298 research outputs found
DNA damage by lipid peroxidation products: implications in cancer, inflammation and autoimmunity
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2017
- Field of study
Oxidative stress and lipid peroxidation (LPO) induced by inflammation, excess metal storage and excess caloric intake cause generalized DNA damage, producing genotoxic and mutagenic effects. The consequent deregulation of cell homeostasis is implicated in the pathogenesis of a number of malignancies and degenerative diseases. Reactive aldehydes produced by LPO, such as malondialdehyde, acrolein, crotonaldehyde and 4-hydroxy-2-nonenal, react with DNA bases, generating promutagenic exocyclic DNA adducts, which likely contribute to the mutagenic and carcinogenic effects associated with oxidative stress-induced LPO. However, reactive aldehydes, when added to tumor cells, can exert an anticancerous effect. They act, analogously to other chemotherapeutic drugs, by forming DNA adducts and, in this way, they drive the tumor cells toward apoptosis. The aldehyde-DNA adducts, which can be observed during inflammation, play an important role by inducing epigenetic changes which, in turn, can modulate the inflammatory process. The pathogenic role of the adducts formed by the products of LPO with biological macromolecules in the breaking of immunological tolerance to self antigens and in the development of autoimmunity has been supported by a wealth of evidence. The instrumental role of the adducts of reactive LPO products with self protein antigens in the sensitization of autoreactive cells to the respective unmodified proteins and in the intermolecular spreading of the autoimmune responses to aldehyde-modified and native DNA is well documented. In contrast, further investigation is required in order to establish whether the formation of adducts of LPO products with DNA might incite substantial immune responsivity and might be instrumental for the spreading of the immunological responses from aldehyde-modified DNA to native DNA and similarly modified, unmodified and/or structurally analogous self protein antigens, thus leading to autoimmunity
Coexistence of the spin-density-wave and superconductivity in the (Ba,K)Fe2As2
- Author
- Chen G. F.
- Ding H.
- Dong J.
- G. Wu
- H. Chen
- Liu C. Samolyuk G. D. Lee Y. Ni N. Kondo T. Santander-Syro A. F. Budko S. L. McChesney J. L. Rotenberg E. Valla T.
- Luetkens H. Klauss H.-H. Kraken M. Litterst F. J. Dellmann T. Klingeler R. Hess C. Khasanov R. Amato A. Baines C.
- Margadonna S. Takabayashi Y. McDonald M. T. Brunelli M. Wu G. Liu R. H. Chen X. H. Prassides K.
- Q. Huang
- R. H. Liu
- Ren Z. A.
- Ren Z. A.
- Ren Z.-A.
- Rotter M. Pangerl M. Tegel M. Johrendt D.
- T. Wu
- Takeshita S. Ryosuke Kadono M. H. Miyazaki M. Koda A. Kamihara Y. Hosono H.
- Wang C.
- Wei Bao
- Wu G.
- X. F. Wang
- X. H. Chen
- Y. L. Xie
- Y. Qiu
- Y. Ren
- Yang L. X. Ou H. W. Zhao J. F. Zhang Y. Shen D. W. Zhou B. Wei J. Chen F. Xu M. He C. et al
- Zhao J. Huang Q. de la Cruz C. Li S. Lynn J. W. Chen Y. Green M. A. Chen G. F. Li G. Li Z.
- Zhao L.
- Publication venue
- 'IOP Publishing'
- Publication date
- 24/07/2008
- Field of study
The relation between the spin-density-wave (SDW) and superconducting order is
a central topic in current research on the FeAs-based high Tc superconductors.
Conflicting results exist in the LaFeAs(O,F)-class of materials, for which
whether the SDW and superconductivity are mutually exclusive or they can
coexist has not been settled. Here we show that for the (Ba,K)Fe2As2 system,
the SDW and superconductivity can coexist in an extended range of compositions.
