90 research outputs found
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
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- Alagoz E
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- Albayrak EA
- Albergo S
- Albrow M
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- Alexander J
- Aliev T
- Almeida N
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- Wissing C
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- Wood J
- Wood JS
- Worm SD
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- 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
- '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
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
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- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
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- 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
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- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
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- Zoeller MH
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- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Structural brain abnormalities in the common epilepsies assessed in a worldwide ENIGMA study
- Author
- 41
- 44
- 45
- 48
- 54
- Absil J
- Alhusaini S
- Altmann A
- Alvim Mkm
- Auvinen P
- Bargalló
- Bartolini E
- Bender B26
- Bergo Fpg
- Bernardes T
- Bernasconi A
- Bernasconi N
- Bernhardt Bc
- Blü
- Blackmon K
- Botí
- Braga B
- Caligiuri Me
- Calvo A
- Carlson C
- Carr Sj
- Cavalleri Gl
- Cendes F
- Chen J
- Chen S
- Cherubini A
- Concha L
- David P
- Delanty N
- Depondt C
- Devinsky O
- Doherty CP51
- Domin M
- Focke Nk
- Foley S
- Franç
- Gambardella A
- Guerrini R
- Haaker G
- Hamandi K
- Hibar Dp
- Isaev D
- Jackson Gd
- Jahanshad N
- Kä
- Keller Ss
- Kochunov P
- Kotikalapudi R
- Kowalczyk Ma
- Kuzniecky R
- Kwan P
- Labate A
- Langner S
- Lenge M
- Leyden Km
- Liu M
- Loi Rq
- Martin P
- Mascalchi M
- McDonald Cr
- Meletti S
- Morita Me
- O&apos
- Ourselin S
- Pariente Jc
- Richardson MP Striano P
- Rodrí
- Rummel C
- Ryten M
- Saavalainen T
- Semmelroch Mk
- Severino M
- Sisodiya Sm.
- Thesen T
- Thomas Rh
- Thompson Pm
- Tondelli M
- Tortora D
- Vaudano AE39
- Vezzani A
- Vivash L40
- von Podewils F42
- Wagner J43
- Weber B43
- Whelan Cd
- Wiest R
- Yao Y46
- Yasuda CL7
- Zhang G47
- Zhang J
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2018
- Field of study
Progressive functional decline in the epilepsies is largely unexplained. We formed the ENIGMA-Epilepsy consortium to understand factors that influence brain measures in epilepsy, pooling data from 24 research centres in 14 countries across Europe, North and South America, Asia, and Australia. Structural brain measures were extracted from MRI brain scans across 2149 individuals with epilepsy, divided into four epilepsy subgroups including idiopathic generalized epilepsies (n =367), mesial temporal lobe epilepsies with hippocampal sclerosis (MTLE; left, n = 415; right, n = 339), and all other epilepsies in aggregate (n = 1026), and compared to 1727 matched healthy controls. We ranked brain structures in order of greatest differences between patients and controls, by meta-analysing effect sizes across 16 subcortical and 68 cortical brain regions. We also tested effects of duration of disease, age at onset, and age-by-diagnosis interactions on structural measures. We observed widespread patterns of altered subcortical volume and reduced cortical grey matter thickness. Compared to controls, all epilepsy groups showed lower volume in the right thalamus (Cohen's d = -0.24 to -0.73; P < 1.49 Ă 10-4), and lower thickness in the precentral gyri bilaterally (d = -0.34 to -0.52; P < 4.31 Ă 10-6). Both MTLE subgroups showed profound volume reduction in the ipsilateral hippocampus (d = -1.73 to -1.91, P < 1.4 Ă 10-19), and lower thickness in extrahippocampal cortical regions, including the precentral and paracentral gyri, compared to controls (d = -0.36 to -0.52; P < 1.49 Ă 10-4). Thickness differences of the ipsilateral temporopolar, parahippocampal, entorhinal, and fusiform gyri, contralateral pars triangularis, and bilateral precuneus, superior frontal and caudal middle frontal gyri were observed in left, but not right, MTLE (d = -0.29 to -0.54; P < 1.49 Ă 10-4). Contrastingly, thickness differences of the ipsilateral pars opercularis, and contralateral transverse temporal gyrus, were observed in right, but not left, MTLE (d = -0.27 to -0.51; P < 1.49 Ă 10-4). Lower subcortical volume and cortical thickness associated with a longer duration of epilepsy in the all-epilepsies, all-other-epilepsies, and right MTLE groups (beta, b < -0.0018; P < 1.49 Ă 10-4). In the largest neuroimaging study of epilepsy to date, we provide information on the common epilepsies that could not be realistically acquired in any other way. Our study provides a robust ranking of brain measures that can be further targeted for study in genetic and neuropathological studies. This worldwide initiative identifies patterns of shared grey matter reduction across epilepsy syndromes, and distinctive abnormalities between epilepsy syndromes, which inform our understanding of epilepsy as a network disorder, and indicate that certain epilepsy syndromes involve more widespread structural compromise than previously assumed
A systems-level analysis highlights microglial activation as a modifying factor in common epilepsies
- Author
- Absil J
- Alhusaini S
- Altmann A
- Alvim MKM
- Auvinen P
- Avbersek A
