61 research outputs found
Dynamic temporary blood facility location-allocation during and post-disaster periods
- Author
- A Ahmadi-Javid
- A Bozorgi-Amiri
- A Ishizaka
- A Jabbarzadeh
- A Klose
- A Rahmani
- Armin Jabbarzadeh
- AY Chen
- B Balcik
- B Fahimnia
- B Zahiri
- Bharat Malhotra
- Bhuvnesh Sharma
- BL Golden
- BP Nepal
- C Kahraman
- CH Schultz
- CL Yang
- CY Lee
- D Delen
- D Ghosh
- D Skorin-Kapov
- DA Richardson
- E Rolland
- EK Burke
- EK Burke
- Erkan Celik
- F Barzinpour
- F Glover
- F Pezzella
- FS Salman
- H Abolghasemi
- H Jia
- HC An
- Ä° AkgĂźn
- I Dogan
- Ä° ErtuÄrul
- J BeliĂŤn
- J Chakrapani
- J Skorin-Kapov
- J Xu
- JA DÄąaz
- JB Sheu
- JG Klincewicz
- JM Marcelin
- JR Hess
- KL Maass
- KL Teo
- KS Al-Sultan
- KS Chin
- L Zhen
- L Ăzdamar
- LV Snyder
- LV Snyder
- M Esmaeilikia
- M Najafi
- M Ramkumar
- M Ramkumar
- M Ramkumar
- M Ramkumar
- M Rezaei-Malek
- M Sakawa
- M Sun
- M. Ramkumar
- MA Arostegui
- MR Korupolu
- MT Melo
- MT Melo
- Nachiappan Subramanian
- P Guo
- R Abounacer
- R Dubey
- R Hochreiter
- R Ramezanian
- RA Hadiguna
- RS Garfinkel
- S Cheraghi
- S Jharkharia
- S Roh
- SH Amin
- SH Stanger
- SJ Rennemo
- SY Chou
- T Cui
- T Papadopoulos
- V Ghezavati
- World Health Organization (WHO)
- World Health Organization (WHO)
- X Wang
- XT Deng
- Y Gao
- YC Huang
- Z Drezner
- Z Lu
- Z LĂź
- Ă Taillard
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 26/10/2017
- Field of study
The key objective of this study is to develop a tool (hybridization or integration of different techniques) for locating the temporary blood banks during and post-disaster conditions that could serve the hospitals with minimum response time. We have used temporary blood centers, which must be located in such a way that it is able to serve the demand of hospitals in nearby region within a shorter duration. We are locating the temporary blood centres for which we are minimizing the maximum distance with hospitals. We have used Tabu search heuristic method to calculate the optimal number of temporary blood centres considering cost components. In addition, we employ Bayesian belief network to prioritize the factors for locating the temporary blood facilities. Workability of our model and methodology is illustrated using a case study including blood centres and hospitals surrounding Jamshedpur city. Our results shows that at-least 6 temporary blood facilities are required to satisfy the demand of blood during and post-disaster periods in Jamshedpur. The results also show that that past disaster conditions, response time and convenience for access are the most important factors for locating the temporary blood facilities during and post-disaster periods
Constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quarks in the full CDF data set
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- A. aa
- A. aa
- A. aa
- A. ab
- A. aqar
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- A. az
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- A. bc
- A. bdbebf
- A. bi
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- A. fg
- A. M. bd
- A. p
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- Aaltonen
- Amerio
- Amidei
- Anastassov A. p
- Annovi A. r
- Antos
- Apollinari G. p
- Appel J. A. p
- Arisawa
- Artikov A. n
- Asaadi
- Ashmanskas W. p
- Auerbach B. b
- Aurisano
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- B. L. aj
- B. p
- Badgett W. p
- Bae
- Barbaro Galtieri
- Barnes
- Barnett B. A. x
- Barria
- Bartos
- Bauce
- Bedeschi
- Behari S. p
- Bellettini
- Bellinger
- Benjamin D. o
- Beretvas A. p
- Bhatti
- Bland K. R. e
- Blumenfeld B. x
- Bocci A. o
- Bodek
- Bortoletto
- Boudreau
- Boveia A. l
- Brigliadori
- Bromberg
- Brucken
- Budagov J. n
- Budd
- Burkett K. p
- Busetto
- Bussey P. t
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- Buzatu A. t
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- Camarda S. d
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- Canelli F. l
- Carls B. w
- Carlsmith
- Carosi
- Carrillo S. q
- Casal B. j
- Casarsa
- Castro
- Catastini P. u
- CAUZ Diego
- Cavaliere V. w
- Cerri
- Cerrito
- Chen Y. C. a
- Chertok M. h
- Chiarelli
- Chlachidze G. p
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- Chokheli D. n
- Clark A. s
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- Conway J. h
- Corbo M. p
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- Cox C. A. h
- Cox D. J. h
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- Culbertson R. p
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- D. bm
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- D. J. zbqbrbsbtbubv
- Datta M. p
