobban O
- Lockyer N
- Loken J
- Loreti M
- Lou XC
- Lucchesi D
- Luitz S
- Lukens P
- Lusin S
- Luth V
- Lynch HL
- Lyons L
- Lys J
- Madrak R
- Maeshima K
- Maksimovic P
- Malferrari L
- Mangano M
- Mariotti M
- Marsiske H
- Martignon G
- Martin A
- Matthews JAJ
- Mayer J
- Mazzanti P
- McFarland KS
- McIntyre P
- McKigney E
- Menguzzato M
- Menke S
- Menzione A
- Merkel P
- Mesropian C
- Messner R
- Meyer A
- Meyer TI
- Miao T
- Miller JS
- Miller R
- Minato H
- Miscetti S
- Mishina M
- Mitselmakher G
- Moffeit KC
- Moggi N
- Moore E
- Moore R
- Morita Y
- Moulik T
- Mount R
- Mukherjee A
- Mulhearn M
- Muller DR
- Muller T
- Munar A
- Murat P
- Murgia S
- Nachtman J
- Nagaslaev V
- Nahn S
- Nakada H
- Nakano I
- Neal H
- Nelson C
- Nelson T
- Neu C
- Neuberger D
- Newman-Holmes C
- Ngan CYP
- Nielsen J
- Niu H
- Nodulman L
- Nomerotski A
- O'Grady CP
- Oh SH
- Oh YD
- Ohmoto T
- Ohsugi T
- Oishi R
- Okusawa T
- Olsen J
- Orejudos W
- Pagliarone C
- Palmonari F
- Pan Y
- Panvini RS
- Paoletti R
- Papadimitriou V
- Partos D
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett D
- Perl M
- Pescara L
- Petrak S
- Phillips TJ
- Piacentino G
- Pitts KT
- Pompili A
- Pompos A
- Pondrom L
- Pope G
- Popovic M
- Prepost R
- Prokoshin F
- Proudfoot J
- Ptohos F
- Pukhov O
- Punzi G
- Quinn H
- Rakitine A
- Ratcliff BN
- Ratnikov F
- Reher D
- Reichold A
- Ribon A
- Riegler W
- Rimondi F
- Ristori L
- Riveline M
- Roat C
- Robertson SH
- Robertson WJ
- Robinson A
- Rochester LS
- Rodrigo T
- Rolli S
- Roney JM
- Roodman A
- Rosenson L
- Roser R
- Rossin R
- Rott C
- Roy A
- Ruiz A
- Safonov A
- Sakumoto WK
- Saltzberg D
- Sanchez C
- Sansoni A
- Santi L
- Sato H
- Savard P
- Schietinger T
- Schindler RH
- Schlabach P
- Schmidt EE
- Schmidt MP
- Schmitt M
- Schwiening J
- Scodellaro L
- Scott A
- Scott IJ
- Scribano A
- Segler S
- Seidel S
- Seiya Y
- Sekula SJ
- Semenov A
- Semeria F
- Serbo VV
- Shah T
- Shapiro MD
- Shepard PF
- Shibayama T
- Shimojima M
- Shochet M
- Sidoti A
- Siegrist J
- Sill A
- Sinervo P
- Singh P
- Slaughter AJ
- Sliwa K
- Smith C
- Smol A
- Snider FD
- Snyder A
- Soha A
- Solodsky A
- Spalding J
- Spanier SM
- Speer T
- Sphicas P
- Spiegel L
- Spinella F
- Spiropulu M
- St Denis R
- Steele J
- Stefanini A
- Stelzer J
- Strologas J
- Strumia F
- Stuart D
- Su D
- Sullivan MK
- Sumorok K
- Suzuki T
- Takano T
- Takashima R
- Takikawa K
- Tamburello P
- Tanaka HA
- Tanaka M
- Tannenbaum B
- Tecchio M
- Teng PK
- Terashi K
- Tesarek R
- Tether S
- Thompson AS
- Thurman-Keup R
- Tipton P
- Tkaczyk S
- Toback D
- Tollefson K
- Tollestrup A
- Tonelli D
- Toyoda H
- Trischuk W
- Tseng J
- Turcotte M
- Turini N
- Ukegawa F
- Va'vra J
- Vaiciulis T
- Valls J
- van den Brink S
- Vejcik S
- Velev G
- Veramendi G
- Vidal R
- Vila I
- Vilar R
- Volobouev I
- von der Mey M
- von Wimmerspeig-Toeller JH
- Vuagnin G
- Vucinic D
- Wagner RG
- Wagner RL
- Wagner SR
- Wallace NB
- Wan Z
- Wang C
- Wang MJ
- Ward B
- Waschke S
- Watanabe T
- Waters D
- Watts T
- Webb R
- Weidemann AW
- Weinstein AJR
- Wenzel H
- Wester WC
- Wicklund AB
- Wicklund E
- Wilkes T
- Williams HH
- Wilson P
- Winer BL
- Winn D
- Wisniewski WJ
- Wolbers S
- Wolbers S
- Wolinski D
- Wolinski D
- Wolinski J
- Wolinski J
- Wolinski S
- Wolinski S
- Worm S
- Worm S
- Wright DH
- Wu SL
- Wu X
- Wu X
- Wu X
- Wuerthwein F
- Wyss J
- Wyss J
- Wyss J
- Yang UK
- Yao W
- Yao W
- Yao W
- Yeh GP
- Yeh GP
- Yeh GP
- Yeh P
- Yeh P
- Yeh P
- Yi K
- Yoh J
- Yoh J
- Yoh J
- Yosef C
- Yosef C
- Yosef C
- Yoshida T
- Yoshida T
- Yoshida T
- Young CC
- Yu I
- Yu I
- Yu I
- Yu S
- Yu S
- Yu S
- Yu S
- Yu Z
- Yu Z
- Yu Z
- Yu Z
- Yu Z
- Yun JC
- Zanetti A
- Zanetti A
- Zanetti A
- Zanetti A
- Zanin D
- Zetti F
- Zetti F
- Zetti F
- Zetti F
- Zetti F
- Zetti Fi A
- Zobernig H
- Zucchelli S
- Zucchelli S Yu I
- Zucchelli Scchelli Sam I
- Zucchelli Sm S
- Zucchelli Snetti A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 09/08/2001
- Field of study
We report a study of the decays B0 -> J/psi K(*)0 pi+ pi-, which involve the
creation of a u u-bar or d d-bar quark pair in addition to a b-bar -> c-bar(c
s-bar) decay. The data sample consists of 110 1/pb of p p-bar collisions at
sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron
collider during 1992-1995. We measure the branching ratios to be BR(B0 -> J/psi
K*0 pi+ pi-) = (8.0 +- 2.2 +- 1.5) * 10^{-4} and BR(B0 -> J/psi K0 pi+ pi-) =
(1.1 +- 0.4 +- 0.2) * 10^{-3}. Contributions to these decays are seen from
psi(2S) K(*)0, J/psi K0 rho0, J/psi K*+ pi-, and J/psi K1(1270)
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- 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
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- 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
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
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- 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
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Yamato
- Yang
- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Cockerill DJA
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- Yilmaz Y
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- Yun JC
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- Zumerle G
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- 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
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Adiguzel A
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- Afanasiev S
- Agostino L
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- Brochero Cifuentes JA
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- Chang YW
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- Chao Y
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- Ciulli V
- Civinini C
- Claes DR
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- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Codispoti G
- Colafranceschi S
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- Cooper SI
- Cornelis T
- Correa Martins Junior M
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- Costantini S
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- Coughlan JA
- Cousins R
- Covarelli R
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
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- Da Costa EM
