680 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
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- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su W
- Suchek S
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tame ZPA
- Tamir NM
- Tanaka J
- Tanaka M
- Tanaka R
- Tapprogge S
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor AJ
- Taylor GN
- Taylor W
- Tee AS
- Tehrani FS
- Teixeira-Dias P
- Ten Kate H
- Teoh JJ
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theveneaux-Pelzer T
- Thiele F
- Thomas DW
- Thomas JO
- Thomas JP
- Thompson PD
- Thomsen LA
- Thomson E
- Thorpe EJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CAM
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa KG
- Tomoto M
- Tompkins L
- Tong B
- Tornambe P
- Toro RC
- Torrence E
- Torres H
- Torres RET
- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-L
- Tsiareshka P
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra RT
- Tuts PM
- Tzamarias S
- Tzovara E
- Ucchielli G
- Uchida K
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Vale MAB
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Viaux Maira N
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
f(R) theories
- Author
- A Balcerzak
- A Balcerzak
- A Billyard
- A Borisov
- A Borzou
- A Codello
- A Cooray
- A Cruz-Dombriz de la
- A Cruz-Dombriz de la
- A Cruz-Dombriz de la
- A Dev
- A Einstein
- A Einstein
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Felice De
- A Gruzinov
- A Hindawi
- A Hindawi
- A Iglesias
- A Linde
- A Lue
- A Macorra de la
- A Nicolis
- A Núñez
- A Palatini
- A Riazuelo
- A Shojai
- A Toporensky
- A Upadhye
- A Vilenkin
- AA Starobinsky
- AA Starobinsky
- AA Starobinsky
- AA Starobinsky
- AA Starobinsky
- AA Starobinsky
- AA Starobinsky
- AD Dolgov
- AD Linde
- AE Domínguez
- AF Zakharov
- AG Riess
- AG Riess
- AH Guth
- AI Vainshtein
- AJ Bustelo
- AK Sanyal
- AL Berkin
- AL Erickcek
- AO Barvinsky
- AR Liddle
- AR Liddle
- AR Liddle
- AV Frolov
- AW Brookfield
- B Bertotti
- B Boisseau
- B Jain
- B Li
- B Li
- B Li
- B Li
- B Li
- B Li
- B Li
- B Modak
- B Ratra
- B Vakili
- B Vakili
- B Zwiebach
- BA Bassett
- BA Bassett
- BC Paul
- BM Gripaios
- BM Leith
- BN Breizman
- C Baccigalupi
- C Barragán
- C Brans
- C Cartier
- C Cherubini
- C Corda
- C Corda
- C Deffayet
- C Deffayet
- C Deffayet
- C Deffayet
- C Deffayet
- C Eling
- C Frigerio Martins
- C Lanczos
- C Porto Di
- C Rham de
- C Ringeval
- C Schimd
- C Wetterich
- C-G Shao
- C-P Ma
- CF Kolda
- CG Boehmer
- CG Boehmer
- CG Böhmer
- CSJ Pun
- CW Misner
- D Bazeia
- D Hilbert
- D Huterer
- D Kazanas
- D Kazanas
- D La
- D La
- D Lovelock
- D Polarski
- D Psaltis
- D Wands
- DA Easson
- DF Torres
- DH Lyth
- DJ Eisenstein
- DJ Gross
- DJ Gross
- DN Spergel
- DN Spergel
- DN Vollick
- DN Vollick
- E Babichev
- E Barausse
- E Barausse
- E Bertschinger
- E Dyer
- E Elizalde
- E Elizalde
- E Gunzig
- E Komatsu
- E Komatsu
- E Kretschmann
- E Rosenthal
- ED Stewart
- EJ Copeland
- EJ Copeland
- EJ Weinberg
- EV Linder
- EV Linder
- EW Kolb
- F Bernardeau
- F Briscese
- F Cooper
- F Perrotta
- F Perrotta
- F Schmidt
- F Schmidt
- F Schmidt
- FC Carvalho
- FP Silva
- FR Klinkhamer
- FSN Lobo
- FW Hehl
- G Allemandi
- G Allemandi
- G Allemandi
- G Allemandi
- G Calcagni
- G Calcagni
- G Chirco
- G Cognola
- G Cognola
- G Cognola
- G Dvali
- G Esposito-Farèse
- G Lambiase
- G Magnano
- G Marmo
- G Morandi
- G-B Zhao
- G-B Zhao
- GB Zhao
- GF Smoot
- GFR Ellis
- GFR Ellis
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GJ Olmo
- GN Felder
- GR Dvali
- GR Dvali
- H Davoudiasl
- H Kodama
- H Mohseni Sadjadi
- H Motohashi
- H Oyaizu
- H Oyaizu
- H Sadjadi
- H Yajima
- H-J Schmidt
- HA Buchdahl
- HF Stabenau
- I Antoniadis
- I Laszlo
- I Navarro
- I Navarro
- I Sawicki
- I Thongkool
- I Thongkool
- I Zlatev
- IP Neupane
- IP Neupane
- J García-Bellido
- J Guzik
- J Khoury
- J Khoury
- J Klusoň
- J Klusoň
- J Martin
- J Moldenhauer
- J Novak
- J O’Hanlon
- J Saavedra
