382 research outputs found
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- 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
- Aloisio A
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- Angelozzi I
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- Argyropoulos S
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- Arslan O
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- Butterworth JM
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- Chalupkova I
- Chang P
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- Chapman JD
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- Charlton DG
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- Chernyatin V
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- De Mendizabal JB
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Alberghi GL
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- Alconada Verzini MJ
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- Zhemchugov A
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV using the ATLAS detector
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- Zhemchugov A
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- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb−1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurement of the W±Z boson pair-production cross section in pp collisions at √s=13TeV with the ATLAS detector
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- Wiglesworth C
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- Wildauer A
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- Winklmeier F
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- Worm SD
- Wosiek BK
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- Yamanaka T
- Yamauchi K
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- Yao W-M
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- 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
- 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 new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid 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
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
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- Zhemchugov A
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- 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 fb−1 of √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 EmissT>150 GeV and EmissT>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 presented
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at root s = 8 TeV with the ATLAS detector (vol 75, 299, 2015)
- Author
- Aad G
- Abbott B
- Abdallah J
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- Yanush S
- Yao L
- Yao W-M
- Yasu Y
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- 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
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang J
- Zhang L
- 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 N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- 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
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ 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
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães Da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
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- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
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- Bernardi G
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- Berta P
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- Bessidskaia Bylund O
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- Biebel O
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- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
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- Biswal JP
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- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
- Brandt O
- Braren F
- Bratzler U
- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Bruckman De Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
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- Burmeister I
- Burr JTP
- Buschmann E
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- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Büscher D
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
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- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carrá S
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
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- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković 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 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ 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 57.0−5.9 +6.0 (stat.) −3.3 +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
Measurements of Higgs boson production and couplings in the four-lepton channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
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- Abdallah J
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- Zanzi D
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- Zhemchugov A
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- Zimine NI
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- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/08/2014
- Field of study
The final ATLAS Run 1 measurements of Higgs boson production and couplings in the decay channel H→ZZ∗→ℓ+ℓ−ℓ'+ℓ'−, where ℓ,ℓ′=e or μ, are presented. These measurements were performed using pp collision data corresponding to integrated luminosities of 4.5 and 20.3 fb−1 at center-of-mass energies of 7 and 8 TeV, respectively, recorded with the ATLAS detector at the LHC. The H→ZZ∗→4ℓ signal is observed with a significance of 8.1 standard deviations, with an expectation of 6.2 standard deviations, at mH=125.36 GeV, the combined ATLAS measurement of the Higgs boson mass from the H→γγ and H→ZZ∗→4ℓ channels. The production rate relative to the Standard Model expectation, the signal strength, is measured in four different production categories in the H→ZZ∗→4ℓ channel. The measured signal strength, at this mass, and with all categories combined, is 1.44+0.40−0.33. The signal strength for Higgs boson production in gluon fusion or in association with tt¯ or bb¯ pairs is found to be 1.7+0.5−0.4, while the signal strength for vector-boson fusion combined with WH/ZH associated production is found to be 0.3+1.6−0.9
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
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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 fb−1 of proton-proton collision data at √s =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.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). 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] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
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