539 research outputs found
UNCLES: Method for the identification of genes differentially consistently co-expressed in a specific subset of datasets
- Author
- A Huber
- A PreliÄ
- AA Shabalin
- AP Gasch
- Asoke K. Nandi
- B Abu-Jamous
- B Abu-Jamous
- Basel Abu-Jamous
- C Koch
- CH Wade
- CT Harbison
- D Dikicioglu
- D Liu
- DA Orlando
- David J. Roberts
- IS Dhillon
- J Bahler
- J Yang
- JK Choi
- JK Limb
- JM Pena
- JM Stuart
- KC Li
- KC Li
- KY Yeung
- KY Yeung
- L Lazzeroni
- LP Zhao
- MB Eisen
- P Cahan
- P Grandi
- PC Roberts
- PT Spellman
- R Fa
- R LletÄąĚa
- R Nilsson
- RJ Cho
- RM Piro
- Rui Fa
- S Chu
- S Fujii
- S Sharma
- S Vega-Pons
- T Hayata
- T Murali
- T Pramila
- TC Fleischer
- VA Gennarino
- X Liu
- Y Cheng
- Y Kluger
- Z Tao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 04/06/2015
- Field of study
Background: Collective analysis of the increasingly emerging gene expression datasets are required. The recently proposed binarisation of consensus partition matrices (Bi-CoPaM) method can combine clustering results from multiple datasets to identify the subsets of genes which are consistently co-expressed in all of the provided datasets in a tuneable manner. However, results validation and parameter setting are issues that complicate the design of such methods. Moreover, although it is a common practice to test methods by application to synthetic datasets, the mathematical models used to synthesise such datasets are usually based on approximations which may not always be sufficiently representative of real datasets. Results: Here, we propose an unsupervised method for the unification of clustering results from multiple datasets using external specifications (UNCLES). This method has the ability to identify the subsets of genes consistently co-expressed in a subset of datasets while being poorly co-expressed in another subset of datasets, and to identify the subsets of genes consistently co-expressed in all given datasets. We also propose the M-N scatter plots validation technique and adopt it to set the parameters of UNCLES, such as the number of clusters, automatically. Additionally, we propose an approach for the synthesis of gene expression datasets using real data profiles in a way which combines the ground-truth-knowledge of synthetic data and the realistic expression values of real data, and therefore overcomes the problem of faithfulness of synthetic expression data modelling. By application to those datasets, we validate UNCLES while comparing it with other conventional clustering methods, and of particular relevance, biclustering methods. We further validate UNCLES by application to a set of 14 real genome-wide yeast datasets as it produces focused clusters that conform well to known biological facts. Furthermore, in-silico-based hypotheses regarding the function of a few previously unknown genes in those focused clusters are drawn. Conclusions: The UNCLES method, the M-N scatter plots technique, and the expression data synthesis approach will have wide application for the comprehensive analysis of genomic and other sources of multiple complex biological datasets. Moreover, the derived in-silico-based biological hypotheses represent subjects for future functional studies.The National Institute for Health Research (NIHR) under its Programme Grants for Applied Research
Programme (Grant Reference Number RP-PG-0310-1004)
Visualization and detection of live and apoptotic cells with fluorescent carbon nanoparticles
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Two-pion Bose-Einstein correlations in central Pb-Pb collisions at sNNââ = 2.76 TeV
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- Rui R.
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- Venaruzzo M.
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- W.H. Trzaskaaf
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- Y. Wangbl
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- Y. Zoccarato bq
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- Y.W. Baekk
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- Z. Buthelezi bm
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- Z.L. Matthews an
- Publication venue
- 'Elsevier BV'
- Publication date
- 21/12/2010
- Field of study
The first measurement of two-pion Bose-Einstein correlations in central Pb-Pb
collisions at sNNââ=2.76 TeV at the Large Hadron Collider is
presented. We observe a growing trend with energy now not only for the
longitudinal and the outward but also for the sideward pion source radius. The
pion homogeneity volume and the decoupling time are significantly larger than
those measured at RHIC.Comment: 17 pages, 5 captioned figures, 1 table, authors from page 12,
published version, figures at
http://aliceinfo.cern.ch/ArtSubmission/node/388
Suppression of charged particle production at large transverse momentum in central Pb-Pb collisions at sNNââ=2.76 TeV
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- A. Abrahantes Quintana b
- A. Ahmad Masoodi j
- A. Akindinov l
- A. Alici o
- A. Alkinp
- A. Andronic s
- A. Arendab
- A. Asryant
- A. Augustinus f
- A. Badal\ue0 ag
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- A. Reshetinck
- A. Rivetti n
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- A. Sevcencoca
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- A. Zeninbc
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- A.J. Rubio Montero az
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- A.K. Dubeyi
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- A.M. Adared
- A.R. Reolonaw
- A.R. Timmins at
- B. Alessandro n
- B. Bathenap
- B. Batyunyaaq
- B. Boyerbf
- B. Chang af
- B. Cheynis bp
- B. D\uf6nigus s
- B. Espagnonbf
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- B. Guerzoni o
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- B. Potukuchi av
- B. Sitarbi
- B. von Haller f
- B. Vulpescu ak
- B. Wagnera
- B. Windelband bk
- B.C. Sinha i
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- C. Andrei u
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- C. Cheshkovbp
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- C. Geuna aj
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- C. Ivans
- C. Klein-B\uf6sing ap
- C. Kottachchi Kankanamge Don at
- C. Kuhn as
- C. Larav
- C. Lazzeroni an
- C. Lippmann f
- C. Loizidesct
- C. Luzzi f
- C. Mitu ca
- C. Nattrass db
- C. Nygaard ar
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- C. Pajaresad
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- C. Soos f
- C. Suire bf
- C. Tagridis cm
- C. Terrevoli r
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- C.H. Christensen ar
- C.W. Fabjanf
- D. Adamov\ue1c
- D. Aleksandrovm
- D. Blaum
- D. Budnikovbj
- D. Caffarri y
