160 research outputs found
Finite Element Analysis of Osteosynthesis Screw Fixation in the Bone Stock: An Appropriate Method for Automatic Screw Modelling
- Author
- AD Heiner
- Andreas Fritsche
- AR Cross
- B Seral
- Boris Rubinsky
- C Ohman
- CL Lin
- CL Tai
- D Kluess
- HJ Wilke
- HY Cheng
- J Cegonino
- JA BeltrĂĄn-FernĂĄndez
- Jan Wieding
- K Polgar
- K Zweymuller
- KJ Wilkens
- L Cristofolini
- LD Blecha
- M Hussain
- M Viceconti
- MS Atac
- P Cronier
- P Schuller-Gotzburg
- PJ Prendergast
- Rainer Bader
- RJ Otto
- Robert Souffrant
- SH Kim
- SM Perren
- ST Lovald
- TF Higgins
- TM Keaveny
- Wolfram Mittelmeier
- WR Taylor
- Publication venue
- Public Library of Science
- Publication date
- 28/03/2012
- Field of study
The use of finite element analysis (FEA) has grown to a more and more important method in the field of biomedical engineering and biomechanics. Although increased computational performance allows new ways to generate more complex biomechanical models, in the area of orthopaedic surgery, solid modelling of screws and drill holes represent a limitation of their use for individual cases and an increase of computational costs. To cope with these requirements, different methods for numerical screw modelling have therefore been investigated to improve its application diversity. Exemplarily, fixation was performed for stabilization of a large segmental femoral bone defect by an osteosynthesis plate. Three different numerical modelling techniques for implant fixation were used in this study, i.e. without screw modelling, screws as solid elements as well as screws as structural elements. The latter one offers the possibility to implement automatically generated screws with variable geometry on arbitrary FE models. Structural screws were parametrically generated by a Python script for the automatic generation in the FE-software Abaqus/CAE on both a tetrahedral and a hexahedral meshed femur. Accuracy of the FE models was confirmed by experimental testing using a composite femur with a segmental defect and an identical osteosynthesis plate for primary stabilisation with titanium screws. Both deflection of the femoral head and the gap alteration were measured with an optical measuring system with an accuracy of approximately 3 Âľm. For both screw modelling techniques a sufficient correlation of approximately 95% between numerical and experimental analysis was found. Furthermore, using structural elements for screw modelling the computational time could be reduced by 85% using hexahedral elements instead of tetrahedral elements for femur meshing. The automatically generated screw modelling offers a realistic simulation of the osteosynthesis fixation with screws in the adjacent bone stock and can be used for further investigations
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
- 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
- Cabrera S
- 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
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- 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
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- da Costa JG
- Dagenhart D
- Dahmes B
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- Datta M
- de Barbaro P
- de Barbaro P
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- Devoto F
- Di Canto A
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- Dittmann JR
- Dobur D
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- Jayatilaka B
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- Jindal P
- Jindariani S
- Johnson KF
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- Jun SY
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- Yao WM
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- Yi K
- Yi K
- Yilmaz Y
- Yoh J
- Yoo HD
- Yoon AS
- Yorita K
- Yoshida T
- Yu GB
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Yun JC
- Zabel J
- Zablocki J
- Zakaria M
- Zanetti A
- Zanetti M
- Zang SL
- Zatserklyaniy A
- Zeng Y
- Zennamo J
- Zhang J
- Zheng Y
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- 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
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
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- Xiao H
