337 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
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- Achkar B
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- Vadla KOH
- Vaidya A
- Valderanis C
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- Valentinetti S
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- Vallance RA
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- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vaniachine A
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- Vasquez GA
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- Vazquez JGP
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- Verducci M
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- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
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- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- 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
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- 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 M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- 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 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Patterns of Loss and Regeneration of Tropical Dry Forest in Madagascar: The Social Institutional Context
- Author
- A Bertrand
- AF Richard
- B Locatelli
- CA Kull
- CB Barrett
- CC Gibson
- CD Clark
- Chantal Radimilahy
- CM Tucker
- DM Olson
- E Lambin
- E Ostrom
- E Ostrom
- EF Lambin
- Elisabeth Rabakonandrianina
- F Achard
- Fanambinantsoa Rakotondrasoa
- G Heurtebize
- G Sheperd
- GM Green
- GW Luck
- HR Grau
- IM Turner
- J Fairhead
- J Kaufmann
- J Koechlin
- J Swift
- JB Pascarella
- JB Pascarella
- JWJ Rouse
- K McGarigal
- KA Brown
- KJ Willis
- KS Bawa
- L-JR Raharison
- M Fenn
- M Holmgren
- M Leach
- M Tengö
- M Tiffen
- M Westoby
- Maria Tengö
- Markku Pyykönen
- Michael Somers
- MR Guariguata
- N Seddon
- NR Horning
- OA Ramirez
- P Henderson
- R Battistini
- R Rabesandratana
- R Watson
- RE Dewar
- RL Chazdon
- RR Dunn
- RW Sussman
- RW Sussman
- RW Sussman
- S Kvale
- T Casse
- T Dietz
- T Elmqvist
- Thomas Elmqvist
- TK Rudel
- TM Lillesand
- W McConnell
- WB Cohen
- WL Silver
- Publication venue
- Public Library of Science
- Publication date
- 02/05/2007
- Field of study
Loss of tropical forests and changes in land-use/land-cover are of growing concern worldwide. Although knowledge exists about the institutional context in which tropical forest loss is embedded, little is known about the role of social institutions in influencing regeneration of tropical forests. In the present study we used Landsat images from southern Madagascar from three different years (1984, 1993 and 2000) and covering 5500 km(2), and made a time-series analysis of three distinct large-scale patterns: 1) loss of forest cover, 2) increased forest cover, and 3) stable forest cover. Institutional characteristics underlying these three patterns were analyzed, testing the hypothesis that forest cover change is a function of strength and enforcement of local social institutions. The results showed a minor decrease of 7% total forest cover in the study area during the whole period 1984â2000, but an overall net increase of 4% during the period 1993â2000. The highest loss of forest cover occurred in a low human population density area with long distances to markets, while a stable forest cover occurred in the area with highest population density and good market access. Analyses of institutions revealed that loss of forest cover occurred mainly in areas characterized by insecure property rights, while areas with well-defined property rights showed either regenerating or stable forest cover. The results thus corroborate our hypothesis. The large-scale spontaneous regeneration dominated by native endemic species appears to be a result of a combination of changes in precipitation, migration and decreased human population and livestock grazing pressure, but under conditions of maintained and well-defined property rights. Our study emphasizes the large capacity of a semi-arid system to spontaneously regenerate, triggered by decreased pressures, but where existing social institutions mitigate other drivers of deforestation and alternative land-use
Exploitation of Herpesvirus Immune Evasion Strategies to Modify the Immunogenicity of Human Mesenchymal Stem Cell Transplants
- Author
- A Bartholomew
- A Corcione
- A Daga
- A Rehm
- A Uccelli
- A Zdoroveac
- AD Hislop
- AD LipiĆska
- AM Rodriguez
- Anabel S. de la Garza-Rodea
- Antoine A. F. de Vries
- AS de la Garza-Rodea
- CC Leong
