434 research outputs found
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anh T. Vu
- Anisimov A
- Antillon E
- Antipov P
- Antonelli L
- Anttila E
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arnold B
- Arora S
- Artamonov A
- Asaadi J
- Asghar MI
- Ashby S
- Askew A
- Atac M
- Atramentov O
- Auffray E
- Aurisano A
- Autermann C
- Avery P
- Avetisyan A
- Avila C
- Awan MIM
- Ayan AS
- Ayhan A
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babb J
- Babucci E
- Baccaro S
- Bacchetta N
- Bacchi W
- Bachtis M
- Baden D
- Badgett W
- Baechler J
- Baer H
- Baesso P
- Baffioni S
- Bagby L
- Bagliesi G
- Bahk SY
- Bailleux D
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Baldin B
- Ball G
- Ball H
- Ballin J
- Bally SL
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Banicz K
- Bansal S
- Banzuzi K
- Barashko V
- Barbagli G
- Barberis E
- Barbone L
- Barcala JM
- Barcellan L
- Bard R
- Bargassa P
- Baringer P
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Bartalini P
- Bartoloni A
- Bartz E
- Basegmez S
- Battilana C
- Baty C
- Baud A
- Bauer G
- Bauer J
- Bauerdick LAT
- Baur U
- Bawa HS
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaumont W
- Bechtel F
- Bedjidian M
- Bedoya CF
- Beetz CP
- Behrens U
- Bejar JC
- Belforte S
- Beliy N
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Benaglia A
- Bencze G
- Bendavid J
- Bender W
- Benedetti D
- Benelli G
- Benettoni M
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Berengueres JOL
- Beretvas A
- Bergauer H
- Bergauer T
- Beri SB
- Bernardini J
- Bernet C
- Berntzon L
- Berretta L
- Berry D
- Berry E
- Berryhill J
- Bertani M
- Bertl W
- Bertoldi M
- Berzano U
- Besancon M
- Besson A
- Betchart B
- Betev B
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Biallass P
- Bianchini L
- Bianco S
- Biasini M
- Biasotto M
- Biery K
- Biino C
- Bilei GM
- Bilki B
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- Bisello D
- Bitioukov S
- Blaha J
- Blekman F
- Bloch D
- Bloch I
- Bloch P
- Bloom K
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- Blum P
- Blumenfeld B
- Blyweert S
- Boccali T
- Bocci A
- Bockelman B
- Bodek A
- Bodin D
- Boeriu O
- Boldini M
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bona M
- Bonacorsi D
- Bonato A
- Bondar N
- Bontenackels M
- Boos E
- Borcherding F
- Borgia MA
- Bornheim A
- Borras K
- Borrello L
- Borsato E
- Bortoletto D
- Bos J
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- Bosi F
- Bostock F
- Botta C
- Boudoul G
- Bouhali O
- Bourgeois N
- Bourilkov D
- Bourrel T
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Brauer R
- Braunschweig W
- Breedon R
- Brett AM
- Breuker H
- Brew C
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- Briggs R
- Brigljevic V
- Broccolo G
- Brom JM
- Brooke JJ
- Brown RM
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- Bruno G
- Buchmuller O
- Budd H
- Buege V
- Buehler M
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burkett K
- Burtovoy V
- Busson P
- Busza W
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- Butler PH
- Butt J
- Butz E
- Bylsma B
- Caballero IG
- Cabrillo IJ
- Cafaro VD
- Cai J
- Caiazza SS
- Cakir A
- Cakir I. Turk
- Calderon A
- Cali IA
- Callner J
- Calloni M
- Calvo E
- Calzolari F
- Camanzi B
- Caminada L
- Campagnari C
- Campbell A
- Campderros JD
- Campi D
- Camporesi T
- Cankocak K
- Cano E
- Capiluppi P
- Caponeri B
- Cardaci M
- Carleton M
- Carlin R
- Carlsmith D
- Carroll R
- Cartiglia N
- Carvalho W
- Case M
- Cassel D
- Castaldi R
- Castellani L
- Castello R
- Castro A
- Castro E
- Castro MA
- Cattai A
- Caudron J
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceballos GG
- Cebra D
- Cepeda M
- Cerati GB
- Cerci S
- Cerizza G
- Cerminara G
- Ceron C
- Cerrada M
- Chabert EC
- Chan M
- Chandra A
- Chang P
- Chang S
- Chang YH
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chatelain JP
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Chauvey M
- Checchia P
- Checcucci B
- Chekhovsky V
- Chen EA
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen M
- Chen WT
- Chen Z
- Cheng TL
- Chertok M
- Chetluru V
- Cheung HWK
- Chien CY
- Chierici R
- Chiochia V
- Chiorboli M
- Chipaux R
- Chiumarulo F
- Chlebana F
- Choi M
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury RK
- Christian G
- Christiansen T
- Chtchipounov L
- Chuang SH
- Chung J