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- 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
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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
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
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- Agostino L
- Akgun B
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- Albayrak EA
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- Aurisano A
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- Baarmand MM
- Baden A
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- Bakken JA
- Bandurin D
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- Ciobanu CI
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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
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- da Costa JG
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- Dahmes B
- Das S
- Datta M
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- Deluca C
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- Deng J
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- Eshaq Y
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- Eusebi R
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- Everett A
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- Farrington S
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- Feindt M
- Ferencek D
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- Flacher H
- Flanagan G
- Ford WT
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- Freeman J
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- Fu Y
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- Gallinaro M
- Galyardt J
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- Garcia-Bellido A
- Garcia-Solis EJ
- Garfinkel AF
- Garfinkel AF
- Garosi P
- Gartner J
- Gaultney V
- Gecse Z
- Gerbaudo D
- Gerber CE
- Gerberich H
- Gerchtein E
- Geurts FJM
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- Giakoumopoulou V
- Giannetti P
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- Ginsburg CM
- Giokaris N
- Giromini P
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- Glagolev V
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- Godang R
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- Gritsan AV
- Gronberg J
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- Group RC
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- Gunay-Unalan Z
- Gunthoti K
- Guo ZJ
- Guragain S
- Gutay L
- Gutsche O
- Haas J
- Haber C
- Hadley NJ
- Hagopian S
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- Hahn A
- Hahn KA
- Hahn SR
- Halkiadakis E
- Halyo V
- Hamaguchi A
- Han J
- Han JY
- Hanlon J
- Happacher F
- Hara K
- Hare D
- Hare M
- Harel A
- Harr RF
- Harris P
- Harris RM
- Hatakeyama K
- Haupt J
- Hays C
- Hebda P
- Heck M
- Heinrich J
- Heltsley B
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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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
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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
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- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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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 the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Abbaneo D
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Performance of CMS muon reconstruction in pp collision events at âËĹĄs = 7TeV
- Author
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- '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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- Publication venue
- Publication date
- 01/01/2012
- Field of study
Peer reviewe
CMS Data Processing Workflows during an Extended Cosmic Ray Run
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
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- Civinini C
- Claes DR
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- Colafranceschi S
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- Colling D
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- Contardo D
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- Cortabitarte RV
