67 research outputs found
Erratum to: Combined analysis of Belle and Belle II data to determine the CKM angle ϕ3 using B+ → D(K0Sh+h−)h+ decays
- Author
- Abudinén F.
- Aggarwal L.
- Ahmed H.
- Aihara H.
- Akopov N.
- Al Said S.
- Aloisio A.
- Anh Ky N.
- Asner D. M.
- Atmacan H.
- Aushev V.
- Ayad R.
- Babu V.
- Bacher S.
- Baehr S.
- Bahinipati S.
- Bambade P.
- Banerjee Sw
- Bansal S.
- Baudot J.
- Becker J.
- Behera P. K.
- BELLE and Belle II collaborations
- Belous K.
- Bennett J. V.
- Bernlochner F. U.
- Bertemes M.
- Bertholet E.
- Bessner M.
- Bettarini S.
- Bianchi F.
- Bilka T.
- Biswas D.
- Bobrov A.
- Bodrov D.
- Bonvicini G.
- Borah J.
- Bozek A.
- Branchini P.
- Bračko M.
- Briere R. A.
- Browder T. E.
- Budano A.
- Bussino S.
- Campajola M.
- Cao L.
- Casarosa G.
- Cecchi C.
- Cheema P.
- Chekelian V.
- Chen A.
- Cheon B. G.
- Chilikin K.
- Chirapatpimol K.
- Cho H-E.
- Cho S-J.
- Choi S-K.
- Choi Y.
- Choudhury S.
- Cinabro D.
- Corona L.
- Cunliffe S.
- Czank T.
- Das S.
- Dattola F.
- De La Cruz-Burelo E.
- de Marino G.
- De Nardo G.
- De Nuccio M.
- De Pietro G.
- de Sangro R.
- De Yta-Hernandez A.
- Destefanis M.
- Dey S.
- Dhamija R.
- Di Canto A.
- Doležal Z.
- Domínguez Jiménez I.
- Dong T. V.
- Dorigo M.
- Dossett D.
- Dubey S.
- Dujany G.
- Eliachevitch M.
- Epifanov D.
- Feichtinger P.
- Ferlewicz D.
- Fillinger T.
- Fiore S.
- Fodor A.
- Forti F.
- Fulsom B. G.
- Gabrielli A.
- Ganiev E.
- Garcia-Hernandez M.
- Gaur V.
- Gaz A.
- Gioi L. Li
- Giordano R.
- Giri A.
- Glazov A.
- Godang R.
- Goldenzweig P.
- Golob B.
- Gradl W.
- Graziani E.
- Greenwald D.
- Gu T.
- Guan Y.
- Gudkova K.
- Guilliams J.
- Hadjivasiliou C.
- Halder S.
- Hara T.
- Hartbrich O.
- Hayasaka K.
- Hayashii H.
- Hazra S.
- Heredia de la Cruz I.
- Hershenhorn A.
- Higuchi T.
- Hill E. C.
- Hou W-S.
- Hsu C-L.
- Iijima T.
- Inami K.
- Ishikawa A.
- Iwasaki M.
- Jacobs W. W.
- Jang E-J.
- Jin Y.
- Junkerkalefeld H.
- Kaliyar A. B.
- Kang K. H.
- Karl R.
- Karyan G.
- Kato Y.
- Ketter C.
- Kiesling C.
- Kim C-H.
- Kim D. Y.
- Kim K-H.
- Kim Y-K.
- Kinoshita K.
- Kodyš P.
- Koga T.
- Kohani S.
- Korpar S.
- Kovalenko E.
- Kraetzschmar T. M. G.
- Križan P.
- Krokovny P.
- Kuhr T.
- Kumar J.
- Kumar M.
- Kumar R.
- Kumara K.
- Kuzmin A.
- Kwon Y-J.
- La Licata C.
- Lacaprara S.
- Lai Y-T.
- Lanceri L.
- Lange J. S.
- Leboucher R.
- Lee S. C.
- Leitl P.
- Li J.
- Li S. X.
- Libby J.
- Lieret K.
- Liptak Z.
- Liu Q. Y.
- Liventsev D.
- Longo S.
- Lueck T.
- Lyu C.
- Maggiora M.
- Maiti R.
- Maity S.
- Manfredi R.
- Manoni E.
- Marcello S.
- Martini A.
- Massaccesi L.
- Masuda M.
- Matsuoka K.
- Matvienko D.
- Maurya S. K.
- McKenna J. A.
- Meier F.
- Merola M.
- Metzner F.
- Milesi M.
- Miller C.
- Miyabayashi K.
