40 research outputs found
Prospect theory and tax evasion: a reconsideration of the Yitzhaki puzzle
- Author
- A al-Nowaihi
- A al-Nowaihi
- A Bruhin
- A Isoni
- A Piolatto
- A Tversky
- Amedeo Piolatto
- B KĆszegi
- C Camerer
- CT Clotfelter
- D Kahneman
- D Prelec
- DE Bell
- G Yaniv
- GW Harrison
- HJ Kleven
- J Alm
- J Apesteguia
- J Poterba
- J Reinganum
- JPF Gordon
- JS Feinstein
- L Santos-Pinto
- M Bernasconi
- M Bernasconi
- Matthew D. Rablen
- MD Rablen
- MM Ali
- N Friedland
- N Hashimzade
- N Kamdar
- NC Barberis
- R DellâAnno
- R Fisman
- R Masatlioglu
- S Dhami
- S Yitzhaki
- SE Crane
- U Schmidt
- V Köbberling
- V Sadiraj
- W Neilson
- WW Pommerehne
- Y Kim
- Y Kim
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 14/11/2016
- Field of study
The standard expected utility (EUT) model of tax evasion predicts that evasion is decreasing in the marginal tax rate (the Yitzhaki puzzle). Recent literature shows cases in which incorporating prospect theory (PT) does and does not overturn the Puzzle. In a general environment that nests both PT and EUT preferences, we provide a detailed study of how the elements of PT affect the Puzzle. PT does not always reverse the Puzzle, hence we give and interpret conditions for when it does and does not. When allowing for stigma and/or variable audit probability, PT reverses the Puzzle in the same way and with the same limitations as does EUT, if equally augmented
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- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aimeâ C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Almond J
- Alonso AG
- Alpana K
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amaral SMSD
- Amarilo KM
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- Kyriakis A
- Köseyan OK
- La Cruz IH-D
- Laflotte I
- Laha A
- Laktineh IB
- Lam T
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- Lamichhane K
- Lammel S
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- Lanaro A
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- Landsberg G
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- Le Bihan A-C
- Lechner L
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- Ledovskoy A
- Lee H
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- Leggat D
- Legger F
- Lehti S
- Leiton AGS
- Lelas D
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- Lemaitre V
- Lemos DS
- Lenzi B
- Lenzi P
- Leonardo N
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- Lesauvage A
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- Letts J
- Levchuk L
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- Ligabue F
- Liko D
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- Lizzo M
- Lo KH
- Lobanov A
- Locci E
- Loeliger A
- Lohmann W
- Lokhtin I
- Lomidze I
- Long K
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- Longo E
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- Lotfy A
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- Mcgrady C
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- Menendez JF
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- Meng F
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- Mikulec I
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- Negro G
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- Neutelings I
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- Nikitenko A
- Niknejad T
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- Norjoharuddeen NB
- Novaes SF
- Novak A
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- NĂŒrnberg A
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- Panagiotou A
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- Perraguin AB
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- Petkov P
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- Potenza R
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- Presilla M
- Prieels C
- Primavera F
- Prisciandaro J
- Priyanka P
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- Prosper H
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- Raspereza A
- Rastogi A
- Rath Y
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- Ravera F
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- Razis PA
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- Redjimi R
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- Regnery B
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- Reichmann M
