611 research outputs found
Stage II/III rectal cancer with intermediate response to preoperative radiochemotherapy: Do we have indications for individual risk stratification?
- Author
- A Habr-Gama
- B Michael Ghadimi
- C Rodel
- C Rodel
- CC Earle
- CG Willett
- E Kapiteijn
- EJ Morris
- FL Greene
- G Theodoropoulos
- GJ Chang
- Hans Christiansen
- Heinz Becker
- Hilka Rothe
- HM Quah
- IC Lavery
- ID Nagtegaal
- JE Krook
- JE Tepper
- JK MacFarlane
- JP Gerard
- JW Huh
- Klaus Jung
- L Collette
- Lena C Conradi
- LH Sobin
- M Miyoshi
- MC Kaminsky-Forrett
- MC Steel
- MJ Gosens
- MW Wichmann
- NN Baxter
- O Dworak
- R Fietkau
- R Sauer
- RE Wijesuriya
- RJ Heald
- S Merkel
- TH Kim
- Thilo Sprenger
- Torsten Liersch
- UICC
- W Schmiegel
- YW Kim
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Response to preoperative radiochemotherapy (RCT) in patients with locally advanced rectal cancer is very heterogeneous. Pathologic complete response (pCR) is accompanied by a favorable outcome. However, most patients show incomplete response. The aim of this investigation was to find indications for risk stratification in the group of intermediate responders to RCT.</p> <p>Methods</p> <p>From a prospective database of 496 patients with rectal adenocarcinoma, 107 patients with stage II/III cancers and intermediate response to preoperative 5-FU based RCT (ypT2/3 and TRG 2/3), treated within the German Rectal Cancer Trials were studied. Surgical treatment comprised curative (R0) total mesorectal excision (TME) in all cases. In 95 patients available for statistical analyses, residual transmural infiltration of the mesorectal compartment, nodal involvement and histolologic tumor grading were investigated for their prognostic impact on disease-free (DFS) and overall survival (OS).</p> <p>Results</p> <p>Residual tumor transgression into the mesorectal compartment (ypT3) did not influence DFS and OS rates (p = 0.619, p = 0.602, respectively). Nodal involvement after preoperative RCT (ypN1/2) turned out to be a valid prognostic factor with decreased DFS and OS (p = 0.0463, p = 0.0236, respectively). Persistent tumor infiltration of the mesorectum (ypT3) and histologic tumor grading of residual tumor cell clusters were strongly correlated with lymph node metastases after neoadjuvant treatment (p < 0.001).</p> <p>Conclusions</p> <p>Advanced transmural tumor invasion after RCT does not affect prognosis when curative (R0) resection is achievable. Residual nodal status is the most important predictor of individual outcome in intermediate responders to preoperative RCT. Furthermore, ypT stage and tumor grading turn out to be additional auxiliary factors. Future clinical trials for risk-adapted adjuvant therapy should be based on a synopsis of clinicopathologic parameters.</p
Evaluation of the HadGEM3-A simulations in view of detection and attribution of human influence on extreme events in Europe
- Author
- A Stegehuis
- AB Pezza
- Andrew Ciavarella
- B Christiansen
- B Christiansen
- B Geyer
- B Kirtman
- B Legras
- B Mueller
- B Quesada
- B Rockel
- Bo Christiansen
- C Burke
- C Cassou
- C Deser
- C Rosenzweig
- Carmen Alvarez-Castro
- Cathy Nangini
- CD Jones
- E Kalnay
- F Lott
- FC Lott
- Francisco Doblas-Reyes
- Fraser Lott
- G Hegerl
- Gabriele Hegerl
- Geert Jan van Oldenborgh
- GJ Oldenborgh van
- GJ Oldenborgh van
- H Kapitza
- IC Harris
- Ioana Colfescu
- J Cattiaux
- JM Eden
- Jonathan Eden
- JW Hurrell
- Katharina Klehmet
- KD Williams
- L Alexander
- Laura Wilcox
- LJ Wilcox
- M Hauser
- M Hauser
- M Hirschi
- M Hollander
- Mathias Hauser
- MP Baldwin
- MR Haylock
- N Christidis
- N Christidis
- N Schaller
- NA Rayner
- Nikolaos Christidis
- Nils Hempelmann
- NL Bindoff
- O Angelil
- O Bellprat
- O Bellprat
- O Krueger
- Omar Bellprat
- P Pall
- PA Michelangeli
- PA Stott
- Pascal Yiou
- Peter Stott
- R Haren van
- R Kistler
- R Orth
- R Vautard
- R Vautard
- René Orth
- Robert Vautard
- S Coles
- S Sippel
- Sabine Radanovics
- SE Perkins
- SI Seneviratne
- SI Seneviratne
- SI Seneviratne
- Simon Tett
- Sonia I. Seneviratne
- T Corti
- T Cowan
- T Cowan
- TB McKee
- Tim Cowan
- V Blauhut
- Y Zhao
- YJ Orsolini
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