- Mizuk R.
- Mohanty G. B.
- Molina-Gonzalez N.
- Moser H-G.
- Mueller F.
- Murphy C.
- Mussa R.
- Nakamura K. R.
- Nakano T.
- Nakao M.
- Naruki M.
- Narwal D.
- Natochii A.
- Nayak L.
- Nayak M.
- Nazaryan G.
- Nisar N. K.
- Nishida S.
- Nishimura K.
- Onishchuk Y.
- Ono H.
- Oskin P.
- Pakhlova G.
- Paladino A.
- Panta A.
- Paoloni E.
- Parham K.
- Park S-H.
- Passeri A.
- Pathak A.
- Patra S.
- Pestotnik R.
- Piilonen L. E.
- Podobnik T.
- Pokharel S.
- Polat L.
- Praz C.
- Prell S.
- Prencipe E.
- Prim M. T.
- Purwar H.
- Rabusov A.
- Rados P.
- Raiz S.
- Reiter S.
- Remnev M.
- Ripp-Baudot I.
- Rizzo G.
- Rizzuto L. B.
- Robertson S. H.
- Roney J. M.
- Rostomyan A.
- Rout N.
- Röhrken M.
- Sahoo D.
- Sanders D. A.
- Sandilya S.
- Santelj L.
- Sato Y.
- Savinov V.
- Scavino B.
- Schnell G.
- Schueler J.
- Schwartz A. J.
- Seino Y.
- Selce A.
- Senyo K.
- Sevior M. E.
- Shapkin M.
- Sharma C.
- Shillington T.
- Shwartz B.
- Sibidanov A.
- Simon F.
- Singh J. B.
- Soffer A.
- Solovieva E.
- Spataro S.
- Spruck B.
- Stefkova S.
- Stottler Z. S.
- Stroili R.
- Sumisawa K.
- Sutcliffe W.
- Suzuki S. Y.
- Tabata M.
- Takizawa M.
- Tanida K.
- Tenchini F.
- Tiwary R.
- Tonelli D.
- Torassa E.
- Trabelsi K.
- Uchida M.
- Ueda I.
- Uglov T.
- Uno K.
- Uno S.
- Ushiroda Y.
- Vahsen S. E.
- van Tonder R.
- Varvell K. E.
- Vinokurova A.
- Vitale L.
- Wakeling H. M.
- Wang E.
- Wang M-Z.
- Wang X. L.
- Warburton A.
- Watanuki S.
- Werbycka O.
- Wessel C.
- Won E.
- Yabsley B. D.
- Yan W.
- Ye H.
- Yoshihara K.
- Yusa Y.
- Zani L.
- Zhai Y.
- Zhang Y.
- Zhilich V.
- Zhou Q. D.
- Zhou X. Y.
- Zhukova V. I.
- Červenkov D.
- Publication venue
- Scuola Internazionale Superiore di Studi Avanzati
- Publication date
- 25/09/2023
- Field of study
Tevatron Run II combination of the effective leptonic electroweak mixing angle
- Author
- A. A. and Jones
- A. A. and Shears
- A. B. and Wilbur
- A. F. and Garosi
- A. K. A. and Madar
- A. L. and Lys
- A. M. and Zeng
- A. P. and Heintz
- A. S. and Ivanov
- A. S. and Sato
- A. T. and Goulianos
- A. T. and Lammel
- A. V. and Kozelov
- A. V. and Kraus
- A. V. and Poprocki
- A. W. and Junk
- A. Y. and Vernieri
- A. and Amerio
- A. and Annovi
- A. and Antos
- A. and Asaadi
- A. and Atkins
- A. and Aushev
- A. and Barberis
- A. and Bedeschi
- A. and Beri
- A. and Bland
- A. and Bodek
- A. and Boehnlein
- A. and Boline
- A. and Brandt
- A. and Brandt
- A. and Brown
- A. and Calamba
- A. and Camacho-Perez
- A. and Catastini
- A. and Cerrito
- A. and Chapon
- A. and Clarke
- A. and d'Ascenzo
- A. and Di Ruzza
- A. and Donati
- A. and Drutskoy
- A. and Dubey
- A. and Dudko
- A. and Dutt
- A. and Ellison
- A. and Evdokimov
- A. and Feng
- A. and Garcia-Gonzalez
- A. and Golovanov
- A. and Grosso-Pilcher
- A. and Harr
- A. and Hoeneisen
- A. and Jabeen
- A. and Jayatilaka
- A. and Kajfasz
- A. and Kato
- A. and Kharchilava
- A. and Kharzheev
- A. and Kupco
- A. and Kurata
- A. and Lincoln
- A. and Liu
- A. and Lockwitz
- A. and Lokajicek
- A. and Lueck
- A. and Mansour
- A. and Mazzanti
- A. and Mehtala
- A. and Menezes
- A. and Meyer
- A. and Miyake
- A. and Mulhearn
- A. and Narain
- A. and Palencia
- A. and Pauletta
- A. and Prewitt
- A. and Quinn
- A. and Rodriguez
- A. and Royon
- A. and Russ
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- A. and Sawyer
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- A. and Suslov
- Aaltonen
- And Manousakis-Katsikakis
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- B. C. K. and Castilla-Valdez
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- D. A. and Strauss
- D. H. and Kim
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- S. and Barbaro-Galtieri
- S. and Bellantoni
- S. and Bhatnagar
- S. and Bloom
- S. and Burkett
- S. and Campanelli
- S. and Casal
- S. and Cauz
- S. and CDF Collaboration and D0 Collaboration
- S. and Chan
- S. and Chokheli