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- D. De Gruttolacd
- D. Di Bari r
- D. Eliace
- D. Emschermann ap
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- D. Krumbhorn bk
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- D. Perini f
- D. Perrino r
- D. R\uf6hrich a
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- D. Stocco aa
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- D.P. Mahapatra cb
- D.S. Hwangcs
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- D.T. Larsen a
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- E. Almar\ue1z Avi\uf1a h
- E. Belmont-Moreno h
- E. Berdermanns
- E. Biolcati ah
- E. Bruna d
- E. Calvo Villar bn
- E. Chiavassa n
- E. Cresciobv
- E. Cuautle by
- E. D\ue9nes g
- E. Fragiacomo cl
- E. Gladysz-Dziadus ao
- E. Incani cf
- E. Kang k
- E. Karpechevck
- E. Korna\ub4s ao
- E. Kryshenau
- E. L\uf3pez Torres b
- E. Montesaz
- E. Mudniccp
- E. Nappi ce
- E. Quercigh f
- E. Ryabinkin m
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- E. Scomparinn
- E. Serradilla az
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- E. Stenlundbs
- E. Vercellin ah
- E. Zabrodin bg
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- F. Antinori y
- F. Barile r
- F. Bellini o
- F. Blanco az
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- G. Luparello ah
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- G. Mazza n
- G. Nazarov bj
- G. Nooren br
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- G. Puddu cf
- G. Scioli o
- G. Segato y
- G. Shabratova aq
- G. Simonetti f
- G. Stefanek cg
- G. Stefanini f
- G. Steynbl
- G. Tejeda Mu\uf1oz bw
- G. Viesti y
- G. Volpe r
- G. Wilk cg
- G. Zinovjev p
- G.D. Erasmo r
- G.E. Bruno r
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- G.L. Usai cf
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- G.M. Urciuoli ch
- G.O.V. de Barros cc
- G.S. Pappalardo ag
- G.T. Jonesan
- G.V. Margagliotti bh
- H. Appelsh\ue4user ab
- H. B\uf8ggild ar
- H. Beck ab
- H. Borel aj
- H. Buesching ab
- H. Cainesd
- H. Delagrange aa
- H. Engel v
- H. Gonz\ue1lez Santosbw
- H. Gutbrods
- H. Hamagaki cr
- H. Helstrupci
- H. Jungk
- H. Le\uf3n Vargasab
- H. M\ufcller f
- H. Obayashi dd
- H. Oeschlercv
- H. Qvigstad bg
- H. Ricaud cv
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- H. Torii dd
- H. Yang aj
- H. Yokoyamabt
- H. Zbroszczyk cn
- H.A. Erdal ci
- H.H. Dalsgaard ar
- H.N. Kimk
- H.R. Schmidt s
- I. Altsybeevt
- I. Belikovas
- I. Berceanuu
- I. Cort\ue9s Maldonado bw
- I. Dasbe
- I. Dom\uednguez by
- I. H\u2c7rivn\ue1\u2c7cov\ue1 bf
- I. Ilkivcg
- I. Kisel v
- I. Kr\ue1likal
- I. Krauscv
- I. Le\uf3n Monz\uf3nco
- I. Maldonado Cervantes by
- I. Martashvili db
- I. Otterlundbs
- I. Pshenichnov ck
- I. Rusanovf
- I. Stanca
- I. Szarkabi
- I. Yushmanovm
- I. Zguraca
- I.-K. Yoo dj
- I.C. Arsene s
- I.G. Bearden ar
- J. \uc4yst\uf6af
- J. B\ue1nal
- J. Bartkeao
- J. Biel\u2c7c\uedk ax
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- J. Book ab
- J. Castillo Castellanos aj
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- J. Kral af
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- J. Milosevic bg
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- L. Milano ah
- L. Molnarf
- L. Monta\uf1o Zetinabv
- L. Musaf
- L. Pinsky ba
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- M. Bombarabd
- M. Botjeay
- M. Bregant bh
- M. Brozbi
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- M. Lunardony
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- M. Malaev au
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- M. Petrisu
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- M. Rammler ap
- M. Richtera
- M. Rodr\uedguez Cahuantzi bw
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- M. Shimomura bt
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- M. Stolpovskiy bc
- M. Tavletf
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- M. van Leeuwen br
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- M. Verweij br
- M. Wildeap
- M. Zhalovau
- M. Zynovyev p
- M.A. Lisa w
- M.A. Mazzoni ch
- M.A. Subieta V\ue1squez ah
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- M.K. K\uf6hlers
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- M.M. Khanj
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- M.R. Dutta Majumdar i
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- W.H. Trzaskaaf
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- X. Zhang bm
- X.-G. Lubk
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- Y. Hori cr
- Y. Kharlovbc
- Y. Kucheriaevm
- Y. Kwoncw
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- Y. Maobm
- Y. Martynov p
- Y. Miake bt
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- Y. Wangbk
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- Z.L. Matthews an
- Publication venue
- 'Elsevier BV'
- Publication date
- 07/12/2010
- Field of study
Inclusive transverse momentum spectra of primary charged particles in Pb-Pb
collisions at sNNâââ = 2.76 TeV have been measured by the ALICE
Collaboration at the LHC. The data are presented for central and peripheral
collisions, corresponding to 0-5% and 70-80% of the hadronic Pb-Pb cross
section. The measured charged particle spectra in âŁÎˇâŁ<0.8 and 0.3<pTâ<20 GeV/c are compared to the expectation in pp collisions at the same
sNNââ, scaled by the number of underlying nucleon-nucleon
collisions. The comparison is expressed in terms of the nuclear modification
factor RAAâ. The result indicates only weak medium effects (RAAââ 0.7) in peripheral collisions. In central collisions, RAAâ
reaches a minimum of about 0.14 at pTâ=6-7GeV/c and increases
significantly at larger pTâ. The measured suppression of high-pTâ particles is stronger than that observed at lower collision energies,
indicating that a very dense medium is formed in central Pb-Pb collisions at
the LHC.Comment: 15 pages, 5 captioned figures, 3 tables, authors from page 10,
published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/98
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
- 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
- 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
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- 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
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
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- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
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- Avetisyan A
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- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
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- Cooper SI
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- Coughlan JA
