43 research outputs found
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in pp collisions at root s=13 TeV with the ATLAS detector
- 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
- Adachi S
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- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
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- Yildiz HD
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- Zahreddine J
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
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- Zhang G
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- Zhang Z
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2020
- Field of study
A search for long-lived particles decaying into hadrons and at least one muon is presented. The analysis selects events that pass a muon or missing-transverse-momentum trigger and contain a displaced muon track and a displaced vertex. The analyzed dataset of proton-proton collisions at
√
s
=
13 TeV
was collected with the ATLAS detector and corresponds to
136
fb
−
1. The search employs dedicated reconstruction techniques that significantly increase the sensitivity to long-lived particle decays that occur in the ATLAS inner detector. Background estimates for Standard Model processes and instrumental effects are extracted from data. The observed event yields are compatible with those expected from background processes. The results are presented as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model, and interpreted as exclusion limits in scenarios with pair production of long-lived top squarks that decay via a small
R
-parity-violating coupling into a quark and a muon. Top squarks with masses up to 1.7 TeV are excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01 ns and 30 ns
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
- Author
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- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abhayasinghe Dk
- Abidi Sh
- Abouzeid Os
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- Abramowicz H
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- Abulaiti Y
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- Achkar B
- Adachi S
- Adam Bourdarios C
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- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
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- Al Khoury K
- Alberghi Gl
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- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
- Alexandre D
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- Alfonsi A
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- Ali B
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- Bobbink Gj
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- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov Ag
- Bohm C
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- Breaden Madden Wd
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- Briglin Dl
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- Brock I
- Brock R
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- Brooks Wk
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- Broughton Jh
- Bruckman De Renstrom Pa
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- Bruni A
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- Bruno S
- Brunt Bh
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Buhrer F
- Bulekov O
- Burch Tj
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- Burr Jtp
- Burton Cd
- Burzynski Jc
- Buscher V
- Buschmann E
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Butti P
- Buttinger W
- Buxo Vazquez Cj
- Buzatu A
- Buzykaev Ar
- Cabras G
- Cabrera Urban 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
- Calvet S
- Calvet Tp
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido Mdm
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson Bt
- Carminati L
- Carney Rmd
- Caron S
- Carquin E
- Carra S
- Carter Jws
- Casado Mp
- Casha Af
- Casper Dw
- Castelijn R
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerny K
- Cerqueira As
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chan Sk
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chau Cc
- Che S
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chelstowska Ma
- Chen B
- Chen C
- Chen Ch
- Chen H
- Chen J
- Chen J
- Chen S
- Chen Sj
- Chen X
- Chen Y
- Chen Y-
- Cheng Hc
- Cheng Hj
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalerias Tja
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu I
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chouridou S
- Chow Ys
- Chu Mc
- Chu X
- Chudoba J
- Chuinard Aj
- Chwastowski Jj
- Chytka L
- Cieri D
- Ciesla Km
- Cinca D
- Cindro V
- Cioara Ia
- Ciocio A
- Cirotto F
- Citron Zh
- Citterio M
- Ciubotaru Da
- Ciungu Bm
- Clark A
- Clark Mr
- Clark Pj
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra Aec
- Colasurdo L
- Cole B
- Colijn Ap
- Collot J
- Conde Muino P
- Coniavitis E
- Connell Sh
- Connelly Ia
- Constantinescu S
- Conventi F
- Cooper-Sarkar Am
- Cormier F
- Cormier Kjr
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cowan G
- Cowley Jw
- Crane J
- Cranmer K
- Crawley Sj
- Creager Ra
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman Ar
- Cunningham Wr
- Czekierda S
- Czodrowski P
- D'Amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio M
- Da Cunha Sargedas De Sousa Mj
- Da Fonseca Pinto Jv
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damp J
- Dandoy Jr
- Daneri Mf
- Dang Np
- Dann Ns
- Danninger M
- Dao V
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- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- De Jong P