- De Barbaro
- Demortier
- Deninno M. f
- Devoto
- Di Canto
- Di Ruzza
- Dittmann J. R. e
- Donati
- Dorigo
- Driutti
- E. ap
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- E. J. zbqbrbsbtbubv
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- Ebina
- Edgar
- Elagin
- Erbacher R. h
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- Esham B. w
- F. am
- F. aq
- F. aq
- F. aqar
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- F. ba
- F. bh
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- Farrington
- FernaĚndez Ramos
- Field R. q
- Flanagan G. p
- Forrest R. h
- Franklin M. u
- Freeman J. C. p
- Frisch H. l
- Funakoshi
- G. ab
- G. ae
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- Garfinkel
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- Gerberich H. w
- Gerchtein E. p
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- Giakoumopoulou V. c
- Gibson
- Ginsburg C. M. p
- Giokaris N. c
- Giromini P. r
- Glagolev V. n
- Glenzinski D. p
- Gold
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- Golossanov A. p
- Gomez Ceballos
- Gomez G. j
- Goncharov
- GonzaĚlez LoĚpez
- Gorelov
- Goshaw A. T. o
- Goulianos
- Gramellini E. f
- Grosso Pilcher
- Group
- Guimaraes Da Costa
- H. aj
- H. aw
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- H. bj
- H. H. ap
- H. S. ay
- H. S. zbqbrbsbtbubv
- H. S. zbqbrbsbtbubv
- Hahn S. R. p
- Han
- Happacher F. r
- Hara
- Hare
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- Harrington Taber
- Hatakeyama K. e
- Hays
- Heinrich
- Herndon
- Hocker A. p
- Hong
- Hopkins W. p
- Hou S. a
- Hughes
- Husemann
- Hussein
- Huston
- I. ad
- I. ah
- I. ai
- I. ak
- I. bj
- I. zbqbrbsbtbubv
- Introzzi
- Iori
- Ivanov A. h
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- J. S. af
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- J. u
- J. Y. ay
- James E. p
- Jang D. k
- Jayatilaka B. p
- Jeon
- Jindariani S. p
- Jones
- Joo
- Jun S. Y. k
- Junk T. R. p
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- K. bk
- K. K. zbqbrbsbtbubv
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- Kambeitz M. y
- Kamon
- Karchin
- Kasmi A. e
- Kato
- Ketchum W. l
- Keung
- Kilminster B. p
- Kim
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- Kim Y. K. l
- Kimura
- Kirby M. p
- Knoepfel K. p
- Kondo
- Kong
- Konigsberg J. q
- Kotwal A. V. o
- Kreps M. y
- Kroll
- Kruse M. o
- Kuhr T. y
- Kurata
- L. ac
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- L. fg
- L. paq
- Laasanen
- Lammel S. p
- Lancaster
- Lannon
- Latino
- Lee
- Lee
- Leo S. w
- Leone
- Lewis J. D. p
- Limosani A. o
- Lipeles
- Lister A. s
- Liu
- Liu
- Liu T. p
- Lockwitz
- Loginov
- LucaĚ A. r
- Lucchesi
- Lueck J. y
- Lujan
- Lukens P. p
- Lungu
- Lys
- Lysak
- M. ab
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- M. fg
- M. J. aqat
- Madrak R. p
- Maestro
- Malik
- Manca
- Manousakis Katsikakis
- Marchese L. f
- Margaroli
- Marino
- Matera K. w
- Mattson
- Mazzacane A. p
- Mazzanti P. f
- McNulty
- Mehta
- Mehtala
- Mesropian
- Miao T. p
- Mietlicki
- Mitra A. a
- Miyake
- Moed S. p
- Moggi N. f
- Moon C. S. p
- Moore R. p
- Morello
- Mukherjee A. p
- Muller T. y
- Murat P. p
- Mussini
- N. bk
- Nachtman J. p
- Nagai
- Naganoma
- Nakano
- Napier
- Nett
- Neu
- Nigmanov
- Nodulman L. b
- Noh
- Norniella O. w
- O. ad
- Oakes
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- Oh S. H. o
- Oksuzian
- Okusawa
- Orava
- Ortolan L. d
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- Pagliarone
- Palencia E. j
- Palni
- Papadimitriou V. p
- Parker
- PAULETTA Giovanni
- Paulini M. k
- Paus
- Phillips T. J. o
- Piacentino G. p
- Pianori
- Pilot J. h
- Pitts K. w
- Plager C. i
- Pondrom
- Poprocki S. p
- Potamianos
- Pranko
- Prokoshin F. n
- Ptohos F. r
- Punzi
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- R. ab
- R. af
- R. aq
- R. C. pbj
- R. E. aj
- R. F. bl
- R. mbo
- R. t
- R. vbp
- Redondo FernaĚndez
- Renton
- Rescigno
- Rimondi F. f
- Ristori
- Robson A. t
- Rodriguez
- Rolli
- Ronzani
- Roser R. p
- Rosner J. L. l
- Ruffini
- Ruiz A. j
- Russ J. k
- Rusu V. p
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- S. az
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- S. H. bh
- S. mbo
- S. Y. zbqbrbsbtbubv
- S. zbqbrbsbtbubv
- S.t. Denis
- Sakumoto
- Sakurai
- SANTI Lorenzo Gianni
- Sato
- Saveliev V. p
- Savoy Navarro
- Schlabach P. p
- Schmidt E. E. p
- Schwarz
- Scodellaro L. j
- Scuri
- Seidel
- Seiya
- Semenov A. n
- Sforza
- Shalhout S. Z. h
- Shears
- Shepard
- Shimojima
- Shochet M. l
- Shreyber Tecker
- Simonenko A. n
- Sliwa
- Smith J. R. h
- Snider F. D. p
- Song
- Sorin V. d
- Stancari M. p
