10 research outputs found
The performance of the jet trigger for the ATLAS detector during 2011 data taking
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- Abolins M
- 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
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- 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
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- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
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- Antonelli M
- Antonov A
- Antos J
- 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
- Asquith L
- Assamagan K
- Astalos R
- 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
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- Balestri T
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- Balunas WK
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- Bannoura AAE
- Barajas CAC
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- Chernyatin V
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- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2016
- Field of study
The performance of the jet trigger for the ATLAS
detector at the LHC during the 2011 data taking period is
described. During 2011 the LHC provided proton–proton
collisions with a centre-of-mass energy of 7 TeV and heavy
ion collisions with a 2.76 TeV per nucleon–nucleon collision
energy. The ATLAS trigger is a three level system designed
to reduce the rate of events from the 40 MHz nominal maximum
bunch crossing rate to the approximate 400 Hz which
can be written to offline storage. The ATLAS jet trigger is the
primary means for the online selection of events containing
jets. Events are accepted by the trigger if they contain one
or more jets above some transverse energy threshold. During
2011 data taking the jet trigger was fully efficient for
jets with transverse energy above 25 GeV for triggers seeded
randomly at Level 1. For triggers which require a jet to be
identified at each of the three trigger levels, full efficiency is
reached for offline jets with transverse energy above 60 GeV.
Jets reconstructed in the final trigger level and corresponding
to offline jets with transverse energy greater than 60 GeV,
are reconstructed with a resolution in transverse energy with
respect to offline jets, of better than 4 % in the central region
and better than 2.5 % in the forward direction
On the role of moisture in triggering out-of-plane displacement in paper : from the network level to the macroscopic scale
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2018
- Field of study
The response of paper to humidity variations is a complex, inherently multi-scale problem. The hygroscopic swelling of individual fibres and their interactions within the fibrous network govern the macroscopic, sheet-level response. At this scale, moisture induced instabilities and out-of-plane deformations may occur, which are critical for a number of industrial applications. This work specifically focuses on several aspects of this important issue. A macroscopic phenomenological hygro-mechanical model is first proposed, which aims at predicting moisture induced out-of-plane deformations in paper sheets. The constitutive model is based on the relation between these deformations and typical irreversible phenomena associated to the history of paper manufacturing, i.e. the release of dried-in strains. The model is used to describe bending induced by moisture gradients through the thickness of the sheet as well as buckling due to moisture variation in the presence of mechanical constraints. The results of the model show that the anisotropic sheet-level hygro-expansion has a strong influence on the instability phenomena. Moreover, a comparison with experiments provides adequate semi-quantitative estimates. An additional step is made towards the multi-scale understanding of paper hygro-mechanics. The fundamental physical mechanisms governing the macroscopic moisture induced response are investigated on the basis of the underlying fibrous network. To this aim, a meso-structural model is developed which consists of a network of fibres randomly positioned in a planar region according to an orientation probability density function. A series of network simulations reveals that upon moisture content variations the expansion of the inter-fibre bonding regions essentially drives the overall deformation. Particularly in the case of anisotropic fibre orientation, this explains the origin of the macro-scale anisotropic hygro-expansion, which is essential for the observed sheet-level instability phenomena
A Review of Recent Trends and Challenges in Computational Modeling of Paper and Paperboard at Different Scales
- Author
- A Airoldi
- A Alajami
- A Auslender
- A Cerrone
- A Cherkaev
- A Cherkaev
- A DeMaio
- A Ekman
- A Ekman
- A Giampieri
- A Hagman
- A Hagman
- A Harrysson
- A Harrysson
- A Karakoç
- A Kulachenko
- A Ojha
- A Spencer
- A Torgnysdotter