- S. and Claes
- S. and D'Onofrio
- S. and Deterre
- S. and Eads
- S. and Esham
- S. and Faure
- S. and Funakoshi
- S. and Giakoumopoulou
- S. and Greenlee
- S. and Gruenewald
- S. and Howley
- S. and Jaffre
- S. and Johns
- S. and Ketchum
- S. and Lammers
- S. and Lancaster
- S. and Leone
- S. and Lewis
- S. and Loginov
- S. and Malik
- S. and Malyshev
- S. and Moggi
- S. and Rominsky
- S. and Seiya
- S. and Shchukin
- S. and Soldner-Rembold
- S. and Song
- S. and Tokmenin
- S. and Torretta
- S. and Uvarov
- S. and Uzunyan
- S. and Van Kooten
- S. and Williams
- S. and Wolfmeister
- S. and Yang
- T. G. and Zhou
- T. J. and Piacentino
- T. R. and Juste
- T. R. and Xiang
- T. and Abazov
- T. and Agnew
- T. and Artikov
- T. and Bagby
- T. and da Costa
- T. and Hatakeyama
- T. and Hebbeker
- T. and Hedin
- T. and Hobbs
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- T. and Kumar
- T. and Kuzmin
- T. and Liu
- T. and Miconi
- T. and Nodulman
- T. and Oakes
- T. and Orava
- T. and Ramos
- T. and Rolli
- T. and Schamberger
- T. and Schwienhorst
- T. and Shepard
- T. and Tonelli
- T. and Wu
- T. and Yang
- T. and Yatsunenko
- T. and Youn
- Th. and Murat
- U. K. and Yang
- U. and Bauce
- U. and Hensel
- U. and Hussein
- V. A. and Laasanen
- V. D. and Enari
- V. E. and Barnett
- V. L. And
- V. M. and Abbott
- V. M. and Pondrom
- V. N. and Farrington
- V. V. and Lipeles
- V. V. and Sajot
- V. V. and Tollefson
- V. and Aushev
- V. and Bean
- V. and Bhatti
- V. and Bunichev
- V. and Burdin
- V. and Cerri
- V. and Geng
- V. and Gibson
- V. and Glenzinski
- V. and Iashvili
- V. and Parashar
- V. and Park
- V. and Savitskyi
- V. and Shaw
- V. and Simonenko
- V. and Soustruznik
- V. and Titov
- W. -M. and Yasuda
- W. C. and Whiteson
- W. E. and Corbo
- W. K. and Sakurai
- W. M. and Lei
- W. M. and Varelas
- W. and Askew
- W. and Bae
- W. and Fisk
- W. and Gerber
- W. and Hou
- W. and Keung
- W. and Partridge
- W. and Ye
- X. B. and Budagov
- X. and Lellouch
- X. and Wu
- Y. -T. and Tsybychev
- Y. A. and Ye
- Y. C. and Chertok
- Y. C. and Yao
- Y. D. and Okusawa
- Y. J. and Kim
- Y. K. and Kimura
- Y. N. and Kilminster
- Y. Y. and Galloni
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- Y. and Erbacher
- Y. and Giagu
- Y. and Illingworth
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- Y. and Lobodenko
- Y. and Naganoma
- Y. and Petridis
- Y. and Sanchez-Hernandez
- Y. and Schellman
- Y. and Sekaric
- Y. and Sukhanov
- Y. and Tang
- Y. and Xie
- Y. and Yamada
- Y. and Zennamo
- Z. and Hopkins
- Z. and Hughes
- Z. and Wyatt
- Z. and Yeh
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Drell-Yan lepton pairs produced in the process pp→â.,"+â.,"-+X through an intermediate γ∗/Z boson have an asymmetry in their angular distribution related to the spontaneous symmetry breaking of the electroweak force and the associated mixing of its neutral gauge bosons. The CDF and D0 experiments have measured the effective-leptonic electroweak mixing parameter sin2θefflept using electron and muon pairs selected from the full Tevatron proton-antiproton data sets collected in 2001-2011, corresponding to 9-10 fb-1 of integrated luminosity. The combination of these measurements yields the most precise result from hadron colliders, sin2θefflept=0.23148±0.00033. This result is consistent with, and approaches in precision, the best measurements from electron-positron colliders. The standard model inference of the on-shell electroweak mixing parameter sin2θW, or equivalently the W-boson mass MW, using the zfitter software package yields sin2θW=0.22324±0.00033 or equivalently, MW=80.367±0.017 GeV/c2
INCLUSIVE MEASUREMENTS OF THE K+/- AND P/(P)OVER-BAR PRODUCTION IN HADRONIC Z(0) DECAYS
- Publication venue
- Publication date
- 01/01/1995
- Field of study
This analysis, based on a sample of 170000 hadronic Z(0) decays,
