1,488 research outputs found
Assessing Disease Activity in Psoriatic Arthritis: A Literature Review
- Author
- A Kavanaugh
- A Kavanaugh
- A Mumtaz
- AB Gottlieb
- AM Orbai
- AW Armstrong
- CT Ritchlin
- D Aletaha
- D Beaton
- D Hughes
- DE Beaton
- E Christophers
- G Kilic
- HY Lin
- J Fransen
- JA Walsh
- JF Merola
- JF Scoggins
- JR Kirwan
- JS Smolen
- K Kaarela
- L Eder
- L Gossec
- L Gossec
- LC Coates
- LC Coates
- LC Coates
- LC Coates
- LC Coates
- LC Coates
- LE Kristensen
- M Bharmal
- M Carlo Di
- MA DβAgostino
- MA Radtke
- MJ Atkinson
- MJ Atkinson
- ML Schaarschmidt
- MM Schoels
- PJ Healy
- PJ Healy
- PJ Mease
- PP Khanna
- PS Helliwell
- PS Helliwell
- PS Helliwell
- R Holland
- R Queiro
- RB Haynes
- S Delestras
- SM Verstappen
- T Fredriksson
- T Taylor
- TY Zhu
- U Kalyoncu
- VP Nell-Duxneuner
- W Tillett
- W Tillett
- W Tillett
- W Zhang
- WP Maksymowych
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Psoriatic arthritis (PsA) is a multifaceted disease, with a high impact on patientsβ psychological and physical well-being. There is increasing recognition that assessment of both clinical aspects of disease and patient identified concerns, such as fatigue, work disability, and treatment satisfaction need to be addressed. Only then can we fully understand disease burden and make well-informed treatment decisions aimed at improving patientsβ lives. In recent years, there has been much progress in the development of unidimensional and composite measures of disease activity, as well as questionnaires capturing the patientβs perspective in psoriatic disease. Despite these advances, there remains disagreement amongst clinicians as to which instruments should be used. As a consequence, they are yet to receive widespread implementation in routine clinical practice. This review aims to summarize currently available clinical and patient-derived assessment tools, which will provide clinicians with a practical and informative resource
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
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- Yamashita S
- Yang BZ
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- Zachariadou K
- Zalewska A
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- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
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- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
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- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- 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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- 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
Observation of associated near-side and away-side long-range correlations in βsNN=5.02ββTeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
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- Zhemchugov A
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ΞΟ) and pseudorapidity (ΞΞ·) are measured in βsNN=5.02ββTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ββΞΌb-1 of data as a function of transverse momentum (pT) and the transverse energy (Ξ£ETPb) summed over 3.1<Ξ·<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|ΞΞ·|<5) βnear-sideβ (ΞΟβΌ0) correlation that grows rapidly with increasing Ξ£ETPb. A long-range βaway-sideβ (ΞΟβΌΟ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small Ξ£ETPb, is found to match the near-side correlation in magnitude, shape (in ΞΞ· and ΞΟ) and Ξ£ETPb dependence. The resultant ΞΟ correlation is approximately symmetric about Ο/2, and is consistent with a dominant cosβ‘2ΞΟ modulation for all Ξ£ETPb ranges and particle pT
Compressed representation of a partially defined integer function over multiple arguments
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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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- 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
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- Ziebarth EB
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- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Cutajar M
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- Czellar S
- D'Agnolo RT
- D'Alessandro R
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- Da Costa EM
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- Karapostoli G
- Karavakis E
- Karchin PE
- Karim M
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- Karjavin V
- Karmgard DJ
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- Kataria SK
- Katkov I
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- Kaufman GN
- Kaur M
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- Kellogg RG
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- Khachatryan V
- Khakzad M
- Khalatyan S
- Khalil S
- Khan A
- Khan WA
- Kharchilava A
- Khatiwada R
- Khotilovich V
- Khukhunaishvili A
- Khurshid T
- Kiesenhofer W
- Killewald P
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- Kinnunen R
- Kirakosyan M
- Kirsanov M
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- Klanner R
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- Klima B
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- Klingebiel D
- Kluge H
- Klukas J
- Klute M
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- Ko W
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- Kodolova O
- Kohli JM
- Kokkas P
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- Korablev A
- Korpela A
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- Kreis B
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- Paoletti S
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- Papageorgiou A
- Pape L
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- Parashar N
- Pardo P
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- Pesaresi M
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- Petrucciani G
- Petrushanko S
- Petyt D
- Pfeiffer A
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- Piccolo D
- Pieri M
- Pierini M
- Pierro GA
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- Pimia M
- Pin A
- Pineda AM
- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Piroue R
- Pivarski J
- Plager C
- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popescu S
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Pugliese G
- Puigh D
- Puljak I
- Punz T
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radicci V
- Ragazzi S
- Rahatlou S
- Rahmat R
- Raics P
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- Rakness G
- Ralich R
- Ralph D
- Ramos FD
- Ramos JP
- Rander J
- Ranieri R
- Rappoccio S
- Raspereza A
- Ratnikov F
- Raupach F
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- Razis PA
- Rebane L
- Rebassoo E
- Redaelli N
- Redjimi R
- Redondo I
- Reeder D
- Regenfus C
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Rhee HB
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Rikova MI
- Riley D
- Rios AAO
- Rivero C
- Rizzi A
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- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rogan C
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- Rohringer H