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- Creanza D
- Cremaldi LM
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- Crotty I
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- Cutts D
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- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Pirollet B
- Piroue P
- Pivarski J
- Plager C
- Plestina R
- Poettgens M
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Pompili A
- Ponzio B
- Pooth O
- Popescu S
- Postema H
- Postoev VE
- Postolache V
- Potenza R
- Pozdnyakov A
- Pozniak K
- Pozzobon N
- Prescott C
- Prettner E
- Prokofyev O
- Prosper H
- Ptochos F
- Pugliese G
- Puigh D
- Puljak I
- Pullia A
- Punz T
- Puzovic J
- Qazi S
- Qian SJ
- Quast G
- Quertenmont L
- Rabbertz K
- Raboso AG
- Racz A
- Radicci V
- Raffaelli F
- Ragazzi S
- Rahatlou S
- Rahmat R
- Raics P
- Raidal M
- Rajan R
- Rakness G
- Ralich R
- Ramos JPF
- Rander J
- Ranieri A
- Ranieri R
- Ranjan K
- Raposo L
- Rappoccio S
- Rapsevicius V
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Ravat S
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Reeder D
- Regenfus C
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Renz M
- Reucroft S
- Rew SB
- Rhee HB
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richman J
- Rios AAO
- Rivera R
- Rivero CM
- Rivetta CH
- Rizzi A
- Roberts J
- Robles J
- Robmann P
- Rodrigo T
- Rodrigues NB
- Rodriguez JL
- Rogan C
- Roh Y
- Rohe T
- Rohlf J
- Rohringer H
- Roinishvili N
- Roinishvili V
- Roland C
- Roland G
- Rolandi G
- Romaniuk R
- Romano F
- Romero A
- Romero DR
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Ronquest M
- Ronzhin A
- Rose A
- Rose K
- Roselli G
- Rosemann C
- Rosowsky A
- Rossato K
- Rossi AM
- Rossin R
- Rossman P
- Rougny R
- Rouhani S
- Rousseau D
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Rugovac S
- Ruiz MB
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
- Russ J
- Russo A
- Ryan MJ
- Ryckbosch D
- Ryd A
- Ryjov V
- Ryu S
- Ryutin R
- Sabbatini L
- Sabonis T
- Sacchi R
- Safarzadeh B
- Safonov A
- Safronov G
- Saha A
- Saini LK
- Sakharov A
- Sakulin H
- Sala L
- Sala S
- Salerno R
- Sampaio S
- Samyn D
- Sanabria JC
- Sanchez AK
- Sanchez JG
- Sanchez MCD
- Sander C
- Sanders DA
- Sanders S
- Sani M
- Santacruz N
- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Sanudo MS
- Sanzeni C
- Saout C
- Sarkar S
- Sartisohn G
- Sarycheva L
- Satpathy A
- Sauce H
- Sauerland P
- Savin A
- Savrin V
- Sawley MC
- Schael S
- Schafer C
- Scheurer A
- Schieferdecker P
- Schilling FP
- Schlatter WD
- Schlein P
- Schleper P
- Schmid S
- Schmidt A
- Schmidt I
- Schmidt R
- Schmitt M
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schott G
- Schreiner T
- Schroder M
- Schroeder M
- Schul N
- Schum T
- Schumann J
- Schwering G
- Schwick C
- Sciaba A
- Sciacca C
- Scodellaro L
- Scurlock B
- Searle M
- Sedov A
- Seez C
- Segneri G
- Segoni I
- Seixas J
- Sekhri V
- Sekmen S
- Selvaggi G
- Selvaggi M
- Semenov R
- Semenov S
- Sen S
- Sengupta S
- Serban AT
- Serin M
- Servoli L
- Sever R
- Sexton-Kennedy E
- Sfiligoi I
- Sguazzoni G
- Shabalina E
- Shahzad H
- Sharma A
- Sharma A
- Sharma S
- Sharma V
- Sharp P
- Shaw TM
- Shcheglov Y
- Shchetkovskiy A
- Sheldon P
- Shen BC
- Shepherd-Themistocleous CH
- Shi X
- Shinde Y
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shpakov D
- Shreyber I
- Shukla P
- Shumeiko N
- Siamitros C
- Sibille J
- Sidiropoulos G
- Siegrist N
- Siegrist P
- Sierra RV
- Signal T
- Sikler F
- Sill A
- Sillou D
- Silva J
- Silva P
- Silvestris L
- Sim KS
- Simon S
- Simonetto F
- Simonis HJ
- Sinanis N
- Singh A
- Singh JB
- Singh SP
- Singovsky A
- Sirois Y
- Siroli G
- Sirunyan AM
- Sknar V
- Skuja A
- Skup E
- Slabospitsky S
- Slaunwhite J
- Smiljkovic N
- Smirnov I
- Smirnov V
- Smith J
- Smith K
- Smith RP
- Smith VJ
- Smith WH
- Smolin D
- Smoron A
- Snigirev A
- Snow GR
- Soares D
- Sobol A
- Sobrier T
- Sogut K
- Soha A
- Solano A
- Solin A
- Solovey A
- Solovey A
- Somalwar S
- Son DC
- Song S
- Sonmez N
- Sonnek P
- Sonnenschein L
- Sordini V
- Sordo HN
- Soroka D
- Sourkov A
- Sousa M
- Souza MHG
- Sowa M
- Spagnolo P
- Spalding WJ
- Spanier S
- Speck J
- Speer T