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- Reimers A
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- Reissel C
- Reitenspiess T
- Reithler H
- Rembser J
- Revering M
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- Ricardo RES
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- Richman J
- Rieger M
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- Rinkevicius A
- Ristic B
- Ristori L
- Rivero CM
- Rizzi A
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- Robutti E
- Rodozov M
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- Rodriguez KJP
- RodrĂguez SC
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- Ryu MS
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- Safonov A
- Saggio A
- Sagir S
- Saha G
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- Sahasransu AR
- Sahin MĂ
- Sahu B
- Saibel A
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- Sakulin H
- Salerno R
- Salfeld-Nebgen J
- Saltzberg D
- Salur S
- Salvatico R
- Salvini P
- Salyer K
- Samalan A
- Sanchez A
- Sanchez MCDLB
- Sandeep K
- Sanders S
- Santanastasio F
- Santocchia A
- Santoro A
- Saoulidou N
- Saradhy R
- Sarica U
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- Schnetzer S
- Schroeder N
- Schröder M
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- Schönenberger M
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- Sciacca C
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- Sfar HR
- Sguazzoni G
- Shafiei N
- Shah A
- Shah MA
- Shalaev V
- Shang V
- Sharan M
- Sharma A
- Sharma A
- Sharma A
- Sharma R
- Sharma S
- Sharma V
- Sharma V
- Shchablo K
- Shchelina K
- Sheldon P
- Shepherd-Themistocleous CH
- Sheplock J
- Shi K
- Shi W
- Shi Z
- Shmatov S
- Shoaib M
- Shopova M
- Shtipliyski A
- Shukla P
- Shulha S
- Shvetsov I
- Si W
- Siado JE
- Siddireddy P
- Siikonen H
- Sikdar AK
- Sikler F
- Silva GC
- Silva P
- Silvestris L
- Simone FM
- Simonetto F
- Simonis HJ
- Simsek AE
- Singh A
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- Sirois Y
- Siroli GP
- Siviero F
- Skinnari L
- Skovpen K
- Skovpen Y
- Skuja A
- Slabospitskii S
- Smirnov I
- Smirnov V
- Smith C
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- Smith VJ
- Smith WH
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- Snoeys W
- Snow GR
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- Sobol A
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- Sola V
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- Sonnadara DUJ
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- Sorrentino G
- Sosnov D
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- Spiga D
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- Spiropulu M
- Spitzbart D
- Sreekala JM
- Srimanobhas N
- Stadie H
- Stafford D
- Stahl A
- Staiano A
- Stakia A
- Stampf V
- Starling E
- Starodumov A
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- SteinbrĂŒck G
- Stenson K
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- Teague D
- Tedeschi T
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- Terkulov A
- Teroerde M
- Terrill W
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- Tiras E
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- Tiwari PC
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- Tobar ĂN
- Tok UG
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- Tomalin IR
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- Toms M
- Tonelli G
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- Toropin A
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- Touquet G
- Townsend A
- Tramontano R
- Tran NV
- Tran TT
- Trapote A
- Treille D
- Trembath-Reichert S
- Trevisani N
- Tricomi A
- Trocino D
- Trocsanyi ZL
- Troshin S
- Tsamalaidze Z
- Tsatsos A
- Tsipolitis G
- Tsirou A
- Tully C
- Tumasyan A
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- Tuominen E
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- Turini N
- Turkcapar S
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- Ujvari B
- Ulmer KA
- Ulrich R
- Uniyal R
- Uplegger L
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
- Valencia FV
- Valsecchi D
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- Van Putte S
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- Vanden Bemden M
- Vander Donckt M
- Vander Velde C
- Vanlaer P
- Vannerom D
- Varela J
- Varelas N
- Vartak A
- Vats D
- Vazzoler F
- Veckalns V
- Veelken C
- Velasco M