- De La Torre H
- De Maria A
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Vasconcelos Corga K
- De Vivie De Regie Jb
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- Debenedetti C
- Dedovich Dv
- Deiana Am
- Del Gaudio M
- Del Peso J
- Delabat Diaz Y
- Delgove D
- Deliot F
- Delitzsch Cm
- Dell'Acqua A
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- Demers S
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- Demontigny G
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- Denysiuk D
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- Di Donato C
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- Flores Castillo Lr
- Flores L
- Follega Fm
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- Formica A
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- Wingerter-Seez I
- Winkels E
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- Wittgen M
- Wobisch M
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- Wolter Mw
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- Woods Nl
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- Wosiek Bk
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- Wu Sl
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- Wyatt Tr
- Wynne Bm
- Xella S
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- Xiao X
- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
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- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
- Young Cjs
- Yu J
- Yuan R
- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou Ms
- 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
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Measurement of the transverse momentum distribution of Drell–Yan lepton pairs in proton–proton collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud A
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich L
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- 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
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
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- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- The European Physical Journal C
- Publication date
- 01/01/2020
- Field of study
Abstract: This paper describes precision measurements of the transverse momentum pTℓℓ (ℓ=e, μ) and of the angular variable ϕη∗ distributions of Drell–Yan lepton pairs in a mass range of 66–116 GeV. The analysis uses data from 36.1 fb-1 of proton–proton collisions at a centre-of-mass energy of s=13TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton–proton collisions at s=7 and 8TeV, these new measurements probe perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. They reach a precision of 0.2% for the normalized spectra at low values of pTℓℓ. The data are compared with different QCD predictions, where it is found that predictions based on resummation approaches can describe the full spectrum within uncertainties
Search for direct production of electroweakinos in final states with missing transverse momentum and a Higgs boson decaying into photons in pp collisions at s = 13 TeV with the ATLAS detector
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- Yildiz H
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- Zahreddine J
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- Zakharchuk N
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- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang DF
- Zhang G
- Zhang H
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- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou C
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- Zhu CG
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- 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
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- Journal of High Energy Physics
- Publication date
- 01/01/2020
- Field of study
Abstract: A search for a chargino-neutralino pair decaying via the 125 GeV Higgs boson into photons is presented. The study is based on the data collected between 2015 and 2018 with the ATLAS detector at the LHC, corresponding to an integrated luminosity of 139 fb−1 of pp collisions at a centre-of-mass energy of 13 TeV. No significant excess over the expected background is observed. Upper limits at 95% confidence level for a massless χ˜10 are set on several electroweakino production cross-sections and the visible cross-section for beyond the Standard Model processes. In the context of simplified supersymmetric models, 95% confidence-level limits of up to 310 GeV in mχ˜1±/χ˜20, where mχ˜10 = 0.5 GeV, are set. Limits at 95% confidence level are also set on the χ˜1±χ˜20 cross-section in the mass plane of mχ˜1±/χ˜20 and mχ˜10, and on scenarios with gravitino as the lightest supersymmetric particle. Upper limits at the 95% confidence-level are set on the higgsino production cross-section. Higgsino masses below 380 GeV are excluded for the case of the higgsino fully decaying into a Higgs boson and a gravitino
Search for new phenomena in final states with large jet multiplicities and missing transverse momentum using s = 13 TeV proton-proton collisions recorded by ATLAS in Run 2 of the LHC
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud A
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich L
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
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- Alshehri AA
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
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- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
