226 research outputs found
The disruption of proteostasis in neurodegenerative diseases
- Author
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- Mayer MP
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- Walker LC LeVine H
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- Zolkiewski M
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2015
- Field of study
Cells count on surveillance systems to monitor and protect the cellular proteome which, besides being highly heterogeneous, is constantly being challenged by intrinsic and environmental factors. In this context, the proteostasis network (PN) is essential to achieve a stable and functional proteome. Disruption of the PN is associated with aging and can lead to and/or potentiate the occurrence of many neurodegenerative diseases (ND). This not only emphasizes the importance of the PN in health span and aging but also how its modulation can be a potential target for intervention and treatment of human diseases.info:eu-repo/semantics/publishedVersio
Effects of rapid urbanisation on the urban thermal environment between 1990 and 2011 in Dhaka Megacity, Bangladesh
- Author
- Adams J
- Ahmed B Kamruzzaman M, Zhu X, et al.
- Artis DA Carnahan WH
- Azad A Kitada T
- Black D Henderson V
- Brown M Lewis HG, Gunn SR
- Carlson TN Arthur ST
- Carlson TN Gillies RR, Perry EM
- Carlson TN Ripley DA
- Carnahan WH Larson RC
- Chander G Markham B
- Chander G Markham BL, Helder DL
- Chen XL Zhao HM, Li P, et al.
- Dewan AM Yamaguchi Y
- Foley JA Defries R, Asner GP, et al.
- Giri C Pengra B, Zhu Z, et al.
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- Hasan S Mulamoottil G
- Hashizume M Dewan AM, Sunahara T, et al.
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- Jiménez-Muñoz JC Sobrino JA
- Kovats S Akhtar H
- Li J Song C, Cao L, et al.
- Li J Wang J, Ma J, et al.
- Li Y Zhang H, Kainz W
- Liu H Weng Q
- Lo CP Quattrochi DA
- Ma Y Kuang Y, Huang N
- Mackey CW Lee X, Smith RB
- Mas J
- Owen TW Carlson TN, Gillies RR
- Patz JA Olson SH
- Qin Z Karnieli A, Berliner P
- Rana MMP
- Roth M Oke TR, Emery WJ
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- Streutker DR
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- Voogt JA Oke TR
- Voogt JA Oke TR
- Weng Q
- Weng Q
- Weng Q Hu X, Lu D
- Weng Q Lu D
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- Wong NH Yu C
- Wu C
- Xiao H Weng Q
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- Xu H Dongfeng L, Tang F
- Yang X Liu Z
- Yow DM
- Yuan F Bauer ME
- Zha Y Gao J, Ni S
- Zhang X Zhong T, Wang K, et al.
- Zhou X Wang YC
- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2017
- Field of study
This study investigates the influence of land-use/land-cover (LULC) change on land surface temperature (LST) in Dhaka Megacity, Bangladesh during a period of rapid urbanisation. LST was derived from Landsat 5 TM scenes captured in 1990, 2000 and 2011 and compared to contemporaneous LULC maps. We compared index-based and linear spectral mixture analysis (LSMA) techniques for modelling LST. LSMA derived biophysical parameters corresponded more strongly to LST than those produced using index-based parameters. Results indicated that vegetation and water surfaces had relatively stable LST but it increased by around 2 °C when these surfaces were converted to built-up areas with extensive impervious surfaces. Knowledge of the expected change in LST when one land-cover is converted to another can inform land planners of the potential impact of future changes and urges the development of better management strategies
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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
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- Aubert B
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- Avolio G
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- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
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- Balek P
- Banas E
- Banerjee P
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- Banfi D
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- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
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- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
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- Barnett BM
- Barnett RM
- Barojas CAC
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartsch V
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- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Bauer F
- Bawa HS
- Beale S
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
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- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Begel M
- Behera PK
- Beimforde N
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- Belenguer AJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
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- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benjarnin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
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- Berlingen JM
- Bernat P
- Bernhard R
