49 research outputs found
Cancer Biomarker Discovery: The Entropic Hallmark
- Author
- A Alcaraz
- A Arabzadeh
- A Bagri
- A Balbin
- A Bantis
- A Ben-Naim
- A Bolander
- A Buhmeida
- A Burykin
- A Chetcuti
- A de Baey
- A Efeyan
- A Eroglu
- A Fabarius
- A Forget
- A Fujita
- A Geirsson
- A Geirsson
- A Geirsson
- A Guffanti
- A Hugel
- A Inoue
- A Isidoro
- A Jang
- A Kollara
- A Kuzmanov
- A Lundqvist
- A Maria McCrohan
- A Marreiros
- A Mendes
- A Mitra
- A Nassar
- A Petitjean
- A Petitjean
- A Pinzon-Charry
- A Richmond
- A Roesch
- A Santinelli
- A Schmidt
- A Shapiro
- A Sreekumar
- A Takeno
- A Urbanucci
- A Winter
- A Yemelyanov
- AA Babiker
- AA Babiker
- AA Tarhini
- AC Dudley
- AD Judge
- AD Ortega
- AG Puebla-Mora
- AH Fox
- AH Fox
- AI Riker
- AJ Liu
- AK Meeker
- AK Panigrahi
- AK Witkiewicz
- AL Cheung
- AL Fachin
- AL Gartel
- AL Okorokov
- AM Craig
- AM Lena
- AM Levin
- AM Tokes
- AP South
- AS Payne
- AS Verkman
- AS Verkman
- AS Verkman
- AS Wierzbicki
- AV Skamrov
- AW Maniccia
- B Cinar
- B Gao
- B Ouyang
- B Ren
- B Ryu
- B Tycko
- B Vukovic
- B Wu
- B Wu
- BD Dimitrov
- BF Gilmore
- BF Goncalves
- BF Skinnider
- BK Zehentner
- BL Adamsen
- BL de Groot
- BR Johnson
- BR Middleman
- BS Strauss
- C Adami
- C Bastide
- C Cao
- C Cybulski
- C Haqq
- C Hayashi
- C Hornig
- C Ivorra
- C Kumar-Sinha
- C Langner
- C Magi-Galluzzi
- C Magi-Galluzzi
- C Muller-Tidow
- C Nessler-Menardi
- C Nunez
- C Pequeux
- C Rajesh
- C Xu
- C Yuli
- CD Sturgis
- CD Truong
- CG Pham
- CG Rogers
- CG Rogers
- CJ Hutchison
- CJ Pronk
- CK Mavis
- CL Stewart
- CL Wu
- CM Caves
- CM Caves
- CM Clemson
- CM Perou
- CP Gray
- CP Gray
- CP Gray
- CR Mangahas
- CS Bond
- D Acehan
- D Bonn
- D Denhardt
- D Fu
- D Gilley
- D Gisselsson
- D Hanahan
- D Javelaud
- D Kroepfl
- D Lodygin
- D Maraldo
- D Ouazia
- D Scadden
- D Wang
- D Wang
- D Wang
- D Weckermann
- D Wodarz
- DA Shoskes
- DA Tennant
- DE Hansel
- DF Gleason
- DG Albertson
- DG Tenen
- DH Palmer
- DJ Darley
- DJ Grignon
- DJ Smit
- DJ Son
- DJ Wong
- DJC MacKay
- DK Koynova
- DK Lee
- DM Kube
- DM Peehl
- DR Wonsey
- DS Perez
- DV Makarov
- DV Makarov
- E Beitz
- E Beitz
- E Cabuy
- E Fagiani
- E Flannery
- E Geissinger
- E Kikuchi
- E Kruse
- E Sbisa
- E Sprecher
- E Tajkhorshid
- EA Ostrander
- EH Feng
- EH Feng
- EM Rosen
- EM Rosen
- EM Schaeffer
- EO Kehinde
- ET Canepa
- EV Vykhovanets
- EY Lin
- EY Tan
- F Bai
- F Bonetto
- F Boralevi
- F Buback
- F Colotta
- F Langer
- F Saad
- F Tas
- F Yang
- FS Krause
- G Benga
- G Bhanot
- G Blandino
- G Buchanan
- G Kaic
- G Kristiansen
- G Kristiansen
- G Kroemer
- G Murugaiyan
- G Petrovics
- G Pirtskhalaishvili
- G Russo
- G Sardana
- G Stirling
- G Tscheudschilsuren
- G Untergasser
- G Venkataraman
- G von Figura
- GA Jarvis
- GE Crooks
- GF Azzone
- GF Ding
- GL Shen-Ong
- GP Bienert
- GQ Daley
- GR Ribeiro
- GS Palapattu
- GV Glinsky
- GV Glinsky
- H Chang-zheng
- H Chen
- H Dzojic
- H Gronberg
- H Haghnegahdar
- H Harant
- H Harlin
- H Kida
- H Li
- H Liu
- H Miyake
- H Nemoto
- H Ostrer
- H Pilch
- H Rangaswami
- H Rangaswami
- H Rangaswami
- H Ren
- H Roca
- H Roca
- H Samaratunga
- H Savli
- H Schlechte
- H Schoder
- H Sheng
- H Sunwoo
- H Then
- H Wang
- H Wang
- HC Lee
- HG Thomas
- HJ Worman
- HL Winfield
- HS Leff
- HT Quan
- HY Vu
- HZ Zhang
- I Agalliu
- I Bae
- I Ben-Porath
- I Grosse
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- I Leav
- I Marinescu
- I Moll
- I Sakai
- IE Wertz
- IK Lim
- IL Tourkova
- IM Bachmann
- IM Shih
- IW Reiniger
- IY Dodin
- J Bartkova
- J Edwards
- J Fellenberg
- J Gille
- J Graells
- J Jaeger
- J Johnson
- J Lammerding
- J Laoukili
- J Lapointe
- J Linden
- J Luo
- J Luo
- J Luo
- J Mandelin
- J Melamed
- J Moser
- J Rangel
- J Rapley
- J Reimand
- J Ruiz-Ederra
- J Schmitz
- J Schultz
- J Soikkeli
- J Stewart
- J Suh
- J Walter-Yohrling
- J Wang
- J Wang
- J Weiske
- J Xu
- J Yang
- J Yang
- J Zheng
- JA Camargo
- JA Douglas
- JA Hackett
- JA Karam
- JA McGrath
- JA McGrath
- JA McGrath
- JA McGrath
- JA Mobley
- JA Pettus
- JB Roche
- JC Cheville