- CL Hsieh
- D Faustman
- D Horst
- D Koppers-Lalic
- D Koppers-Lalic
- Derya Unutmaz
- Dirk W. van Bekkum
- EF Eppens
- EJ Wiertz
- EJ Wiertz
- EJ Wiertz
- Emmanuel J. H. J. Wiertz
- F Morandi
- F Tögel
- G Chen
- GC Hassink
- GM Spaggiari
- GW Wilkinson
- HE Farrell
- Hester Boersma
- HG Ljunggren
- I Rasmusson
- Ietje van der Velde-van Dijke
- J Loureiro
- J van Tuyn
- J van Tuyn
- J Zhang
- JR Smith
- JS Orange
- K Le Blanc
- K Le Blanc
- K Le Blanc
- K Lee
- K Viswanathan
- L Montoliu
- L Zangi
- M Chopp
- M Compte
- M Di Nicola
- MA Gonçalves
- Marieke C. Verweij
- MF Pittenger
- MT Barel
- MT Barel
- MT Barel
- MT Barel
- MT Vossen
- MZ Dewan
- N Eliopoulos
- N Eliopoulos
- N Kotobuki
- O Ringdén
- P Pakzaban
- PA Sotiropoulou
- R Ramasamy
- R Romieu-Mourez
- Rob C. Hoeben
- RP Machold
- S Gasser
- S KnaÀn-Shanzer
- S KnaÀn-Shanzer
- S Li
- S Swift
- Shoshan KnaÀn-Shanzer
- T Kojaoghlanian
- TB Prigozhina
- TH Hansen
- TJ Radosevich
- TM Coyne
- VK Jain
- WM Duan
- XX Jiang
- Y Wang
- Y Ye
- Z Xia
- Publication venue
- Public Library of Science
- Publication date
- 06/01/2011
- Field of study
BACKGROUND: Mesenchymal stem cells (MSCs) are multipotent cells residing in the connective tissue of many organs and holding great potential for tissue repair. In culture, human MSCs (hMSCs) are capable of extensive proliferation without showing chromosomal aberrations. Large numbers of hMSCs can thus be acquired from small samples of easily obtainable tissues like fat and bone marrow. MSCs can contribute to regeneration indirectly by secretion of cytokines or directly by differentiation into specialized cell types. The latter mechanism requires their long-term acceptance by the recipient. Although MSCs do not elicit immune responses in vitro, animal studies have revealed that allogeneic and xenogeneic MSCs are rejected. METHODOLOGY/PRINCIPAL FINDINGS: We aim to overcome MSC immune rejection through permanent down-regulation of major histocompatibility complex (MHC) class I proteins on the surface of these MHC class II-negative cells through the use of viral immune evasion proteins. Transduction of hMSCs with a retroviral vector encoding the human cytomegalovirus US11 protein resulted in strong inhibition of MHC class I surface expression. When transplanted into immunocompetent mice, persistence of the US11-expressing and HLA-ABC-negative hMSCs at levels resembling those found in immunodeficient (i.e., NOD/SCID) mice could be attained provided that recipients' natural killer (NK) cells were depleted prior to cell transplantation. CONCLUSIONS/SIGNIFICANCE: Our findings demonstrate the potential utility of herpesviral immunoevasins to prevent rejection of xenogeneic MSCs. The observation that down-regulation of MHC class I surface expression renders hMSCs vulnerable to NK cell recognition and cytolysis implies that multiple viral immune evasion proteins are likely required to make hMSCs non-immunogenic and thereby universally transplantable
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- 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
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya S Tapia
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimaraes da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Bell AS
- Bella G
- Bella L Aperio
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Bertsche C
- Besjes GJ
- Bessner M
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier Dr
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boeriu OE Vickey
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
- Brandt O
- Braren F
- Bratzler U
- Brau B
- Brau JE
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret M Cano
- Briglin DL
- Bristow TM
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher D
- Buescher V
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I Turk
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cantero J
- Cao T
- Cao Y
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo F
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo LR Flores
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
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- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to ÏÎœ using proton-proton collisions at âs=13 TeV produced by the Large Hadron Collider is presented. Only Ï-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fbâ1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible ÏÎœ production cross section. Heavy WâČ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2â3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Combined measurement of differential and total cross sections in the HâŻââŻÎłÎł and the HâŻââŻZZ*âŻââŻ4â decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