- Chung K
- Chung YS
- Churin I
- Chwalek T
- Cihangir S
- Cimmino A
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clemente A
- Clemente F
- Clerbaux B
- Cline D
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Colling D
- Colonna D
- Conetti S
- Contardo D
- Conte E
- Conti E
- Conway J
- Cooper SI
- Cordonnier AM
- Cortabitarte RV
- Cossutti F
- Costa M
- Costa S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Crawford M
- Creanza D
- Cremaldi LM
- Cripps N
- Crotty I
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cuscela G
- Cushman P
- Cussans D
- Cutts D
- Cwiok M
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Angelo P
- D'Antone I
- D'Enterria D
- D'Hondt J
- Dabrowski R
- Dafinei I
- Dagenhart W
- Dahmes B
- Dal Corso F
- Dallavalle GM
- Dambach S
- Damgov J
- Damiao DD
- Dammann D
- Daniel M
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
- Dasu S
- Dattola D
- Daubie E
- David A
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- Davies G
- de Abril IM
- de Abril MM
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De La Cruz B
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- de Monchenault GH
- De Palma M
- De Robertis G
- De Roeck A
- De Souza SF
- de Troconiz JF
- De Visscher S
- De Weirdt S
- De Wolf EA
- Debbins P
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- Deiters K
- Dejardin M
- Del Alamo MB
- del Arbol PMR
- Del Re D
- Delachenal V
- Delaere C
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Dellacasa G
- Delmeire E
- Demaria N
- Demarteau M
- Demin P
- Demina R
- Demir D
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- Denegri D
- Denisov A
- Deniz M
- Depasse P
- Dermenev A
- Dero V
- Derylo G
- Descamps J
- Devroede O
- Deyrail D
- Dharmaratna WGD
- Di Calafiori DRDS
- Di Giovanni GP
- Di Marco E
- Di Vincenzo S
- Dias MAF
- Diemoz M
- Dierlamm A
- Dimitrov A
- Dimitrov L
- Dinardo ME
- Dinu N
- Dirkes G
- Dissertori G
- Dittmar M
- Djaoshvili N
- Djordjevic M
- Do Amaral SMS
- Dobrzynski L
- Dobur D
- Dolen J
- Dolgopolov A
- Dominguez A
- Dominik W
- Donckt MV
- Donvito G
- Dorigo T
- Doroba K
- Dos Santos S
- Dosselli U
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- Druzhkin D
- Dubinin M
- Duda M
- Dudero PR
- Dudko L
- Dugad S
- Dughera G
- Dumanoglu I
- Dumitrache F
- Dupasquier T
- Dupont T
- Duric S
- Durkin LS
- Duru F
- Dusinberre E
- Dutta D
- Dutta S
- Dvornikov O
- Dykstra D
- Dyulendarova M
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edera LM
- Efron J
- Egeland R
- Eggel C
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- Elgammal S
- Elias JE
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- Erdmann M
- Erdmann W
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- Eskut E
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- Eugster J
- Eulisse G
- Eusebi R
- Evangelou I
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- Fabbricatore P
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- Fabozzi F
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- Fasanella D
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- Fernandez M
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- Ferri F
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- Filozova I
- Finger M
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- Fisk I
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- Gentit FX
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- Zachariadou A
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- Zhukova V
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Aligning the CMS Muon Chambers with the Muon Alignment System during an Extended Cosmic Ray Run
- Author
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- Publication venue
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
First measurement of the |t|-dependence of coherent J/ψ photonuclear production
- Author
- Acharya S
- Acosta FT
- Adam J
- Adamova D
- Adler A
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
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- Altsybeev I
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- Andreou D
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