- JD French
- JD Licchesi
- JD Owen
- JE Lai-Cheong
- JE Sleeman
- JE Wilusz
- JG Wen
- JH Lee
- JH Luo
- JJ Brey
- JJ Park
- JJ Raffoul
- JJ Tseng
- JJ Van den Oord
- JK Wahl 3rd
- JL Broers
- JL Herrmann
- JL Phillips
- JM Brandner
- JM Bridger
- JM Cummins
- JM Gonzalez
- JM Lizcano
- JM Muller
- JM Muller
- JM Parrondo
- JM Saffin
- JN Hutchinson
- JN Mubiru
- JN Mubiru
- JN Mubiru
- JP Arbitrario
- JP Clark
- JP Ehlers
- JP Fruehauf
- JP Struewing
- JR Cansino Alcaide
- JR McMillan
- JS Butler
- JS Butler
- JS Fang
- JS Hub
- JS Lee
- JS Mattick
- JS Mattick
- JS Mattick
- JT Bishoff
- JT Chang
- JW Denham
- K Armstrong
- K Fujita
- K Ishibashi
- K Ishitani
- K Kami
- K Kasuno
- K Kumagai
- K Mizutani
- K Namiki
- K Ruan
- K Ruan
- K Shilo
- K Sircar
- K Suzuki
- K Swisshelm
- K Takahara
- K Tani
- K Tokunaga
- K Tomkova
- K Trpkov
- K Yamada
- KA Tasken
- KA Zuhlke
- KH Hoffmann
- KH Tsui
- KL Nastiuk
- KL Simpson
- KL van Golen
- KN Ekdahl
- KP Porkka
- KR Ghani
- KV Prasanth
- L Capparuccia
- L Carlsson
- L Cheng
- L de Meis
- L Galluzzi
- L Kneisel
- L Lessard
- L Li
- L Moro
- L Moro
- L O'Regan
- L Packer
- L Pasini
- L True
- L Verdoucq
- L Verschooten
- L Xu
- L Zheng
- LA Diaz-Martinez
- LB Mora
- LE Clarke
- LE Finlan
- LF Brown
- LF Zerbini
- LL Chen
- LL Smith
- LL Smith
- LM Godsel
- LP Kunju
- M Aalamian-Matheis
- M Aghaei
- M Bakhanashvili
- M Boury-Jamot
- M Boury-Jamot
- M Buxade
- M Chellaiah
- M Cimitan
- M Craig
- M Dumas
- M Dundr
- M Esteller
- M Estler
- M Fabbri
- M Fukunaga-Kalabis
- M Fukunaga-Kalabis
- M Furuno
- M Gilbert
- M Hara-Chikuma
- M Hara-Chikuma
- M Hara-Chikuma
- M Hara-Chikuma
- M Hatzfeld
- M Hatzfeld
- M Heenen
- M Ismail
- M Karaivanov
- M Kashani-Sabet
- M Kato
- M Katoh
- M Kinoshita
- M Korabiowska
- M Kulesz-Martin
- M Lei
- M Lisovsky
- M Marko
- M Mellado
- M Mishima
- M Mockenhaupt
- M Moghaddami
- M Moghaddami
- M Nessling
- M Olsson
- M Onaitis
- M Parisi
- M Schostak
- M Tischkowitz
- M Traka
- M Tribus
- M Varma
- M Venoux
- M Watanabe
- M Yang
- M Yasui
- M Zhou
- M Zhou
- M Zhou
- MA Castro
- MA Chekmareva
- MA Chellaiah
- MA Ficazzola
- MA Halsey
- MA Roder
- MA Rubin
- MA Rubin
- MA Rubin
- MB Martens
- MB Rettig
- MC Caino
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- ME Grossmann
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- MK Thomsen
- MM Petrovic
- MM Rashid
- MR Rosner
- MS O'Connor
- MS Tretiakova
- MT Kalcioglu
- MT Ling
- MT Martin
- MT Sung
- MV Blagosklonny
- MY Lee
- N Bahamontes-Rosa
- N Donin
- N Konishi
- N Lapteva
- N Maeda
- N Nadiminty
- N Rabiau
- N Singh
- NG Hussein
- NI Andreyev
- NJ Fisch
- NV Whittock
- NV Whittock
- O Bettendorf
- O Canbolat
- O Itzhaki
- O Kwon
- OA Rosso
- OW Rokhlin
- P Agre
- P Agre
- P Agre
- P Agre
- P Allavena
- P Berthon
- P Boukamp
- P Cossu-Rocca
- P Dhawan
- P Dhawan
- P Duesberg
- P Duesberg
- P Duesberg
- P Hainaut
- P Ji
- P Karakiewicz
- P Koivisto
- P Roy-Burman
- P Rustin
- P Sini
- P Slijepcevic
- P Sotomayor
- P Sotomayor
- P Steigemann
- P Zhang
- Pablo Moscato
- PD Walden
- PG Gallagher
- PH Gumerlock
- PH Konig
- PI Nedvetsky
- PJ Gray Jr
- PJ Zielie
- PL Chang
- PM Lacal
- PM Lacal
- PM Mordaka
- PM Steijlen
- PT Landsberg
- PT Went
- PU Malmstrom
- PW Kuchel
- PW Lamberti
- Q Lu
- Q Zhou
- R Agarwal
- R Berretta
- R Birnie
- R Bordoni
- R Casalini
- R Das
- R Dobson
- R Halaban
- R Horuk
- R Klimek
- R Klimek
- R Kuefer
- R Lin
- R Mazzucchelli
- R Mukherjee
- R Radosavljevic
- R Rai
- R Sougrat
- RA Craven
- RA Hegele
- RA Sturm
- RA Weinberg
- RC Lee
- RD Ballal
- RD Loberg
- RD Loberg
- RD Loberg
- RD Loberg
- Regina Berretta
- RG Uzzo
- RJ Jin
- RJ Urban
- RJ Webster
- RL Boguslavsky
- RL Shattuck
- RMH Lopez-Ruiz
- RP Ciavarra
- RP Ciavarra
- RP Singh
- RS Weinstein
- RT Nitta
- RW DeVere White
- S Ashida
- S Brychtova
- S Cardinale
- S Das
- S Das
- S Dettwiler
- S Di Cesare
- S Doratiotto
- S Ersoy-Evans
- S Fan
- S Gagos
- S Ghosh
- S Gunia
- S Hanada
- S Hauptmann
- S Hiratsuka
- S Horsburgh
- S Huerta-Yepez
- S Jhavar
- S Jhavar
- S Kuwahara