- Stentz D. p
- Strologas
- Sudo
- Sukhanov A. p
- Suslov I. n
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- T. p
- T. vbp
- T. zbcbqbrbsbtbubv
- T. zbqbrbsbtbubv
- Takemasa
- Takeuchi
- Tang J. l
- Tecchio
- Teng P. K. a
- Thom J. p
- Thomson
- Thukral
- Toback
- Tokar
- Tollefson
- Tomura
- Tonelli D. p
- Torre S. r
- Torretta D. p
- Totaro
- Trovato
- U. bn
- U. K. zbqbrbsbtbubv
- Ukegawa
- Uozumi
- V. bc
- V. E. ax
- VaĚzquez F. q
- Velev G. p
- Vellidis C. p
- Vernieri
- Vidal
- Vilar R. j
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- Volpi G. r
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- Wallny R. p
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- Wicklund A. B. b
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- Wilson
- Wilson P. p
- Winer
- Wittich P. p
- Wolbers S. p
- Wolfe
- Wright
- Wu X. s
- Wu Z. e
- Y. al
- Y. al
- Y. bh
- Y. bh
- Y. bh
- Y. bk
- Y. bk
- Y. C. zbqbrbsbtbubv
- Y. D. zbqbrbsbtbubv
- Y. J. zbqbrbsbtbubv
- Yamamoto
- Yamato
- Yang
- Yang
- Yang T. p
- Yao
- Yeh G. P. p
- Yi K. p
- Yoh J. p
- Yorita
- Yoshida
- Yu
- Yu G. B. o
- Z. bc
- Zanetti
- Zeng Y. o
- Zhou C. o
- Zucchelli S. fg
- Publication venue
- Publication date
- 01/01/2015
- Field of study
A search for particles with the same mass and couplings as those of the standard model Higgs boson but different spin and parity quantum numbers is presented. We test two specific alternative Higgs boson hypotheses: a pseudoscalar Higgs boson with spin-parity JP=0- and a gravitonlike Higgs boson with JP=2+, assuming for both a mass of 125GeV/c2. We search for these exotic states produced in association with a vector boson and decaying into a bottom-antibottom quark pair. The vector boson is reconstructed through its decay into an electron or muon pair, or an electron or muon and a neutrino, or it is inferred from an imbalance in total transverse momentum. We use expected kinematic differences between events containing exotic Higgs bosons and those containing standard model Higgs bosons. The data were collected by the CDF experiment at the Tevatron proton-antiproton collider, operating at a center-of-mass energy of s=1.96TeV, and correspond to an integrated luminosity of 9.45fb-1. We exclude deviations from the predictions of the standard model with a Higgs boson of mass 125GeV/c2 at the level of 5 standard deviations, assuming signal strengths for exotic boson production equal to the prediction for the standard model Higgs boson, and set upper limits of approximately 30% relative to the standard model rate on the possible rate of production of each exotic state
Measurement of the t-channel single top quark production cross section in pp collisions at âs = 7TeV
- 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
- Afanasiev S
- 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
- 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
- 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
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
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- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
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- Banerjee S
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- Bani L
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- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
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- Barker A
- Barnes VE
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- Barney D
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- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
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- Beaudette F
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- Bellinger JN
- Belotelov I
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- Betchart B
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- Cerrada M
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- Chakaberia I
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- Chertok M
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- Chou JP
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Electroweak production of the top quark is measured for the first time in pp collisions at âs=7ââTeV, using a data set collected with the CMS detector at the LHC and corresponding to an integrated luminosity of 36ââpb-1. With an event selection optimized for t-channel production, two complementary analyses are performed. The first one exploits the special angular properties of the signal, together with background estimates from the data. The second approach uses a multivariate analysis technique to probe the compatibility with signal topology expected from electroweak top-quark production. The combined measurement of the cross section is 83.6Âą29.8(stat+syst)Âą3.3(lumi)ââpb, consistent with the standard model expectation