- A Torgnysdotter
- A Turon
- A Vishtal
- AA Rahman
- AH Bedane
- AL Erkkilä
- AP Karafillis
- B Svendsen
- BF Sørensen
- C Andersson
- C Barbier
- C Barbier
- C Czibula
- C Fellers
- C Fellers
- C Ganser
- C Lorbach
- C Lorbach
- C Marulier
- C Marulier
- C Miehe
- C Oria
- C Sellén
- CA Dominic
- CAS Deganutti
- CG van der Sman
- D Höwer
- DC Drucker
- DD Choi
- DD Tjahjanto
- DV Wilbrink
- DW Coffin
- DW Coffin
- DW Spring
- E Borgqvist
- E Borgqvist
- E Borgqvist
- E Bosco
- E Bosco
- E Linvill
- E Linvill
- E Linvill
- E Linvill
- E Sozumert
- E Zappa
- ELG Wernersson
- F Confalonieri
- F Confalonieri
- F Jiang
- F Martoïa
- FJ Schmied
- G Bolzon
- G Bolzon
- G Chinga-Carrasco
- G Chinga-Carrasco
- GJF Ring
- H Andrä
- H Askfelt
- H Askfelt
- H Askfelt
- H Huang
- H Huang
- H Huang
- H Huang
- H Li
- H Rappel
- HL Cox
- HR Motamedian
- HR Motamedian
- HW Haslach
- J Alfthan
- J Dirrenberger
- J Kouko
- J Kouko
- J Lübke
- J Persson
- J Sliseris
- J Sliseris
- J Sorvari
- J Strömbro
- J Strömbro
- J Tryding
- J Tryding
- J Viguié
- J Zechner
- J Zechner
- JA Ketoja
- JE Bronlund
- JW Simon
- JW Simon
- JX Liu
- JX Liu
- K Park
- K Park
- K Park
- K Persson
- K Robertsson
- KC Bennett
- KC Bennett
- KW Neale
- L Chen
- L Czechowski
- L Kappel
- L Kappel
- L Kappel
- L Meherishi
- LAA Beex
- LAA Beex
- LAA Beex
- M Alava
- M Alexandersson
- M Alimadadi
- M Awais
- M Awais
- M Domaneschi
- M Jajcinovic
- M Jajcinovic
- M Klingberg
- M Lindner
- M Nygårds
- M Nygårds
- M Nygårds
- M Nygårds
- M Nygårds
- M Nygårds
- M Pfeiffer
- M Pfeiffer
- M Schneider
- M Wallmeier
- M Wallmeier
- M Zaheer
- MA Charfeddine
- MA Charfeddine
- MS Magnusson
- MS Magnusson
- MS Magnusson
- N Chen
- N Hallbäck
- N Hallbäck
- N Navaranjan
- N Stenberg
- N Stenberg
- N Stenberg
- NS Ottosen
- O Girlanda
- OT Bruhns
- P Bergström
- P Groche
- P Groche
- P Hämäläinen
- P Isaksson
- P Isaksson
- P Isaksson
- P Isaksson
- P Isaksson
- P Lipponen
- P Mäkelä
- P Mäkelä
- P Saketi
- PAM Zapata
- PP Camanho
- QS Xia
- R Bedzra
- R Dimitri
- R Gutkin
- R Haj-Ali
- R Hill
- R Hägglund
- R Hägglund
- R Mansour
- RC McKee
- RC Neagu
- S Borodulina
- S Borodulina
- S Borodulina
- S Deogekar
- S El-Sayed
- S Goutianos
- S Hossain
- S Hussain
- S Lavrykov
- S Lee
- S Nagasawa
- S Nagasawa
- S Reese
- S Reichel
- S Reichel
- S Staub
- T Câmpean
- T Ebner
- T Fadiji
- T Fadiji
- T Fadiji
- T Leppänen
- T Leppänen
- TM Berry
- U Hirn
- V Krasnoshlyk
- V Köstner
- V Köstner
- V Negi
- VD Luong
- W Batchelor
- W Jina
- WJ Fischer
- X Huang
- XZ Lu
- Y Li
- Y Li
- Y Li
- Y Li
- Y Li
- Y Li
- Y Sharma
- YH Ma
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the forward-backward asymmetry of electron and muon pair-production in pp collisions at s ? =7
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Aberghi GL
- Abi B
- Abolins M
- Abouzedi OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguiar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Araque JP
- Arce ATH
- Arguin JF
- Argyropoulos S
- Arik M
- Aring kesson TPA
- Aring sman B
- Armadans RC
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee S
- Bannoura AAE
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Bartsch V
- Bassalat A
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia M
- Battistin M
- Bauer F
- Bawa HS
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beecherle R
- Beemster LJ
- Beermann TA
- Begel M
- Behr K
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benjamin DP
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Berlingen JM
- Bernard C
- Bernat P
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertsche D
- Besana MI
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bhimji W
- Bianchi RM
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- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Black AM
- Black CW
- Black JE
- Blackburn D
- Blair RE
- Blanchard JB
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boddy CR
- Boehler M
- Boek J
- Boek TT
- Boeriu OEV
- Bogaerts JA
- Bogdanchikov AG
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutouil S
- Boveia A
- Boyd J
- Boyko IR
- Bozovic-Jeisavcic I
- Bracinik J
- Brandt A
- Brandt G
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- Brau B
- Brau JE
- Braun HM
- Brazzale SF
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- Brennan AJ
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- Bret MC
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- Bristow TM
- Britton D
- Brochu FM
- Brock I
- Brock R
- Bromberg C
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- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Brown G
- Brown J
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Bryngemark L
- Buanes T
- Buat Q
- Bucci F
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Buehrer F
- Bueso XP
- Bugge L
- Bugge MK
- Bulekov O
- Bundock AC
- Burckhart H
- Burdin S
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Buscher D
