320 research outputs found
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Modification of the National Weather Service Distributed Hydrologic Model for subsurface water exchanges between grids
- Publication venue
- eScholarship, University of California
- Publication date
- 13/07/2011
- Field of study
To account for spatial variability of precipitation, as well as basin physiographic properties, the National Weather Service (NWS) has developed a distributed version of its hydrologic component, termed the Hydrology Laboratory-Research Distributed Hydrologic Model (HL-RDHM). Because channels are the only source of water exchange between neighboring computational elements, the absence of such exchange has been identified as a weakness in the model. The primary objective of this paper is to modify the model structure to account for subsurface water exchanges without dramatically altering the conceptual framework of the water balance module. The subsurface exchanges are established by partitioning the slow response components released from the lower layer storages into two parts: the first part involves the grid's conceptual channel, while the second is added to the lower layer storages of the downstream pixel. Realizing the deficiency of the water balance module to locate the lower zone layers in sufficient depths, a complementary study is conducted to test the feasibility of further improvement in the modified model by equally shifting downward the lower zone layers of all pixels over the basin. The Baron Fork at Eldon, Oklahoma, is chosen as the test basin. Ten years of grid-based multisensor precipitation data are used to investigate the effects of the modification, plus shifting the lower zone layers on model performance. The results show that the modified-shifted HL-RDHM can markedly improve the streamflow simulations at the interior point, as well as very high peak-flow simulations at the basin's outlet. Copyright 2011 by the American Geophysical Union
Pyrosequencing as a tool for better understanding of human microbiomes
- Author
- Aas JA
- Aas JA
- Ahn J
- Al Masalma M
- Andersson AF
- Armougom F
- Ashraf F. Fouad
- Becker MR
- Bik EM
- Charlson ES
- Clarridge JE
- Cole JR
- Corby PM
- Costello EK
- Crielaard W
- De Filippo C
- De Lillo A
- DeSantis TZ
- Dethlefsen L
- Dethlefsen L
- Dewhirst FE
- Dominguez-Bello MG
- Dowd SE
- Dowd SE
- Edwards RA
- Egert M
- Eid J
- Engelbrektson A
- Faveri M
- Fierer N
- Fierer N
- Finegold SM
- Fouad AF
- Ghannoum MA
- Gonzalez A
- Griffen AL
- Haraszthy VI
- Higuchi R
- Huse SM
- Isabela N. Rôças
- Jakobsson HE
- Jordan JA
- José F. Siqueira
- Kanasi E
- Kazor CE
- Keijser BJ
- Koren O
- Kuczynski J
- Kumar PS
- Kumar PS
- Kunin V
- Larsen N
- Lazarevic V
- Lazarevic V
- Lemos LN
- Ley RE
- Li L
- Ling Z
- Lozupone C
- Luna RA
- Mardis ER
- Metzker ML
- Meyer F
- Munson MA
- Munson MA
- Nakamura S
- Nasidze I
- Olsen I
- Parameswaran P
- Paster BJ
- Paster BJ
- Paster BJ
- Ravel J
- Reeder J
- Relman DA
- Ribeiro AC
- Rothberg JM
- Saito D
- Sakamoto M
- Sakamoto M
- Santos AL
- Schloss PD
- Shendure J
- Siqueira JF
- Siqueira JF
- Siqueira JF
- Smith DM
- Sogin ML
- Sundquist A
- Tringe SG
- Turnbaugh PJ
- Turnbaugh PJ
- Turnbaugh PJ
- Varshney RK
- Voelkerding KV
- Whitman WB
- Wolcott RD
- Wu GD
- Xie G
- Xu J
- Zaura E
- Zhang H
- Publication venue
- Co-Action Publishing
- Publication date
- 01/01/2012
- Field of study
Next-generation sequencing technologies have revolutionized the analysis of microbial communities in diverse environments, including the human body. This article reviews several aspects of one of these technologies, the pyrosequencing technique, including its principles, applications, and significant contribution to the study of the human microbiome, with especial emphasis on the oral microbiome. The results brought about by pyrosequencing studies have significantly contributed to refining and augmenting the knowledge of the community membership and structure in and on the human body in healthy and diseased conditions. Because most oral infectious diseases are currently regarded as biofilm-related polymicrobial infections, high-throughput sequencing technologies have the potential to disclose specific patterns related to health or disease. Further advances in technology hold the perspective to have important implications in terms of accurate diagnosis and more effective preventive and therapeutic measures for common oral diseases
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
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- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
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- Bandyopadhyay A
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- Bannoura AAE
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- Barisits M-S
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- Barklow T
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- Barnovska-Blenessy Z
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- Barreiro Guimarães da Costa J
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- Beddall A
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- Bednyakov VA
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- Benjamin DP
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- Bessidskaia Bylund O
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- Blazek T
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- Bobbink GJ
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- Boonekamp M
- Borecka-Bielska HM
- Borisov A
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- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
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- Campoverde A
- Canale V
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- Cantero J
- Cao T
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- Capeans Garrido MDM
- Caprini I
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- Catmore JR
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- Cervelli A
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- Chafaq A
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- Chargeishvili B
- Charlton DG
- Chau CC
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- Chelkov GA
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- Cheplakov A
- Cheremushkina E
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- Christodoulou V
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- Cueto A
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- Da Cunha Sargedas De Sousa MJ
- Da Via C
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- De Vivie De Regie JB
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- Denysiuk D
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- Di Ciaccio A
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- Diehl EB
- Dietrich J
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- Djuvsland JI