A detailed analysis is carried out to assess the HadGEM3-A global atmospheric model skill in simulating extreme temperatures, precipitation and storm surges in Europe in the view of their attribution to human influence. The analysis is performed based on an ensemble of 15 atmospheric simulations forced with observed Sea Surface Temperature of the 54 year period 1960-2013. These simulations, together with dual simulations without human influence in the forcing, are intended to be used in weather and climate event attribution. The analysis investigates the main processes leading to extreme events, including atmospheric circulation patterns, their links with temperature extremes, land-atmosphere and troposphere-stratosphere interactions. It also compares observed and simulated variability, trends and generalized extreme value theory parameters for temperature and precipitation. One of the most striking findings is the ability of the model to capture North Atlantic atmospheric weather regimes as obtained from a cluster analysis of sea level pressure fields. The model also reproduces the main observed weather patterns responsible for temperature and precipitation extreme events. However, biases are found in many physical processes. Slightly excessive drying may be the cause of an overestimated summer interannual variability and too intense heat waves, especially in central/northern Europe. However, this does not seem to hinder proper simulation of summer temperature trends. Cold extremes appear well simulated, as well as the underlying blocking frequency and stratosphere-troposphere interactions. Extreme precipitation amounts are overestimated and too variable. The atmospheric conditions leading to storm surges were also examined in the Baltics region. There, simulated weather conditions appear not to be leading to strong enough storm surges, but winds were found in very good agreement with reanalyses. The performance in reproducing atmospheric weather patterns indicates that biases mainly originate from local and regional physical processes. This makes local bias adjustment meaningful for climate change attribution
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anielski J
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche L
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bach M
- Badala A
- Baek YW
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Bari DD
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barros GOVD
- Barroso VC
- Bartke J
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bjelogrlic S
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
- Bornec YL
- Bose S
- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
- Broz M
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camerini P
- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
- Catanescu V
- Cavicchioli C
- Cepila J
- Cerello P
- Cervantes IM
- Chang B
- Chapeland S
- Charvet JL
- Chattopadhyay S
- Chattopadhyay S
- Chawla I
- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chinellato DD
- Chochula P
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Coccetti F
- Colamaria F
- Colella D
- Collaboration ALICE
- Constantin P
- Contin G
- Contreras JG
- Corchero MAD
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cuveland JD
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash A
- Dash S
- Davalos AM
- De S
- Delagrange H
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Diaz AC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
- Dubey AK
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Engel H
- Erasmo GD
- Erdal HA
- Espagnon B
- Estienne M
- Esumi S
- Evans D
- Eyyubova G
- Fabris D
- Faivre J
- Falchieri D
- Falco AD
- Fantoni A
- Fasel M
- Fearick R
- Fedunov A
- Fehlker D
- Feldkamp L
- Felea D
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo MAS
- Filchagin S
- Filho EPDO
- Filho NC
- Finogeev D
- Fionda FM
- Fiore EM
- Floris M
- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
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- Gaardhoje JJ
- Gagliardi M
- Gago A
- Gallio M
- Gangadharan DR
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- Gheata A
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- Giglio CD
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- Gladysz-Dziadus E
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- Godoy DAMD
- Gomez R
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- Grabski V
- Graczykowski LK
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- Harris JW
- Hartig M
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- Hatzifotiadou D
- Hayrapetyan A
- Heckel ST
- Heide M
- Helstrup H
- Herghelegiu A
- Hernandez JFC
- Herrmann N
- Hetland KF
- Hicks B
- Hille PT
