71 research outputs found
Entanglement, space-time and the Mayer-Vietoris theorem
- Author
- A Hamma
- A Kitaev
- A Patrascu
- A Strominger
- Andrei T. Patrascu
- AS Schwarz
- AT Patrascu
- CD Jaekel
- CD Jakel
- D Buchholz
- D Zhou
- DR Terno
- E Schrödinger
- F Mintert
- FL Thorp-Greenwood
- FM Haehl
- FSN Lobo
- H Reeh
- H Sati
- I Ibnouhsein
- J Anandan
- J Audretsch
- J Maldacena
- L Derkacz
- L Vietoris
- LH Kauffman
- M Raamsdonk Van
- MC Palmer
- MC Palmer
- MD Kruskal
- N Bao
- O Ben-Ami
- O Viro
- R Colella
- R Verch
- S Ryu
- S Schlieder
- SA Werner
- SJ Summers
- SJ Summers
- SJ Summers
- TP Oliveira
- Y Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV 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
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- 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
- Alvarez Piqueras D
- 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
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJ
- Anulli F
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- Arabidze G
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Search for bottom-squark pair production in pp collision events at √s=13 TeV with hadronically decaying τ-leptons, b-jets, and missing transverse momentum using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
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- Adamek L
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- Aguilar-Saavedra JA
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- Ahmed WS
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- Akesson TPA
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- Alberghi GL
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- Aleksandrov IN
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- Zhemchugov A
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- Zorbas TG
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2021
- Field of study
A search for pair production of bottom squarks in events with hadronically decaying
τ
-leptons,
b
-tagged jets, and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at
√
s
=
13
TeV
delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of
139
fb
−
1
. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino
˜
χ
0
2
and a bottom quark, with
˜
χ
0
2
decaying into a Higgs boson and the lightest neutralino
˜
χ
0
1
. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying
τ
-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the
˜
χ
0
2
, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between
˜
χ
0
2
and
˜
χ
0
1
. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model
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
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- Zhemchugov A
- Zheng Z
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- Zieminska D
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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.]
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
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- Middleton RP
- Miguens JM
- Mikenberg G
- Mikestikova M
- Mikuz M
- Mildner H
- Milic A
- Milke CD
- Miller DW
- Miller LS
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minashvili IA
- Mince L
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- Mineev M
- Minegishi Y
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- Mir LM
- Mironova M
- Mitani T
- Mitrevski J
- Mitsou VA
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- Miu O
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- Miyagawa PS
- Mizukami A
- Mjornmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
- Mobius S
- Mochizuki K
- Moder P
- Mogg P
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- Montella M
- Monticelli F
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- Morgenstern S
- Mori D
- Morii M
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- Morisbak V
- Morley AK
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- Moschovakos P
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- Moskvitina P
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- Muenstermann D
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- Mullier GA
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- Murrone A
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- Muskinja M
- Mwewa C
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- Napolitano F
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- Naryshkin I
- Naseri M
- Naumann T
- Navarro G
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- Nechaeva PY
- Nechansky F
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- Nelson ME
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- Nessi M
- Neubauer MS
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- Newhouse R
- Newman PR
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- Nickerson RB
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- Nielsen J
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- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Nisati A
- Nishu N
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- Nitsche I
- Nitta T
- Nobe T
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- Noguchi Y
- Nomidis I
- Nomura MA
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- Novak J
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- Novgorodova O
- Novotny R
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- Nurse E
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- O'Neil DC
- O'neill AP
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- Oakham FG
- Ocariz J
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- Okazaki Y
- Okumura Y
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- Oleiro Seabra LF
- Olivares Pino SA
- Oliveira MVS
- Oliver JL
- Olsson MJR
- Olszewski A
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- Onofre A
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Orellana GE
- Orestano D
- Orlando N
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- Otero Y Garzon G
- Otono H
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- Ottino GJ
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- Owen RE
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- Pacheco Pages A
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- Palacino G
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- Pani P
- Panizzo G
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- Papadatos C
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- Paraskevopoulos C
- Pardos CD
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- Parsons JA
- Parzefall U
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- Pascuzzi VR
- Pasner JMP
- Pasquali F
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- Pastor ET
- Pastore F
- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
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- Perego MM
- Pereira Peixoto AP
- Pereira RA
- Perepelitsa D
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- Petersen BA
- Petersen TC
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- Pezoa R
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- Phipps MW
- Piacquadio G
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- Piegaia R
- Pietreanu D
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pinto JVDF
- Pitt M
- Pizzimento L
- Pizzini A
- Pleier M-A
- Plesanovs V
- Pleskot V
- Plotnikova E
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Portales L
- Pospisil S
- Potamianos K
- Potrap IN
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- Powell TD
- Pownall G
- Pozo Astigarraga ME
- Prades Ibanez A
- Pralavorio P
- Prapa MM
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- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
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- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
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- Rebuzzi DM
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- Reikher D
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- Renardi A
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- Rendel MB
- Rennie AG
- Renous DS
- Renteria CG
- Resconi S
- Resseguie ED
- Rettie S
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- Reynolds E
- Rezanova OL
- Reznicek P
- Ricci E
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- Richter S
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- Rieck P
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- Rimoldi A
- Rimoldi M
- Rinaldi L
- Rinn TT
- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
- Rizvi E
- Rizzi C
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- Robin M
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- Rocchi A
- Roda C
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- Rodriguez AR
- Roe S
- Roggel J
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- Rojas RA
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- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
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- Rosser BJ
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- Rossi LP
- Rossini L
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- Roy D
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Ruggeri TA
- Ruhr F
- Ruiz-Martinez A
- Rummler A
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- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Ruttinger EM
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- Rybkin G
- Rye EB
- Ryzhov A
- Sabater Iglesias JA
- Sabatini P
- Sabetta L
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- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Safdari M
- Saha P
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Salamani D
- Salamanna G
- Salnikov A
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- Salvador Salas A
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- Samarati J
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
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- Sanchez LP
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
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- Santpur SN
- Santra A
- Santurio EV
- Saoucha KA
- Sapronov A
- Saraiva JG
- Sasaki O
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- Sayago Galvan I
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- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
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- Schafer U
- Schaffer AC
- Schaile D
- Schamberger RD
- Schanet E
- Scharf C
- Scharmberg N
- Schegelsky VA
- Scheirich D
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- Schillaci ZM
- Schioppa EJ
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- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schulte A
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Scyboz LM
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Semprini-Cesari N
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- Sforza F
- Sfyrla A
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- Shahinian JD
- Shaikh NW
- Shan LY
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- Sharma A
- Sharma AS
- Shatalov PB
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- Shaw SM
- Shehade M
- Shen Y
- Sherman AD
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- Shimmin CO
- Shimogama Y
- Shimojima M
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
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- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Silva M
- Silverstein SB
- Simion S
- Simoniello R
- Simpson-allsop CJ
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjolin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
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- Snesarev AA
- Snoek HL
- Snyder IM
- Snyder S
- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov O
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song W
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
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- Stamas BL
- Stamen R
- Stamenkovic M
- Stampekis A
- Stanecka E
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Staroba P
- Starovoitov P
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- Steinhebel AL
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- Stewart GA
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- Stolarski M
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- Straessner A
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- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strohmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
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- Suarez NB
- Suarez RG
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
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- Taenzer J
- Taffard A
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- Taibah RHM
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- Tarna G
- Tartarelli GF
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- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor AJ
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- Tee AS
- Tehrani FS
- Teixeira-Dias P
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- Teoh JJ
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- Terron J
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- Theveneaux-Pelzer T
- Thomas DW
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- Thorpe EJ
- Tikhomirov VO
- Tikhonov YA
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- Tisserant S
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- Trofymov A