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- Ahmadov F
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- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
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- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Zobernig G
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- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fbâ1 of 13 TeV protonâproton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured Hâγγ and HâZZ*(â4â event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0â5.9 +6.0 (stat.) â3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for the direct production of charginos and neutralinos in final states with tau leptons in âs=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
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- Zalieckas J
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- Zeng JC
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- Zhemchugov A
- Zhou B
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zivkovic L
- Zobernig G
- Zoccoli A
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- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fbâ1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ËÏ+1 ËÏâ1 pair production and of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the Ë ÏL state is set to be halfway between the masses of the Ëϱ1 and the ËÏ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ËÏ+1 ËÏâ1 for a massless ËÏ01. Common Ëϱ1 and ËÏ02 masses up to 760 GeV are excluded in the case of production of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 assuming a massless ËÏ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the Ëϱ1 and the ËÏ01 are also studied by varying the Ë ÏL mass between the masses of the Ëϱ1 and the ËÏ01
Performance of missing transverse momentum reconstruction with the ATLAS detector using protonâproton collisions at âs = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- 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
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in protonâproton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying Ï -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fbâ1
Measurement of differential cross sections and W + /W â cross-section ratios for W boson production in association with jets at âs =8 TeV with the ATLAS detector
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- Zhemchugov A
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- Zibell A
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- Zimmermann C
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W â cross-section ratio, both in association with jets, in proton--proton collisions at s â =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb â1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W â the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Measurement of the cross section for inclusive isolated-photon production in pp collisions at âs=13TeV using the ATLAS detector
- Author
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- Aad G
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- Lapertosa A
- Laplace S
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Lau TS
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
- Le B
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee GR
- Lee L
- Lee SC
- Lefebvre B
- Lefebvre G
- Lefebvre M
- Legger F
- Leggett C
- Lei X
- Leight WA
- Leite MAL
- Leitner R
- Lellouch D
- Lemmer B
- Leney KJC
- Lenz T
- Lenzi B
- Leone R
- Leone S
- Leonidopoulos C
- Lerner G
- Leroy C
- Les R
- Lesage AAJ
- Lester CG
- Levchenko M
- Leveque J
- Levin D
- Levinson LJ
- Levy M
- Lewis D
- Li B
- Li C
- Li H
- Li L
- Li Q
- Li Q
- Li S
- Li X
- Li Y
- Liang Z
- Liberti B
- Liblong A
- Lie K
- Liebal J
- Liebig W
- Limosani A
- Lin CY
- Lin K
- Lin SC
- Lin TH
- Linck RA
- Lindquist BE
- Lionti AE
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
- Litke AM
- Liu B
- Liu H
- Liu H
- Liu J
- Liu JB
- Liu JKK
- Liu K
- Liu L
- Liu M
- Liu Y
- Liu YL
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loebinger FK
- Loesle A
- Loew KM
- Lohse T
- Lohwasser K
- Lokajicek M
- Long BA
- Long JD
- Long RE
- Longo L
- Looper KA
- Lopez JA
- Lorenz J
- Losada M
- Losel PJ
- Lou X
- Lounis A
- Love J
- Love PA
- Loyola JES
- Lu H
- Lu N
- Lu YJ
- Lubatti HJ
- Luci C
- Lucotte A
- Luedtke C
- Luehring F
- Lukas W
- Luminari L
- Lund-Jensen B
- Lundberg O
- Lutz MS
- Luzi PM
- Lynn D
- Lysak R
- Lytken E