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- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
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- Black KM
- Blair RE
- Blanchard J-B
- Blazek T
- Bloch I
- Blocker C
- Blocki J
- Blum W
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- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
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- Boeriu OEV
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
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- Bold T
- Boldea V
- Bolnet NM
- Bomben M
- Bona M
- Boonekamp M
- Bordoni S
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- Borisov A
- Borissov G
- Borjanovic I
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozovic-Jelisavcic I
- Bracinik J
- Branchini P
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brazzale SF
- Brelier B
- Bremer J
- Brendlinger K
- Brenner R
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- Bristow TM
- Britton D
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- Brock I
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- Brooijmans G
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- Bruncko D
- Bruneliere R
- Brunet S
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- Bruschi M
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- Bugge L
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- Bundock AC
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- Buran T
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- Burdin S
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- Busato E
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- Bustos ACF
- Buszello CP
- Butler B
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- Buttar CM
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- Buttinger W
- Byszewski M
- Cabrera Urban S
- Cadfort T
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi H
- Calvet D
- Calvet S
- Camarri P
- Cameron D
- Camillocci ES
- Caminada LM
- Caminal Armadans R
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Cantrill R
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castro NF
- Cataldi C
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani C
- Caughron S
- Cavalcanti TP
- Cavaliere V
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- Cavsinni V
- Ceradini F
- Cerqueira AS
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- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
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- Chapleau B
- Chapman JD
- Chapman JW
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
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- Cheplakov A
- Chernyatin V
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- Chiefari C
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- Childers JT
- Chilingarov A
- Chiodini C
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
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- Sivoklokov SY
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- Sjursen TB
- Skinnari LA
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- Tsukerman II
- Tsulaia V
- Tsung J-W
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- Tua A
- Tudorache A
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- Tuggle JM
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- Urbaniec D
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- Viehhauser GHA
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- Vivarelli I
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- Vladoiu D
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- von Radziewski H
- von Toerne E
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- Zhemchugov A
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- Zobernig G
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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 τ 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, φ, 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 β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Pan-cancer analysis of whole genomes
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- vx Ong
- Vyas
- Vázquez-García
- W. abo
- W. ae
- W. B. xu
- W. bk
- W. g Valencia
- W. ia
- W. K. aav
- W. lf
- W. M. zy
- W. mn
- W. nn
- W. tw
- W. zc
- Waddell
- Waddell
- Wadi L. k
- Wagener
- Wang
- Wang
- Wang
- Wang
- Wang
- Waring
- Warnatz
- Warrell
- Warren
- Weichenhan
- Weinberger
- Weinstein
- Weischenfeldt J. g
- Weisenberger
- Welch
- Wendl M. C. z
- wf Amary
- Whalley
- Wheeler
- wi Futreal
- Wigle
- Wilkerson M. D. v
- Williams
- Wilmott
- Wilson G. W. k
- Wilson R. K. z
- Wintersinger
- Wiznerowicz
- Wolf
- Wong
- Wong
- Woo
- Wood
- Wouters
- Wright
- Wright
- Wright A. J. k
- ws Ang
- Wu
- Wu
- Wu
- wv abg
- wz Hupp
- x Eils
- x Yung
- X. abp
- X. at
- X. bk
- X. cq
- X. ez
- X. ez
- X. fh
- X. fv
- X. fv
- X. fv
- X. fv
- X. k Mbabaali
- X. oi
- X. S. wd
- X. tc
- X. zv
- xb Danilova
- xb Felau
- xc Lovat
- xh Curley
- xh Fulton
- Xi
- Xia
- Xiang
- Xiong
- xo Abeshouse
- xp Benz
- xp Edwards
- xr Ghori
- xs Gundem
- Xue
- xv Luxton
- xw McDermott
- xy Visakorpi
- xz Whitaker
- Y. -E. ot
- Y. -J. k
- Y. -J. xn
- Y. abp
- Y. ae
- Y. ae
- Y. ae
- Y. ae
- Y. ai