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- Anastopoulos C
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- Andeen T
- Anders CF
- Anders JK
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- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
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- Aoki M
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- Astigarraga MEP
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- Zemaityte G
- Zeng JC
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- Zhemchugov A
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- Journal of High Energy Physics
- Publication date
- 01/01/2020
- Field of study
Abstract: Results of a search for new particles decaying into eight or more jets and moderate missing transverse momentum are presented. The analysis uses 139 fb−1 of proton-proton collision data at s = 13 TeV collected by the ATLAS experiment at the Large Hadron Collider between 2015 and 2018. The selection rejects events containing isolated electrons or muons, and makes requirements according to the number of b-tagged jets and the scalar sum of masses of large-radius jets. The search extends previous analyses both in using a larger dataset and by employing improved jet and missing transverse momentum reconstruction methods which more cleanly separate signal from background processes. No evidence for physics beyond the Standard Model is found. The results are interpreted in the context of supersymmetry-inspired simplified models, significantly extending the limits on the gluino mass in those models. In particular, limits on the gluino mass are set at 2 TeV when the lightest neutralino is nearly massless in a model assuming a two-step cascade decay via the lightest chargino and second-lightest neutralino
Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in s = 13 TeV pp collisions using the ATLAS detector
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- Yildiz H
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- Zahreddine J
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- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- The European Physical Journal C
- Publication date
- 01/01/2020
- Field of study
Abstract: A search for the electroweak production of charginos and sleptons decaying into final states with two electrons or muons is presented. The analysis is based on 139 fb-1 of proton–proton collisions recorded by the ATLAS detector at the Large Hadron Collider at s=13 TeV. Three R-parity-conserving scenarios where the lightest neutralino is the lightest supersymmetric particle are considered: the production of chargino pairs with decays via either W bosons or sleptons, and the direct production of slepton pairs. The analysis is optimised for the first of these scenarios, but the results are also interpreted in the others. No significant deviations from the Standard Model expectations are observed and limits at 95% confidence level are set on the masses of relevant supersymmetric particles in each of the scenarios. For a massless lightest neutralino, masses up to 420 Ge are excluded for the production of the lightest-chargino pairs assuming W-boson-mediated decays and up to 1 TeV for slepton-mediated decays, whereas for slepton-pair production masses up to 700 Ge are excluded assuming three generations of mass-degenerate sleptons
Systemic Lupus Erythematosus and the Kidney
- Author
- A Chang
- A Ghafari
- A Ho
- A Ho
- A Kaser
- A Kuhn
- A Kuroki
- A McKinley
- A Perna
- A Rietveld
- A Satoskar
- A Siso
- A Smyth
- A Tandon
- AE Prada
- AI Quintero-Del-Rio
- AI Quintero-del-Rio
- AJ Howie
- AJW Branten
- AK Wiglesworth
- AS Al Arfaj
- ASA Arfaj
- AT Tieng
- B Alchi
- B Griffiths
- B Liang
- B Mittal
- B Pons-Estel
- BA Kiberd
- BH Hahn
- BH Hahn
- BH Rovin
- BH Rovin
- BH Rovin
- BH Rovin
- BH Rovin
- BH Rovin
- C Baecher-Allan
- C Fiehn
- C Fiehn
- C Gordon
- C Grootscholten
- C Grootscholten
- C Krishnan
- C Mok
- C Orellana
- C Skamra
- C Xie
- C Zoja
- CC Mok
- CC Mok
- CC Mok
- CC Mok
- CC Mok
- CC Najafi
- CC Szeto
- CF Mojcik
- CH Hinze
- CL Anderson
- CT Weaver
- D Askenazi
- D Ge
- D Gomez
- D Isenberg
- D Jayne
- D Koffler
- D Malide
- D Philibert
- DI Daikh
- DJ Birmingham
- DJ Birmingham
- DJ Birmingham
- DJ Birmingham
- DJ Wallace
- DM Fine
- DM Ricker
- DN Spetie
- DT Boumpas
- DY Chen
- E Baranowska-Daca
- E Bettelli
- E Daugas
- E Imbasciati
- E Sousa
- E Tsakonas
- E Villanueva
- EC Baechler
- EC Sommers
- ECF Wilson
- EK Li
- EM Ginzler
- EM Tan
- FA Houssiau
- FA Houssiau
- FA Houssiau
- FB Karassa
- FB Karassa
- FG Cosio
- FJ Barrat
- FM Ribeiro
- FS Zhang
- G Biesecker
- G Biesecker
- G Carvalheiras
- G Cassese
- G Contreras
- G Contreras
- G Contreras
- G Jego
- G Moroni
- G Moroni
- G Moroni
- G Moroni
- G Moroni
- G PerezLema
- G Remuzzi
- G Wang
- GB Appel
- GG Illei
- GH Tesch
- GJ Pons-Estel
- GK Bertsias
- GMN Daleboudt
- GS Hill
- GS Hill
- GS Hill
- GS Hill
- GS Markowitz
- GS Markowitz
- H Bagavant
- H Bagavant
- H Bao
- H Dobnig
- H Gonzalez-Dettoni
- H Hemmi
- H Kato
- H Ogawa
- H Ogawa
- H Wu
- H Yokoyama
- HA Austin III
- HA Austin III
- HA Austin III
- HC Nossent
- HD Pettigrew
- HI Brunner
- HJ Anders
- HJ Ramos
- HK Goyal
- HM Bastian
- HN Reich
- HR Deicher
- HR Holman
- HR Koene
- HW Lim
- HY Wang
- I Gunnarsson
- I Gunnarsson
- IEM Coremans
- IT Harley
- J Ermann
- J Font
- J Radhakrishnan
- J Schifferli
- J Yates
- J Zavada
- J-H Yen
- JA Schifferli
- JB Winfield
- JC Crispin
- JC Oates
- JD Hron
- JD Ordonez
- JE Salmon
- JE Teixeira
- JJ Weening
- JM Esdaile
- JM Esdaile
- JM Esdaile
- JM Esdaile
- JM Esdaile
- JP Grande
- JP Paccaud