- Lyu F
- Lyubushkin V
- Ma H
- Ma LL
- Ma Y
- Maccarrone G
- Macchiolo A
- Macdonald CM
- Macek B
- Machado Miguens J
- Madaffari D
- Madar R
- Madden WDB
- Mader WF
- Madsen A
- Madysa N
- Maeda J
- Maeland S
- Maeno T
- Maettig P
- Maevskiy AS
- Magerl V
- Maiani C
- Maidantchik C
- Maier T
- Maio A
- Maira NV
- Majersky O
- Majewski S
- Makida Y
- Makovec N
- Malaescu B
- Malecki P
- Maleev VP
- Malek F
- Mallik U
- Malon D
- Malone C
- Maltezos S
- Malyukov S
- Mamuzic J
- Mancini G
- Mandic I
- Maneira J
- Manghi FL
- Manh TN
- Manhaes de Andrade Filho L
- Mankinen KH
- Mann A
- Manousos A
- Mansoulie B
- Mansour JD
- Mantifel R
- Mantoani M
- Manzoni S
- Mapelli L
- Marceca G
- March L
- Marchese L
- Marchiori G
- Marcisovsky M
- Marjanovic M
- Marley DE
- Marroquima F
- Marsden SP
- Marshall Z
- Martensson MUF
- Marti-Garcia S
- Martin CB
- Martin TA
- Martin VJ
- Martin-Haugh S
- Martinez M
- Martinez NL
- Martoiu VS
- Martyniuk AC
- Marzin A
- Masetti L
- Mashimo T
- Mashinistov R
- Masik J
- Maslennikov AL
- Mason LH
- Massa L
- Mastrandrea P
- Mastroberardino A
- Masubuchi T
- Maurer J
- Maxfield SJ
- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- Mc Fadden NC
- Mc Goldrick G
- Mc Kee SP
- McCarn A
- McCarthy RL
- McCarthy TG
- McClymont LI
- McDonald EF
- Mcfayden JA
- Mchedlidze G
- McMahon SJ
- McNamara PC
- McNicol CJ
- McPherson RA
- Meehan S
- Megy TJ
- Mehlhase S
- Mehta A
- Meideck T
- Meier K
- Meirose B
- Melini D
- Mellado Garcia BR
- Mellenthin JD
- Melo M
- Meloni F
- Melzer A
- Menary SB
- Meng L
- Meng XT
- Mengarelli A
- Menke S
- Meoni E
- Mergelmeyer S
- Merino JL
- Merlassino C
- Mermod P
- Merola L
- Meroni C
- Merritt FS
- Messina A
- Metcalfe J
- Mete AS
- Meyer C
- Meyer J
- Meyer J-P
- Miano F
- Middleton RP
- Miglioranzi S
- Mijovic L
- Mikenberg G
- Mikestikova M
- Mikuz M
- Milesi M
- Milic A
- Millar DA
- Miller DW
- Mills C
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minami Y
- Minashvili IA
- Mincer AI
- Mindur B
- Mineev M
- Minegishi Y
- Ming Y
- Miotto GL
- Mir LM
- Mirto A
- Mistry KP
- Mitani T
- Mitrevski J
- Mitsou VA
- Miucci A
- Miyagawa PS
- Mizukami A
- Mjoernmark JU
- Mkrtchyan T
- Mlynarikovan M
- Moa T
- Mochizuki K
- Moenig K
- Mogg P
- Mohapatra S
- Molander S
- Moles-Valls R
- Mondragon MC
- Monk J
- Monnier E
- Montalbano A
- Monticelli F
- Monzani S
- Moore RW
- Morange N
- Moreno D
- Morettini P
- Morgenstern S
- Mori D
- Mori T
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Mornacchi G
- Morris JD
- Morvaj L
- Moschovakos P
- Mosidze M
- Moss HJ
- Moss J
- Motohashi K
- Mount R
- Mountricha E
- Moyse EJW
- Muanza S
- Mueller J
- Mueller RSP
- Muellerm F
- Muenstermann D
- Mullen P
- Mullier GA
- Murray WJ
- Musheghyan H
- Muskinja M
- Myagkov AG
- Myska M
- Nachman BP
- Nackenhorst O
- Nagai K
- Nagai R
- Nagano K
- Nagasaka Y
- Nagata K
- Nagel M
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nakamura T
- Nakano I
- Narayan R
- Naryshkin I
- Naumann T
- Navarro G
- Navarro JLLR
- Nayyar R
- Neal HA
- Nechaeva PY
- Neep TJ
- Negri A
- Negrini M
- Nektarijevic S
- Nellist C
- Nelson A
- Nelson ME
- Nemecek S
- Nemethy P
- Nessi M
- Neubauer MS
- Neumann M
- Newman PR
- Ng TY
- Ng YS
- Nickerson RB
- Nicolaidou R
- Nielsen J
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Ninomiya Y
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Noccioli EB
- Noguchi Y
- Nomachi M
- Nomidis I
- Nomura MA
- Nooney T
- Nordberg M
- Norjoharuddeen N
- Novgorodova O
- Nozaki M
- Nozka L
- Ntekas K
- Nurse E
- Nuti F
- O'connor K
- O'Neil DC
- O'Rourke AA
- O'Shea V
- Oakham FG
- Oberlack H
- Obermann T
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
- Oda S
- Odaka S
- Oh A
- Oh SH
- Ohm CC
- Ohman H
- Oide H
- Okawa H
- Okumura Y
- Okuyama T
- Olariu A
- Oleiro Seabra LF
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onogi K
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Oren Y
- Orestano D
- Orlando N
- Orr RS
- Ortiz NGG
- Osculati B
- Ospanov R
- Otero y Garzon G
- Otono H
- Ouchrif M
- Ould-Saada F
- Ouraou A
- Oussoren KP
- Outschoorn VIM
- Ouyang Q
- Owen M
- Owen RE
- Ozcan VE
- Ozturk N
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- Padilla Aranda C
- Paganini M
- Pages AP
- Paige F
- Palacino G
- Palazzoa S
- Palestini S
- Palka M
- Pallin D
- Panagoulias I
- Pandini CE
- Pani P
- Panitkin S
- Pantea D
- Paolozzi L
- Papadopoulou TD
- Papageorgiou K
- Paramonov A
- Parker AJ
- Parker KA
- Parker MA
- Parodi F
- Parsons JA
- Parzefall U
- Pascuzzi VR
- Pasner JM
- Pasqualucci E
- Passaggio S
- Pastor ET
- Pastore F
- Pataraia S