- Bacigaluppi M
- Bargallo N
- Bartolini E
- Bender B
- Bergo FPG
- Bernardes T
- Bernasconi A
- Bernasconi N
- Bernhardt BC
- Blackmon K
- BotĂa JA
- Braga B
- Caligiuri ME
- Calvo A
- Carlson C
- Carr SJ
- Cavalleri GL
- Cendes F
- Cerovic M
- Chen J
- Chen S
- Cherubini A
- Concha L
- David P
- Delanty N
- Depondt C
- Devinsky O
- Di Nunzio M
- Di Sapia R
- Doherty CP
- Domin M
- ENIGMA-Epilepsy Working Group .
- EpiPGX Consortium .
- Focke NK
- Foley S
- Franca W
- Gambardella A
- Guerrini R
- Hamandi K
- Hibar DP
- Iori V
- Isaev D
- Jackson GD
- Jahanshad N
- Kalviainen R
- Keller SS
- Kochunov P
- Kotikalapudi R
- Kowalczyk MA
- Kuzniecky R
- Kwan P
- Labate A
- Langner S
- Lenge M
- Leu C
- Liu M
- Martin P
- Mascalchi M
- McDonald CR
- Meletti S
- Micotti E
- Morita-Sherman ME
- O'Brien TJ
- Palma E
- Pariente JC
- Ravizza T
- Reynolds RH
- Richardson MP
- Rodriguez-Cruces R
- Ruffolo G
- Rummel C
- Ryten M
- Saavalainen T
- Semmelroch MK
- Severino M
- Sisodiya SM
- Somani A
- Striano P
- Thesen T
- Thom M
- Thomas RH
- Thompson P
- Tolomeo D
- Tondelli M
- Tortora D
- Vaudano AE
- Vezzani A
- Vivash L
- von Podewils F
- Wagner J
- Weber B
- Whelan CD
- Wiest R
- Yasuda CL
- Zhang G
- Zhang J
- Publication venue
- 'Foundation for Cellular and Molecular Medicine'
- Publication date
- 05/09/2021
- Field of study
Aims: The causes of distinct patterns of reduced cortical thickness in the common human epilepsies, detectable on neuroimaging and with important clinical consequences, are unknown. We investigated the underlying mechanisms of cortical thinning using a systems-level analysis. //
Methods: Imaging-based cortical structural maps from a large-scale epilepsy neuroimaging study were overlaid with highly spatially resolved human brain gene expression data from the Allen Human Brain Atlas. Cell-type deconvolution, differential expression analysis and cell-type enrichment analyses were used to identify differences in cell-type distribution. These differences were followed up in post-mortem brain tissue from humans with epilepsy using Iba1 immunolabelling. Furthermore, to investigate a causal effect in cortical thinning, cell-type specific depletion was used in a murine model of acquired epilepsy. //
Results: We identified elevated fractions of microglia and endothelial cells in regions of reduced cortical thickness. Differentially expressed genes showed enrichment for microglial markers, and in particular, activated microglial states. Analysis of post-mortem brain tissue from humans with epilepsy confirmed excess activated microglia. In the murine model, transient depletion of activated microglia during the early phase of the disease development prevented cortical thinning and neuronal cell loss in the temporal cortex. Although the development of chronic seizures was unaffected, the epileptic mice with early depletion of activated microglia did not develop deficits in a non-spatial memory test seen in epileptic mice not depleted of microglia. //
Conclusions: These convergent data strongly implicate activated microglia in cortical thinning, representing a new dimension for concern and disease modification in the epilepsies, potentially distinct from seizure control
Performance of CMS muon reconstruction in pp collision events at âËĹĄs = 7TeV
- Author
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- Abbiendi G
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- Kuessel Y
- Kuhr T
- Kukartsev G
- Kumar A
- Kumar A
- Kumar A
- Kumar V
- Kunde GJ
- Kunori S
- Kuo CM
- Kurca T
- Kurenkov A
- Kurt P
- Kuznetsova E
- Kwan S
- Kyberd P
- Kypreos T
- Kyriakis A
- Laasanen AT
- Lacaprara S
- Lacroix F
- Lae CK
- Lagana C
- Laird E
- Lamichhane P
- Lampen T
- Lanaro A
- Lander R
- Landsberg G
- Lanev A
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- Lange W
- Langenegger U
- Lannon K
- Lanske D
- Lariccia P
- Lassila-Perini K
- Lath A
- Lawson P
- Lazaridis C
- Lazic D
- Lazo-Flores J
- Lazzizzera I
- Le Bihan AC
- Le Grand T
- Lebolo LM
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- Lemaitre V
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- Leonard J
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- Leonidov A
- Leslie D
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- Letts J
- Levchenko P
- Levchuk L
- Li SW
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- Libeiro T
- Ligabue F
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- Lloret Iglesias L
- Lobelle Pardo P
- Locci E
- Lohmann W
- Lomidze D
- Lomtadze T
- Long OR
- Longo E
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- Lopez EL
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- Loukas D
- Lourenco C
- Loveless R
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- Lucaroni A
- Luckey PD
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- Lujan P
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- Lungu G
- Luo W
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- Lustermann W
- Luthra A
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- Maeki T
- Maenpaa T
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- Magana Villalba R
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- Mantovani G
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- Marienfeld M
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- Maruyama S
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- Mathias B
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- Matos Figueiredo D
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- Mavrommatis C
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- McCliment E
