485 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â 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
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- Achkar B
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- 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 fbâ1 of â 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
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ï lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ï, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Uhlenbrock M
- Uhrmacher M
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- Zaitsev AM
- Zajacova Z
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Oral manifestations of systemic disease
- Author
- A Eguia del Valle
- AM Michalek
- AMT Chau
- AWT Konings
- BC Muzyka
- C Gilvetti
- C Scully
- C Scully
- CF Kuo
- D Capalbo
- D Compilato
- DA Al-Hakeem
- E Cozzani
- E Lindh
- ET Stoopler
- F Lanternier
- FA Santoro
- H Dan
- H LĂ€hteenoja
- HH Xu
- JC Leao
- JG Routsias
- JJ Castillo
- K Kisand
- K Ryan
- K Triantafillidou
- KA Al-Johani
- KG Brooks
- L Capoccia
- L Mandel
- L RadoĂŻ
- LK Jeffers
- LL Patton
- LM Al-Otaibi
- LS Chan
- M Bidarra
- M Kasperkiewicz
- M Sticherling
- M Voulgarelis
- MK Shephard
- MM Nico
- N Aoun
- R Burger-Calderon
- R Iatta
- RS Rao
- S Jurge
- S Said
- S Stojanov
- S. Fedele
- S. R. Porter
- SB Jensen
- SE Ilyas
- SG Fitzpatrick
- SR Porter
- SR Porter
- SR Porter
- SV Lourenço
- T Kelesidis
- TR Reksten
- V Deshpande
- V. Mercadante
- VS Mahajan
- WM Wong
- Y Shacham
- Publication venue
- Publication date
- 10/11/2017
- Field of study
While the majority of disorders of the mouth are centred upon the direct action of plaque, the oral tissues can be subject to change or damage as a consequence of disease that predominantly affects other body systems. Such oral manifestations of systemic disease can be highly variable in both frequency and presentation. As lifespan increases and medical care becomes ever more complex and effective it is likely that the numbers of individuals with oral manifestations of systemic disease will continue to rise. The present article provides a succinct review of oral manifestations of systemic disease. In view of this article being part of a wider BDJ themed issue on the subject of oral medicine, this review focuses upon oral mucosal and salivary gland disorders that may arise as a consequence of systemic disease
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
- I Haritoglou
- 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
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- MH Vaarala
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- MK Thomsen
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- MM Rashid
- MR Rosner
- MS O'Connor
- MS Tretiakova
- MT Kalcioglu
- MT Ling
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- 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
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- PM Lacal
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- PW Kuchel
- PW Lamberti
- Q Lu
- Q Zhou
- R Agarwal
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- 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
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- RJ Webster
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- RP Singh
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- RW DeVere White
- S Ashida
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- S Kyle
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- S Rankin
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- S Satoh
- S Sur
- S Takahashi
- S Takahashi
- S Tancharoen
- S Verdier-Sevrain
- S Yeh
- S Zha
- S Zha
- S Zha
- SA Narod
- SH Lin
- SJ Yeung
- SK Kang
- SL Kong
- SL Zheng
- SM Edwards
- SM Ho
- SM Saparov
- SQ Xie
- SR Alonso
- SS Kadkol
- SV Setzer
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- T Mirtti
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- T Schlomm
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- T Takahashi
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- T Yu
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- TD Prickett
- TH Ecke
- TJ McDonnell
- TJ Park
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- TR Mercer
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- VL Verstraeten
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- 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
Pan-cancer analysis of whole genomes
- Author
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- The ICGC/TCGA Pan-Cancer Analysis of Whole Genomes Consortium View Correspondence (jump link)
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- zt Kim
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- Ă. A. th
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- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
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
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- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Acharya BS
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- Adelman J
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- Zhemchugov A
- Zheng Z
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- 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 cross section for inclusive isolated-photon production in pp collisions at âs=13TeV using the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
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- Allbrooke BMM
- Allen BW
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- Aloisio A
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- Alvarez Piqueras D
- Alviggi MG
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- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yuen SPY
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- Zaidan R
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- Zakharchuk N
- Zalieckas J
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
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- Zerwas D
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- Zhang Z
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- Zhao Y
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- Zhemchugov A
- Zhou B
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fbâ1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Charged-particle distributions at low transverse momentum in âs=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
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- Aad G
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- Abdallah J
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in protonâproton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 ÎŒb â1 ÎŒbâ1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Measurement of the inelastic proton-proton cross section at âs=13 TeV with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
This Letter presents a measurement of the inelastic proton-proton cross section using 60ââÎŒb â1 of pp collisions at a center-of-mass energy âs of 13 TeV with the ATLAS detector at the LHC. Inelastic interactions are selected using rings of plastic scintillators in the forward region (2.0710 â6 , where M X is the larger invariant mass of the two hadronic systems separated by the largest rapidity gap in the event. In this Ο range the scintillators are highly efficient. For diffractive events this corresponds to cases where at least one proton dissociates to a system with M X >13ââGeV . The measured cross section is compared with a range of theoretical predictions. When extrapolated to the full phase space, a cross section of 78.1±2.9ââmb is measured, consistent with the inelastic cross section increasing with center-of-mass energy
- âŠ