- Pater JR
- Pauly T
- Paz IL
- Pearson B
- Pedraza Lopez S
- Pedro R
- Peleganchuk SV
- Penc O
- Peng C
- Peng H
- Penwell J
- Peralva BS
- Perego MM
- Perepelitsa DV
- Perez MV
- Peri F
- Perini L
- Pernegger H
- Perrella S
- Peschke R
- Peshekhonov VD
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
- Petit E
- Petridis A
- Petridou C
- Petroff P
- Petrolo E
- Petrov M
- Petrucci F
- Pettersson NE
- Peyaud A
- Pezoa R
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- Phillips PW
- Piacquadio G
- Pianori E
- Picazio A
- Pickering MA
- Piegaia R
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pino SAO
- Pirumov H
- Pitt M
- Plazak L
- Pleier M-A
- Pleskot V
- Plotnikova E
- Pluth D
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Pommes K
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popeneciu GA
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Pralavorio P
- Pranko A
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- Price D
- Primavera M
- Prince S
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
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- Przybycien M
- Puri A
- Puzo P
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- Qin Y
- Quadt A
- Queitsch-Maitland M
- Quilty D
- Quintero DMP
- Raddum S
- Radeka V
- Radescu V
- Radhakrishnan SK
- Radloff P
- Rados P
- Ragusa F
- Rahal G
- Raine JA
- Rajagopalan S
- Ramos JM
- Rangel-Smith C
- Rashid T
- Raspopov S
- Ratti MG
- Rauch DM
- Rauscher F
- Rave S
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- Rawling JH
- Raymond M
- Read AL
- Readioff NP
- Reale M
- Rebuzzi DM
- Redelbach A
- Redlinger G
- Reece R
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- Reeves K
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- Ren H
- Rescigno M
- Resconi S
- Resseguie ED
- Rettie S
- Reynolds E
- Rezanova OL
- Reznicek P
- Rezvani R
- Richter R
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- Richter-Was E
- Ricken O
- Ridel M
- Rieck P
- Riegel CJ
- Rieger J
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Ripellino G
- Ristic B
- Ritsch E
- Riu I
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts RT
- Robertson SH
- Robichaud-Veronneau A
- Robinson D
- Robinson JEM
- Robson A
- Rocco E
- Roda C
- Rodina Y
- Rodriguez Bosca S
- Rodriguez Perez A
- Rodriguez Rodriguez D
- Rodriguez LP
- Roe S
- Rogan CS
- Rohne O
- Roloff J
- Romaniouk A
- Romano Saez SM
- Romano M
- Romero Adam E
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
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- Rose P
- Rosien N-A
- Rossi E
- Rossi LP
- Rosten JHN
- Rosten R
- Rotaru M
- Rothberg J
- Rousseau D
- Roy D
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Rubbo F
- Ruehr F
- Ruettinger EM
- Ruiz-Martinez A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rutherfoord JP
- Ruthmann N
- Ryabov YF
- Rybar M
- Rybkin G
- Ryu S
- Ryzhov A
- Rzehorz GF
- Saadi DS
- Saavedra AF
- Sabato G
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saha P
- Sahinsoy M
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Sakurai Y
- Salamanna G
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- Salihagic D
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- Salvatore D
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- Salvucci A
- Salzburger A
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez Martinez V
- Sanchez CAS
- Sanchez FJM
- Sanchez J
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- Sandbach RL
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- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
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- Santoni C
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- Sapronov A
- Saraiva JG
- Sargedas De Sousa MJDC
- Sarrazin B
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- Sato K
- Sauvan E
- Savage G
- Savard P
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- Saxon J
- Sbarra C
- Sbrizzi A
- Scanlon T
- Scannicchio DA
- Schaarschmidt J
- Schacht P
- Schachtner BM
- Schaefer D
- Schaefer L
- Schaefer R
- Schaefer U
- Schaeffer J
- Schaepe S
- Schaetzel S
- Schaffer AC
- Schaile D
- Schamberger RD
- Schegelsky VA
- Scheirich D
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- Schernau M
- Schiavi C
- Schier S
- Schildgen LK
- Schillo C
- Schioppa M
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schmitz S
- Schnoor U
- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder TV
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Searcy J
- Seema P
- Seidel SC
- Seiden A
- Seixas JM
- Sekhniaidze G
- Sekhon K
- Sekula SJ
- Semprini-Cesari N
