540 research outputs found
An Evaluation of an Augmented Reality Multimodal Interface Using Speech and Paddle Gestures
- Publication venue
- University of Canterbury. Human Interface Technology Laboratory.
- Publication date
- 01/01/2006
- Field of study
Get PDFThis paper discusses an evaluation of an augmented reality (AR)
multimodal interface that uses combined speech and paddle gestures for interaction
with virtual objects in the real world. We briefly describe our AR multimodal
interface architecture and multimodal fusion strategies that are based on the
combination of time-based and domain semantics. Then, we present the results
from a user study comparing using multimodal input to using gesture input
alone. The results show that a combination of speech and paddle gestures improves
the efficiency of user interaction. Finally, we describe some design recommendations
for developing other multimodal AR interfaces
Perioperative infusion of low- dose of vasopressin for prevention and management of vasodilatory vasoplegic syndrome in patients undergoing coronary artery bypass grafting-A double-blind randomized study
- Author
- A Delmas
- A Mekontso-Dessap
- A Noto
- B Mets
- B Patel
- C Torqersen
- CL Holmes
- D Morales
- D Morales
- DL Morales
- DW Landry
- E Tayama
- Efstratios Apostolakis
- Efstratios Koletsis
- Eleni Sintou
- G Bragadottir
- G Luckner
- G Mutlu
- G Shanmugam
- Georgios Papadopoulos
- JG Laffey
- KJ Tuman
- M Argengiano
- M Argenziano
- M Argenziano
- M Leone
- MB Malay
- MW Duenser
- MW Duenser
- MW Duenser
- Nikolaos G Baikoussis
- P Masetti
- PM Mannucci
- R Suojaranta-Ylinen
- RL Levin
- S Novella
- S Raja
- Stavros Siminelakis
- T Albright
- T Carrel
- T Carrel
- T Treschan
- V Wenzel
- V Wenzel
- V Wenzel
- WJ Gomes
- WJ Gomes
- X Sun
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Get PDFPreoperative medication by inhibitors of angiotensin-converting enzyme (ACE) in coronary artery patients predisposes to vasoplegic shock early after coronary artery bypass grafting. Although in the majority of the cases this shock is mild, in some of them it appears as a situation, "intractable" to high-catecholamine dose medication. In this study we examined the possible role of prophylactic infusion of low-dose vasopressin, during and for the four hours post-bypass after cardiopulmonary bypass, in an effort to prevent this syndrome. In addition, we studied the influence of infused vasopressin on the hemodynamics of the patients, as well as on the postoperative urine-output and blood-loss. In our study 50 patients undergoing coronary artery bypass grafting were included in a blind-randomized basis. Two main criteria were used for the eligibility of patients for coronary artery bypass grafting: ejection fraction between 30-40%, and patients receiving ACE inhibitors, at least for four weeks preoperatively. The patients were randomly divided in two groups, the group A who were infused with 0.03 IU/min vasopressin and the group B who were infused with normal saline intraoperativelly and for the 4 postoperative hours. Measurements of mean artery pressure (MAP), central venous pressure (CVP), systemic vascular resistance (SVR), ejection fracture (EF), heart rate (HR), mean pulmonary artery pressure (MPAP), cardiac index (CI) and pulmonary vascular resistance (PVR) were performed before, during, and after the operation. The requirements of catecholamine support, the urine-output, the blood-loss, and the requirements in blood, plasma and platelets for the first 24 hours were included in the data collected. The incidence of vasodilatory shock was significantly lower (8% vs 20%) in group A and B respectively (p = 0,042). Generally, the mortality was 12%, exclusively deriving from group B. Postoperatively, significant higher values of MAP, CVP, SVR and EF were recorded in the patients of group A, compared to those of group B. In group A norepinephrine was necessary in fewer patients (p = 0.002) and with a lower mean dose (p = 0.0001), additive infusion of epinephrine was needed in fewer patients (p = 0.001), while both were infused for a significant shorter infusion-period (p = 0.0001). Vasopressin administration (for group A) was associated with a higher 24 hour diuresis) (0.0001)
Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
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- Abbiendi G.
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- Acosta D.
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- Adam N.
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- Adiguzel A.
- Adler V.
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe production of b jets in association with a Z/gamma* boson is studied
using proton-proton collisions delivered by the LHC at a centre-of-mass energy
of 7 TeV and recorded by the CMS detector. The inclusive cross section for
Z/gamma* + b-jet production is measured in a sample corresponding to an
integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross
section with Z/gamma* to ll (where ll = ee or mu mu) for events with the
invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level
with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and
the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.)
+(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also
studied and found to be in agreement with the predictions made by the MadGraph
event generator with the parton shower and the hadronisation performed by
PYTHIA.Comment: Submitted to the Journal of High Energy Physic
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
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- Yilmaz Y
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
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- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zhang Z
- Zheng Y
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- Zhu B
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- Zhukov V
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- Ziebarth EB
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- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe 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
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
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- Kharchilava A
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- Khurana R
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- Kiesenhofer W
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- Nikitenko A
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- Pompili A
- Pooth O
- Popov A
- Popov V
- Potenza A
- Potenza R
- Pozdnyakov A
- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Quintario Olmeda A
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- Racz A
- Radburn-Smith BC
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- Raidal M
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- Rander J
- Ranjan K
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- Rodozov M
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- Rodriguez-Marrero AY
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- Roland C
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- Safonov A
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- Sarkar S
- Sarycheva L
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- Savin A
- Savrin V
- Scarborough T
- Schaefer C
- Schael S
- Schettler H
- Scheurer A
- Schilling F-P
- Schizzi A
- Schlein P
- Schleper P
- Schlieckau E
- Schmidt A
- Schmidt R
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schul N
- Schum T
- Schwick C
- Scodellaro L
- Searle M
- Seez C
- Segala M
- Segoni I
- Seidel M
- 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
- Sguazzoni G
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- Sharan M
- 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
- Sigamani M
- Sikler F
- Silkworth C
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- Silvers D
- Silverwood H
- Silvestris L
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
- Singh J
- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
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- Smirnov I
- Smirnov V
- Smith J
- Smith JG
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- Smith WH
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
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- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
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- Solano A
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- Sonmez N
- Sonnenschein L
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- Souza MHG
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- Spalding WJ
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- Sparrow A
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- Sperka D
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- Spiga D
- Spiridonov A
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- Staykova Z
- Steggemann J
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- Stephans GSF
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- Stieger B
- Stober FM
- Stoeckli F
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- Stone R
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- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strom D
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- Suarez I
- Sudano E
- Sudhakar K
- Sulak L
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- Sultanov G
- 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
- Tambe N
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- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
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- Tcholakov V
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- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
- Thom J
- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- Tlisov D
- To W
- Toback D
- Tomalin IR
- Tonelli G
- Tonjes MB
- Tonwar SC
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- Topaksu AK
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- Toropin A
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- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Tropiano A
- Troshin S
- Tsamalaidze Z
- 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
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ulrich R
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzunian A
- Vaandering EW
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanelderen L
- Vanini S
- Vanlaer P
- Varela J
- Varelas N
- Vartak A
- Vasquez Sierra R
- Vaughan J
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- Vazquez Acosta M
- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Venditti R
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal Marono M
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Virto AL
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan X
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickramage N
- Widl E
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- 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
- 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
Get PDFA 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe 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
- 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
- Andreev Y
- Andrews W
- Androsov K
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asin I
- Askew A
- Aslanoglou X
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bahtiyar H
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
Get PDFIn 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
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFJet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
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