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- Medvedeva T
- Mehdiabadi SP
- Mehta MZ
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- Meijers F
- Mejias BM
- Mekterovic D
- Melo A
- Melzer-Pellmann I-A
- Menasce D
- Mendez H
- Meneghelli M
- Meneguzzo AT
- Meng X
- Menichelli M
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- Mercier D
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- Merola M
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- Mestvirishvili A
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- Mikulec I
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- Militaru O
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- Mossolov V
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- Muniz L
- Munoz Sanchez FJ
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- Musenich R
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- Musienko Y
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- Nesvold E
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- Neumeister N
- Newbold DM
- Newman HB
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- Newsom CR
- Nguyen D
- Nguyen H
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- Nicolaou C
- Niegel M
- Nikitenko A
- Nirunpong K
- Nishu N
- Nogima H
- Noonan D
- Norbeck E
- Nourbakhsh S
- Novaes SF
- Nowack A
- Nowak F
- Ntomari E
- Nuernberg A
- Nuttens C
- Nuzzo S
- O'Brien C
- O'Dell V
- Oberst O
- Obertino MM
- Obraztsov S
- Ocalan K
- Ochando C
- Ochesanu S
- Odell N
- Odorici F
- Oehler A
- Ofierzynski RA
- Oguri V
- Ojalvo I
- Olaiya E
- Olbrechts A
- Oliveros S
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- Organtini G
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- Osorio Oliveros AF
- Ostapchuk A
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- Panagiotou A
- Pandolfi F
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- Panwalkar S
- Paoletti S
- Paolucci P
- Papacz P
- Papadopoulos I
- Papageorgiou A
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- Paramatti R
- Paramesvaran S
- Parashar N
- Parida B
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- Parracho PGF
- Pashenkov A
- Passaseo M
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- Pastrone N
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- Peltola T
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- Perelygin V
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- Perfilov M
- Perieanu A
- Perloff A
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- Perries S
- Perrotta A
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- Pesaresi M
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- Petrukhin A
- Petrushanko S
- Petyt D
- Pfeiffer A
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- Piedra Gomez J
- Pieri M
- Pierini M
- Pierro GA
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- Pimiae M
- Pin A
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- Piotrzkowski K
- Piparo D
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- Piroue P
- Pitzl D
- Pivarski J
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov V
- Pordes R
- Potenza A
- Potenza R
- Pozdnyakov A
- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radi A
- Ragazzi S
- Rahatlou S
- Rahbaran B
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Ralph D
- Rander J
- Ranieri R
- Ranjan K
- Rappoccio S
- Raspereza A
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reece W
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- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Rikova MI
- Rinkevicius A
- Rios AAO
- Rizzi A
- Ro SR
- Roberts J
- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rodriguez-Marrero AY
- Roe J
- Roecker S
- Rogan C
- Rogerson S
- Roh Y
- Rohe T
- Rohlf J
- Rohringer C
- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romano F
- Romanowska-Rybinska K
- Romeo F
- Romero A
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Rose A
- Rose K
- Rosin M
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
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- Ryckbosch D
- Ryd A
- Ryu G
- Ryutin R
- Sabes D
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- Safonov A
- Safronov G
- Saha A
- Saini LK
- Saka H
- Sakharov A
- Sakulin H
- Sakuma T
- Sakumoto W
- Sala L
- Sala S
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
- Salur S
- Salvati E
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- Sanabria JC
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- Sanchez-Hernandez A
- Sander C
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- Sanders S
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- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Saoulidou N
- Saout C
- Sarkar S
- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Sawley M-C
- Scarborough T
- Schaefer C
- Schael S
- Schettler H
- Scheurer A
- Schieferdecker P
- Schilling F-P
- Schlein P
- Schleper P
- Schlieckau E
- Schmanau M
- Schmidt A
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- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schul N
- Schum T
- Schwarz T
- Schwick C
- Scodellaro L
- Scurlock B
- Searle M
- Seez C
- Segala M
- Segoni I
- Seitz C
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- Sekmen S
- Sellers P
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- Selvaggi M
- Semenov S
- Sen N
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- Sengupta S
- Senkin S
- Seo E
- Seo H
- Serban AT
- Serin M
- Sever R
- Sexton-Kennedy E
- Sfiligoi I
- Sguazzoni G
- Shah MA
- Sharma A
- Sharma A