- Buscher V
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
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- Buttinger W
- Buzatu A
- Bylund OB
- Byszewski M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Calvet D
- Calvet S
- Camarda S
- Cameron D
- Camillocci ES
- Caminada LM
- Campanam S
- Campanelli M
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Cardarelli R
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- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Castanheira MTD
- Castelli A
- Castillo IS
- Castillo LRF
- Castro NF
- Catastini P
- Catastini-Miranda E
- Catinaccio A
- Catmore JR
- Cattai A
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- Cavaliere V
- Cavalli D
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- Cavasinni V
- Cellerstedt K
- Cemme C
- Cemmell A
- Centile S
- Ceradini F
- Cerio BC
- Cerny K
- Cerqueira AS
- Cerri A
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- Cerutti F
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- Cervelli A
- Cetin SA
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- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Charfeddine D
- Charlton DG
- Chau CC
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
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- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiefaril G
- Childers JT
- Chilingarov A
- Chiodini G
- Chisholm AS
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- Chizhov MV
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- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Chwastowski JJ
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- Ciftci AK
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- Cinca D
- Cindro V
- Ciocio A
- Cirkovic P
- Citron ZH
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- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
- Clement C
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- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshal J
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- Colijn AP
- Collot J
- Colombo T
- Colon G
- Compostella G
- Coniavitis E
- Conidi MC
- Connell SH
- Connelly IA
- Consonni SM
- Consorti V
- Constantinescua S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cuciuc CM
- Cummings J
- Curatolo M
- Cuthbert C
- Czirr H
- Czodrowski P
- Czyczula Z
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Daniells AC
- Dao V
- Darbo G
- Darmora S
- Dassoulas J
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davison P
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Andrade LM
- de Asmundis R
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Sousa MJDS
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Deigaard I
- Del Peso J
- Del Prete T
- Delgado AT
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaz MA
- Diehl EB
- Dietrich J
- Dietzsch TA
- Diglio S
- Dimitrievska A
- Dingfelder J
- DioniSi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- do Vale MAB
- Doan TKO
- Dobos D
- Doglioni C
- Doherty T
- Dohmae T
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- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donati S
- Dondero P
- Donini J
- Donszelmann TC
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- Dos Santos SPA
- Dova MT
- Doyle AT
- Dris M
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- Dube S
- Dubreuil E
- Duchovni E
- Duckeck G
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- Dudarev A
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- Durglishvili A
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- El Moursli RC
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- Elmsheuser J
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- Emeliyanov D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
This paper presents measurements from the ATLAS experiment of the forward-backward asymmetry in the reaction pp -> Z/gamma* -> l(+)l(-), with l being electrons or muons, and the extraction of the effective weak mixing angle. The results are based on the full set of data collected in 2011 in pp collisions at the LHC at root s = 7 TeV, corresponding to an integrated luminosity of 4.8 fb(-1). The measured asymmetry values are found to be in agreement with the corresponding Standard Model predictions. The combination of the muon and electron channels yields a value of the effective weak mixing angle of sin(2) theta(lept)(eff) = 0.2308 +/- 0.0005(stat.)+/- 0.0006(syst.)+/- 0.0009(PDF), where the first uncertainty corresponds to data statistics, the second to s ystematic effects and the third to knowledge of the parton density functions. This result agrees with the current world average from the Particle Data Group fit
Search for flavour-changing neutral current top-quark decays to q Z in pp collision data collected with the ATLAS detector at root s=8 TeV
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- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi D