provides a measurement of the K-+/- and p/()overbarpdifferentialcrosssectionswhichiscomparedtostring−andclusterfragmentationmodels.ThetotalmultiplicitiesforK−+/−andpipperhadroniceventwerefoundtobe:N−K=2.26+/−0.18andN−p=1.07+/−0.14.Thepositionsxi∗ofthemaximaofthedifferentialcrosssectionsasafunctionofxi=In(1/x(p))forK−+/−andp/() over bar p were
determined to be 2.63 +/- 0.07 and 2.96 +/- 0.16 respectively. A
comparison of the xi* values for various identified particles measured
at LEP with the prediction of the Modified Leading Logarithm
Approximation with Local Parton Hadron Duality model has been performed.
The measured xi* position as a function of the hadron mass, after
corrections due to particle decays, is in agreement with the model
calculation
Lambda(b) polarization in Z(0) decays at LEP
- Publication venue
- Publication date
- 01/01/2000
- Field of study
The longitudinal polarization of the Lambda(b) baryon is measured at the
LEP e(+)e(-) collider by DELPHI. It is determined from the charged
lepton and neutrino energy spectra in 249 +/- 19 Lambda(b) semileptonic
decays reconstructed in approximate to 3.5 million hadronic Z(0) decays
using Lambda(0)-lepton correlations. The measured polarization is:
P-Lambda b = -0.49(-0.30)(+0.32)(stat.) +/- 0.17(syst.). (C) Elsevier
Science B.V. All rights reserved
OBSERVATION OF SHORT-RANGE 3-PARTICLE CORRELATIONS IN E(+)E(-) ANNIHILATIONS AT LEP ENERGIES
- Publication venue
- Publication date
- 01/01/1995
- Field of study
Measurements are presented of short range three-particle correlations in
e(+)e(-) annihilations at LEP using data collected by the DELPHI
detector. At small values of the four-momentum difference, strong
three-particle correlations are observed for like-sign (+++ and —) and
for unlike-sign (++- and +–) pion combinations which are not a
consequence of two-particle correlations. A possible explanation of the
observed effects in like-sign combinations is the existence of higher
order Bose-Einstein interference, which significantly changes the
particle distributions in jets
Search for charginos in e(+)e(-) interactions at root s=189 GeV
- Publication venue
- Publication date
- 01/01/2000
- Field of study
An update of the searches for charginos and gravitinos is presented,
based on a data sample corresponding to the 158 pb(-1) recorded by the
DELPHI detector in 1998, at a centre-of-mass energy of 189 GeV. No
evidence for a signal was found. The lower mass limits are 4-5 GeV/c(2)
higher than those obtained at a centre-of-mass energy of 183 GeV. The
(mu, M-2) MSSM domain excluded by combining the chargino searches with
neutralino searches at the Z resonance implies a limit on the mass of
the lightest neutralino which, for a heavy sneutrino, is constrained to
be above 31.0 GeV/c(2) for tan beta greater than or equal to 1. (C) 2000
Elsevier Science B.V. All rights reserved
Rapidity-rank structure of p(p)over-bar pairs in hadronic Z(0) decays
- Publication venue
- Publication date
- 01/01/2000
- Field of study
The rapidity-rank structure of pa pairs is used to analyze the mechanism
of baryon production in hadronic Z(0) decay. The relative occurrence of
the rapidity-ordered configuration p M p, where M is a meson, and that
of pp adjacent pairs is compared. The data are found to be consistent
with predictions from a mechanism producing adjacent-rank pp pairs,
without requiring ‘string-ordered’ p M p configurations. An upper limit
of 15% at 90% confidence is determined for the p M p contribution. (C)
2000 Elsevier Science B.V. All rights reserved
Hadronization properties of b quarks compared to light quarks in e(+)e(-)-> q(q)over-bar from 183 to 200 GeV
- Publication venue
- Publication date
- 01/01/2000
- Field of study
The DELPHI detector at LEP has collected 54 pb(-1) of data at a
centre-of-mass energy around 183 GeV during 1997, 158 pb(-1) around 189
GeV during 1998, and 187 pb(-1) between 192 and 200 GeV during 1999.