Indications of suppression of excited ÎĽ states in Pb-Pb collisions at âsNN = 2.76TeV
- Author
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- Zoeller MH
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- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.A comparison of the relative yields of ÎĽ resonances in the Îź+Îź- decay channel in Pb-Pb and pp collisions at a center-of-mass energy per nucleon pair of 2.76 TeV is performed with data collected with the CMS detector at the LHC. Using muons of transverse momentum above 4ââGeV/c and pseudorapidity below 2.4, the double ratio of the ÎĽ(2S) and ÎĽ(3S) excited states to the ÎĽ(1S) ground state in Pb-Pb and pp collisions, [ÎĽ(2S+3S)/ÎĽ(1S)]Pb-Pb/[ÎĽ(2S+3S)/ÎĽ(1S)]pp, is found to be 0.31-0.15+0.19(stat)Âą0.03(syst). The probability to obtain the measured value, or lower, if the true double ratio is unity, is calculated to be less than 1%
Search for same-sign top-quark pair production at root s=7 TeV and limits on flavour changing neutral currents in the top sector
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zalewski P
- Zanetti M
- Zang J
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- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
An inclusive search for same-sign top-quark pair production in pp collisions at root s = 7 TeV is performed using a data sample recorded with the CMS detector in 2010, corresponding to an integrated luminosity of 35 pb(-1). This analysis is motivated by recent studies of p (p) over bar -> t (t) over bar reporting mass-dependent forward-backward asymmetries larger than expected from the standard model. These asymmetries could be due to Flavor Changing Neutral Currents (FCNC) in the top sector induced by t -channel exchange of a massive neutral vector boson (Z'). Models with such a Z' also predict enhancement of same-sign top-pair production in pp or pp collisions. Limits are set as a function of the Z' mass and its couplings to u and t quarks. These limits disfavour the FCNC interpretation of the Tevatron results
Search for supersymmetry in events with b jets and missing transverse momentum at the LHC
- Author
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- Abbiendi G
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- 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
- Zang SL
- 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
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
A search for supersymmetry is presented using a sample of events with b jets and missing transverse momentum. The search uses a data sample of proton-proton collisions at a centre-of-mass energy of 7TeV, corresponding to an integrated luminosity of 35 pb(-1), collected with the CMS detector. A total of 0.33(-0.33)(+0.43) (stat.) +/- 0.13 (syst.) events is predicted, using control samples in the data, to arise from standard model processes, and one event is observed in the data. Upper limits are set at the 95% confidence level on the cross sections of benchmark supersymmetric models
Search for new physics with a monojet and missing transverse energy in pp collisions at âs=7 TeV
- 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
- Afanasiev S
- 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
- AldĂĄ JĂşnior 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
- 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
- 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
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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zennamo J
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed at the link below.A study of events with missing transverse energy and an energetic jet is performed using pp collision data at a center-of-mass energy of 7 TeV. The data were collected by the CMS detector at the LHC, and correspond to an integrated luminosity of 36ââpb-1. An excess of these events over standard model contributions is a signature of new physics such as large extra dimensions and unparticles. The number of observed events is in good agreement with the prediction of the standard model, and significant extension of the current limits on parameters of new physics benchmark models is achieved
Measurement of the differential cross section for isolated prompt photon production in pp collisions at 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yumiceva F
- Yun JC
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- Zalewski P