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- Zalieckas J
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- Zhemchugov A
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
A search for the flavour-changing neutral-current decay is presented. Data collected by the ATLAS detector during 2012 from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of root s = 8 TeV, corresponding to an integrated luminosity of 20.3 fb(-1), are analysed. Top-quark pair-production events with one top quark decaying through the t -> qZ (q = u,c) channel and the other through the dominant Standard Model mode t -> bW are considered as signal. Only the decays of the Z boson to charged leptons and leptonic W boson decays are used. No evidence for a signal is found and an observed (expected) upper limit on the t -> qZ branching ratio of 7 x 10(-4) (8 x 10(-4)) is set at the 95 % confidence level
Search for squarks and gluinos in final states with jets and missing transverse momentum at root s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
A search for squarks and gluinos in final states containing hadronic jets, missing transverse momentum but no electrons or muons is presented. The data were recorded in 2015 by the ATLAS experiment in root s = 13 TeV proton-proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation was observed in 3.2 fb(-1) of analyzed data. Results are interpreted within simplified models that assume R-parity is conserved and the neutralino is the lightest supersymmetric particle. An exclusion limit at the 95 % confidence level on the mass of the gluino is set at 1.51 TeV for a simplified model incorporating only a gluino octet and the lightest neutralino, assuming the lightest neutralino is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.03 TeV are excluded for a massless lightest neutralino. These limits substantially extend the region of supersymmetric parameter space excluded by previous measurements with the ATLAS detector
Search for pair production of gluinos decaying via stop and sbottom in events with b-jets and large missing transverse momentum in pp collisions at root s=13 TeV with the ATLAS detector
- Author
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- Yorita K
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
A search for supersymmetry involving the pair production of gluinos decaying via third-generation squarks to the lightest neutralino (chi) over tilde (0)(1) is reported. It uses an LHC proton-proton data set at a center-of-mass energy root s = 13 TeV with an integrated luminosity of 3.2 fb(-1) collected with the ATLAS detector in 2015. The signal is searched for in events containing several energetic jets, of which at least three must be identified as b jets, large missing transverse momentum, and, potentially, isolated electrons or muons. Large-radius jets with a high mass are also used to identify highly boosted top quarks. No excess is found above the predicted background. For (chi) over tilde (0)(1) masses below approximately 700 GeV, gluino masses of less than 1.78 TeVand 1.76 TeV are excluded at the 95% C. L. in simplified models of the pair production of gluinos decaying via sbottom and stop, respectively. These results significantly extend the exclusion limits obtained with the root s = 8 TeV data set
Constraints on new phenomena via Higgs boson couplings and invisible decays with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Adam ER
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguiar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Akimov AV
- Alberghi GL
- Alberghi GL
- Albert J
- Albert J
- Albrand S
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amram N
- 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
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- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
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- Anulli F
- Aoki M
- Arabidze G
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- Aranda CP
- Araque JP
- Arce ATH
- Arduh FA
- Arguin JF
- Argyropoulos S
- Arik M
- Aring sman B
- Armadans RC
- Armbruster AJ
- Arnaez O
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- Artamonov A
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- Ashkenazi A
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- Atlay NB
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- Baldin EM
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- Banerjee S
- Bannoura AAE
- Bansil HS
- Barajas CAC
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- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisonzi M
- Barklow T
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- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
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- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
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- Bassalat A
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- Batista SJ