These data were used to measure the average charged particle
multiplicity in e(+)e(-)->b (b) over bar events: (n)(b (b) over bar),
and the difference delta(hl) between (n)(b (b) over bar) and the
multiplicity, (n)(l (l) over bar), in generic light quark (u,d,s)
events:
delta(hl)(183 GeV) = 4.55 +/- 1.31(stat) +/- 0.73(syst),
delta(hl)(189 GeV) = 4.43 +/- 0.85(stat) +/- 0.61(syst),
delta(hl)(200 GeV) = 3.39 +/- 0.89(stat) +/- 1.01 (syst).
This result is consistent with QCD predictions, while it is inconsistent
with calculations assuming that the multiplicity accompanying the decay
of a heavy quark is independent of the: mass of the quark itself. (C)
2000 Elsevier Science B.V. All rights reserved
Measurement of the (B)over-bar -> D-(*)pi l(nu)over-bar(l) branching fraction
- Publication venue
- Publication date
- 01/01/2000
- Field of study
A study of b semileptonic decays into D, D pi(+/-) and D*pi(+/-) final
states is presented. The D-0, D+ and D*(+) mesons are exclusively
reconstructed in Z decay data recorded from 1992 to 1995 in the DELPHI
experiment at LEP. The overall branching fractions are measured to be:
BR(b –> D(0)l(-)<(upsilon)over bar>X-l) = (7.04 +/- 0.34(stat) +/- 0.36
(syst.exp) +/- 0.17(BRD))%,
BR(b –> D(+)l(-)<(upsilon)over bar>X-l) = (2.72 +/- 0.19(stat) +/-
0.16(syst.exp) +/- 0.18(BRD))%,
BR(b –> D*(+)l(-)<(upsilon)over bar>X-l) = (2.75 +/- 0.17(stat) +/-
0.13 (syst.exp) +/- 0.09 (BRD))%,
where the D-0 and D+ results include also contributions from D*(0) and
D*(+) decays. A fit to the distribution of the pi(+/-) impact
parameter to the primary interaction vertex provides a measurement of
the b semileptonic branching fractions into the D(0)pi(+/-)X,
D(+)pi(+/-)X and D*(+)pi(+/-)X final states. Assuming that single pion
decay modes of B mesons dominate, the partial rates for (B) over bar –>
D pi l(-)<(upsilon)over bar>(l) and (B) over bar –> D*pi
l(-)<(upsilon)over bar>(l) have been obtained, corresponding to a total
branching fraction:
BR((B) over bar –> D pi l(-)<(upsilon)over bar>(l)) + BR((B) over bar
–> D*pi l(-)<(upsilon)over bar>(l)) = (3.40 +/- 0.52 (stat) +/- 0.32
(syst))%.
This result agrees well with the observed difference between the total B
semileptonic branching fraction and the sum of the (B) over bar –>
Dl(-) upsilon(l) and D* l(-)<(upsilon)over bar>(l) branching
fractions. (C) 2000 Elsevier Science B.V. All rights reserved
A precise measurement of the tau lepton lifetime
- Publication venue
- Publication date
- 01/01/1996
- Field of study
The tau lepton lifetime has been measured using three different methods
with the DELPHI detector. Two measurements of one-prong decays are
combined, accounting for correlations, giving a result of tau(tau) =
291.8 +/- 3.3 (stat.) +/- 2.0(sys.) fs while the decay length
distribution of three-prong decays gives the result tau(tau) = 286.7 +/-
4.9 (stat.) +/- 3.3 (sys.) fs. Combining the results presented here with
previous DELPHI measurements, we get tau(tau) = 291.4 +/- 3.0 fs and
find that the ratio of the coupling constant for tau decay relative to
that for muon decay is 0.990 +/- 0.009, compatible with lepton
universality
- …