- Velkovska J
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- Venditti R
- Venturi A
- Verbeke W
- Verdini PG
- Veres GI
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- Veszpremi V
- Vesztergombi G
- Vetens W
- Viazlo O
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- Viinikainen J
- Vila I
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- Virdee T
- Virdi AK
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- Vischia P
- Vit M
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- Vlasov E
- Vlimant JR
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- Volkov A
- Volkov S
- Volobouev I
- Von Cube RF
- Vormwald B
- Vorobyev A
- Vourliotis E
- Voutilainen M
- Voytishin N
- VĂĄmi TĂ
- Wadud MA
- Wagner SR
- Walczak M
- Wallny R
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- Waltenberger W
- Walter D
- Wamorkar T
- Wanczyk J
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- Wang S
- Wang X
- Wang Y
- Wang Z
- Wang Z
- Waqas M
- Wardle N
- Warner Z
- Wassmer M
- Watson IJ
- Wayne M
- Webb SN
- Weber HA
- Weber M
- Wei K
- Wen Y
- Wertz S
- West C
- Wezenbeek L
- Whitbeck A
- White R
- White S
- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
- Williams A
- Williams J
- Williams T
- Willmott C
- Wilson G
- Wilson J
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wolf M
- Wolf R
- Wolfe E
- Wong K
- Wong WY
- Wood D
- Wozniak KA
- Wozniewski S
- Wright D
- Wu HY
- Wu Z
- Wuchterl S
- Wulz C-E
- Wunsch S
- Wyslouch B
- WĂŒrthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yang S
- Yang S
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yetkin EA
- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang S
- Zhang W
- Zhang Y
- Zhang Y
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- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 26/04/2022
- Field of study
The leptonic and inclusive hadronic decay branching fractions of the W boson are measured using
proton-proton collision data collected at ffiffi s p Œ 13 TeV by the CMS experiment at the CERN LHC,
corresponding to an integrated luminosity of 35.9 fbâ1. Events characterized by the production of one or
two W bosons are selected and categorized based on the multiplicity and flavor of reconstructed leptons, the
number of jets, and the number of jets identified as originating from the hadronization of b quarks. A
binned maximum likelihood estimate of the W boson branching fractions is performed simultaneously in
each event category. The measured branching fractions of the W boson decaying into electron, muon, and
tau lepton final states are Ă°10.83 0.10Ă%, Ă°10.94 0.08Ă%, and Ă°10.77 0.21Ă%, respectively,
consistent with lepton flavor universality for the weak interaction. The average leptonic and inclusive
hadronic decay branching fractions are estimated to be Ă°10.89 0.08Ă% and Ă°67.32 0.23Ă%, respec tively. Based on the hadronic branching fraction, three standard model quantities are subsequently derived: the sum of squared elements in the first two rows of the CabibboâKobayashiâMaskawa (CKM) matrix
P ij jVijj 2 Œ 1.984 0.021, the CKM element jVcsj Œ 0.967 0.011, and the strong coupling constant at
the W boson mass scale, αSĂ°m2 WĂ ÂŒ 0.095 0.033
Recommended from our members
Search for light Higgs bosons from supersymmetric cascade decays in pp collisions at âs=13TeV
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abercrombie D
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- Zuolo D
- Zygala L
- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 06/07/2023
- Field of study
A search is reported for pairs of light Higgs
bosons (H1) produced in supersymmetric cascade decays in
f
inal states with small missing transverse momentum. A data
set of LHC pp collisions collected with the CMS detector
at âs = 13TeV and corresponding to an integrated lumi
nosity of 138fbâ1 is used. The search targets events where
both H1 bosons decay into bÂŻb pairs that are reconstructed
as large-radius jets using substructure techniques. No evi
dence is found for an excess of events beyond the back
ground expectations of the standard model (SM). Results
from the search are interpreted in the next-to-minimal super
symmetric extension of the SM, where a âsinglinoâ of small
mass leads to squark and gluino cascade decays that can pre
dominantly end in a highly Lorentz-boosted singlet-like H1
andasinglino-likeneutralinoofsmalltransversemomentum.