The first measurement of the cross section for coherent J/ψ photoproduction as a function of |t|, the square of the momentum transferred between the incoming and outgoing target nucleus, is presented. The data were measured with the ALICE detector in ultra-peripheral Pb–Pb collisions at a centre-of-mass energy per nucleon pair sNN=5.02TeV with the J/ψ produced in the central rapidity region |y|<0.8, which corresponds to the small Bjorken-x range (0.3−1.4)×10−3.
The measured |t|-dependence is not described by computations based only on the Pb nuclear form factor, while the photonuclear cross section is better reproduced by models including shadowing according to the leading-twist approximation, or gluon-saturation effects from the impact-parameter dependent Balitsky–Kovchegov equation. These new results are therefore a valid tool to constrain the relevant model parameters and to investigate the transverse gluonic structure at very low Bjorken-x.publishedVersio
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17, the gravitational-wave event GW170817 was observed by the Advanced LIGO and Virgo detectors, and the gamma-ray burst (GRB) GRB 170817A was observed independently by the Fermi Gamma-ray Burst Monitor, and the Anti-Coincidence Shield for the Spectrometer for the International Gamma-Ray Astrophysics Laboratory. The probability of the near-simultaneous temporal and spatial observation of GRB 170817A and GW170817 occurring by chance is 5.0×10−8. We therefore confirm binary neutron star mergers as a progenitor of short GRBs. The association of GW170817 and GRB 170817A provides new insight into fundamental physics and the origin of short GRBs. We use the observed time delay of (+1.74±0.05)s between GRB 170817A and GW170817 to: (i) constrain the difference between the speed of gravity and the speed of light to be between −3×10−15 and +7×10−16 times the speed of light, (ii) place new bounds on the violation of Lorentz invariance, (iii) present a new test of the equivalence principle by constraining the Shapiro delay between gravitational and electromagnetic radiation. We also use the time delay to constrain the size and bulk Lorentz factor of the region emitting the gamma-rays. GRB 170817A is the closest short GRB with a known distance, but is between 2 and 6 orders of magnitude less energetic than other bursts with measured redshift. A new generation of gamma-ray detectors, and subthreshold searches in existing detectors, will be essential to detect similar short bursts at greater distances. Finally, we predict a joint detection rate for the Fermi Gamma-ray Burst Monitor and the Advanced LIGO and Virgo detectors of 0.1-1.4 per year during the 2018-2019 observing run and 0.3-1.7 per year at design sensitivity
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
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- Aakvaag E
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- Abicht NJ
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- Zenger DT
- Zenin O
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- Zhang X
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- Zhang Y
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- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
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- Zhou Y
- Zhu CG
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- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zgubič M
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- Zhang DF
- Zhang G
- Zhang J
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alhroob M
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- Ali S
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- Alimonti G
- Allaire C
- Allbrooke BMM
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- Allport PP
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- Alves FLL
- Alviggi MG
- Ambler A
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- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
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- Anelli CR
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- Zahreddine J
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- Zakharchuk N
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- Zeissner SV
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- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang DF
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- Zhang M
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
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