- S Kyle
- S Landreville
- S Makovets
- S Morohashi
- S Olgac
- S Philip
- S Philip
- S Prislei
- S Rankin
- S Rankin
- S Satoh
- S Sur
- S Takahashi
- S Takahashi
- S Tancharoen
- S Verdier-Sevrain
- S Yeh
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- S Zha
- S Zha
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- SK Kang
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- SL Zheng
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- T Dalmay
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- T Sobolik-Delmaire
- T Sun
- T Takahashi
- T Takeda
- T Thornburg
- T Watanabe
- T Yu
- TB Lewis
- TD Prickett
- TH Ecke
- TJ McDonnell
- TJ Park
- TL Schmit
- TL Schmit
- TO Nielsen
- TR Mercer
- U Brinck
- U Graeven
- U Gruneberg
- UV Wesley
- V Ambros
- V Barak
- V Fradet
- V Molinie
- V Molinie
- V Molinie
- V Molinie
- V Molinie
- V Molinie
- V Pekovic
- V Rajaram
- V Samanna
- V Wessagowit
- V Winnepenninckx
- VD Acevedo
- VK Vanguri
- VL Verstraeten
- W Chen
- W Cosme-Blanco
- W Gade
- W Ritchie
- W Spirkl
- W Tettelbach
- W Wang
- W Weichert
- W Weichert
- W Weichert
- WB Isaacs
- WD Dunsmuir
- WE Naugler
- William C. S. Cho
- WK Kaufmann
- WK Lee
- X Chen
- X Cheng
- X Dong
- X Dong
- X Huang
- X Li
- X Liu
- X Liu
- X Meng
- X Ouyang
- X Tang
- X Wu
- X Zhang
- XJ Yang
- XQ Wang
- Y Bu
- Y Cai
- Y Deng
- Y Ito
- Y Katagiri
- Y Kozuka
- Y Lai
- Y Liu
- Y Lu
- Y Lu
- Y Ohyama
- Y Shav-Tal
- Y Sugiyama
- Y Sun
- Y Wang
- Y Wang
- Y Wu
- Y Yamamoto
- Y Yang
- Y Zhou
- YB Lim
- YC Chao
- YJ Ko
- YL Liu
- YN Liu
- YT Sasaki
- YT Sasaki
- YU Katagiri
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Jiang
- Z Rudzki
- ZA Dotan
- ZR Yurkovetsky
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Background: It is a commonly accepted belief that cancer cells modify their transcriptional state during the progression of the disease. We propose that the progression of cancer cells towards malignant phenotypes can be efficiently tracked using high-throughput technologies that follow the gradual changes observed in the gene expression profiles by employing Shannon's mathematical theory of communication. Methods based on Information Theory can then quantify the divergence of cancer cells' transcriptional profiles from those of normally appearing cells of the originating tissues. The relevance of the proposed methods can be evaluated using microarray datasets available in the public domain but the method is in principle applicable to other high-throughput methods. Methodology/Principal Findings: Using melanoma and prostate cancer datasets we illustrate how it is possible to employ Shannon Entropy and the Jensen-Shannon divergence to trace the transcriptional changes progression of the disease. We establish how the variations of these two measures correlate with established biomarkers of cancer progression. The Information Theory measures allow us to identify novel biomarkers for both progressive and relatively more sudden transcriptional changes leading to malignant phenotypes. At the same time, the methodology was able to validate a large number of genes and processes that seem to be implicated in the progression of melanoma and prostate cancer. Conclusions/Significance: We thus present a quantitative guiding rule, a new unifying hallmark of cancer: the cancer cell's transcriptome changes lead to measurable observed transitions of Normalized Shannon Entropy values (as measured by high-throughput technologies). At the same time, tumor cells increment their divergence from the normal tissue profile increasing their disorder via creation of states that we might not directly measure. This unifying hallmark allows, via the the Jensen-Shannon divergence, to identify the arrow of time of the processes from the gene expression profiles, and helps to map the phenotypical and molecular hallmarks of specific cancer subtypes. The deep mathematical basis of the approach allows us to suggest that this principle is, hopefully, of general applicability for other diseases
