176 research outputs found
ATLAS detector and physics performance: Technical Design Report, 1
- Author
- Abdinov O.B.
- Abolins M.
- Abramowicz H.
- Acerbi E.
- Ackermann K.
- Ackers M.
- Aderholz M.
- Ahlen S.
- Aielli G.
- Airapetian A.
- Akerman D.
- Akesson T.
- Akhmedov A.
- Akhoundov A.
- Akimov A.
- Alam S.
- Aleksa M.
- Aleppo M.
- Alessandria F.
- Alexa C.
- Alexander G.
- Alexandrov I.
- Alexeev G.
- Alforque S.
- Alikov B.
- Allport P.P.
- Almehed S.
- Aloisio A.
- Alviggi M.G.
- Amadon A.
- Amako K.
- Amaral P.
- Ambrosini G.
- Amelin D.V.
- Ammosov V.V.
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- Wunsch M.
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- Wyllie K.H.
- Xie Y.G.
- Xu G.F.
- Xue L.
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- Yamartino J.M.
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- Zitek K.
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- Zmouchhko V.
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- Fasssouliotis D.
- Publication venue
- Union of Concerned Scientists
- Publication date
- 01/01/1999
- 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
- A. and Sanders
- A. and Sawyer
- A. and Severini
- A. and Skubic
- A. and Suslov
- Aaltonen
- And Manousakis-Katsikakis
- B. A. and Barria
- B. C. K. and Castilla-Valdez
- B. L. and Wittich
- B. S. and Adams
- B. and Acharya
- B. and Augsten
- B. and Bandurin
- B. and Bocci
- B. and Carlsmith
- B. and Casarsa
- B. and Cihangir
- B. and Diehl
- B. and Evans
- B. and Hogan
- B. and Jeon
- B. and Kim
- B. and Perfilov
- B. and Ratoff
- B. and Tully
- B. and Zhou
- C. A. and Cox
- C. E. and Gerberich
- C. L. and McNulty
- C. M. and Ginther
- C. P. and Butti
- C. P. and Yi
- C. R. and Snow
- C. S. and Moore
- C. and Azfar
- C. and Bross
- C. and Clutter
- C. and DeVaughan
- C. and Garbincius
- C. and Gruenendahl
- C. and Hays
- C. and Heredia-De La Cruz
- C. and Meyer
- C. and Pal
- C. and Penning
- C. and Pleier
- C. and Rubinov
- C. and Saveliev
- C. and Schwarz
- C. and Ukegawa
- C. and Verkheev
- C. and Vertogradov
- C. and Wang
- C. and Zhu
- D. A. and Strauss
- D. H. and Kim
- D. J. and Cremonesi
- D. J. and Konigsberg
- D. R. and Wright
- D. V. and Banerjee
- D. and Anastassov
- D. and Beretvas
- D. and Boos
- D. and Borysova
- D. and Brucken
- D. and Carosi
- D. and Cavaliere
- D. and Choudhary
- D. and Clark
- D. and Cuevas
- D. and Das
- D. and Denisov
- D. and Elagin
- D. and Gogota
- D. and Golossanov
- D. and Hegab
- D. and Jayasinghe
- D. and Kasmi
- D. and Li
- D. and Linnemann
- D. and Luca
- D. and Mercadante
- D. and Mitra
- D. and Prokopenko
- D. and Stoyanova
- D. and Tokar
- D. and Torre
- D. and Totaro
- D. and Tuchming
- D. and Vilar
- D. and Watts
- D. and Wicklund
- D. and Yang
- D. and Zivkovic
- E. E. and Borisov
- E. E. and Johnson
- E. E. and Schott
- E. J. and Jeong
- E. W. and Vasilyev
- E. and Baringer
- E. and Bu
- E. and Camarda
- E. and Chen
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- V. and Titov
- W. -M. and Yasuda
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- Z. and Hopkins
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- 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
Observation of charge-ordering in particle production in hadronic Z(0) decay
- Publication venue
- Publication date
- 01/01/1997
- Field of study
Analysis of the rapidity structure of charge correlations in hadronic
events from Z(0) decays gives evidence for chain-like charge-ordering of
particle production along the thrust axis, as predicted by
‘QCD-motivated’ string-like fragmentation models. (C) 1997 Published by
Elsevier Science B.V
Search for neutral Higgs bosons in e(+)e(-) collisions at root s=183 GeV
- Publication venue
- Publication date
- 01/01/1999
- Field of study
Neutral Higgs bosons were searched for in the data collected by DELPHI
at a centre-of-mass energy of 183 GeV, corresponding to an integrated
luminosity of 54 pb(-1). The production of the lightest neutral Higgs
boson with either an on-shell Z boson or a neutral pseudo-scalar Higgs
boson was analysed. Lower limits at the 95% confidence level were
obtained on the Higgs boson masses. The limits are 85.7 GeV/c(2) for the
Standard Model Higgs boson and 74.4 GeV/c(2) for the scalar and 75.3
GeV/c(2) for the pseudo-scalar Higgs bosons as predicted by the minimal
super-symmetric extension of the Standard Model with commonly used
assumptions on the model parameters, plus the assumption that the mass