The availability of single crystalline samples and high value of the energy
gaps would make the materials a model system to investigate the high Tc
ferropnictide superconductivity.Comment: 4 pages, 5 figure
Perspectives on the use of transcriptomics to advance biofuels
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2015
- Field of study
As a field within the energy research sector, bioenergy is continuously expanding. Although much has been achieved and the yields of both ethanol and butanol have been improved, many avenues of research to further increase these yields still remain. This review covers current research related with transcriptomics and the application of this high-throughput analytical tool to engineer both microbes and plants with the penultimate goal being better biofuel production and yields. The initial focus is given to the responses of fermentative microbes during the fermentative production of acids, such as butyric acid, and solvents, including ethanol and butanol. As plants offer the greatest natural renewable source of fermentable sugars within the form of lignocellulose, the second focus area is the transcriptional responses of microbes when exposed to plant hydrolysates and lignin-related compounds. This is of particular importance as the acid/base hydrolysis methods commonly employed to make the plant-based cellulose available for enzymatic hydrolysis to sugars also generates significant amounts of lignin-derivatives that are inhibitory to fermentative bacteria and microbes. The article then transitions to transcriptional analyses of lignin-degrading organisms, such as Phanerochaete chrysosporium, as an alternative to acid/base hydrolysis. The final portion of this article will discuss recent transcriptome analyses of plants and, in particular, the genes involved in lignin production. The rationale behind these studies is to eventually reduce the lignin content present within these plants and, consequently, the amount of inhibitors generated during the acid/base hydrolysis of the lignocelluloses. All four of these topics represent key areas where transcriptomic research is currently being conducted to identify microbial genes and their responses to products and inhibitors as well as those related with lignin degradation/formation.clos
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
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- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Adye T
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- Aguilar-Saavedra JA
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- Akesson TPA
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- Akimov AV
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- Alam MS
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- Aleksandrov IN
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- Yamaguchi H
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- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
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- Yang Z
- Yanush S
- Yao Y
- Yasu Y
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- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
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- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 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 pT≥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 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{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
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
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- 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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- MA Rubin
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- MB Martens
- MB Rettig
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- MK Thomsen
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- 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
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- 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
- S Zha
- S Zha
- S Zha
- SA Narod
- SH Lin
- SJ Yeung
- SK Kang
- SL Kong
- SL Zheng
- SM Edwards
- SM Ho
- SM Saparov
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- SR Alonso
- SS Kadkol
- SV Setzer
- T Dalmay
- T Drewa
- T Hoevel
- T Ishiyama
- T Jamaspishvili
- T Kusumi
- T Litman
- T Ma
- T Mirtti
- T Murakami
- T Oyama
- T Schlomm
- T Schlomm
- T Sheridan
- T Shimizu
- 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 Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovina T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fb−1 of proton-proton collision data at √s =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV using the ATLAS detector
- Author
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- Winklmeier F
- Winter BT
- Wittgen M
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- Wollstadt SJ
- Wolter MW
- Wolters H
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- Wosiek BK
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- Yorita K
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- Yoshihara K
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
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- Zanzi D
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- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb−1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurement of the W±Z boson pair-production cross section in pp collisions at √s=13TeV with the ATLAS detector
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- Zalieckas J
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- Zhemchugov A
- Zhong J
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Search for scalar diphoton resonances in the mass range 65-600 GeV with the ATLAS detector in pp collision data at √s = 8 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
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- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amorim A
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- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
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- Angelozzi I
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- Antonaki A
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- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
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- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Baas A
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
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- Barisonzi M
- Barklow T
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- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
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- Bartsch V
- Bassalat A
- Basye A
- Bates RL
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- Battaglia M
- Battistin M
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- Beauchemin PH
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- Bedikian S
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- Belanger-Champagne C
- Belenguer MJ
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- Bell WH
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- Bellerive A
- Bellomo M
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- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
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- Benjamin DP
- Bensinger JR
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- Bernard C
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- Berry T
- Berta P
- Bertella C
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- Bessidskaia O
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- Blair RE
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- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boddy CR
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- Boek TT
- Boeriu OEV
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- Bogdanchikov AG
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutouil S
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
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- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brazzale SF
- Brelier B
- Brendlinger K
- Brennan AJ
- Brenner R
- Bressler S
- Bret MC
- Bristow K
- Bristow TM
- Britton D
- Brochu FM
- Brock I
- Brock R
- Bromberg C
- Bronner J
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- Brosamer J
- Brost E
- Brown J
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
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- Bruschi M
- Bryngemark L
- Buanes T
- Buat Q
- Bucci F
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Buehrer F
- Buescher D
- Buescher V
- Bueso XP
- Bugge L
- Bugge MK
- Bulekov O
- Bundock AC
- Burckhart H
- Burdin S
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Byszewski M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Calvet D
- Calvet S
- Camarda S
- Cameron D
- Caminada LM
- Campana S
- Campanelli M
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Castaneda-Miranda E
- Castanheira MTD
- Castelli A
- Castillo IS
- Castillo LRF
- Castro NF
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio B
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen L
- Chen S
- Chen X
- Chen Y
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefari G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Chouridou S
- Chow BKB
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
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- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshall J
- Cole B
- Cole S
- Colijn AP
- Collaboration ATLAS
- Collot J
- Colombo T
- Colon G
- Compostella G
- Coniavitis E
- Conidi MC
- Connell SH
- Connelly IA
- Consonni SM
- Consorti V
- Constantinescu S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cuciuc C-M
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darmora S
- Dassoulas JA
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- De Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Deigaard I
- Del Peso J
- Del Prete T
- Delgado AT
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
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- y Garzon GO
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- Yamaguchi Y
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- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A search for scalar particles decaying via narrow resonances into two photons in the mass range 65–600 GeV is performed using 20.3 fb−¹ of √s=8 TeV pp collision data collected with the ATLAS detector at the Large Hadron Collider. The recently discovered Higgs boson is treated as a background. No significant evidence for an additional signal is observed. The results are presented as limits at the 95% confidence level on the production cross section of a scalar boson times branching ratio into two photons, in a fiducial volume where the reconstruction efficiency is approximately independent of the event topology. The upper limits set extend over a considerably wider mass range than previous searches
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