Measurement of VH, H â b b ÂŻ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
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- Arce ATH
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- Armitage LJ
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- Castillo FL
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- Wingerter-Seez I
- Winkels E
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- Wittgen M
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- Woelker RW
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- Yallup DP
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- Yildiz HD
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- Yoshihara K
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- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang DF
- Zhang F
- Zhang G
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- 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
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the tÂŻtZ and tÂŻtW cross sections in proton-proton collisions at âs=13âTeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Abulaiti Y
- Acharya BS
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- Adelman J
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- Albert J
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- Aleksa M
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- Zhemchugov A
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- Zobernig G
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- Zou R
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- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (tÂŻt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1ââfbâ1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The tÂŻtZ and tÂŻtW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are ÏtÂŻtZ=0.95±0.08stat±0.10systâpb and ÏtÂŻtW=0.87±0.13stat±0.14systâpb in agreement with the Standard Model predictions. The measurement of the tÂŻtZ cross section is used to set constraints on effective field theory operators which modify the tÂŻtZ vertex
Constraints on mediator-based dark matter and scalar dark energy models using root s= 13 TeV pp collision data collected by the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Zhang F
- Zhang G
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Constraints on selected mediator-based dark matter models and a scalar dark energy model using up to 37 fbâ1sâ = 13 TeV pp collision data collected by the ATLAS detector at the LHC during 2015-2016 are summarised in this paper. The results of experimental searches in a variety of final states are interpreted in terms of a set of spin-1 and spin-0 single-mediator dark matter simplified models and a second set of models involving an extended Higgs sector plus an additional vector or pseudo-scalar mediator. The searches considered in this paper constrain spin-1 leptophobic and leptophilic mediators, spin-0 colour-neutral and colour-charged mediators and vector or pseudo-scalar mediators embedded in extended Higgs sector models. In this case, also sâ = 8 TeV pp collision data are used for the interpretation of the results. The results are also interpreted for the first time in terms of light scalar particles that could contribute to the accelerating expansion of the universe (dark energy).ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW, Austria; FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq, Brazil; FAPESP, Brazil; NSERC, Canada; NRC, Canada; CFI, Canada; CERN; CONICYT, Chile; CAS, China; MOST, China; NSFC, China; COLCIENCIAS, Colombia; MSMT CR, Czech Republic; MPO CR, Czech Republic; VSC CR, Czech Republic; DNRF, Denmark; DNSRC, Denmark; IN2P3-CNRS, CEA-DRF/IRFU, France; SRNSFG, Georgia; BMBF, Germany; HGF, Germany; MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, Israel; Benoziyo Center, Israel; INFN, Italy; MEXT, Japan; JSPS, Japan; CNRST, Morocco; NWO, Netherlands; RCN, Norway; MNiSW, Poland; NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia, Russian