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- Zeuner WD
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Ăzbek M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
A measurement of the differential cross section for the inclusive production of isolated prompt photons in proton-proton collisions at a center-of-mass energy of 7 TeV is presented. The data sample corresponds to an integrated luminosity of 36 pb(-1) recorded by the CMS detector at the LHC. The measurement covers the pseudorapidity range vertical bar eta vertical bar < 2.5 and the transverse energy range 25 < E-T < 400 GeV, corresponding to the kinematic region 0.007 < x(T) < 0.114. Photon candidates are identified with two complementary methods, one based on photon conversions in the silicon tracker and the other on isolated energy deposits in the electromagnetic calorimeter. The measured cross section is presented as a function of E-T in four pseudorapidity regions. The next-to-leading-order perturbative QCD calculations are consistent with the measured cross section
Measurement of the inclusive jet cross section in pp collisions at âs = 7TeV
- Author
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- Cockerill DJA
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- Da Silva WLP
- Dahmes B
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- Damiao DD
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- Darmenov N
- Das S
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- Daubie E
- David A
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- Davies G
- de Barbaro P
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- de Cassagnac RG
- De Cosa A
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- de Monchenault GH
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- de Troconiz JF
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- Yilmaz S
- Yilmaz Y
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- Yohay R
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- Yoon AS
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- Yumiceva F
- Yun JC
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- Zaganidis N
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- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zeinali M
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- Zeyrek M
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- Zhang Z
- Zheng Y
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- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
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- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.The inclusive jet cross section is measured in pp collisions with a center-of-mass energy of 7 TeV at the Large Hadron Collider using the CMS experiment. The data sample corresponds to an integrated luminosity of 34ââpb-1. The measurement is made for jet transverse momenta in the range 18â1100 GeV and for absolute values of rapidity less than 3. The measured cross section extends to the highest values of jet pT ever observed and, within the experimental and theoretical uncertainties, is generally in agreement with next-to-leading-order perturbative QCD predictions
Long-range and short-range dihadron angular correlations in central PbPb collisions at âsNN=2.76 TeV
- Author
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- Eugster J
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- Fabbro B
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- Killewald P
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- Kwan S
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- Zoeller MH
- Zorbilmez C
- Zou W
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article, which can be accessed from the link below.First measurements of dihadron correlations for charged particles are presented
for central PbPb collisions at a nucleon-nucleon center-of-mass energy of 2.76TeV over a broad range in relative pseudorapidity ( ) and the full range of relative azimuthal angle ( ). The data were collected with the CMS detector, at the LHC. A broadening of the away-side ( ) azimuthal correlation is observed at all , as compared to the measurements in pp collisions. Furthermore, long-range dihadron correlations in are observed for particles with similar values. This phenomenon, also known as the \ridge",
persists up to at least j j = 4. For particles with transverse momenta (pT) of 2-4 GeV/c, the ridge is found to be most prominent when these particles are correlated with particles of pT = 2-6 GeV/c, and to be much reduced when paired with particles of pT = 10-12 GeV/c
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