- JPA Ioannidis
- JR Sedor
- JS Cameron
- JS Navratil
- JV Donadio
- JV Donadio
- JW Bauer
- JW Bauer
- JW Huang
- K Abe
- K Abe
- K Iida
- K Masutani
- K Vlam de
- KE Sada
- KE Taylor
- KE Taylor
- Kidney Disease
- KJ Scalapino
- KJ Scalapino
- KL Moser
- KM Gallagher
- KR Kozak
- KS Peterson
- KT Ellington
- L Bennett
- L Christopher-Stine
- L Mercadal
- L Morel-Maroger
- L Rauova
- LA Hebert
- LA Hebert
- LA Hebert
- LA Trouw
- LC Korb
- LE Ronnblom
- LJ Mason
- LM Ong
- LT Hiraki
- M Abbate
- M Adler
- M Arora
- M Chelamcharla
- M Dall’Era
- M Faurschou
- M Faurschou
- M Garcia-Carrasco
- M Haubitz
- M Kalaaji
- M Marchini
- M Matsumoto
- M Mizuno
- M Pitashny
- M Ramos-Casals
- M Roland
- M Suzuki
- M Suzuki
- M Trendelenburg
- M Tucci
- M Tucci
- M Tucci
- M Urowitz
- MA Dooley
- MA Dooley
- MC Pickering
- MD Kazatchkine
- ME Devey
- MF Denny
- MG Tektonidou
- MG Tektonidou
- MH Park
- MI Danila
- MJ Fritzler
- MJ Siedner
- MJ Walport
- MM Schwartz
- MM Schwartz
- MM Schwartz
- MM Ward
- MR Gonzalez-Crespo
- MW Taal
- MY Karim
- N Charles
- N Hiramatsu
- N Iikuni
- N Jacob
- N Kasitanon
- N Marto
- N Rothfield
- N Ruperto
- N Zahr
- O Traitanon
- OM Steinmetz
- OT Chan
- P Bossu
- P Lertdumrongluk
- PAM Warmerdam
- PD Walker
- PI Burgos
- PJ Verroust
- PM Izmirly
- PP Sfikakis
- PS Ramos
- Q Fu
- R Campbell Jr
- R Flierman
- R Gerli
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- R Hirschberg
- R Kaiser
- R Lafyatis
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- RA Sinico
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
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- Publication venue
- 'Indian Society for Education and Environment'
- Publication date
- Field of study
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in pp collisions at s=13 TeV with the ATLAS detector
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- Aad G
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- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
- Zgubic M
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- Zhang G
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- Physical Review D
- Publication date
- 01/01/2020
- Field of study
A search for long-lived particles decaying into hadrons and at least one muon is presented. The analysis selects events that pass a muon or missing-transverse-momentum trigger and contain a displaced muon track and a displaced vertex. The analyzed dataset of proton-proton collisions at s=13 TeV was collected with the ATLAS detector and corresponds to 136 fb−1. The search employs dedicated reconstruction techniques that significantly increase the sensitivity to long-lived particle decays that occur in the ATLAS inner detector. Background estimates for Standard Model processes and instrumental effects are extracted from data. The observed event yields are compatible with those expected from background processes. The results are presented as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model, and interpreted as exclusion limits in scenarios with pair-production of long-lived top squarks that decay via a small R-parity-violating coupling into a quark and a muon. Top squarks with masses up to 1.7 TeV are excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01 ns and 30 ns
Search for resonances decaying into a weak vector boson and a Higgs boson in the fully hadronic final state produced in proton-proton collisions at s =13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Vos M
- Vossebeld JH
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- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
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- Walkowiak W
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- Weingarten J
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- Wenaus T
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- Weston TD
- Whalen K
- Whallon NL
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- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilk F
- Wilkens HG
- Wilkins LJ
- Williams HH
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- Winter BT
- Wittgen M
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- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
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- Yan Z
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- Yao W-M
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- Yexley MR
- Yigitbasi E
- Yildiz H
- Yorita K
- Yoshihara K
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- Young CJS
- Yu J
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- Yue X
- Yuen SPY
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
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- Zhang G
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- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2020
- Field of study
A search for heavy resonances decaying into a W or Z boson and a Higgs boson produced in proton-proton collisions at the Large Hadron Collider at s=13 TeV is presented. The analysis utilizes the dominant W→qq¯′ or Z→qq¯ and H→bb¯ decays with substructure techniques applied to large-radius jets. A sample corresponding to an integrated luminosity of 139 fb-1 collected with the ATLAS detector is analyzed and no significant excess of data is observed over the background prediction. The results are interpreted in the context of the heavy vector triplet model with spin-1 W′ and Z′ bosons. Upper limits on the cross section are set for resonances with mass between 1.5 and 5.0 TeV, ranging from 6.8 to 0.53 fb for W′→WH and from 8.7 to 0.53 fb for Z′→ZH at the 95% confidence level