712 research outputs found
The nucleolus: a paradigm for cell proliferation and aging
- Author
- Bazett-Jones DP
- Bell SP
- Bell SP
- Bell SP
- Cavanaugh AH
- Comai L
- Comai L
- Copenhaven GP
- Damania B
- Damania B
- Derenzini M
- Eberhard D
- Fanning E
- Gotta M
- Gray MD
- Grummt I
- Hadjiolov AA
- Haltiner MM
- Hisatake K
- Jantzen HM
- Jantzen HM
- Johnston SD
- Kennedy BK
- Learned RM
- Learned RM
- Marciniak RA
- McStay B
- Melese T
- Mishima Y
- Moss T
- Nagamine M
- Nevins JR
- O'Mahony DJ
- O'Mahony DJ
- Paule MR
- Sinclair DA
- Sinclair DA
- Thweatt R
- Tuan J
- Voit R
- Voit R
- Voit R
- Watt PM
- Weinberg RA
- White RJ
- Zhai W
- Zhai W
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Pulmonary Abnormalities in Mice with Paracoccidioidomycosis: A Sequential Study Comparing High Resolution Computed Tomography and Pathologic Findings
- Author
- A Abdollahi
- A GonzĂĄlez
- A Restrepo
- A Restrepo
- A Restrepo
- AM Cock
- Angela Restrepo
- AS Souza Jr
- B Bustamante-Simon
- Bernardo Miguel de Oliveira Pascarelli
- C Nagaishi
- C Plathow
- CJ Green
- D Cavanaugh
- Damaris Lopera
- DP Schuster
- E Marchiori
- EL Gasparetto
- FH Netter
- Henrique Leonel Lenzi
- JA Vanoirbeek
- Jairo Hernando PatiĂąo
- JF Murray
- JG McEwen
- JosĂŠ Miguel Hidalgo
- KA Johnson
- L Franco
- LA Colby
- LC Junqueira
- Luz Elena Cano
- M Funari
- M Tatsumi
- MJ Paulus
- RJ Klinck
- RM Tuder
- Rodrigo Correa-Oliveira
- S Greschus
- S Restrepo
- Tonny Naranjo
- V Petraitis
- VL Calich
- WD Gude
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Paracoccidioidomycosis (PCM) is a fungal infection caused by the dimorphic fungus Paracoccidioides brasiliensis. It occurs preferentially in rural workers in whom the disease is severe and may cause incapacitating pulmonary sequelae. Assessment of disease progression and treatment outcome normally includes chest x-rays or CT studies. Existing experimental PCM models have focused on several aspects, but none has done a radiologic or image follow-up evaluation of pulmonary lesions considered as the fungus primary target. In this study, the lungs of mice infected with fungal conidia were studied sequentially during the chronic stage of their experimental mycosis by noninvasive high resolution medical computed tomography, and at time of sacrifice, also by histopathology to characterize pulmonary abnormalities. Three basic lung lesion patterns were revealed by both techniques: nodular-diffuse, confluent and pseudo-tumoral which were located mainly around the hilus thus accurately reflecting the situation in human patients. The experimental design of this study decreases the need to sacrifice a large number of animals, and serves to monitor treatment efficacy by means of a more rational approach to the study of human pulmonary diseases. The findings we are reporting open new avenues for experimental research, increase our understanding of the mycosis pathogenesis and consequently have repercussions in patients' care
Measurement of the Forward-Backward Asymmetry in the B -> K(*) mu+ mu- Decay and First Observation of the Bs -> phi mu+ mu- Decay
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Blocker C
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
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- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
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- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Cabrera S
- Calamba A
- Calancha C
- Cali IA
- Callner J
- Camarda S
- Campanelli M
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- Canepa A
- Cankocak K
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
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- Casarsa M
- Castro A
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- Cavaliere V
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- Chasco M
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- Chertok M
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- Chlachidze G
- Chlebana F
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- Chokheli D
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- Yi K
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- Yilmaz Y
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- Yoo HD
- Yoon AS
- Yorita K
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- Yun JC
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- Zablocki J
- Zakaria M
- Zanetti A
- Zanetti M
- Zang SL
- Zatserklyaniy A
- Zeng Y
- Zennamo J
- Zhang J
- Zheng Y
- Zhu RY
- Zhukova V
- Ziegler J
- Zielinski M
- Zucchelli SZucchelli Sira D
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We reconstruct the rare decays B+âK+Îź+Îźâ, B0âKâ(892)0Îź+Îźâ, and Bs0ââĎ(1020)Îź+Îźâ in a data sample
corresponding to 4.4fbâ1 collected in ppËâ collisions at
sâ=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121Âą16 B+âK+Îź+Îźâ and 101Âą12 B0âKâ0Îź+Îźâ decays we report the branching ratios. In addition, we report
the measurement of the differential branching ratio and the muon
forward-backward asymmetry in the B+ and B0 decay modes, and the Kâ0
longitudinal polarization in the B0 decay mode with respect to the squared
dimuon mass. These are consistent with the theoretical prediction from the
standard model, and most recent determinations from other experiments and of
comparable accuracy. We also report the first observation of the Bs0ââĎÎź+Îźâdecayandmeasureitsbranchingratio{\mathcal{B}}(B^0_s \to
\phi\mu^+\mu^-) = [1.44 \pm 0.33 \pm 0.46] \times 10^{-6}using27 \pm 6signalevents.ThisiscurrentlythemostrareB^0_s$ decay observed.Comment: 7 pages, 2 figures, 3 tables. Submitted to Phys. Rev. Let
Measurements of the properties of Lambda_c(2595), Lambda_c(2625), Sigma_c(2455), and Sigma_c(2520) baryons
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
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- Zanetti M
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- Zatserklyaniy A
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- Zeng Y
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- Zucchelli S Zucchelli Slli Sira D
