219 research outputs found
Search for lepton flavor violating decays of a heavy neutral particle in p-pbar collisions at root(s)=1.8 TeV
- Author
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2003
- Field of study
We report on a search for a high mass, narrow width particle that decays
directly to e+mu, e+tau, or mu+tau. We use approximately 110 pb^-1 of data
collected with the Collider Detector at Fermilab from 1992 to 1995. No evidence
of lepton flavor violating decays is found. Limits are set on the production
and decay of sneutrinos with R-parity violating interactions.Comment: Figure 2 fixed. Reference 4 fixed. Minor changes to tex
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
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- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
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- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
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- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
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- Batley JR
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- Battistin M
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- Bedikian S
- Bednyakov VA
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- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
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- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
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- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
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- Bitenc U
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- Boeriu OEV
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- Bogdanchikov A
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- Boorman G
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- Bosman M
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- Botterill D
- Bouchami J
- Boudreau J
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- Brandt O
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- Bremer J
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- Bressler S
- Breton D
- Britton D
- Brochu FM
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- Brodet E
- Broggi F
- Bromberg C
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- Brunet S
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- Caloi R
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- Camarri P
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- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
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- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
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- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
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- Yusuff I
- Zabinski B
- Zaidan R
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- 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
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- Zhang H
- Zhang J
- Zhang L
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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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- Zhou L
- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- 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 the direct production of charginos and neutralinos in final states with tau leptons in âs=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Albergh GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
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- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
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- Amadio BT
- Amelung C
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- Amoroso S
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- Anders CF
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- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
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- Arslan O
- Artamonov A
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- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barajas CA Chavez
- Barak L
- Barberio EL
- Barberis D
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- Barklow T
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- Baroncelli A
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- Barranco Navarro L
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- Basalaev A
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- Caforio D
- Cairo VM
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- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
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- Castro NF
- Catinaccio A
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- Caudron J
- Cavaliere V
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- Cerda Alberich L
- Cerqueira AS
- Cerri A
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- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Che S
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- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
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- Cheng HJ
- Cheplakov A
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- da Costa J Barreiro Guimaraes
- Da Costa J Goncalves Pinto Firmino
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dai T
- Dale O
- Dallaire F
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- Dam M
- Damazio D Oliveira
- Dandoy JR
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- de Andrade Filho L Manhaes
- de Asmundis R
- De Benedetti A
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- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DE Ferreira
- De Lorenzi F
- De Maria A
- De Pedis D
- De Regie JB De Vivie
- de Renstrom PA Bruckman
- De Salvo A
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- Dehghanian N
- Deigaard I
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- della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
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- Demers S
- Demichev M
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- Denysiuk D
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- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Bello FA
- Di Ciaccio A
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- Di Clemente WK
- Di Donato C
- Di Girolamo A
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- Di Micco B
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- Di Petrillo KF
- Di Simone A
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- Yao W-M
- Yap YC
