1,178 research outputs found
An Overview of Kinematic and Calibration Models Using Internal/External Sensors or Constraints to Improve the Behavior of Spatial Parallel Mechanisms
- Author
- Agheli
- Ahmad
- Altuzarra
- Ana C. Majarena
- Bai
- Ball
- Bamberger
- Ben-Horin
- Bhatia
- Borm
- Caccavale
- Carretero
- Ceccarelli
- Chablat
- Chen
- Cheng
- Cheng
- Chiu
- Cui
- Dafaoui
- Daney
- Dasgupta
- Dasgupta
- David Samper
- De Jalon
- Denavit
- Dhingra
- Driels
- Dunlop
- Dwarakanath
- Everett
- Fichter
- Gallardo
- Gallardo
- Gallardo
- Gao
- García
- Gogu
- Gong
- Gosselin
- Gosselin
- Gough
- Hesselbach
- Hilera
- Hollerbach
- Hollerbach
- Hollerbach
- Horne
- Huang
- Huang
- Hunt
- Hunt
- Husty
- Innocenti
- Innocenti
- Innocenti
- Jorge Santolaria
- Juan J. Aguilar
- Judd
- Khalil
- Khoukhi
- Kim
- Kim
- Last
- Lee
- Levenberg
- Li
- Lipson
- Liu
- Liu
- Liu
- Lopes
- Lu
- Marquardt
- Martín del Brío
- Merlet
- Merlet
- Merlet
- Nabat
- Nielsen
- Nielsen
- Oiwa
- Patel
- Paul
- Pritschow
- Raghavan
- Rao
- Rauf
- Ren
- Renaud
- Renaud
- Renders
- Rodriguez
- Roth
- Saglia
- Sansoni
- Santolaria
- Shim
- Shimizu
- Sommer
- Staicu
- Tsai
- Wampler
- Wampler
- Wang
- Wang
- Wen
- Whitney
- Yang
- Yang
- Zanganeh
- Zhu
- Zhuang
- Zhuang
- Zhuang
- Publication venue
- Molecular Diversity Preservation International (MDPI)
- Publication date
- 01/11/2010
- Field of study
This paper presents an overview of the literature on kinematic and calibration models of parallel mechanisms, the influence of sensors in the mechanism accuracy and parallel mechanisms used as sensors. The most relevant classifications to obtain and solve kinematic models and to identify geometric and non-geometric parameters in the calibration of parallel robots are discussed, examining the advantages and disadvantages of each method, presenting new trends and identifying unsolved problems. This overview tries to answer and show the solutions developed by the most up-to-date research to some of the most frequent questions that appear in the modelling of a parallel mechanism, such as how to measure, the number of sensors and necessary configurations, the type and influence of errors or the number of necessary parameters
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A Search for Dark Higgs Bosons
- Author
- Acosta JG
- Adam N
- Adametz A.
- Adye T.
- Ahmed H.
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- Akchurin N
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- Alverson G
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- Asaadi J
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Atramentov O
- Ayad R.
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- Barker A
- Barlow R. J.
- Barnes VE
- Barnett BA
- Bartoldus R.
- Batignani G.
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- Baumgartel D
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- Wu S. L.tkin T
- Wulsin H. W.
- Xie S
- Yan M
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- Yang ZC
- Yazgan E
- Yeche Ch
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
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- Zablocki J
- Zallo A.
- Zanetti M
- Zatserklyaniy A
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- Zheng Y
- Zhukova V
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- Ziegler V.
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Recent astrophysical and terrestrial experiments have motivated the proposal
of a dark sector with GeV-scale gauge boson force carriers and new Higgs
bosons. We present a search for a dark Higgs boson using 516 fb-1 of data
collected with the BABAR detector. We do not observe a significant signal and
we set 90% confidence level upper limits on the product of the Standard
Model-dark sector mixing angle and the dark sector coupling constant.Comment: 7 pages, 5 postscript figures, published version with improved plots
for b/w printin
Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV
- Author
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- Bodek A
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- Bonato A
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- Bortoletto D
- Bortoletto D
- Bose S
- Boudreau J
- Boulahouache C
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- Zucchelli Slli Sira D
- Zucchelli SYun JC
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- 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 W′ decaying
to an electron-neutrino pair in ppˉ 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 σ⋅B(W′→eν). Assuming standard
model couplings to fermions and the neutrino from the W′ boson decay to
be light, we exclude a W′ boson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
Measurement of the Forward-Backward Asymmetry in the B -> K(*) mu+ mu- Decay and First Observation of the Bs -> phi mu+ mu- Decay
- Author
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- Jayatilaka B
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- Kamon T
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- Khukhunaishvili A
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- Zucchelli SZucchelli Sira D
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We reconstruct the rare decays B+→K+μ+μ−, B0→K∗(892)0μ+μ−, and Bs0→ϕ(1020)μ+μ− in a data sample
corresponding to 4.4fb−1 collected in ppˉ collisions at
s=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121±16 B+→K+μ+μ− and 101±12 B0→K∗0μ+μ− 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 K∗0
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 Bs0→ϕμ+μ−decayandmeasureitsbranchingratio{\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
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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
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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- Yilmaz Y
- Yohay R
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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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- Ziebarth EB
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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
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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- Wasserbaech S
- Wayne M
- Weber H
- Weber HA
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- Wehrli L
- Weiler T
- Weinberg M
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- Xiao H
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
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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
- 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
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
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- Acosta JG
- Acosta MV
- Adair A
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- Adiguzel A
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- Afanasiev S
- Agostino L
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- Andreev Y
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- Civinini C
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- Cline D
- CMS Collaboration
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- Cockerill DJA
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- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
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- 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
- 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
- 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
- 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
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
- 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
- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
- Andreev V
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- Andrews W
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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
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