- Sharma S
- Sharma V
- Sharma V
- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
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- Shukla P
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- Sierra RV
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- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
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- Simon M
- Simon S
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- Simonis HJ
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- Singh G
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- Singovsky A
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- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slaunwhite J
- Smirnov I
- Smith J
- Smith JG
- Smith K
- Smith VJ
- Smith WH
- Smolin D
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
- Soares Jorge L
- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
- Sogut K
- Sola V
- Solano A
- Somalwar S
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- Sonnenschein L
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- Souza MHG
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- Spiridonov A
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- Stephans GSF
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- Stieger B
- Stiliaris E
- Stober FM
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- Stoye M
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- Strauss J
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- Strom D
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- Suarez I
- Suarez RG
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- Sudhakar K
- Sulak L
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- Sultanov G
- Summers D
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- Sumowidagdo S
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- Surat UE
- Svintradze I
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- Tatarinov A
- Taurok A
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- Tcholakov V
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- Teo WD
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- Teyssier D
- Thea A
- Theofilatos K
- Thiebaux C
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- Thomsen J
- Thyssen F
- Tiko A
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- Tiras E
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
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- Tonelli G
- Tonjes MB
- Tonwar SC
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- Topaksu AK
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- Toropin A
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- Traczyk P
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- Trayanov R
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- Triantis FA
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- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
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- Tsirou A
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- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
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- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
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- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wardrope D
- Wasserbaech S
- Wayne M
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- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
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- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
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- Yang ZC
- Yazgan E
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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
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
arXiv:1206.4071v2.-- Chatrchyan, S. et al.The performance of muon reconstruction, identification, and triggering in CMS has been studied using 40 pb -1 of data collected in pp collisions at 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/c is above 95% over the whole region of pseudorapidity covered by the CMS muon system, < 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 GeVc is higher than 90% over the full Ă¡ 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 100GeV/c and, using cosmic rays, it is shown to be better than 10% in the central region up to pT = 1 TeV/c. Observed distributions of all quantities are well reproduced by the Monte Carlo simulation.This work was supported by the Austrian Federal Ministry of Science and Research; the Belgium Fonds de la Recherche Scientifique, and Fonds voor Wetenschappelijk Onderzoek; the Brazilian Funding Agencies (CNPq, CAPES, FAPERJ, and FAPESP); the Bulgarian Ministry of Education and Science; CERN; the Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation of China; the Colombian Funding Agency (COLCIENCIAS); the Croatian Ministry of Science, Education and Sport; the Research Promotion Foundation Cyprus; the Estonian Academy of Sciences and NICPB; the Academy of Finland, Finnish Ministry of Education and Culture, and Helsinki Institute of Physics; the Institut National de Physique NuclĂŠaire et de Physique des Particules / CNRS, and Commissariat ĂĄ l'Energie Atomique et aux Energies Alternatives/CEA, France; the Bundesministerium fĂźr Bildung und Forschung, Deutsche Forschungsgemeinschaft, and Helmholtz-Gemeinschaft Deutscher Forschungszentren, Germany; the General Secretariat for Research and Technology, Greece; the National Scientific Research Foundation, and National Office for Research and