- Yasu Y
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- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang G
- Zhang H
- Zhang J
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- Zhang L
- Zhang M
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- Zhang R
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- 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
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fbâ1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ËÏ+1 ËÏâ1 pair production and of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the Ë ÏL state is set to be halfway between the masses of the Ëϱ1 and the ËÏ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ËÏ+1 ËÏâ1 for a massless ËÏ01. Common Ëϱ1 and ËÏ02 masses up to 760 GeV are excluded in the case of production of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 assuming a massless ËÏ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the Ëϱ1 and the ËÏ01 are also studied by varying the Ë ÏL mass between the masses of the Ëϱ1 and the ËÏ01
Jet energy measurement and its systematic uncertainty in protonâproton collisions at âs=7 TeV with the ATLAS detector
- Author
- A Buckley
- A Buckley
- A Sherstnev
- A. A. Carter
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Ahmad
- A. Aloisio
- A. Alonso
- A. Altheimer
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Antonaki
- A. Antonov
- A. Artamonov
- A. Astbury
- A. B. Fenyuk
- A. Bangert
- A. Baroncelli
- A. Bassalat
- A. Basye
- A. Beddall
- A. Bellerive
- A. Belloni
- A. Bingul
- A. Bocci
- A. Bogouch
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Buzatu
- A. C. Bundock
- A. C. Daniells
- A. C. Florez Bustos
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Cervelli
- A. Chafaq
- A. Cheplakov
- A. Chilingarov
- A. Chitan
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Corso-Radu
- A. Cortes-Gonzalez
- A. D. Hawkins
- A. D. Pilkington
- A. Dafinca
- A. De Salvo
- A. De Santo
- A. DellâAcqua
- A. Demilly
- A. Dewhurst
- A. Di Ciaccio
- A. Di Domenico
- A. Di Girolamo
- A. Di Mattia
- A. Di Simone
- A. Do Valle Wemans
- A. Doria
- A. Dos Anjos
- A. Dotti
- A. Dudarev
- A. DâOrazio
- A. E. Barton
- A. E. Kiryunin
- A. E. Loevschall-Jensen
- A. Ereditato
- A. F. Saavedra
- A. Farbin
- A. Farilla
- A. Favareto
- A. Ferrari
- A. Ferrer
- A. Ferretto Parodi
- A. FilipÄiÄ
- A. Firan
- A. Floderus
- A. Formica
- A. Forti
- A. G. Bogdanchikov
- A. G. Buckley
- A. G. Goussiou
- A. G. Leister
- A. G. Myagkov
- A. G. Olchevski
- A. Gabrielli
- A. Gabrielli
- A. Gemmell
- A. Gershon
- A. Glazov
- A. Gomes
- A. GoriĆĄek
- A. Grohsjean
- A. Haas
- A. Hamilton
- A. Harvey
- A. Henrichs
- A. Hoecker
- A. Hoummada
- A. Huettmann
- A. I. Butt
- A. I. Etienvre
- A. I. Mincer
- A. Irles Quiles
- A. J. Armbruster
- A. J. Barr
- A. J. Beddall
- A. J. Lankford
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- X. Hu
- X. Ju
- X. Li
- X. Lou
- X. Portell Bueso
- X. Prudent
- X. Ruan
- X. S. Anduaga
- X. Sun
- X. Wang
- X. Wu
- X. Zhang
- X. Zhuang
- Y. A. Kurochkin
- Y. Abulaiti
- Y. Amaral Coutinho
- Y. Arai
- Y. Azuma
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Hasegawa
- Y. Hernåndez Jiménez
- Y. Huang
- Y. Ikegami
- Y. Inamaru
- Y. J. Schnellbach
- Y. Jiang
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Liu
- Y. Makida
- Y. Ming
- Y. Munwes
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Pylypchenko
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Suzuki
- Y. Takahashi
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. V. Grishkevich
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhu
- Yu. A. Tikhonov
- Z. Czyczula
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. J. Grout
- Z. Kohout
- Z. L. Ren
- Z. Liang
- Z. Marshall
- Z. Rurikova
- Z. V. Krumshteyn
- Z. Vykydal
- Z. Weng
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS detector using protonâproton collision data with a centre-of-mass energy of âs=7 TeV corresponding to an integrated luminosity of 4.7 fb â1. Jets are reconstructed from energy deposits forming topological clusters of calorimeter cells using the anti-kt algorithm with distance parameters R=0.4 or R=0.6, and are calibrated using MC simulations. A residual JES correction is applied to account for differences between data and MC simulations. This correction and its systematic uncertainty are estimated using a combination of in situ techniques exploiting the transverse momentum balance between a jet and a reference object such as a photon or a Z boson, for 20â€pTjet1 TeV. The calibration of forward jets is derived from dijet pT balance measurements. The resulting uncertainty reaches its largest value of 6 % for low-pT jets at |η|=4.5. Additional JES uncertainties due to specific event topologies, such as close-by jets or selections of event samples with an enhanced content of jets originating from light quarks or gluons, are also discussed. The magnitude of these uncertainties depends on the event sample used in a given physics analysis, but typically amounts to 0.5â3 %
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biondi S
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blanco JE
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OE Vickey
- Boerner D
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
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- 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
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particleâhole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Abolins M
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- Aleksandrov IN
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- Zhemchugov A
- Zheng S
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Charged-particle distributions at low transverse momentum in âs=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
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- Abdallah J
- Abdinov O
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- Ruschke A
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- Scarfone V
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- Schoeffel L
- Schoening A
- Schoenrock BD
- Schopf E
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- Schroeder TV
- Schuh N
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- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwegler P
- Schweiger H
- Schwemling P
- Schwienhorst R
- Schwindling J
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- Sciolla G
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- Searcy J
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- Seliverstov DM