- J Santos
- J-C Hwang
- J-C Hwang
- J-C Hwang
- J-C Hwang
- J-C Hwang
- J-C Hwang
- J-M Gérard
- J-P Uzan
- J-Q Xia
- JAR Cembranos
- JC Hwang
- JCC Souza de
- JD Barrow
- JD Barrow
- JD Barrow
- JD Barrow
- JD Barrow
- JD Bekenstein
- JD Bekenstein
- JD Evans
- JF Navarro
- JH Traschen
- JM Bardeen
- JM Bardeen
- JM Bardeen
- JM Cline
- K Atazadeh
- K Atazadeh
- K Bamba
- K Bamba
- K Bamba
- K Bamba
- K Henttunen
- K Hinterbichler
- K Kainulainen
- K Kainulainen
- K Kainulainen
- K Koyama
- K Koyama
- K Koyama
- K Sato
- K Uddin
- K Uddin
- K Yamamoto
- K-I Maeda
- K-I Maeda
- K-I Maeda
- KA Malik
- KN Ananda
- KS Stelle
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Amendola
- L Hui
- L Iorio
- L Järv
- L Knox
- L Kofman
- L Kofman
- L Perivolaropoulos
- L Pogosian
- L Randall
- L Randall
- L Wang
- LA Kofman
- LH Ford
- LM Sokolowski
- M Abdelwahab
- M Akbar
- M Akbar
- M Akbar
- M Alimohammadi
- M Alimohammadi
- M Amarzguioui
- M Bartelmann
- M Borunda
- M Capone
- M Fairbairn
- M Fairbairn
- M Ferraris
- M Fierz
- M Fierz
- M Gasperini
- M Gasperini
- M Gasperini
- M Gasperini
- M Ishak
- M Ishak
- M Ishak
- M Kamionkowski
- M Kolanovic
- M Kolanović
- M Kowalski
- M Kunz
- M Libanov
- M Martinelli
- M Mohseni
- M Parry
- M Porrati
- M Salgado
- M Sami
- M Takada
- M Tegmark
- M Tegmark
- M Viel
- MA Luty
- MB Mijić
- MD Seifert
- ME Soussa
- MES Alves
- ML Ruggiero
- ML Ruggiero
- N Agarwal
- N Arkani-Hamed
- N Bartolo
- N Boulanger
- N Boulanger
- N Chow
- N Deruelle
- N Deruelle
- N Deruelle
- N Deruelle
- N Goheer
- N Goheer
- N Kaloper
- N Kaloper
- N Lanahan-Tremblay
- N Makino
- N Ohta
- ND Birrell
- NH Barth
- NJ Poplawski
- NW McLachlan
- O Bertolami
- O Bertolami
- O Bertolami
- O Mena
- P Astier
- P Binétruy
- P Binétruy
- P Brax
- P Hořava
- P Kanti
- P McDonald
- P Teyssandier
- P Zhang
- P Zhang
- PD Mannheim
- PD Mannheim
- PF Machado
- PG Bergmann
- PG Ferreira
- PJ Steinhardt
- PJ Zhang
- PJE Peebles
- PJE Peebles
- PJE Peebles
- Q Exirifard
- R Bean
- R Brustein
- R Dick
- R Easther
- R Fakir
- R Fakir
- R Gannouji
- R Gannouji
- R Maartens
- R Saffari
- R-G Cai
- RC Souza de
- RC Souza de
- RE Smith
- RH Dicke
- RK Sheth
- RM Wald
- RM Wald
- RP Woodard
- RR Caldwell
- RR Metsaev
- S Alexeyev
- S Baghram
- S Baghram
- S Baghram
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Capozziello
- S Carloni
- S Carloni
- S Carloni
- S Dodelson
- S Fay
- S Fay
- S Kawai
- S Kawai
- S Lee
- S Mendoza
- S Mukohyama
- S Nesseris
- S Nesseris
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Perlmutter
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Tsujikawa
- S Weinberg
- S-F Wu
- S-F Wu
- S-Y Zhou
- SA Appleby
- SA Appleby
- SA Hayward
- SA Hayward
- SA Hayward
- SCC Ng
- SE Perez Bergliaffa
- SF Daniel
- SM Carroll
- SM Carroll
- SM Carroll
- SM Carroll
- SM Carroll
- SM Carroll
- SS Seahra
- SV Ketov
- SW Hawking
- SW Hawking
- SW Hawking
- SY Khlebnikov
- T Chiba
- T Chiba
- T Chiba
- T Chiba
- T Chiba
- T Chiba
- T Clifton
- T Clifton
- T Damour
- T Damour
- T Faulkner
- T Futamase
- T Jacobson
- T Jacobson
- T Kobayashi
- T Kobayashi
- T Kobayashi
- T Koivisto
- T Koivisto
- T Koivisto
- T Koivisto
- T Koivisto
- T Koivisto
- T Multamaki
- T Multamäki
- T Multamäki
- T Multamäki
- T Multamäki
- T Narikawa
- T Padmanabhan
- T Rador
- T Rador
- T Saidov
- T Shiromizu
- T Tamaki
- T Tatekawa
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TP Sotiriou
- TV Ruzmaikina
- U Alam
- U Alam
- U Alam
- U Günther
- U Günther
- V Acquaviva
- V Acquaviva
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Faraoni
- V Miranda
- V Müller
- V Sahni
- V Sahni
- VF Mukhanov
- VF Mukhanov
- VF Mukhanov
- VI Afonso
- W Hu
- W Hu
- W Hu
- W Israel
- WJ Percival
- WL Freedman
- X Wu
- X-D Ji
- XH Meng
- XH Meng
- XH Meng
- Y Bisabr
- Y Ezawa
- Y Fujii
- Y Fujii
- Y Gong
- Y Shtanov
- Y Sobouti
- Y-S Song
- Y-S Song
- Y-S Song
- Y-S Song
- YB Zel’dovich
- YS Song
- YS Song
- Z-K Guo
- Á Cruz-Dombriz de la