- Hippolyte B
- Horaguchi T
- Hori Y
- Hristov P
- Hrivnacova I
- Huang M
- Huber S
- Humanic TJ
- Hwang DS
- Ichou R
- Ilkaev R
- Ilkiv I
- Inaba M
- Incani E
- Innocenti GM
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
- Ivanov A
- Ivanov M
- Ivanov V
- Ivanytskyi O
- Jacholkowski A
- Jacobs PM
- Jancurova L
- Jang HJ
- Jangal S
- Janik MA
- Janik R
- Jayarathna PHSY
- Jena S
- Jirden L
- Jones PG
- Jung H
- Jusko A
- Kaidalov AB
- Kakoyan V
- Kalcher S
- Kalinak P
- Kalisky M
- Kalliokoski T
- Kalweit A
- Kanaki K
- Kang JH
- Kaplin V
- Karampatsos LX
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- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
- Khan MM
- Khan P
- Khan SA
- Khanzadeev A
- Kharlov Y
- Kileng B
- Kim B
- Kim DJ
- Kim DW
- Kim JH
- Kim JS
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- Kim SH
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- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Klay JL
- Klein J
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- Kliemant M
- Kluge A
- Knichel ML
- Knospe AG
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- Kohler MK
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- Kolojvari A
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- Kondratyeva N
- Konevskikh A
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- Kour R
- Kowalski M
- Kox S
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Krawutschke T
- Krelina M
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- Krivda M
- Krizek F
- Krus M
- Kryshen E
- Krzewicki M
- Kucheriaev Y
- Kuhn C
- Kuijer PG
- Kurashvili P
- Kurepin A
- Kurepin AB
- Kuryakin A
- Kushpil S
- Kushpil V
- Kvaerno H
- Kweon MJ
- Kwon Y
- Lakomov I
- Langoy R
- Lara C
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- Lazzeroni C
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- Lehnert J
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- Windelband B
- Yang H
- Yang S
- Yasnopolskiy S
- Yi J
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon J
- Yu W
- Yuan X
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zelnicek P
- Zetina LM
- Zgura IS
- Zhalov M
- Zhang X
- Zhou D
- Zhou F
- Zhou Y
- Zhu X
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Precise measurement of the W-boson mass with the CDF II detector
- Author
- Aaltonen T.
- Abbaneo D
- Adzic P
- Aguilar-Benitez M
- Ahmad M
- Ahmed I
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- Auffray E
- Aurisano A.
- Auzinger G
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- Azhgirey I
- Badgett W.
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- Barnett B. A.
- Barney D
- Barria P.
- Bartos P.
- Battilana C
- Bauce M.
- Bedeschi F.
- Bedoya CF
- Beecher D.
- Behari S.
- Bell AJ
- Bellettini G.
- Bellinger J.
- Belotelov I
- Benedetti D
- Benjamin D.
- Beretvas A.
- Bernet C
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- Bialas W
- Bilinskas MJ
- Binkley M.
- Bisello D.
- Bitioukov S
- Bizjak I.
- Bland K. R.
- Bloch P
- Blumenfeld B.
- Bocci A
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- Bodek A.
- Bolognesi S
- Bondar N
- Boos E
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Breuker H
- Brigliadori L.
- Bromberg C.
- Brona G
- Brucken E.
- Budagov J.
- Budd H. S.
- Bunin P
- Bunkowski K
- Burelo ED
- Burkett K.
- Busetto G.
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- Butler PH
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- Caballero IG
- Cabrillo IJ
- Calamba A.
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- Calderon A
- Calvo E
- Camarda S.
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- Campderros JD
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- Lipeles E.
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- Loginov A.
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- Macpherson A
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- Mattson M. E.
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- McIntyre P.
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- Milosevic J
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- Mukherjee A.
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- Muller Th.
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- Papadimitriou V.
- Paramonov A. A.
- Pardo PL
- Pardos CD
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- Park IC
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- Parracho PGF
- Pashenkov A
- Patrick J.
- Pauletta G.
- Paulini M.