- Zucchelli SZanetti A
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report measurements of the resonance properties of Lambda_c(2595)+ and
Lambda_c(2625)+ baryons in their decays to Lambda_c+ pi+ pi- as well as
Sigma_c(2455)++,0 and Sigma_c(2520)++,0 baryons in their decays to Lambda_c+
pi+/- final states. These measurements are performed using data corresponding
to 5.2/fb of integrated luminosity from ppbar collisions at sqrt(s) = 1.96 TeV,
collected with the CDF II detector at the Fermilab Tevatron. Exploiting the
largest available charmed baryon sample, we measure masses and decay widths
with uncertainties comparable to the world averages for Sigma_c states, and
significantly smaller uncertainties than the world averages for excited
Lambda_c+ states.Comment: added one reference and one table, changed order of figures, 17
pages, 15 figure
Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
- Adam N
- Adams MR
- Adams T
- Agostino L
- Akgun B
- Akgun U
- Alagoz E
- Albayrak EA
- Albrow M
- Alexander J
- Almenar CC
- Alver B
- Alverson G
- Amerio S
- Amidei D
- Anastassov A
- Anastassov A
- Anderson J
- Anghel IM
- Annovi A
- Antonelli L
- Antos J
- Apanasevich L
- Apollinari G
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Atac M
- Auerbach B
- Aurisano A
- Avery P
- Azfar F
- Baarmand MM
- Baden A
- Badgett W
- Bai Y
- Bakken JA
- Bandurin D
- Banerjee S
- Barbaro-Galtieri A
- Barberis E
- Baringer P
- Barnes VE
- Barnes VE
- Barnett BA
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Bendavid J
- Benelli G
- Benjamin D
- Beretvas A
- Beretvas A
- Berry D
- Berry E
- Berryhill J
- Betchart B
- Betts RR
- Bhat PC
- Bhatti A
- Bilki B
- Binkley M
- Biselli A
- Bisello D
- Bizjak I
- Bland KR
- Blekman F
- Bloch I
- Bloom K
- Blumenfeld B
- Blumenfeld B
- Bocci A
- Bochenek J
- Bodek A
- Bodek A
- Boeriu O
- Bolla G
- Bolton T
- Bonato A
- Borcherding F
- Borrello L
- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Burkett K
- Busetto G
- Bussey P
- Busza W
- Butler JN
- Butt J
- Butz E
- Buzatu A
- Bylsma B
- Calamba A
- Calancha C
- Cali IA
- Callner J
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Cankocak K
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carroll R
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cavanaugh R
- Ceballos GG
- Ceron C
- Cerri A
- Cerrito L
- Chakaberia I
- Chan M
- Chasco M
- Chatterjee A
- Chen J
- Chen M
- Chen YC
- Chertok M
- Chetluru V
- Cheung HWK
- Chiarelli G
- Chlachidze G
- Chlebana F
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Chung YS
- Cihangir S
- Ciobanu CI
- Ciocci MA
- Cirino G
- Claes DR
- Clarida W
- Clark A
- Cole P
- Compostella G
- Convery ME
- Conway J
- Cooper SI
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Cremaldi LM
- Crescioli F
- Cuevas J
- Culbertson R
- Cumalat JP
- Cuplov V
- Cushman P
- d'Ascenzo N
- d'Errico M
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- da Costa JG
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- Zucchelli Slli Sira D
- Zucchelli SYun JC
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2010
- Field of study
We present a search for a new heavy charged vector boson WⲠdecaying
to an electron-neutrino pair in ppËâ collisions at a center-of-mass
energy of 1.96\unit{TeV}. The data were collected with the CDF II detector
and correspond to an integrated luminosity of 5.3\unit{fb}^{-1}. No
significant excess above the standard model expectation is observed and we set
upper limits on Ďâ
B(Wâ˛âeν). Assuming standard
model couplings to fermions and the neutrino from the WⲠboson decay to
be light, we exclude a WⲠboson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
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- Affholderbach K
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- Ainsley C
- Akesson PF
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- Alemanni G
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- Anagnostou G
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- Zhuang HL
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- Zobernig G
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- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Adam W
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- Yi K
- Yildirim E
- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
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- Zoeller MH
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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
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
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- Civinini C
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- Cooper SI
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- Costanza F
- Couderc F
- Coughlan JA
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- Creanza D
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- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cussans D
- Custodio A
- Cutajar M
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- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Dabrowski A
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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
Second Order Dimensionality Reduction Using Minimum and Maximum Mutual Information Models
- Author
- A Globerson
- AJ Kim
- AL Fairhall
- CA Atencio
- DJ Heeger
- DJ Heeger
- DL Ruderman
- DR Cantrell
- E de Boer
- EH Adelson
- EP Simoncelli
- F Rieke
- G Felsen
- GD Horwitz
- GD Horwitz
- H Barlow
- H Barlow
- J Pillow
- J Touryan
- J Touryan
- JA Movshon
- JD Fitzgerald
- Jeffrey D. Fitzgerald
- JH van Hateren
- JL Fox
- JR Cavanaugh
- L Paninski
- L Paninski
- Lawrence C. Sincich
- LC Sincich
- LC Sincich
- M Carandini
- M Maravall
- M Meister
- N Brenner
- N Brenner
- NC Rust
- O Schwartz
- O Schwartz
- Olaf Sporns
- P Dayan
- R Malouf
- RE Bellman
- RJ Rowekamp
- RM Shapley
- RR de Ruyter van Steveninck
- Ryan J. Rowekamp
- S Tanabe
- T Hastie
- T Sharpee
- T von der Twer
- Tatyana O. Sharpee
- TM Cover
- W Bialek
- X Chen
- Y Karklin