- Daci N
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- Dahms T
- Dallavalle GM
- Damgov J
- Dammann D
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- Das S
- Daskalakis G
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- Daubie E
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- Davies G
- de Barbaro P
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- de Cassagnac RG
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- de Fatis TT
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- De La Cruz B
- De La Cruz-Burelo E
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- De Mattia M
- de Monchenault GH
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- 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
- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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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
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
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- Acosta JG
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
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- Zang J
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- Zheng Y
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- Zhukov V
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- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- D'Agnolo RT
- D'Alessandro R
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- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
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- Das S
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- Daubie E
- David A
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- Davies G
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- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
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- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
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- de Monchenault GH
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- de Troconiz JF
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- Eugster J
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- Kharchilava A
- Khatiwada R
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- Kopecky A
- Korablev A
- Korpela A
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- Papadopoulos I
- Papageorgiou A
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- Piroue R
- Pivarski J
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polese G
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- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popescu S
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Pugliese G
- Puigh D
- Puljak I
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- Qian SJ
- Quan X
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- Radicci V
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- Razis PA
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- Redaelli N
- Redjimi R
- Redondo I
- Reeder D
- Regenfus C
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Rhee HB
- Ribeiro PQ
- Ribnik J
- Riccardi C
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- Richman J
- Rikova MI
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- Robles J
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- Rodozov M
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- Rodriguez JL
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- Roinishvili V
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- Sala L
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- Sammet J
- Sanabria JC
- Sanchez AK
- Sanchez FJ
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- Santanastasio F
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- Santocchia A
- Santoro A
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- Saoulidou N
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- Sauerland P
- Savin A
- Savrin V
- Sawley MC
- Schael S
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- Scheurer A
- Schieferdecker P
- Schilling FP
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- Schleper P
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- Schmitt M
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
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- Sheldon P
- Shen BC
- Shepherd-Themistocleous CH
- Shi X
- Shin S
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
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- Silverwood H
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- Simon S
- Simonetto F
- Simonis HJ
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- Singh JB
- Singh SP
- Singovsky A
- Sirois Y
- Siroli G
- Sirunyan AM
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- Skuja A
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- Squires M
- Srivastava AK
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- Stieger B
- Stober FM
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- Strauss J
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- Suarez RG
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- Tsang KV
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- Tuuva T
- Tuve C
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- Tzeng YM
- Ujvari B
- Ulmer KA
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- Verwilligen R
- Veszpremi V
- Vesztergombi G
- Veverka J
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- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Virto A
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
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- Volyanskyy D
- Vorobiev I
- Vorobyev A
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- Wagner P
- Wagner SR
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- Wakefield S
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- Waltenberger W
- Walzel G
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- Wehrli L
- Weinberg M
- Weinberger M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Wohri HK
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
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- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- 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
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