- ÉÉ Flanagan
- ÉÉ Flanagan
- ÉÉ Flanagan
- Publication venue
- 'Living Reviews'
- Publication date
- 01/06/2010
- Field of study
Over the past decade, f(R) theories have been extensively studied as one of
the simplest modifications to General Relativity. In this article we review
various applications of f(R) theories to cosmology and gravity - such as
inflation, dark energy, local gravity constraints, cosmological perturbations,
and spherically symmetric solutions in weak and strong gravitational
backgrounds. We present a number of ways to distinguish those theories from
General Relativity observationally and experimentally. We also discuss the
extension to other modified gravity theories such as Brans-Dicke theory and
Gauss-Bonnet gravity, and address models that can satisfy both cosmological and
local gravity constraints.Comment: 156 pages, 14 figures, Invited review article in Living Reviews in
Relativity, Published version, Comments are welcom
Influence of Nanogels on Mechanical, Dynamic Mechanical, and Thermal Properties of Elastomers
- Author
- A Ganguly
- AK Bhowmick
- AK Bhowmick
- Anil K. Bhowmick
- CC Ho
- E Guth
- EH Kerner
- EP Giannelis
- G Kraus
- H Acharya
- HJ Smallwood
- JB Donnet
- JW Cho
- K Sanguansap
- LH Sperling
- M Maiti
- M Maiti
- M Pramanik
- N Nakajima
- N Yerina
- RA Vaia
- RP Singh
- S Kawahara
- S Mitra
- S Mitra
- S Sadhu
- S Varghese
- Santanu Chattopadhyay
- SS Ray
- Suman Mitra
- T Lan
- W Hofman
- WH Waddell
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Bell violation in the sky
- Author
- A Albrecht
- A Albrecht
- A Aspect
- A Aspect
- A Einstein
- A Einstein
- A Einstein
- AA Starobinsky
- AD Linde
- AH Guth
- AH Guth
- AH Guth
- AK Ekert
- BG Christensen
- C Beasley
- C Cheung
- CP Burgess
- CP Burgess
- D Baumann
- D Baumann
- E Silverstein
- E Witten
- E Witten
- E Witten
- E Witten
- G Mandal
- J Maldacena
- JM Bardeen
- JS Bell
- JW Sharman
- LP Grishchuk
- LP Grishchuk
- M Ansmann
- M Franco
- M-A Sakagami
- MA Rowe
- N Gisin
- N Iizuka
- N Itzhaki
- P Basu
- P Basu
- P Martineau
- P Svrcek
- R Horodecki
- Rajeev Singh
- RH Brandenberger
- S Choudhury
- S Choudhury
- S Grblacher
- S Panda
- S Panda
- Sayantan Choudhury
- SJ Freedman
- SR Behbahani
- SR Das
- SR Das
- SR Das
- SR Das
- Sudhakar Panda
- SW Hawking
- T Jennewein
- T Noumi
- T Prokopec
- VF Mukhanov
- VF Mukhanov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the t(t)over-bar production cross section in pp collisions at root s=7 TeV in dilepton final states containing a tau
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdulsalam A
- Adam W
- Adiguzel A
- Adler Volker
- Adzic P
- Agram JL
- Aguilar-Benitez M
- Aguilo E
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- Wissing C
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- Worm SD
- Wrochna G
- Wulz CE
- Xiao H
- Xu M
- Yazgan Efe
- Yu I
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- Zaganidis Nikolaos
- Zalewski P
- Zang J
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- Zhukov V
- Ziebarth EB
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The top quark pair production cross section is measured in dilepton events with one electron or muon, and one hadronically decaying tau lepton from the decay t (t) over bar -> (l nu(l))((sic)(h)nu((sic)))b (b) over bar, (l = e, mu). The data sample corresponds to an integrated luminosity of 2.0 fb(-1) for the electron channel and 2.2 fb(-1) for the muon channel, collected by the CMS detector at the LHC. This is the first measurement of the t (t) over bar cross section explicitly including tau leptons in proton- proton collisions at root s = 7 TeV. The measured value sigma(t (t) over bar) = 143 +/- 14(stat) +/- 22(syst) +/- 3(lumi) pb is consistent with the standard model predictions
Search for a Higgs boson decaying into a b-quark pair and produced in association with b quarks in proton-proton collisions at 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
