313 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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- Winkels E
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- Wong VWS
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- Yao W-M
- Yap YC
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- Yexley MR
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- Yildiz HD
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- Zaripovas DR
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- Zeng JC
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- Zhemchugov A
- Zheng Z
- Zhong D
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- 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
Joining S100 proteins and migration:for better or for worse, in sickness and in health
- Author
- A Chandramouli
- A Filipek
- A Gibadulinova
- A Heil
- A Hermani
- A Lawrie
- A Mandinova
- A Mueller
- A Rammes
- A Saha
- A Semov
- A Voss
- AJ Halayko
- AM Flynn
- AV Gribenko
- B Forst
- B Grum-Schwensen
- B Grum-Schwensen
- B Psaila
- B Schmidt-Hansen
- B Schmidt-Hansen
- BR Davies
- BW Moore
- BW Moore
- C EL Naaman
- C Gebhardt
- C Goh Then Sin
- C Kraus
- C Li
- C Ruegg
- C Ryckman
- C Tubaro
- C Xue
- C Zhou
- CJ Cornish
- Connie Goh Then Sin
- CW Ang
- D Chen
- D Foell
- D Kiryushko
- D Kligman
- D Liu
- DB Zimmer
- DB Zimmer
- DB Zimmer
- DB Zimmer
- DK Hapangama
- E Bulk
- E Lapi
- E Leclerc
- E Leclerc
- E Lukanidin
- E McKiernan
- E McNeill
- E Shubbar
- EC Breen
- EC DellâAngelica
- ED Emberley
- EV Skripnikova
- F Benfenati
- F Brozzi
- F Guignard
- F Michetti
- F Regnouf
- F Riuzzi
- F Riuzzi
- F Strutz
- FE Gibbs
- FL Wills
- G Fritz
- G Lominadze
- G Sorci
- G Sorci
- G Wang
- G Wang
- G Wang
- G Wang
- G Zhou
- G Zwadlo
- GD Basu
- GV Sherbet
- H Chen
- H Fukushima
- H Haimoto
- H He
- H Okada
- H Zhang
- HH Luu
- HJ Huttunen
- HJ Whiteman
- HJ Yoo
- HL Ford
- I Krop
- I Marenholz
- I Salama
- ID Guerreiro Da Silva
- J Austermann
- J Baudier
- J Dieck van
- J Goyette
- J Hao
- J Klingelhofer
- J Lin
- J Ritterhoff
- J Roth
- J Vegfors
- J Winston
- J Yano
- JN Tsoporis
- JR Glenney Jr
- JT Parsons
- K Andersen
- K Boye
- K Kataoka
- K Komatsu
- K Kurokawa
- K Odink
- K Ohuchida
- K Sudo
- K Takenaga
- K Takenaga
- K Takenaga
- K Vandal
- K Wolk
- K Zhang
- KA Rygiel
- KD Phipps
- KL OâConnor
- KM Hajra
- KS Choi
- L Bian
- L Duchesne
- L Huang
- L Jiang
- L Santamaria-Kisiel
- L Wang
- L Zhang
- LL Jackson-Grusby
- LP Slomnicki
- M Davies
- M Du
- M Frosch
- M Garbuglia
- M Garbuglia
- M Gimona
- M Grigorian
- M Guarino
- M Ichikawa
- M Moriyama-Kita
- M Naka
- M Sakaguchi
- M Sakaguchi
- M Sakaguchi
- M Schneider
- M Schneider
- M Stary
- M Vicente-Manzanares
- M Vicente-Manzanares
- M Vicente-Manzanares
- MA Hofmann
- MA Reddy
- MD Howell
- MJ Jung
- MK Fuentes
- MP Davies
- MP Manitz
- MR Morgan
- MV Kriajevska
- MW Nasser
- N Ambartsumian
- N Leukert
- N Li
- N Nagy
- N Nagy
- N Zobiack
- NC Strynadka
- NG Dulyaninova
- NL Golitsina
- NR West
- NR West
- NT Wright
- O Dmytriyeva
- O Sbai
- P Madsen
- P Most
- P Most
- P Most
- P Rouleau
- PA Gregory
- PA OâConnell
- Philip S. Rudland
- PR Elliott
- PS Rudland
- PS Rudland
- PS Rudland
- PS Rudland
- R Barraclough
- R Barraclough
- R Barraclough
- R Barraclough
- R Bianchi
- R Donato
- R Donato
- R Donato
- R Donato
- R Donato
- R Donato
- R Donato
- R Glaser
- R Hwang
- R Ramasamy
- R Wolf
- R Wolf
- R Yamasaki
- RA Newton
- RL Eckert
- Roger Barraclough
- RR Bowers
- RR Yammani
- RS Mani
- Rudland S Silva de
- S Barry
- S Bhattacharya
- S Diederichs
- S Hamada
- S Hiratsuka
- S Jamieson
- S Naz
- S Parkkila
- S Taylor
- S Wolf
- S Zhang
- S Zhang
- SE Mikkelsen
- SH Heo
- SK Mishra
- SK Mohan
- SL Merklinger
- SR Gross
- SR Jenkinson
- Stephane R. Gross
- T Arumugam
- T Arumugam
- T Arumugam
- T Cabezon
- T Hibino
- T Ismail
- T Komada
- T Nedjadi
- T Saito
- T Vogl
- T Vogl
- TM Ismail
- U Murzik
- U Sack
- U Sack
- U Stein
- U Stein
- V Gerke
- V Novitskaya
- VN Malashkevich
- W Jiang
- W Ju
- W Lesniak
- WC Tsai
- WX Yan
- X Luo
- X Pang
- X Shang
- X Yang
- XF Pei
- XJ Guo
- XM Tong
- Y Dempsie
- Y Fukata
- Y Ito
- Y Lee
- Y Shi
- Y Tamaki
- Y Watanabe
- YS Deol
- Z Fang
- Z Wang
- Z Xiong
- Z Yang
- ZH Li
- ZH Li
- ZH Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/05/2014
- Field of study
The vast diversity of S100 proteins has demonstrated a multitude of biological correlations with cell growth, cell differentiation and cell survival in numerous physiological and pathological conditions in all cells of the body. This review summarises some of the reported regulatory functions of S100 proteins (namely S100A1, S100A2, S100A4, S100A6, S100A7, S100A8/S100A9, S100A10, S100A11, S100A12, S100B and S100P) on cellular migration and invasion, established in both culture and animal model systems and the possible mechanisms that have been proposed to be responsible. These mechanisms involve intracellular events and components of the cytoskeletal organisation (actin/myosin filaments, intermediate filaments and microtubules) as well as extracellular signalling at different cell surface receptors (RAGE and integrins). Finally, we shall attempt to demonstrate how aberrant expression of the S100 proteins may lead to pathological events and human disorders and furthermore provide a rationale to possibly explain why the expression of some of the S100 proteins (mainly S100A4 and S100P) has led to conflicting results on motility, depending on the cells used. © 2013 Springer Basel
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- AlconadaVerzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos CN
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
- Baines JT
- Baker OK
- Baldin EM
- Balek P
- Balestri T
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
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- Bauer F
- Baw HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
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- Beermann TA
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- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
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- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
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- Benary O
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- Blazek T
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- Blocker C
- Blum W
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- Boeriu OEV
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- Bogdanchikov AG
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- Borisov A
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- Boscherini D
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- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
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- Boyd J
- Boyko IR
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- Brandt A
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- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Bravo AG
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