Upperlimitsaresetontheproductofthesquarkorgluinopair
production cross section and the square of the bÂŻb branching
fraction of the H1 in a benchmark model containing almost
mass-degenerategluinosandlight-flavoursquarks.Underthe
assumption of an SM-like H1 â bÂŻb branching fraction, H1
bosonswithmassesintherange40â120GeVarisingfromthe
decays of squarks or gluinos with a mass of 1200â2500GeV
are excluded at 95% confidence level.SCOA
Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Abreu A
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- Acosta D
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- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/11/2021
- Field of study
Copyright © CERN for the benefit of the CMS collaboration 2022. A search for new long-lived particles decaying to leptons using protonâproton collision data produced by the CERN LHC at sâ=13TeV is presented. Events are selected with two leptons (an electron and a muon, two electrons, or two muons) that both have transverse impact parameter values between 0.01 and 10cm and are not required to form a common vertex. Data used for the analysis were collected with the CMS detector in 2016, 2017, and 2018, and correspond to an integrated luminosity of 118 (113)fbâ1 in the ee channel (eÎŒ and ΌΌ channels). The search is designed to be sensitive to a wide range of models with displaced eÎŒ, ee, and ΌΌ final states. The results constrain several well-motivated models involving new long-lived particles that decay to displaced leptons. For some areas of the available phase space, these are the most stringent constraints to date.SCOAP3
Observation of triple J/Ï meson production in proton-proton collisions
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- AimĂš C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
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- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 19/01/2023
- Field of study
Data availability:
Tabulated results are provided in the HEPData record for this analysis71. Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in CMS data preservation, re-use and open access policy.Code availability:
The CMS core software is publically available at https://github.com/cms-sw/cmssw.Copyright . Protons consist of three valence quarks, two up-quarks and one down-quark, held together by gluons and a sea of quark-antiquark pairs. Collectively, quarks and gluons are referred to as partons. In a proton-proton collision, typically only one parton of each proton undergoes a hard scattering â referred to as single-parton scattering â leaving the remainder of each proton only slightly disturbed. Here, we report the study of double- and triple-parton scatterings through the simultaneous production of three J/Ï mesons, which consist of a charm quark-antiquark pair, in proton-proton collisions recorded with the CMS experiment at the Large Hadron Collider. We observed this process â reconstructed through the decays of J/Ï mesons into pairs of oppositely charged muons â with a statistical significance above five standard deviations. We measured the inclusive fiducial cross-section to be 272+141â104(stat)±17(syst)fb, and compared it to theoretical expectations for triple-J/Ï meson production in single-, double- and triple-parton scattering scenarios. Assuming factorization of multiple hard-scattering probabilities in terms of single-parton scattering cross-sections, double- and triple-parton scattering are the dominant contributions for the measured process.SCOAP3.Change history:
27 February 2023A Correction to this paper has been published: https://doi.org/10.1038/s41567-023-01992-
Recommended from our members
Measurement of the mass dependence of the transverse momentum of lepton pairs in DrellâYan production in protonâproton collisions at âs = 13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aimeâ C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Almond J
- Alonso AG
- Alpana K
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
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- Ăzçelik Ă
- Publication venue
- Springer Nature
- Publication date
- 17/07/2023
- Field of study
Data Availability Statement
This manuscript has no associated data or the data will not be deposited. [Authorsâ comment: Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032 &filename=CMSDataPolicyV1.2.pdf &version=2 CMS data preservation, re-use and open access policy.]A preprint version of the article is available at arXiv:2205.04897v2 [hep-ex], https://arxiv.org/abs/2205.04897v2. Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-20-003 (CMS Public Pages). Report number: CMS-SMP-20-003, CERN-EP-2022-053.The double differential cross sections of the DrellâYan lepton pair (â+â- , dielectron or dimuon) production are measured as functions of the invariant mass mââ , transverse momentum pT(ââ) , and Ïηâ . The Ïηâ observable, derived from angular measurements of the leptons and highly correlated with pT(ââ) , is used to probe the low- pT(ââ) region in a complementary way. Dilepton masses up to 1 TeV are investigated. Additionally, a measurement is performed requiring at least one jet in the final state. To benefit from partial cancellation of the systematic uncertainty, the ratios of the differential cross sections for various mââ ranges to those in the Z mass peak interval are presented. The collected data correspond to an integrated luminosity of 36.3 fb-1 of protonâproton collisions recorded with the CMS detector at the LHC at a centre-of-mass energy of 13 TeV . Measurements are compared with predictions based on perturbative quantum chromodynamics, including soft-gluon resummation.SCOAP3
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Measurement of the differential ttÂŻ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
- Author
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- Yumiceva F
- Yusuff I
- Yzquierdo AP-C
- Zabi A
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- Zaleski S
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- Zanetti M
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- Zecchinelli AG
- Zeid SA
