215 research outputs found
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
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- Dewan AM Yamaguchi Y
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- Jiménez-Muñoz JC Sobrino JA
- Kovats S Akhtar H
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- 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
- Saaroni H Ben-Dor E, Bitan A, et al.
- Sobrino JA Caselles V, Becker F
- Sobrino JA Jiménez-Muñoz JC, Paolini L
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- Song C Woodcock CE, Seto KC
- 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
- Weng Q Lu D, Schubring J
- Wong NH Yu C
- Wu C
- Xiao H Weng Q
- Xiao R Ouyang Z, Zheng H, et al.
- 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 new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
- Achkar B
- Adachi S
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- Adamczyk L
- Adamek L
- Adelman J
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- Akesson TPA
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- Alberghi GL
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- Aleksandrov IN
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- Zhemchugov A
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- 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
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- CM Clemson
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- CP Gray
- CP Gray
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- CR Mangahas
- CS Bond
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- DS Perez
- DV Makarov
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- E Beitz
- E Beitz
- E Cabuy
- E Fagiani
- E Flannery
- E Geissinger
- E Kikuchi
- E Kruse
- E Sbisa
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- E Tajkhorshid
- EA Ostrander
- EH Feng
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- EM Rosen
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- F Yang
- FS Krause
- G Benga
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- G Blandino
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- G Kaic
- G Kristiansen
- G Kristiansen
- G Kroemer
- G Murugaiyan
- G Petrovics
- G Pirtskhalaishvili
- G Russo
- G Sardana
- G Stirling
- G Tscheudschilsuren
- G Untergasser
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- GF Azzone
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- H Then
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- I Sakai
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- IK Lim
- IL Tourkova
- IM Bachmann
- IM Shih
- IW Reiniger
- IY Dodin
- J Bartkova
- J Edwards
- J Fellenberg
- J Gille
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- J Weiske
- J Xu
- J Yang
- J Yang
- J Zheng
- JA Camargo
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- JK Wahl 3rd
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- JS Butler
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- JT Bishoff
- JT Chang
- JW Denham
- K Armstrong
- K Fujita
- K Ishibashi
- K Ishitani
- K Kami
- K Kasuno
- K Kumagai
- K Mizutani
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- K Ruan
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- K Suzuki
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- K Takahara
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- K Trpkov
- K Yamada
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- L Capparuccia
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- M Aalamian-Matheis
- M Aghaei
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- M Boury-Jamot
- M Boury-Jamot
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- M Chellaiah
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- M Craig
- M Dumas
- M Dundr
- M Esteller
- M Estler
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- M Fukunaga-Kalabis
- M Fukunaga-Kalabis
- M Furuno
- M Gilbert
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- M Hara-Chikuma
- M Hara-Chikuma
- M Hara-Chikuma
- M Hatzfeld
- M Hatzfeld
- M Heenen
- M Ismail
- M Karaivanov
- M Kashani-Sabet
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- O Itzhaki
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- V Molinie
- V Molinie
- V Molinie
- V Molinie
- V Molinie
- V Pekovic
- V Rajaram
- V Samanna
- V Wessagowit
- V Winnepenninckx
- VD Acevedo
- VK Vanguri
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- W Chen
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- W Gade
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- 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
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- Thayer
- The ICGC/TCGA Pan-Cancer Analysis of Whole Genomes Consortium View Correspondence (jump link)
- Thiessen
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- Thomas
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- V. ag
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- vo Taniguchi
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- vq Yamamoto
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- Waddell
- Waddell
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- Warnatz
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- Weinberger
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- Wintersinger
- Wiznerowicz
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- Wright
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- wv abg
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- x Eils
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- xc Lovat
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- Xue
- xv Luxton
- xw McDermott
- xy Visakorpi
- xz Whitaker
- Y. -E. ot
- Y. -J. k
- Y. -J. xn
- Y. abp
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- Y. fv
- Y. gl
- Y. hl
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- Y. hq
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- Y. nh
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- Y. nz
- 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
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- Yang
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- Yellapantula
- yh Bathe
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- Yugawa
- z ah
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- Z. ep
- Z. fr
- Z. hv
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- Z. jq
- Z. kt
- Z. oe
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- 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
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
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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 inclusive cross-section for the production of jets in association with a Z boson in proton-proton collisions at 8 TeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Zaripovas DR
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- Zemaityte G
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- Zenin O
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- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhu HL
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
The inclusive cross-section for jet production in association with a Z boson decaying into an electron–positron pair is measured as a function of the transverse momentum and the absolute rapidity of jets using 19.9 fb −1 of s√=8 TeV proton–proton collision data collected with the ATLAS detector at the Large Hadron Collider. The measured Z + jets cross-section is unfolded to the particle level. The cross-section is compared with state-of-the-art Standard Model calculations, including the next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations, corrected for non-perturbative and QED radiation effects. The results of the measurements cover final-state jets with transverse momenta up to 1 TeV, and show good agreement with fixed-order calculations
Identification of boosted Higgs bosons decaying into b-quark pairs with the ATLAS detector at 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alimonti G
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- Amaral Coutinho Y
- Ambler A
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- Amelung C
- Amidei D
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- Anastopoulos C
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- Angerami A
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- Zaripovas DR
- Zeissner S
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- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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- Zinonos Z
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- Zivkovic L
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2019
- Field of study
This paper describes a study of techniques for identifying Higgs bosons at high transverse momenta decaying into bottom-quark pairs, H→bb¯ , for proton–proton collision data collected by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy s√=13 TeV . These decays are reconstructed from calorimeter jets found with the anti- kt R=1.0 jet algorithm. To tag Higgs bosons, a combination of requirements is used: b-tagging of R=0.2 track-jets matched to the large-R calorimeter jet, and requirements on the jet mass and other jet substructure variables. The Higgs boson tagging efficiency and corresponding multijet and hadronic top-quark background rejections are evaluated using Monte Carlo simulation. Several benchmark tagging selections are defined for different signal efficiency targets. The modelling of the relevant input distributions used to tag Higgs bosons is studied in 36 fb −1 of data collected in 2015 and 2016 using g→bb¯ and Z(→bb¯)γ event selections in data. Both processes are found to be well modelled within the statistical and systematic uncertainties
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
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- Zu Theenhausen HM
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root s=13 TeV with the ATLAS Detector
- Author
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- Aad G
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- Buat Q
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- Buckley AG
- Budagov IA
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- Burmeister I
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- Buschmann E
- Bussey PJ
- Butler JM
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- Buzatu A
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- Bylund OB
- Cabras G
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- Caforio D
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- Calace N
- Calafiura P
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- Calderini G
- Calfayan P
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- Calvet D
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- Cardillo FC
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- Carli T
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- Carra S
- Carrillo-Montoya GD
- Casadei D
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- Casha AF
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castillo IS
- Castillo LRF
- Castro NF
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- Christodoulou V
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- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woniak KW
- Woods NL
- Worm SD
- Wosiek BK
- Wraight K
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenic T
- Zenin O
- Zerwas D
- Zgubic M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
fb
−
1
of proton-proton collision data recorded at a center-of-mass energy of
√
s
=
13
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
σ
fid
=
2.89
+
0.51
−
0.48
(
stat
)
+
0.29
−
0.28
(
syst
)
fb
- …