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- Britton D
- Britzger D
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- Brock I
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- Broughton JH
- Bruncko D
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- Bruni LS
- Brunt BH
- Bruschi M
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- Bryant P
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- Cakir O
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Search for 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
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- Assamagan K
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- Atlay NB
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- Avramidou R
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- Azuelos G
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- Bachacou H
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- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
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- Baldin EM
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- Balunas WK
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- Cardillo F
- Carli I
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- 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
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- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen C
- Chen H
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- Chen S
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- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
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- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
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- Clarke RN
- Clement C
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- Coccaro A
- Cochran J
- Colasurdo L
- Cole B
- Colijn AP
- Collaboration ATLAS
- Collot J
- Conde Muino P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga K De Vasconcelos
- Cormier F
- Cormier KJR
- Cornell S Diez
- Corradi M
- Correia AM Henriques
- Corrigan EE
- Corriveau F
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- Costa MJ
- Costanzo D
- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
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- Cristinziani M
- Croft V
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- Cueto A
- Cukierman AR
- Curatolo M
- Cuth J
- Czekierda S
- Czodrowski P
- D'amen G
- D'Auria S
- D'eramo L
- D'Onofrio M
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio D Oliveira
- Dandoy JR
- Daneri MF
- Dang NP
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
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- de Asmundis R
- De Benedetti A
- De Bruin PH Sales
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DE Ferreira
- De Lorenzi F
- De Maria A
- De Pedis D
- De Regie JB De Vivie
- de Renstrom PA Bruckman
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
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- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaconu C
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- Dias do Vale T
- Dias FA
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- Diehl EB
- Dietrich J
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- Doglioni C
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- Dreyer E
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- El Kacimi M
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- Zivkovic L
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- 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
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
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Aleksandrov IN
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- Yao W-M
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- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
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- Zalieckas J
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- Zanzi D
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou N
- Zhu CG
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- 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
- '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
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
- 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
- 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
- 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
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- 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
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- 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
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
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- Zhemchugov A
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- 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
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
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- Bednyakov VA
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- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particleâhole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
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
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
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- Aguilar-Saavedra JA
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- Akesson TPA
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- Aleksandrov IN
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- 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
Charged-particle distributions at low transverse momentum in âs=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
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- Zhemchugov A
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- Zobernig G
- Zoccoli A
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in protonâproton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 ÎŒb â1 ÎŒbâ1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Measurement of the inelastic proton-proton cross section at âs=13 TeV with the ATLAS detector at the LHC
- Author
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
This Letter presents a measurement of the inelastic proton-proton cross section using 60ââÎŒb â1 of pp collisions at a center-of-mass energy âs of 13 TeV with the ATLAS detector at the LHC. Inelastic interactions are selected using rings of plastic scintillators in the forward region (2.0710 â6 , where M X is the larger invariant mass of the two hadronic systems separated by the largest rapidity gap in the event. In this Ο range the scintillators are highly efficient. For diffractive events this corresponds to cases where at least one proton dissociates to a system with M X >13ââGeV . The measured cross section is compared with a range of theoretical predictions. When extrapolated to the full phase space, a cross section of 78.1±2.9ââmb is measured, consistent with the inelastic cross section increasing with center-of-mass energy
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