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- Donini J
- Dopke J
- Doria A
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
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- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abhayasinghe Dk
- Abidi Sh
- Abouzeid Os
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- Abramowicz H
- Abreu H
- Abulaiti Y
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- Achkar B
- Adachi S
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- Adamek L
- Adelman J
- Adersberger M
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- Burzynski Jc
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- Buschmann E
- Bussey Pj
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- Buttinger W
- Buxo Vazquez Cj
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- Caforio D
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- Calafiura P
- Calandri A
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- Camarda S
- Camarero Munoz D
- Camarri P
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- Caminal Armadans R
- Camincher C
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- Campoverde A
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- Capua M
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- Wolf Tmh
- Wolff R
- Wolker Rw
- Wollrath J
- Wolter Mw
- Wolters H
- Wong Vws
- Woods Nl
- Worm Sd
- Wosiek Bk
- Wozniak Kw
- Wraight K
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang Hj
- Yang Ht
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- Yang X
- Yang Y
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
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- Yu J
- Yuan R
- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou Ms
- Zhou N
- Zhou Y
- Zhu C
- Zhu Cg
- Zhu H
- Zhu Hl
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine Ni
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
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- Ahmad A
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- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
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- Alimonti G
- Allaire C
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- Allport PP
- Aloisio A
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- Ambler A
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- Amor Dos Santos SP
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- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce ATH
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- Arguin J-F
- Argyropoulos S
- Arling J-H
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- Ciesla KM
- Cindro V
- Cioară IA
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- Cirotto F
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- Ciubotaru DA
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- Clawson SE
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- Connell SH
- Connelly IA
- Conroy EI
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- Cooke HG
- Cooper-Sarkar AM
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- Corrigan EE
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- Costanza F
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- Cowan G
- Cowley JW
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- Creager RA
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- Cristoforetti M
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- Cueto A
- Cuhadar Donszelmann T
- Cui H
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- Czurylo MM
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- de Jong P
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- Zemaityte G
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- Zhemchugov A
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud A Abed
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
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- Zanzi D
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
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- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud A Abed
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alves FL Lucio
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Aranzabal N
- Araya S Tapia
- Arcangeletti C
- Arce ATH
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- Zhemchugov A
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- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- IOP
- Publication date
- 01/01/2021
- Field of study
Non-ionizing energy loss causes bulk damage to the silicon sensors of the ATLAS pixel and strip detectors. This damage has important implications for data-taking operations, charged-particle track reconstruction, detector simulations, and physics analysis. This paper presents simulations and measurements of the leakage current in the ATLAS pixel detector and semiconductor tracker as a function of location in the detector and time, using data collected in Run 1 (2010–2012) and Run 2 (2015–2018) of the Large Hadron Collider. The extracted fluence shows a much stronger |z|-dependence in the innermost layers than is seen in simulation. Furthermore, the overall fluence on the second innermost layer is significantly higher than in simulation, with better agreement in layers at higher radii. These measurements are important for validating the simulation models and can be used in part to justify safety factors for future detector designs and interventions.publishedVersio
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
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- Zhemchugov A
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 28/04/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139fb−1
139
fb
-
1
of data collected by the ATLAS detector at the Large Hadron Collider during pp collisions at s=13TeV
s
=
13
TeV
. The observable measures the different probability of top and antitop quarks to have the higher energy as a function of the jet scattering angle with respect to the beam axis. The energy asymmetry is measured in the semileptonic ttˉ
t
t
¯
decay channel, and the hadronically decaying top quark must have transverse momentum above 350GeV
350
GeV
. The results are corrected for detector effects to particle level in three bins of the scattering angle of the associated jet. The measurement agrees with the SM prediction at next-to-leading-order accuracy in quantum chromodynamics in all three bins. In the bin with the largest expected asymmetry, where the jet is emitted perpendicular to the beam, the energy asymmetry is measured to be −0.043±0.020
-
0.043
±
0.020
, in agreement with the SM prediction of −0.037±0.003
-
0.037
±
0.003
. Interpreting this result in the framework of the Standard Model effective field theory (SMEFT), it is shown that the energy asymmetry is sensitive to the top-quark chirality in four-quark operators and is therefore a valuable new observable in global SMEFT fits
- …