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Conventional methods used to characterize multidimensional neural feature selectivity, such as spike-triggered covariance (STC) or maximally informative dimensions (MID), are limited to Gaussian stimuli or are only able to identify a small number of features due to the curse of dimensionality. To overcome these issues, we propose two new dimensionality reduction methods that use minimum and maximum information models. These methods are information theoretic extensions of STC that can be used with non-Gaussian stimulus distributions to find relevant linear subspaces of arbitrary dimensionality. We compare these new methods to the conventional methods in two ways: with biologically-inspired simulated neurons responding to natural images and with recordings from macaque retinal and thalamic cells responding to naturalistic time-varying stimuli. With non-Gaussian stimuli, the minimum and maximum information methods significantly outperform STC in all cases, whereas MID performs best in the regime of low dimensional feature spaces
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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- Adler V
- Adzic P
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- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
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- Akchurin N
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- Akin IV
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- Albayrak EA
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- Amsler C
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- Cappello G
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- Carlsmith D
- Carrillo Moreno S
- Carroll R
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- Castaldi R
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- Cavallari F
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- Cavanaugh R
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- Ceballos GG
- Cepeda M
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- Cerizza G
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- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
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- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
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- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
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- Chiochia V
- Chiorboli M
- Chlebana F
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- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
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- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
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- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
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- Conetti S
- Contardo D
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- Cooper SI
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- Correa Martins Junior M
- Cortezon EP
- Cossutti F
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- Costantini S
- Coughlan JA
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- Covarelli R
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- Creanza D
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- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
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- Cutajar M
- Cutts D
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- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
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- 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
- Schmidt R
- Schmitt M
- 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
- Seixas J
- Sekmen S
- Sellers P
- Selvaggi G
- Selvaggi M
- Semenov S
- Sen N
- Sen S
- 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
- Song S
- Sonmez N
- Sonnenschein L
- Sordini V
- Souza MHG
- Spagnolo P
- Spalding WJ
- Spanier S
- Sparrow A
- Speer T
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiridonov A
- Spiropulu M
- Sprenger D
- Squires M
- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Steggemann J
- Stein M
- Steinbrueck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stoeckli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strom D
- Stuart D
- Sturdy J
- Suarez I
- Suarez RG
- Sudano E
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
- Sun W
- Sung K
- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swanson J
- Swartz M
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tadel M
- Takahashi M
- Tali B
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- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
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- Teo WD
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- Teyssier D
- Thea A
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- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
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- Tosi M
- Tosi S
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Turkewitz J
- Turner M
- Tuuva T
- Tuve C
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- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
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- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
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- Weiler T
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- Wenger EA
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- Widl E
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- Winn D
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- 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
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- 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
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- Zoeller MH
- Zotto P
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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
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