- Paus C.
- Pelayo JP
- Pellett D. E.
- Penzo A.
- Perelygin V
- Perez E
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- Petrilli A
- Petrov P
- Petrov V
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- Pfeiffer A
- Phillips T. J.
- Piacentino G.
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- Pierini M
- Pilot J.
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- Potamianos K.
- Pranko A.
- Prokoshin F.
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- Punzi G.
- Qazi S
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- Rahaman A.
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- Redondo I
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- Renton P.
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- Reyes-Santos MA
- Rhee HB
- Ribeiro PQ
- Riddick T.
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- Rivero CM
- Robson A.
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- Rogers E.
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- Safonov A.
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- Vila I.
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- Wallny R.
- Wallny R.
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- Wester W. C. III
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- Whitehouse B.
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- Wicklund A. B.
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- Wicklund E.
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- Wilbur S.
- Williams H. H.
- Williams H. H.
- Willmott C
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- Wilson J. S.
- Wilson P.
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- Wittich P.
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- Wohri HK
- Wolbers S.
- Wolbers S.
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- Wolfe H.
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- Wright T.
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- Wu X.
- Wu X.
- Wu Z.
- Wu Z.
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- Yamamoto K.
- Yamaoka J.
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- Yang T.
- Yang U. K.
- Yang U. K.
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- Yang Y. C.
- Yao W. -M.
- Yao W. -M.
- Yeh G. P.
- Yeh G. P.
- Yi K.
- Yi K.
- Yoh J.
- Yoh J.
- Yorita K.
- Yorita K.
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- Yoshida T.
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- Yu G. B.
- Yu I
- Yu I.
- Yu I.
- Yu S. S.
- Yu S. S.
- Yun J. C.
- Yun J. C.
- Zalewski R
- Zanetti A.
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- Zarubin A
- Zeng Y.
- Zeng Y.
- Zhokin A
- Zhou C.
- Zucchelli S..
- Zucchelli S..ng S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We have measured the W-boson mass MW using data corresponding to 2.2/fb of
integrated luminosity collected in proton-antiproton collisions at 1.96 TeV
with the CDF II detector at the Fermilab Tevatron collider. Samples consisting
of 470126 W->enu candidates and 624708 W->munu candidates yield the measurement
MW = 80387 +- 12 (stat) +- 15 (syst) = 80387 +- 19 MeV. This is the most
precise measurement of the W-boson mass to date and significantly exceeds the
precision of all previous measurements combined
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
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
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- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
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- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
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- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
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- Yilmaz Y
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- Zanetti M
- Zang J
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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 CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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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
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
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- Adiguzel A
- Adler V
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- Agram JL
- Aguilar-Benitez M
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- Ahmad WH
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- Bilki B
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- Breedon R
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- Brigliadori L
- Brigljevic V
- Broccolo G
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
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- Brun H
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- Butler PH
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- Caballero IG
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon A
- Cali IA
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- Caminada L
- Campagnari C
- Campbell A
- Campderros JD
- Camporesi T
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- Chang YH
- Chang YH
- Chang YW
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- Chao Y
- Charaf O
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- Chatterjee A
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- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cifuentes JAB
- Cihangir S
- Cimmino A
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Cole P
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- Collard C
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- Conetti S
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- Cooper SI
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- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- David A
- Davids M
- Davies G
- De Araujo FTD
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Palma M
- De Roeck A
- De Souza SF
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Debreczeni G
- Deisher A
- Deiters K
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- Zumerle G
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- 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
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
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- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- 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
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- Zeuner WD
- Zeyrek M
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- Zheng Y
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- Zhukov V
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- 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
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- Abbiendi G
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- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- 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
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
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- Acosta JG
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- Schott G
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- Shoaib M
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- Ujvari B
- Ulmer KA
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- Uzunian A
- Vaandering EW
- Valls N
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- Veszpremi V
- Vesztergombi G
- Veverka J
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- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Virto AL
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vizan Garcia JM
- Vlasov E
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- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
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- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
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- Wakefield S
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- Waltenberger W
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- Wayand S
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- Weber HA
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- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- Wenger EA
- Werner JS
- West C
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- 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
A 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
- …