Technology, Hungary; the Department of Atomic Energy and the Department of Science and Technology, India; the Institute for Studies in Theoretical Physics and Mathematics, Iran; the Science Foundation, Ireland; the Istituto Nazionale di Fisica Nucleare, Italy; the Korean Ministry of Education, Science and Technology and the World Class University program of NRF, Korea; the Lithuanian Academy of Sciences; the Mexican Funding Agencies (CINVESTAV, CONACYT, SEP, and UASLP-FAI); the Ministry of Science and Innovation, New Zealand; the Pakistan Atomic Energy Commission; the State Commission for Sci- entific Research, Poland; the Fundaçao para a CiĂŞncia e a Tecnologia, Portugal; JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); the Ministry of Science and Technologies of the Russian Federation, the Russian Ministry of Atomic Energy and the Russian Foundation for Basic Research; the Ministry of Science and Technological Development of Serbia; the Ministerio de Ciencia e InnovaciĂłn, and Programa Consolider-Ingenio 2010, Spain; the Swiss Funding Agencies (ETH Board, ETH Zurich, PSI, SNF, UniZH, Canton Zurich, and SER); the National Science Council, Taipei; the Scientific and Technical Research Council of Turkey, and Turkish Atomic Energy Authority; the Science and Technology Facilities Council, U.K.; the US Department of Energy, and the US National Science Foundation. Individuals have received support from the Marie-Curie programme and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation Ă la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); and the Council of Science and Industrial Research, India.Peer Reviewe
Search for quark compositeness in dijet angular distributions from pp collisions at âsĚ = 7 TeV
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- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2012
- Field of study
Peer reviewe
Measurement of the rapidity and transverse momentum distributions of Z bosons in pp collisions at â(s)=7ââTeV
- 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
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
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- Ahmad WH
- Ahuja S
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- Alda Junior WL
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- Wissing C
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- Yazgan E
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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
- 'American Physical Society (APS)'
- Publication date
- 01/10/2011
- Field of study
Measurements of the normalized rapidity (y) and transverse-momentum (qT) distributions of DrellâYan muon and electron pairs in the Z-boson mass region (60<Mââ<120ââGeV) are reported. The results are obtained using a data sample of proton-proton collisions at a center-of-mass energy of 7 TeV, collected by the CMS experiment at the Large Hadron Collider (LHC), corresponding to an integrated luminosity of 36ââpb-1. The distributions are measured over the ranges |y|<3.5 and qT<600ââGeV and compared with quantum chromodynamics (QCD) calculations using recent parton distribution functions to model the momenta of the quarks and gluons in the protons. Overall agreement is observed between the models and data for the rapidity distribution, while no single model describes the Z transverse-momentum distribution over the full range
Measurement of the differential cross section for isolated prompt photon production in pp collisions at 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Adair A
- 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
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- 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
- Ansari MH
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
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- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- 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
- 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
- Banerjee S
- Banerjee S
- Bani L
- 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
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- Bartalini P
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- Basso L
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- Baty C
- Bauer G
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- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
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- Beaudette F
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- Bedjidian M
- Behrenhoff W
- Behrens U
- Belforte S
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- Belknap D
- Bell AJ
- Bell KW
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- 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
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- Yetkin T
- 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
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
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- Zielinski M
- Zito G
- 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
Search for supersymmetry in events with b jets and missing transverse momentum at the LHC
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
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- 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
Indications of suppression of excited ÎĽ states in Pb-Pb collisions at âsNN = 2.76TeV
- Author
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- 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%
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