A search for a neutral Higgs boson decaying to a pair of b quarks, and produced in association with at least one additional b quark, is presented. Multijet final states with three jets identified as originating from b quarks, at least one of which may include a non-isolated muon, are studied. The data used in this analysis correspond to an integrated luminosity of 2.7-4.8 fb(-1), collected by the CMS experiment in proton-proton collisions at the LHC at a center-of-mass energy of 7 TeV. This search is particularly sensitive to Higgs bosons in scenarios of the Minimal Supersymmetric Model (MSSM) with large values of tan beta. No excess over the predicted background from standard model processes is observed. Stringent upper limits on cross section times branching fraction are derived and interpreted as bounds in the MSSM tan beta and m(A) parameter-space. Observed 95% confidence level upper limits reach as low as tang beta approximate to 18 for M-A approximate to 100 GeV
Search for new physics in events with same-sign dileptons and b jets in pp collisions at root s=8 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram JL
- Aguilar Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Aida WL
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
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- Zumerle G
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
A search for new physics is performed using events with isolated same-sign leptons and at least two bottom-quark jets in the final state. Results are based on a sample of proton-proton collisions collected at a center-of-mass energy of 8TeV with the CMS detector and corresponding to an integrated luminosity of 10.5 fb(-1). No excess above the standard model background is observed. Upper limits are set on the number of events from non-standard-model sources and are used to constrain a number of new physics models. Information on acceptance and efficiencies is also provided so that the results can be used to confront an even broader class of new physics models
Search for a W ' or Techni-rho Decaying into WZ in pp Collisions at root s=7 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
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- Akgun B
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- Akin IV
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- Albayrak EA
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- Albrow M
- Alda WL
- Alexander J
- Aliev T
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- Almeida N
- 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
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- Appelt E
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- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
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- Azhgirey I
- Aziz T
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- Baarmand MM
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- Cardaci M
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- Zumerle G
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search is performed in pp collisions at root s 7 TeV for exotic particles decaying via WZ to final states with electrons and muons. The data sample corresponds to an integrated luminosity of approximately 5 fb(-1). No significant excess is observed in the data above the expected standard model background. Upper bounds at 95% confidence level are set on the production cross section of the W' boson described by the sequential standard model and on the W' WZ coupling. W' bosons with masses below 1143 GeV are excluded. Limits are also set in the context of low-scale technicolor models, under a range of assumptions concerning the model parameters
Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in pp collisions at root s=7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Adam W
- Adams JR
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- Adler V
- Adzic P
- Agostino L
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- Aguilar Benitez M