of the pseudo-scalar boson is greater than 20 GeV/c(2). These results
significantly improve the limits reached with previous data
Search for charginos, neutralinos and gravitinos in e(+)e(-) interactions at root s = 183 GeV
- Publication venue
- Publication date
- 01/01/1999
- Field of study
An update of the searches for charginos and neutralinos is presented,
based on a data sample corresponding to the 53.9 pb(-1) recorded by the
DELPHI detector in 1997, at a centre-of-mass energy of 183 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 172 GeV. The
(mu M-2) domain excluded by combining the neutralino and chargino
searches implies a limit on the mass of the Lightest neutralino which,
for a heavy sneutrino, is constrained to be above 29.1 GeV/c(2) for tan
beta greater than or equal to 1. (C) 1999 Elsevier Science B.V. All
rights reserved
Energy dependence of inclusive spectra in e(+)e(-) annihilation
- Publication venue
- Publication date
- 01/01/1999
- Field of study
Inclusive charged hadron distributions as obtained from the DELPHI
measurements at 130, 136, 161, 172 and 183 GeV are presented as a
function of the variables rapidity, xi(p), p and transversal momenta.
Data are compared with event generators and with MLLA calculations, in
order to examine the hypothesis of local parton hadron duality. The
differential momentum spectra show an indication for coherence effects
in the production of soft particles. The relation between the energy
dependence of the charged multiplicity and the rapidity distribution is
examined. (C) 1999 Elsevier Science B.V. All rights reserved
Measurement of the spin density matrix for the rho(0), K*(0)(892) and phi produced in Z(0) decays
- Publication venue
- Publication date
- 01/01/1997
- Field of study
The spin density matrix elements for the rho(0), K-*0(892) and phi
produced in hadronic Z(0) decays are measured in the DELPHI detector.
There is no evidence for spin alignment of the K-*0(892) and phi, in
the region x(p) less than or equal to 0.3 (x(p) = p/p(beam)), where
rho(00) = 0.33 +/- 0.05 and rho(00) = 0.30 +/- 0.04, respectively. In
the fragmentation region, x(p) greater than or equal to 0.4, there is
some indication for spin alignment of the rho(0) and K-*0(892), since
rho(00) = 0.43 +/- 0.05 and rho(00) = 0.46 +/- 0.08, respectively. These
values are compared with those found in meson-induced hadronic
reactions. For the phi, rho(00) = 0.30 +/- 0.04 for x(p) greater than or
equal to 0.4 and 0.55 +/- 0.10 for x(p) greater than or equal to 0.7.
The off-diagonal spin density matrix element rho(1-1) is consistent with
zero in all cases. (C) 1997 Published by Elsevier Science B.V
A search for eta `(c) production in photon-photon fusion at LEP
- Publication venue
- Publication date
- 01/01/1998
- Field of study
A search for the production of the eta(c)’ meson, the first radial
excitation of the ground state of charmonium eta(c)(2980), in the
photon-photon fusion reaction at LEP has been performed using the data
collected by the DELPHI detector during 1992-1996. No evidence of
eta(c)’ production is found in the mass region 3520-3800 MeV/c(2). An
upper limit for the ratio of the two-photon widths of the eta(c)’ and
eta(c) is obtained. (C) 1998 Published by Elsevier Science B.V. All
rights reserved
Search for lightest neutralino and stau pair production in light gravitino scenarios with stau NLSP
- Publication venue
- Publication date
- 01/01/1999
- Field of study
Promptly decaying lightest neutralinos and long-lived staus are searched
for in the context of light gravitino scenarios. It is assumed that the
stau is the next to lightest supersymmetric particle (NLSP) and that the
lightest neutralino is the next to NLSP (NNLSP). Data collected with the
Delphi detector at centre-of-mass energies from 161 to 183 GeV are
analysed. No evidence of the production of these particles is found.
Hence, lower mass limits for both kinds of particles are set at 95%
C.L.. The mass of gaugino-like neutralinos is found to be greater than
71.5 GeV/c(2). In the search for long-lived stau: masses less than 70.0
to 77.5 GeV/c(2) are excluded for gravitino masses from 10 to 150
eV/c(2). Combining this search with the searches for stable heavy
leptons and minimal supersymmetric standard model staus a lower limit of
68.5 GeV/c(2) may be set for the stau mass independent of the mass of
the gravitino
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
- …