- Batley JR
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- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
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- Beauchemin PH
- Beccherle R
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- Beckingham M
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- Beddall A
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- Bednyakov VA
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- Behr JK
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- Bellerive A
- Bellomo M
- Belotskiy K
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- Bender M
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- Benjamin DP
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- Bianchi RM
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- Publication venue
- Publication date
- 01/01/2015
- Field of study
The ATLAS experiment at the LHC has measured the Higgs boson couplings and mass, and searched for invisible Higgs boson decays, using multiple production and decay channels with up to 4.7 fb(-1) of pp collision data at root S = 7 TeV and 20.3 fb(-1) at root s = 8 TeV. In the current study, the measured production and decay rates of the observed Higgs boson in the gamma gamma, ZZ, WW, Z gamma, bb, tau tau, and mu mu decay channels, along with results from the associated production of a Higgs boson with a top-quark pair, are used to probe the scaling of the couplings with mass. Limits are set on parameters in extensions of the Standard Model including a composite Higgs boson, an additional electroweak singlet, and two-Higgs-doublet models. Together with the measured mass of the scalar Higgs boson in the gamma gamma and ZZ decay modes, a lower limit is set on the pseudoscalar Higgs boson mass of m(A) > 370 GeV in the "hMSSM" simplified Minimal Supersymmetric Standard Model. Results from direct searches for heavy Higgs bosons are also interpreted in the hMSSM. Direct searches for invisible Higgs boson decays in the vector-boson fusion and associated production of a Higgs boson with W/Z (Z -> ll, W/Z -> jj) modes are statistically combined to set an upper limit on the Higgs boson invisible branching ratio of 0.25. The use of the measured visible decay rates in a more general coupling fit improves the upper limit to 0.23, constraining a Higgs portal model of dark matter
Measurement of top quark pair differential cross sections in the dilepton channel in pp collisions at root s=7 and 8 TeV with ATLAS
- Author
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- Aad G
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- Abdallah J
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Measurements of normalized differential cross sections of top quark pair (t (t) over bar) production are presented as a function of the mass, the transverse momentum and the rapidity of the t (t) over bar system in proton-proton collisions at center-of-mass energies of root s = 7 and 8 TeV. The data set corresponds to an integrated luminosity of 4.6 fb(-1) at 7 TeV and 20.2 fb(-1) at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a b hadron. The measured distributions are corrected for detector effects and selection efficiency to cross sections at the parton level. The differential cross sections are compared with different Monte Carlo generators and theoretical calculations of t (t) over bar production. The results are consistent with the majority of predictions in a wide kinematic range
Combination of searches for WW, WZ, and ZZ resonances in pp collisions at root s=8 TeV with the ATLAS detector
- Author
- Aad G
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
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- Zhemchugov A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The ATLAS experiment at the CERN Large Hadron Collider has performed searches for new, heavy bosons decaying to WW, WZ and ZZ final states in multiple decay channels using 20.3 fb(-1) of pp collision data at root s = 8 TeV. In the current study, the results of these searches are combined to provide a more stringent test of models predicting heavy resonances with couplings to vector bosons. Direct searches for a charged diboson resonance decaying to WZ in the l nu l'l' (l = mu, e), llq (q) over bar, l nu q (q) over bar and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WZ bosons are compared with predictions of an extended gauge model with a heavy W' boson. In addition, direct searches for a neutral diboson resonance decaying to WW and ZZ in the llq (q) over bar, l nu q (q) over bar, and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the WW and ZZ bosons are compared with predictions for a heavy, spin-2 graviton in an extended Randall-Sundrum model where the Standard Model fields are allowed to propagate in the bulk of the extra dimension. (C) 2016 CERN for the benefit of the ATLAS Collaboration. Published by Elsevier B.V