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- Sforza F
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- Shehu CY
- Sherwood P
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- Shimmin CO
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- Shiyakova M
- Shmeleva A
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- Shojaii S
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
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- Sidiropoulou O
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- Sidoti A
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- Silverstein SB
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- Sivoklokov SY
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- Skottowe HP
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- Slavicek T
- Slawinska M
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- Soloshenko A
- Solovyanov OV
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- Sotiropoulou CL
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- Stenzel H
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- Stonjek S
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- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
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- Sundermann JE
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- Talyshev AA
- Tan KG
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- Tarem S
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
- Tassi E
- Tayalati Y
- Taylor AC
- Taylor GN
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- Taylor W
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- Teischinger FA
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- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
- Terada S
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- Teuscher RJ
- Theenhausen HMZ
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- Trofymov A
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- Trottier-McDonald M
- Trovatelli M
- Truong L
- Trzebinski M
- Trzupek A
- Tseng JC-L
- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
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- Turchikhin S
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- Turgeman D
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- Tyndel M
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urban SC
- Urquijo P
- Urrejola P
- Usai G
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- Valderanis C
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- Valentinetti S
- Valero A
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- Valkar S
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- Van der Deijl PC
- van der Geer R
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- van Vulpen I
- van Woerden MC
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- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
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- Vermeulen JC
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- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Vigne R
- Villa M
- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vittori C
- Vivarelli I
- Vlachos S
- Vlasak M
- Vogel M
- Vokac P
- Volpi G
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- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
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- Vossebeld JH
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- Vrba V
- Vreeswijk M
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- Vukotic I
- Vykydal Z
- Wagner P
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- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weiser C
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- Wells PS
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- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
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- Wilkens HG
- Williams HH
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- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wittkowski J
- Wolter MW
- Wolters H
- Wong KHY
- Worm SD
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
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- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yakabe R
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- 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
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- 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
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- Zhu CG
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in protonâproton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 ÎŒb â1 ÎŒbâ1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Measurement of the inelastic proton-proton cross section at âs=13 TeV with the ATLAS detector at the LHC
- Author
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
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- Komori Y
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- Kotwal A
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- Kourkoumelis C
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- Zobernig G
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- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
This Letter presents a measurement of the inelastic proton-proton cross section using 60ââÎŒb â1 of pp collisions at a center-of-mass energy âs of 13 TeV with the ATLAS detector at the LHC. Inelastic interactions are selected using rings of plastic scintillators in the forward region (2.0710 â6 , where M X is the larger invariant mass of the two hadronic systems separated by the largest rapidity gap in the event. In this Ο range the scintillators are highly efficient. For diffractive events this corresponds to cases where at least one proton dissociates to a system with M X >13ââGeV . The measured cross section is compared with a range of theoretical predictions. When extrapolated to the full phase space, a cross section of 78.1±2.9ââmb is measured, consistent with the inelastic cross section increasing with center-of-mass energy
Study of ordered hadron chains with the ATLAS detector
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- Zanzi D
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- Zemla A
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- Zeng Q
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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
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 ÎŒbâ1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy âs=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
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