- Y. aj
- Y. al
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- Y. dy
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- Y. nk
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- Y. rg
- Y. rj
- Y. rm
- Y. S. jf
- Y. uz
- Y. vr
- Y. wt
- Y. yc
- ya Al-Ahmadie
- Yachida
- Yamaguchi
- Yamaguchi T. N. k
- Yamamoto
- Yamaue
- Yang
- Yang
- Yang
- Yang
- Yang
- Yao
- Yaspo
- Yates
- Yau
- yb Ally
- yd Cherniack
- yd Lai
- yd Schadendorf
- ye Auman
- ye Umbricht
- Yellapantula
- Yellapantula
- yh Bathe
- yj Baylin
- Yoon
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- Yu
- Yu
- Yuan
- Yugawa
- z ah
- Z. ej
- Z. ep
- Z. fr
- Z. hv
- Z. hy
- Z. jq
- Z. kt
- Z. oe
- Zaikova
- Zapatka
- zd Gershenwald
- Zenklusen
- Zeps
- zf Ghossein
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang H. b
- Zhao
- Zheng
- Zhou
- Zhou
- Zhu
- Zhu
- zi zj
- zm Jayaseelan
- Zou
- Zou
- zt Kim
- zw Lewis
- Ó. A. th
- Ø. sk
- 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
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
- MA Halsey
- MA Roder
- MA Rubin
- MA Rubin
- MA Rubin
- MB Martens
- MB Rettig
- MC Caino
- MC Schumacher
- MD Desrosiers
- MD Duff
- MD Lloyd
- ME Blank
- ME Grossmann
- ME Grossmann
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- ME Morrison
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- MH Vaarala
- MK Thomsen
- 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
- 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
- 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 the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV using 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-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
- 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
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
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- Korolkov I
- Korolkova EV
- Korotkov VA
- Kortner O
- Kortner S
- Kostyukhin VV
- Kotov VM
- Kotwal A
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- Zobernig G
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- 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
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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- Zurzolo G
- 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 tt̄W and tt̄Z production cross sections in pp collisions at √s = 8 TeV with the ATLAS detector
- Author
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- Zeng Q
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- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- 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 M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- 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
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The production cross sections of top-quark pairs in association with massive vector bosons have been measured using data from pp collisions at s√ = 8 TeV. The dataset corresponds to an integrated luminosity of 20.3 fb−¹ collected by the ATLAS detector in 2012 at the LHC. Final states with two, three or four leptons are considered. A fit to the data considering the tt̄W and tt̄Z processes simultaneously yields a significance of 5.0σ (4.2σ) over the background-only hypothesis for tt¯Wtt¯W (tt̄Z) production. The measured cross sections are σtt̄W = 369 + 100−91 fb and σtt̄Z = 176 + 58−52 fb. The background-only hypothesis with neither tt̄W nor tt̄Z production is excluded at 7.1σ. All measurements are consistent with next-to-leading-order calculations for the tt̄W and tt̄Z processes
Searches for Higgs boson pair production in the hh→bbττ, γγWW∗, γγbb, bbbb channels with the ATLAS detector
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- Zhemchugov A
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
Searches for both resonant and nonresonant Higgs boson pair production are performed in the hh→bbττ, γγWW∗ final states using 20.3 fb−1 of pp collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of their production is observed and 95% confidence-level upper limits on the production cross sections are set. These results are then combined with the published results of the hh→γγbb, bbbb analyses. An upper limit of 0.69 (0.47) pb on the nonresonant hh production is observed (expected), corresponding to 70 (48) times the SM gg→hh cross section. For production via narrow resonances, cross-section limits of hh production from a heavy Higgs boson decay are set as a function of the heavy Higgs boson mass. The observed (expected) limits range from 2.1 (1.1) pb at 260 GeV to 0.011 (0.018) pb at 1000 GeV. These results are interpreted in the context of two simplified scenarios of the Minimal Supersymmetric Standard Model
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
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- Zhemchugov A
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- Zibell A
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- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zurzolo G
- Zutshi V
- Zwalinski L
- 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
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