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Sprenger D
- Squires M
- Srivastava AK
- St John J
- Stadie H
- Stahl A
- Staiano A
- Stark R
- Starodumov A
- Stefanovitch R
- Steggemann J
- Steinbruck G
- Steininger H
- Stenson K
- Stephans G
- Stettler M
- Stickland D
- Stieger B
- Stilley J
- Stober FM
- Stockli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strang M
- Strauss J
- Stringer R
- Stroiney S
- Stuart D
- Sturdy J
- Sturm P
- Suarez RG
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sun W
- Sung K
- Surat UE
- Suzuki I
- Svintradze I
- Swain J
- Swanson J
- Swartz M
- Sytine A
- Sytnik V
- Szabo Z
- Szczesny H
- Szekely G
- Szillasi Z
- Szleper M
- Sznajder A
- Takahashi M
- Tali B
- Tan P
- Tancini V
- Tanenbaum W
- Tao J
- Tapper A
- Tarakanov V
- Taroni S
- Taurok A
- Tauscher L
- Tavernier S
- Taylor L
- Taylor R
- Teischinger F
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Terentyev N
- Teyssier D
- Thea A
- Themel T
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas M
- Thomas S
- Thomsen J
- Thyssen F
- Tikhonenko E
- Tikhonov A
- Timciuc V
- Timlin C
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tokesi K
- Tolaini S
- Tomalin IR
- Tomei TRFP
- Tonelli G
- Toniolo N
- Tonjes MB
- Tonoiu D
- Tonwar SC
- Toole T
- Topakli H
- Topaksu AK
- Topkar A
- Torassa E
- Tornier D
- Toropin A
- Torre P
- Torromeo G
- Tosi M
- Toteva Z
- Toth N
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Trapani PP
- Travaglini R
- Trayanov R
- Treille D
- Trentadue R
- Triantis FA
- Tricomi A
- Triossi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropea P
- Tropiano A
- Troshin S
- Troska J
- Trub P
- Trunov A
- Tsang KV
- Tsiakkouri D
- Tsirigkas D
- Tsirou A
- Tucker J
- Tully C
- Tumanov A
- Tuominen E
- Tuominiemi J
- Tupputi S
- Tuura L
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ueno K
- Uhl D
- Ujvari B
- Ulmer K
- Ungaro D
- Uplegger L
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdez HC
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Remortel N
- Vander Donckt M
- Vanelderen L
- Vanini S
- Vankov I
- Vanlaer P
- Vardanyan I
- Varela J
- Varelas N
- Vargas JER
- Vasil'ev S
- Vaughan J
- Vaurynovich S
- Vavilov S
- Vedaee A
- Veelken C
- Veillet L
- Velasco M
- Velde CV
- Velichko G
- Velikzhanin Y
- Velthuis J
- Ventura S
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- Verrecchia P
- Verwilligen P
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vicini A
- Vidal R
- Vila I
- Villella I
- Vinogradov A
- Virdee T
- Virto AL
- Visca L
- Vishnevskiy A
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volkov S
- Volobouev I
- Volodko A
- Volpe R
- Volyanskyy D
- von Dratzig AS
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Wagner P
- Wagner SR
- Wagner W
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Waltenberger W
- Walton R
- Walzel G
- Wan Z
- Wang CC
- Wang D
- Wang J
- Wang M
- Wang Z
- Warchol J
- Wardrope D
- Washington E
- Watts TL
- Wayne M
- Weber M
- Weber M
- Wehrli L
- Weinberg M
- Weinberger M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Wenman D
- Wensveen M
- Werner JS
- Wertelaers P
- Wetzel J
- White A
- Whitmore J
- Whyntie T
- Wickens J
- Wicklund E
- Widl E
- Wigmans R
- Wildish T
- Wilke L
- Wilken R
- Wilkinson R
- Williams G
- Williams JC
- Williams JH
- Willmott C
- Wimpenny S
- Wingham M
- Winn D
- Wissing C
- Witherell M
- Wittich P
- Wittmer B
- Wlochal M
- Wohri HK
- Wolf R
- Womersley WJ
- Won S
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu S
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xie S
- Xie Z
- Xue Z
- Yagil A
- Yan M
- Yang X
- Yang Y
- Yang ZC
- Yarba J
- Yaselli I
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
- Yumiceva F
- Yun JC
- Yuste C
- Zabi A
- Zabolotny W
- Zachariadou A
- Zalewski P
- Zampieri A
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Y
- Zhang Z
- Zheng Y
- Zhiltsov V
- Zhokin A
- Zhu B
- Zhu K
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Zielinski M
- Zilizi G
- Zinonos Z
- Zito G
- Zoeller MH
- Zotto P
- Zub S
- Zumerle G
- Zuranski A
- Zuyeuski R
- Zych P
- Publication venue
- INSTITUTE OF PHYSICS PUBLISHING
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
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