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- Cumalat JP
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- Cushman P
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- 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
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
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- Dauncey P
- David A
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- de Barbaro P
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- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
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- De Guio F
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
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- de Troconiz JF
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- Del Re D
- Delaere C
- Delgado Peris A
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- Ecklund KM
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- Xiao H
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
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- Zito G
- Zotto P
- Zou W
- 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
- Acosta D
- Acosta JG
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- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
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- Akgun B
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- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alderweireldt S
- Alexander J
- Aliev T
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
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- Andreev Y
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- Antonelli L
- Antunovic Z
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
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- Akin IV
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- Albayrak EA
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- Anagnostou G
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- Anderson J
- Anderson M
- Andrea J
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- Andrews W
- Anghel IM
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- Antunes JR
- Antunovic Z
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- Apollinari G
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- Azzolini V
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Cirino G
- Cittolin S
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- Civinini C
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- Yilmaz Y
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- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Chou JP
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- Christiansen T
- Chuang SH
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- Chwalek T
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- Clerbaux B
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- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
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- Conway J
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- Cooper SI
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- Cornelis T
- Correa Martins Junior M
- Cortezon EP
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- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
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- Cuevas J
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- Cumalat JP
- Cuplov V
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- Cutajar M
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- Cwiok M
- Czellar S
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- Da Costa EM
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- Ruchti R
- Rudolph M
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
- Russ J
- Rutherford B
- Ryan MJ
- Ryckbosch D
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- Sabes D
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- Safonov A
- Safronov G
- Saha A
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- Sakulin H
- Sakuma T
- Sakumoto W
- Sala L
- Sala S
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
- Salur S
- Salvati E
- Sammet J
- Sanabria JC
- Sanchez AK
- Sanchez-Hernandez A
- Sander C
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- Santaolalla J
- Santocchia A
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- Sawley M-C
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- Schaefer C
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- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
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- Schwick C
- Scodellaro L
- Scurlock B
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- Segoni I
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- Selvaggi G
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- 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
- Shmatov S
- Shoaib M
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
- Sigamani M
- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
- Sim KS
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
- Singh J
- Singh SP
- Singovsky A
- Sinthuprasith T
- 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
- Son DC
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- Spiridonov A
- Spiropulu M
- Sprenger D
- Squires M
- Stadie H
- Stahl A
- Staiano A
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- Stein M
- Steinbrueck G
- Stenson K
- Stephans GSF
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- Stieger B
- Stiliaris E
- Stober FM
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- Stoye M
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- Stoynev S
- Strauss J
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- Suarez RG
- Sudano E
- Sudhakar K
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- Sulimov V
- Sultanov G
- Summers D
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- Sumowidagdo S
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- Taurok A
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- Tiras E
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- Trocsanyi ZL
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- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
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- Ulmer KA
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- Wissing C
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- Won S
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- 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
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- Zoeller MH
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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
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