Federation; NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS, Slovenia; MIZS, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC, Sweden; Wallenberg Foundation, Sweden; SERI, Switzerland; SNSF, Switzerland; Canton of Bern, Switzerland; Canton of Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE, United States of America; NSF, United States of America; BCKDF, Canada; CANARIE, Canada; CRC, Canada; Compute Canada, Canada; COST, European Union; ERC, European Union; ERDF, European Union; Horizon 2020, European Union; Marie Sk lodowska-Curie Actions, European Union; Investissements d' Avenir Labex and Idex, ANR, France; DFG, Germany; AvH Foundation, Germany; Herakleitos programme; Thales programme; Aristeia programme; EU-ESF, Greece; Greek NSRF, Greece; BSF-NSF, Israel; GIF, Israel; CERCA Programme Generalitat de Catalunya, Spain; Royal Society, United Kingdom; Leverhulme Trust, United KingdomOpen access journalThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at [email protected]
Search for excited electrons singly produced in protonâproton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
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- Affolder AA
- Afik Y
- Agapopoulou C
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
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- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at sâ = 13 TeV via a contact interaction qqÂŻâeeâ is presented. The search uses 36.1 fb â1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqqÂŻ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( ÎœW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the ppâeeââeeqqÂŻ and ppâeeââeÎœW production cross sections as a function of the excited electron mass meâ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Î of the model as a function of meâ . For meâ<0.5 TeV , the lower bound for Î is 11 TeV . In the special case of meâ=Î , the values of meâ<4.8 TeV are excluded. The presented limits on Î are more stringent than those obtained in previous searches
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
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- Abdinov O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zinonos Z
- Zinser M
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
â
â
fb
â
1
of proton-proton collision data recorded at a center-of-mass energy of
â
s
=
13
â
â
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
Ï
fid
=
2.89
+
0.51
â
0.48
(
stat
)
+
0.29
â
0.28
(
syst
)
â
â
fb
Dijet azimuthal correlations and conditional yields in pp and p plus Pb collisions at â{S}^NN=5.02 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of forward-forward and forward-central dijet azimuthal angular correlations and conditional yields in proton-proton (pp) and proton-lead (p + Pb) collisions as a probe of the nuclear gluon density in regions where the fraction of the average momentum per nucleon carried by the parton entering the hard scattering is low. In these regions, gluon saturation can modify the rapidly increasing parton distribution function of the gluon. The analysis utilizes 25 pb^{-1} of pp data and 360 mp^{-1} of p + Pb data, both at {S}^NN=5.02 TeV, collected in 2015 and 2016, respectively, with the ATLAS detector at the Large Hadron Collider. The measurement is performed in the center-of-mass frame of the nucleon-nucleon system in the rapidity range between -4.0 and 4.0 using the two highest transverse-momentum jets in each event, with the highest transverse-momentum jet restricted to the forward rapidity range. No significant broadening of azimuthal angular correlations is observed for forward-forward or forward-central dijets in p + Pb compared to pp collisions. For forward-forward jet pairs in the proton-going direction, the ratio of conditional yields in p + Pb collisions to those in pp collisions is suppressed by approximately 20%, with no significant dependence on the transverse momentum of the dijet system. No modification of conditional yields is observed for forward-central dijets
Combination of Searches for Invisible Higgs Boson Decays with the ATLAS Experiment.