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- Zoi I
- Zolkapli Z
- Zorbakir IS
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez CR
- Publication venue
- Springer Nature
- Publication date
- 03/07/2023
- Field of study
Data Availability:
This manuscript has no associated data or the data will not be deposited. [Authorsâ comment: Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in https://cms-docdb.cern.ch/cgibin/PublicDocDB/RetrieveFile?docid=6032 &filename=CMSDataPolicyV1.2.pdf &version=2.]A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production (ttÂŻ
) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400GeV
. The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138fbâ1
. The differential ttÂŻ
production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of 173.06±0.84GeV.SCOAP
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- Author
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- Abbaneo D
- Abbiendi G
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- Springer Nature
- Publication date
- 10/07/2023
- Field of study
A preprint version of the article is available at arXiv (https://arxiv.org/abs/2205.02905).Copyright © CERN for the benefit of the CMS collaboration 2023. New sets of parameter tunes for two of the colour reconnection models, quantum chromodynamics-inspired and gluon-move, implemented in the PYTHIA 8 event generator, are obtained based on the default CMS PYTHIA 8 underlying-event tune, CP5. Measurements sensitive to the underlying event performed by the CMS experiment at centre-of-mass energies sâ=7 and 13TeV , and by the CDF experiment at 1.96TeV
are used to constrain the parameters of colour reconnection models and multiple-parton interactions simultaneously. The new colour reconnection tunes are compared with various measurements at 1.96, 7, 8, and 13TeV including measurements of the underlying-event, strange-particle multiplicities, jet substructure observables, jet shapes, and colour flow in top quark pair (ttÂŻ) events. The new tunes are also used to estimate the uncertainty related to colour reconnection modelling in the top quark mass measurement using the decay products of ttÂŻ events in the semileptonic channel at 13TeV.SCOAP3
Recommended from our members
Measurements of Higgs boson production in the decay channel with a pair of Ï leptons in proton-proton collisions at sâ = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
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- Adams MR
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- Addesa FM
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- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
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- Aguilar-Benitez M
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- Ahmad WH
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- Akgun B
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- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 19/10/2022
- Field of study
A preprint version of the article is available at arXiv:2204.12957v2 [hep-ex], https://arxiv.org/abs/2204.12957v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures and tables, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-19-010 (CMS Public Pages). Report number: CMS-HIG-19-010, CERN-EP-2022-027.Measurements of Higgs boson production, where the Higgs boson decays into a pair of Ï leptons, are presented, using a sample of proton-proton collisions collected with the CMS experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{â1}. Three analyses are presented. Two are targeting Higgs boson production via gluon fusion and vector boson fusion: a neural network based analysis and an analysis based on an event categorization optimized on the ratio of signal over background events. These are complemented by an analysis targeting vector boson associated Higgs boson production. Results are presented in the form of signal strengths relative to the standard model predictions and products of cross sections and branching fraction to Ï leptons, in up to 16 different kinematic regions. For the simultaneous measurements of the neural network based analysis and the analysis targeting vector boson associated Higgs boson production signal strengths are found to be 0.82 ± 0.11 for inclusive Higgs boson production, 0.67 ± 0.19 (0.81 ± 0.17) for the production mainly via gluon fusion (vector boson fusion), and 1.79 ± 0.45 for vector boson associated Higgs boson production.SCOAP3
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Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at sâ = 13 TeV
- Author
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- Ăzçelik Ă
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 09/10/2022
- Field of study
A preprint version of the article is available at arXiv:2206.09466v2 [hep-ex], https://arxiv.org/abs/2206.09466v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at httpS://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-20-013 (CMS Public Pages). Report number: CMS-HIG-20-013, CERN-EP-2022-120.Production cross sections of the standard model Higgs boson decaying to a pair of W bosons are measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analysis targets Higgs bosons produced via gluon fusion, vector boson fusion, and in association with a W or Z boson. Candidate events are required to have at least two charged leptons and moderate missing transverse momentum, targeting events with at least one leptonically decaying W boson originating from the Higgs boson. Results are presented in the form of inclusive and differential cross sections in the simplified template cross section framework, as well as couplings of the Higgs boson to vector bosons and fermions. The data set collected by the CMS detector during 2016-2018 is used, corresponding to an integrated luminosity of 138 fb^â1. The signal strength modifier ÎŒ, defined as the ratio of the observed production rate in a given decay channel to the standard model expectation, is measured to be ÎŒ = 0.95 +0.10â0.09. All results are found to be compatible with the standard model within the uncertainties.SCOAP3