- Troncon C
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- Trzupek A
- Tsai F
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- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra R
- Tuts PM
- Tzamarias S
- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
- Unal M
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
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- Urban J
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
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- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
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- Vranjes N
- Vrba V
- Vu NK
- Vuillermet R
- Vukotic I
- Wada S
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Wakasa R
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
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- Wang C
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- Wanotayaroj C
- Warburton A
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- Ward RJ
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- Webb AF
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- Weber SM
- Wei Y
- Weidberg AR
- Weingarten J
- Weirich M
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- Wells PS
- Wenaus T
- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
- Weston TD
- Whalen K
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Wongel AF
- Woods NL
- Worm SD
- Wosiek BK
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Xella S
- Xiang J
- Xiao X
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- 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 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for dark matter in events with missing transverse momentum and a Higgs boson decaying into two photons in pp collisions at root s=13 TeV with the ATLAS detector
- Author
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2021
- Field of study
A search for dark-matter particles in events with large missing transverse momentum and a Higgs boson candidate decaying into two photons is reported. The search uses 139 fb−1 of proton-proton collision data collected at s√ = 13 TeV with the ATLAS detector at the CERN LHC between 2015 and 2018. No significant excess of events over the Standard Model predictions is observed. The results are interpreted by extracting limits on three simplified models that include either vector or pseudoscalar mediators and predict a final state with a pair of dark-matter candidates and a Higgs boson decaying into two photons
Two-particle azimuthal correlations in photonuclear ultraperipheral Pb plus Pb collisions at 5.02 TeV with ATLAS
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- Zakharchuk N
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- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zimine N
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- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2021
- Field of study
Two-particle long-range azimuthal correlations are measured in photonuclear collisions using
1.7
nb
−
1
of 5.02 TeV
Pb
+
Pb
collision data collected by the ATLAS experiment at the CERN Large Hadron Collider. Candidate events are selected using a dedicated high-multiplicity photonuclear event trigger, a combination of information from the zero-degree calorimeters and forward calorimeters, and from pseudorapidity gaps constructed using calorimeter energy clusters and charged-particle tracks. Distributions of event properties are compared between data and Monte Carlo simulations of photonuclear processes. Two-particle correlation functions are formed using charged-particle tracks in the selected events, and a template-fitting method is employed to subtract the nonflow contribution to the correlation. Significant nonzero values of the second- and third-order flow coefficients are observed and presented as a function of charged-particle multiplicity and transverse momentum. The results are compared with flow coefficients obtained in proton-proton and proton-lead collisions in similar multiplicity ranges, and with theoretical expectations. The unique initial conditions present in this measurement provide a new way to probe the origin of the collective signatures previously observed only in hadronic collision
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton in pp 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 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
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- 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
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
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- Anastopoulos C
- Andari N
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- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
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- Anthony MT
- Antipov E
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- Anulli F
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- Aparisi Pozo JA
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- Araya ST
- Arcangeletti C
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- Arguin J-F
- Argyropoulos S
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- Bostanabad MG
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- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
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- Yallup DP
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- 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 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at s√ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV
Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Publication venue
- IOP
- Publication date
- 01/01/2021
- Field of study
Non-ionizing energy loss causes bulk damage to the silicon sensors of the ATLAS pixel and strip detectors. This damage has important implications for data-taking operations, charged-particle track reconstruction, detector simulations, and physics analysis. This paper presents simulations and measurements of the leakage current in the ATLAS pixel detector and semiconductor tracker as a function of location in the detector and time, using data collected in Run 1 (2010–2012) and Run 2 (2015–2018) of the Large Hadron Collider. The extracted fluence shows a much stronger |z|-dependence in the innermost layers than is seen in simulation. Furthermore, the overall fluence on the second innermost layer is significantly higher than in simulation, with better agreement in layers at higher radii. These measurements are important for validating the simulation models and can be used in part to justify safety factors for future detector designs and interventions.publishedVersio
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