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- Aad G
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- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- Phys Rev Lett
- Publication date
- 01/01/2019
- Field of study
Dark matter particles, if sufficiently light, may be produced in decays of the Higgs boson. This Letter presents a statistical combination of searches for Hâinvisible decays where H is produced according to the standard model via vector boson fusion, Z(ââ)H, and W/Z(had)H, all performed with the ATLAS detector using 36.1ââfb^{-1} of pp collisions at a center-of-mass energy of sqrt[s]=13ââTeV at the LHC. In combination with the results at sqrt[s]=7 and 8Â TeV, an exclusion limit on the Hâinvisible branching ratio of 0.26(0.17_{-0.05}^{+0.07}) at 95%Â confidence level is observed (expected)
Search for heavy charged long-lived particles in the ATLAS detector in 36.1 fbâ1 of proton-proton collision data at âs=13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
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- Annovi A
- Antel C
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- Arabidze G
- Araque JP
- Araya ST
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- Arduh FA
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- Armadans RC
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- Zhemchugov A
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- Ziolkowski M
- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/05/2019
- Field of study
A search for heavy charged long-lived particles is performed using a data sample of
36.1
â
â
fb
â
1
of proton-proton collisions at
â
s
=
13
â
â
TeV
collected by the ATLAS experiment at the Large Hadron Collider. The search is based on observables related to ionization energy loss and time of flight, which are sensitive to the velocity of heavy charged particles traveling significantly slower than the speed of light. Multiple search strategies for a wide range of lifetimes, corresponding to path lengths of a few meters, are defined as model independently as possible, by referencing several representative physics cases that yield long-lived particles within supersymmetric models, such as gluinos/squarks (
R
-hadrons), charginos and staus. No significant deviations from the expected Standard Model background are observed. Upper limits at 95% confidence level are provided on the production cross sections of long-lived
R
-hadrons as well as directly pair-produced staus and charginos. These results translate into lower limits on the masses of long-lived gluino, sbottom and stop
R
-hadrons, as well as staus and charginos of 2000, 1250, 1340, 430, and 1090 GeV, respectively
Measurement of W<sup>±</sup>Z production cross sections and gauge boson polarisation in pp collisions at âs=13 TeV with the ATLAS detector
- Author
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- Aad G
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- Abbott DC
- Abdinov O
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- Charlton DG
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
This work is licensed under a Creative Commons Attribution 4.0 International License.This paper presents measurements of ± production cross sections in pp collisions at a centre-of-mass energy of 13 TeV. The data were collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider, and correspond to an integrated luminosity of 36.1 fbâ1. The ± candidate events are reconstructed using leptonic decay modes of the gauge bosons into electrons and muons. The measured inclusive cross section in the detector fiducial region for a single leptonic decay mode is fid.±âââČââ=63.7± 1.0 (stat.)± 2.3 (syst.)± 1.4 (lumi.) fb, reproduced by the next-to-next-to-leading-order Standard Model prediction of 61.5+1.4â1.3 fb. Cross sections for + and â production and their ratio are presented as well as differential cross sections for several kinematic observables. An analysis of angular distributions of leptons from decays of W and Z bosons is performed for the first time in pair-produced events in hadronic collisions, and integrated helicity fractions in the detector fiducial region are measured for the W and Z bosons separately. Of particular interest, the longitudinal helicity fraction of pair-produced vector bosons is also measured