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- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
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- Andreev Y
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- Cooper SI
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- Cortabitarte RV
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Costanza F
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- CREANZA Donato Maria
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cushman P
- Cussans D
- Custodio A
- 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
- Dabrowski A
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- DE FILIPPIS Nicola
- De Gruttola M
- De Guio F
- De La Cruz B
- De La Cruz Burelo E
- 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
- Deisher A
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- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dermenev A
- Dero V
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
A search is presented for physics beyond the standard model (BSM) in final states with a pair of opposite-sign isolated leptons accompanied by jets and missing transverse energy. The search uses LHC data recorded at a center-of-mass energy root s = 7 TeV with the CMS detector, corresponding to an integrated luminosity of approximately 5 fb(-1). Two complementary search strategies are employed. The first probes models with a specific dilepton production mechanism that leads to a characteristic kinematic edge in the dilepton mass distribution. The second strategy probes models of dilepton production with heavy, colored objects that decay to final states including invisible particles, leading to very large hadronic activity and missing transverse energy. No evidence for an event yield in excess of the standard model expectations is found. Upper limits on the BSM contributions to the signal regions are deduced from the results, which are used to exclude a region of the parameter space of the constrained minimal supersymmetric extension of the standard model. Additional information related to detector efficiencies and response is provided to allow testing specific models of BSM physics not considered in this Letter. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of pp collisions at √s=13 TeV with the ATLAS detector
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- Yue L
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- Zabinski B
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- Zakharchuk N
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- Zenin O
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- Zerwas D
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- Zhao H
- Zhao P
- Zhao T
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
The identification of jets originating from quarks and gluons, often referred to as quark/gluon tagging,
plays an important role in various analyses performed at the Large Hadron Collider, as Standard Model measurements and searches for new particles decaying to quarks often rely on suppressing a large gluon-induced background. This paper describes the measurement of the efficiencies of quark/gluon taggers developed within the ATLAS Collaboration, using √s=13 TeV proton–proton collision data with an integrated luminosity of 140 fb-1 collected by the ATLAS experiment. Two taggers with high performances in rejecting jets from gluon over jets from
quarks are studied: one tagger is based on requirements on the number of inner-detector tracks associated with the
jet, and the other combines several jet substructure observables using a boosted decision tree. A method is established to determine the quark/gluon fraction in data, by using quark/gluon-enriched subsamples defined by the jet
pseudorapidity. Differences in tagging efficiency between data and simulation are provided for jets with transverse
momentum between 500 GeV and 2 TeV and for multiple tagger working points
- …