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Seuster R
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shaikh NW
- Shan LY
- Shang R
- Shank JT
- Shapiro M
- Shatalov PB
- Shaw K
- Shaw SM
- Shcherbakova A
- Shehu CY
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
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- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sickles AM
- Sidebo PE
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva J
- Silverstein SB
- Simak V
- Simic L
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- Simioni E
- Simmons B
- Simon M
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov SY
- Sjolin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Socher F
- Soffer A
- Sogaard A
- Soh DA
- Sokhrannyi G
- Sola JDB
- Solar M
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sopczak A
- Sornajenghi M
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettell F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- St Denis RD
- St Panagiotopoulou E
- Stabile A
- Staerz S
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf BS
- Stapnes S
- Starchenko EA
- Stark GH
- Stark J
- Stark SH
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- Starovoitov P
- Staszewski R
- Stegler M
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- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
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- Stoiceas G
- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeda K
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
- Tanaka R
- Tanaka S
- Tanioka R
- Tannenwald BB
- Tapprogge S
- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tavares Delgado A
- Tayalati Y
- Taylor AC
- Taylor AJ
- Taylor GN
- Taylor PTE
- Taylor W
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- Teixeira-Dias P
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thais SJ
- Theenhausen HMZ
- Theveneaux-Pelzer T
- Thiele F
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson PD
- Thomsen LA
- Thomson E
- Tian Y
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CAM
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- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
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- Tolley E
- Tomlinson L
- Tomoto M
- Tompkins L
- Toms K
- Tong B
- Tornambe P
- Toro RC
- Torrence E
- Torres H
- Torres RET
- Toth J
- Touchard F
- Tovey DR
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tsang KW
- Tseng JC-L
- Tsiareshkar PV
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turra R
- Tuts PM
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Unverdorben C
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallier A
- Valls Ferrer JA
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- van der Graaf H
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez JGP
- Veatch J
- Veeraraghavan V
- Veloce LM
- Veloso F
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- Yao W-M
- Yap YC
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- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- 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
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fbâ1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Study of ordered hadron chains with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Alberghi GL
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- Aleksandrov IN
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- Alimonti G
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- Allbrooke BMM
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- Casadei D
- Casado MP
- Casolino M
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- Castillo Gimenez V
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- Cavaliere V
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- Cavasinni V
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- Ceradini F
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- Cerqueira AS
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- Cervelli A
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- Chafaq A
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- da Costa J Barreiro Guimaraes
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- Zieminska D
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- Zimmermann C
- Zimmermann S
- Zinonos Z
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- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 ÎŒbâ1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy âs=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
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