82 research outputs found
Tracer input for kinetic modelling of liver physiology determined without sampling portal venous blood in pigs
- Author
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
Intraluminal injection of short chain fatty acids diminishes intestinal mucosa injury in experimental ischemia-reperfusion
- Author
- Aguilar-Nascimento JE
- Alberto Bicudo SalomĂŁo
- Chiu C
- Cicalese L
- de Perrot M
- Gangadharan SP
- Gibson DD
- Granger DN
- Grotz MR
- Harward TRS
- José de Souza Neves
- José Eduardo de Aguilar-Nascimento
- Kanwar S
- Kong SE
- Kozar RA
- Kubes P
- Lew JI
- Mariana Nascimento
- McAndrew HF
- Mortensen FV
- Mortensen FV
- Parks DA
- Quaedackers JSLT
- Roediger WE
- Rubens Jardim Nochi Jr.
- Saito H
- Schmitt MG
- Schoenberger MH
- Topcu O
- Zhi-Yong S
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Enhanced mucosal re-epithelialization induced by short chain fatty acids in experimental colitis
- Author
- A.F. de-Oliveira
- Aguilar-Nascimento JE
- Aguilar-Nascimento JE
- Butzner JD
- Clausen MR
- Cummings JH
- D'Argenio G
- D'Argenio G
- Elson CO
- Fabia R
- Forrest RD
- Gardiner KR
- Gyles KW
- Harig JM
- J.E. Aguilar-Nascimento
- Kamm MA
- L.R. França-da-Silva
- M.H. Gomes-da-Silva
- Mortensen FV
- Rahal F
- Roediger WEW
- Roediger WEW
- Roediger WEW
- Roediger WEW
- Rolandelli RH
- Senagore AJ
- Vernia P
- Vernia P
- Wallace JL
- Yamada T
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Evaluation by computerized morphometry of histopathological alterations of the colon wall in segments with and without intestinal transit in rats
- Author
- Adriana Valim Portes
- Barreto Neto PF
- Biondo-SimÔes MLP
- Carlos Augusto Real Martinez
- Denise Gonçalves Priolli
- Edwards CM
- Geraghty JM
- Giardiello FM
- Glotzer DJ
- Habr-Gama A
- Izilda Aparecida Cardinalli
- Jenkins D
- José Aires Pereira
- Keli E
- Kiely EM
- Kissmeyer-Nielsen P
- Korelitz BI
- Lim AG
- Lopes-Paulo F.
- Marcos Vieira de Sousa
- Martinez CAR
- Mortensen FV
- Neut C
- Oliveira-Neto JP
- Orsay CP
- Pearce NW
- Pinto A
- Pinto JĂșnior FEL
- Priolli DG
- Roe AM
- Roedger WE
- Roediger WE
- Velazquez OC
- Velazquez OC
- Violi V
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel 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
- 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
- Alconada Verzini MJ
- 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
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- 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
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- 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
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Aurousseau M
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bacci C
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bain T
- 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
- Barisonzi M
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
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- Batista SJ
- Batley JR
- Battaglia M
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- Beattie MD
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- Beauchemin PH
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- Bechtle P
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- Becot C
- Beddall A
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- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell WH
- Bella G
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- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
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- Bernard C
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
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- Bertsche D
- Besana MI
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
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- Biebel O
- Biedermann D
- Biesuz NV
- Biglietti M
- Bilokon H
- Bindi M
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- Bingul A
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- Bloch I
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- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
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- Boehler M
- Boeriu OEV
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bold T
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- Boldyrev AS
- Bomben M
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- Borisov A
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- Borroni S
- Bortfeldt J
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- Boscherini D
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- Bouhova-Thacker EV
- Boumediene D
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- Bousson N
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozic I
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
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- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
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- Bronner J
- Brooijmans G
- Brooks T
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- Brosamer J
- Brost E
- Bruncko D
- Bruneliere R
- Bruni A
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- Bryngemark L
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- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher D
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- Bugge L
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- Bulekov O
- Bullock D
- Burckhart H
- Burdin S
- Burgard CD
- Burghgrave B
- Burke S
- Burmeister I
- Busato E
- Bussey P
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
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- Caforio D
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- Calafiura P
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- Castanheira MTD
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- Cheplakov A
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- Chernyatin V
- Cheu E
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- Chiarella V
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- Chisholm AS
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- Chromek-Burckhart D
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- Chuinard AJ
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- Collaboration ATLAS
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- Compostella G
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- da Costa JBG
- Da Cunha Sargedas De Sousa MJ
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- Dabrowski W
- Dafinca A
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- Dang NP
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- de Asmundis R
- De Benedetti A
- De Bruin PHS
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- De la Torre H
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- Derendarz D
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- Derue F
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- Deterre C
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- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
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- Di Nardo R
- Di Simone A
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- Djuvsland JI
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- Dobos D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fbâ1 of proton-proton collision data at âs =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.âsyst.). The phase ÎŽ â between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be â0.014Ï Â± 0.036Ï (stat.âsyst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] â [â0.36, 0.10] and Im[g R /V L] â [â0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Modelling Z â ÏÏ processes in ATLAS with Ï-embedded Z â ΌΌ data
- Author
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- Zalieckas J
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- Zemla A
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- Zenin O
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- Zhemchugov A
- Zhong J
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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
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2015
- Field of study