- Roinishvili V
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romano E
- Romanowska-Rybinska K
- Romero A
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Rose A
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- Roselli G
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Rumerio P
- Rusack R
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- Ryckbosch D
- Ryd A
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- Ryu G
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- Sabes D
- Sabonis T
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- Safarzadeh B
- Safonov A
- Safronov G
- Saha A
- Saini LK
- Saka H
- Sakharov A
- Sakulin H
- Sala L
- Sala S
- Salerno R
- Salur S
- Sammet J
- Sanabria JC
- Sanchez AK
- Sanchez FJ
- Sanchez J
- Sanchez MCDLB
- Sander C
- Sanders DA
- Sanders S
- Sani M
- Santanastasio F
- Santaolalla J
- Santocchia A
- Santoro A
- Sanudo M
- Saoulidou N
- Saout C
- Sarkar S
- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Sawley MC
- Schael S
- Schafer C
- Schettler H
- Scheurer A
- Schieferdecker P
- Schilling FP
- Schlein P
- Schleper P
- Schmidt A
- Schmidt R
- Schmitt M
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schott G
- Schroder M
- Schul N
- Schum T
- Schwandt J
- Schwarz T
- Schwick C
- Scodellaro L
- Scurlock B
- Searle M
- Seez C
- Segala M
- Segneri G
- Segoni I
- 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
- Servoli L
- Sever R
- Sexton-Kennedy E
- Sguazzoni G
- Sharma A
- Sharma A
- Sharma S
- Sharma V
- Sharp P
- Sheldon P
- Shen BC
- Shepherd-Themistocleous CH
- Shi X
- Shin S
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
- Sikler F
- Sill A
- Sillou D
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
- Sim KS
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh JB
- Singh SP
- Singovsky A
- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slabospitsky S
- Slaunwhite J
- Smirnov I
- Smirnov V
- Smith J
- Smith JG
- Smith K
- Smith VJ
- Smith WH
- Smoron A
- Snigirev A
- Snoek H
- Snow GR
- Sobol A
- Sogut K
- Soha A
- Sola V
- Solano A
- Somalwar S
- Son D
- 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
- Spiropulu M
- Sprenger D
- Squires M
- Srivastava AK
- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Steggemann J
- Stein M
- Steinbruck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stober FM
- Stockli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strom D
- Stuart D
- Sturdy J
- Suarez RG
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
- Sun W
- Sung K
- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swain J
- Swanson J
- Swartz M
- Szillasi Z
- Szleper M
- Sznajder A
- Tali B
- Tan R
- Tancini V
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Tavernier S
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Terentyev N
- Teyssier D
- Thea A
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas L
- Thomas M
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- Thomsen J
- Thyssen F
- Timciuc V
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tomei TRFP
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
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- Toropin A
- Torre P
- Tosi M
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- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Trentadue R
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropea P
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tsyganov A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
- Valdez HC
- Valencia F
- Valls N
- Valuev V
- Van Doninck W
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- Van Mechelen R
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Vanelderen L
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- Vankov I
- Vanlaer R
- Varela J
- Varelas N
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- Vartak A
- Vaughan J
- Vavilov S
- Vazquez DD
- Veelken C
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- Velasco M
- Velde CV
- Velkovska J
- Venturi A
- Verdier P
- Verdini PG
- Veresil GI
- Vergili LN
- Vergili M
- Verrecchia P
- Verwilligen R
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Virto A
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Volyanskyy D
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang D
- Wang J
- Wang J
- Wang M
- Wang X
- Wang Z
- Warchol J
- Ward S
- Wardrope D
- Wayne M
- Weber H
- Weber M
- Weber M
- Wehrli L
- Weinberg M
- Weinberger M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Wohri HK
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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 L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Wissing C
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- Won S
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- Wood JS
- Worm SD
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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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
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- Amako K
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- Smizanska M
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- Sodomka J
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- Taiblum N
- Takahashi Y
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- Torchiani I
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- Tyrvainen H
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- Uhrmacher M
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- Underwood DG
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- Varnes EW
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- Vorobel V
- Vorobiev AP
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- Vos M
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- Vossebeld JH
- Vranjes N
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- Vukotic I
- Wagner P
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- Wiglesworth C
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- Xie Y
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- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
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- Yamamoto S
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- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
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- Youssef S
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- Yu J
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- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
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- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhuravlov V
- Zieminska D
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- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of βs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTβ₯20 GeV and pseudorapidities {pipe}Ξ·{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}Ξ·{pipe}<0. 8) for jets with 60β€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2β€{pipe}Ξ·{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. Β© 2013 CERN for the benefit of the ATLAS collaboration
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