This paper describes the concept, technical realisation and validation of a largely data-driven method to model events with ZâÏÏ decays. In ZâΌΌ events selected from proton-proton collision data recorded at âs=8 TeV with the ATLAS experiment at the LHC in 2012, the Z decay muons are replaced by Ï leptons from simulated ZâÏÏ decays at the level of reconstructed tracks and calorimeter cells. The Ï lepton kinematics are derived from the kinematics of the original muons. Thus, only the well-understood decays of the Z boson and Ï leptons as well as the detector response to the Ï decay products are obtained from simulation. All other aspects of the event, such as the Z boson and jet kinematics as well as effects from multiple interactions, are given by the actual data. This so-called Ï-embedding method is particularly relevant for Higgs boson searches and analyses in ÏÏ final states, where ZarrowÏÏ decays constitute a large irreducible background that cannot be obtained directly from data control samples. In this paper, the relevant concepts are discussed based on the implementation used in the ATLAS Standard Model HâÏÏ analysis of the full datataset recorded during 2011 and 2012
Measurements of the top quark branching ratios into channels with leptons and quarks 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
- Acharya BS
- Adam ER
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- Adomeit S
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- Affolder AA
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- Aguilar-Saavedra JA
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- Akesson TP
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- Aleksa M
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- Allbrooke BMM
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF Helmholtz Association, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; RGC, Hong Kong SAR, China; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW and NCN, Poland; GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZĆ , Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA) and in the Tier-2 facilities worldwide
Determination of the ratio of b-quark fragmentation fractions fs/fd in pp collisions at âs = 7 TeV with the ATLAS Detector
- Author
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- Zhemchugov A
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
With an integrated luminosity of 2.47ââfbâ1 recorded by the ATLAS experiment at the LHC, the exclusive decays B 0sâJ/ÏÏ and B0dâJ/ÏK*0 of B mesons produced in pp collisions at âs=7ââTeV are used to determine the ratio of fragmentation fractions fs/fd. From the observed B0sâJ/ÏÏ and B0dâJ/ÏK*0 yields, the quantity (fs/fd)[B(B0sâJ/ÏÏ)/B(B 0dâJ/ÏK*0)] is measured to be 0.199±0.004(stat)±0.008(syst). Using a recent theory prediction for [B(B0sâJ/ÏÏ)/B(B0dâJ/ÏK*0)] yields (fs/fd)=0.240±0.004(stat)±0.010(syst)±0.017(th). This result is based on a new approach that provides a significant improvement of the world average
Measurement of the ttÌW and ttÌZ production cross sections in pp collisions at âs = 8 TeV with the ATLAS detector
- Author
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- Schroeder TV
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- Sivoklokov SY
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- Sjursen TB
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- Smakhtin V
- Smart BH
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- Smirnov Y
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- Stramaglia ME
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- Strubig A
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- Sundermann JE
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- Teng PK
- Teoh JJ
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- Thompson EN
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- Tsionou D
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- Tsiskaridze S
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- Tskhadadze EG
- Tsukerman L
- Tsulaia V
- Tsuno S
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- Ueda I
- Ueno R
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- Unal G
- Undrus A
- Unel G
- Ungaro FC
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- Urban J
- Urquijo P
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- Valentinetti S
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- van Vulpen I
- van Woerden MC
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- Viel S
- Vigne R
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- Villar DN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
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- von der Schmitt H
- von Radziewski H
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- Weingarten J
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- Winklmeier F
- Winte R
- Winter BT
- Wittgen M
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
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- Wu SL
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- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamada M
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang Y
- Yange H
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshida R
- Yoshihar K
- Young C
- Young CJS
- Youssef S
- Yu DR
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- Yu JM
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- Yuen SPY
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zalieckas J
- Zanello L
- Zanzi D
- Zarnan A
- Zarnbito S
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
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- Zhang J
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- Zhang R
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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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
- 01/01/2015
- Field of study
The production cross sections of top-quark pairs in association with massive vector bosons have been measured using data from pp collisions at sâ = 8 TeV. The dataset corresponds to an integrated luminosity of 20.3 fbâÂč collected by the ATLAS detector in 2012 at the LHC. Final states with two, three or four leptons are considered. A fit to the data considering the ttÌW and ttÌZ processes simultaneously yields a significance of 5.0Ï (4.2Ï) over the background-only hypothesis for ttÂŻWttÂŻW (ttÌZ) production. The measured cross sections are ÏttÌW = 369 + 100â91 fb and ÏttÌZ = 176 + 58â52 fb. The background-only hypothesis with neither ttÌW nor ttÌZ production is excluded at 7.1Ï. All measurements are consistent with next-to-leading-order calculations for the ttÌW and ttÌZ processes
Searches for Higgs boson pair production in the hhâbbÏÏ, γγWWâ, γγbb, bbbb channels with the ATLAS detector
- Author
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- Abbott B
- Abdallah J
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- Kado M
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- Karastathis N
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- Kosek T
- Kostyukhin VV
- Kotov VM
- Kotwal A
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- Kourkoumelis C
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- Kozanecki W
- Kozhin AS
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
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- Zobernig G
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
Searches for both resonant and nonresonant Higgs boson pair production are performed in the hhâbbÏÏ, γγWWâ final states using 20.3ââfbâ1 of pp collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of their production is observed and 95% confidence-level upper limits on the production cross sections are set. These results are then combined with the published results of the hhâγγbb, bbbb analyses. An upper limit of 0.69 (0.47) pb on the nonresonant hh production is observed (expected), corresponding to 70 (48) times the SM ggâhh cross section. For production via narrow resonances, cross-section limits of hh production from a heavy Higgs boson decay are set as a function of the heavy Higgs boson mass. The observed (expected) limits range from 2.1 (1.1) pb at 260 GeV to 0.011 (0.018) pb at 1000 GeV. These results are interpreted in the context of two simplified scenarios of the Minimal Supersymmetric Standard Model
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