P. Auchincloss
University of Rochester
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Featured researches published by P. Auchincloss.
Physical Review Letters | 1993
F. Abe; M. Albrow; D. Amidei; C. Anway-Wiese; G. Apollinari; M. Atac; P. Auchincloss; P. Azzi; N. Bacchetta; A. Baden; W. Badgett; M. W. Bailey; A. Bamberger; de Barbaro P; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; G. Bauer; T. Baumann; F. Bedeschi; S. Behrends; S. Belforte; G. Bellettini; J. Bellinger; D. Benjamin; J. Benlloch; J. Bensinger; A. Beretvas; J. P. Berge; S. Bertolucci
We present a measurement of the [ital b]-quark cross section in 1.8 TeV [ital p]-[ital [bar p]] collisions recorded with the Collider Detector at Fermilab using muonic [ital b]-quark decays. In the central rapidity region ([vert bar][ital y][sup [ital b]][vert bar][lt]1.0), the cross section is 295[plus minus]21[plus minus]75 nb (59[plus minus]14[plus minus]15 nb) for [ital p][sub [ital T]][sup [ital b]][gt]21 GeV/[ital c] (29 GeV/[ital c]). Comparisons are made to previous measurements and next-to-leading order QCD calculations.
Physics Letters B | 1990
Takashi Sasaki; Y. Yamagishi; R. Tanaka; T. Kojima; S. Matsumoto; T. Yasuda; Y. Ishi; K. Miyano; H. Miyata; P. Kirk; J. Lim; R.R. McNeil; W. Metcalf; S. S. Myung; C.P. Cheng; P. Gu; M.H. Ye; Y.C. Zhu; A. Abashian; K. Gotow; K.P. Hu; A.Z. Lai; E.H. Low; M. E. Mattson; L. E. Piilonen; K.L. Sterner; Y.K. Li; S. Lusin; C. Rosenfeld; A.T.M. Wang
Abstract The photon structure function F2 has been measured at average Q2 values of 73,160 and 390 ( GeV c ) 2 . We compare the x dependence of the Q2 = 73 ( GeV c ) 2 data with theoretical expectations based on QCD. In addition we present results on the Q2 evolution of the structure function for the intermediate x range (0.3⩽ x ⩽0.8). The results are consistent with QCD.
Physical Review Letters | 1993
F. Abe; D. Amidei; C. Anway-Weiss; G. Apollinari; M. Atac; P. Auchincloss; A. Baden; N. Bacchetta; W. Badgett; M. W. Bailey; A. Bamberger; de Barbaro P; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; G. Bauer; T. Baumann; F. Bedeschi; S. Behrends; S. Belforte; G. Bellettini; J. Bellinger; D. Benjamin; J. Benlloch; J. Bensinger; A. Beretvas; J. P. Berge; S. Bertolucci; S. Bhadra; M. Binkley
We present a measurement of jet shapes in [ital [bar p]p] collisions at [radical][ital s] =1.8 TeV at the Fermilab Tevatron using the Collider Detector at Fermilab (CDF). Qualitative agreement is seen with the predictions of recent next-to-leading [[ital O]([alpha][sub [ital s]][sup 3])] calculations and with leading logarithm QCD based Monte Carlo simulations. The dependence of the jet shape on transverse energy is studied.
Physical Review Letters | 1990
F. Abe; D. Amidei; G. Apollinari; M. Atac; P. Auchincloss; A. Baden; A. Bamberger; A. Barbaro-Galtieri; V. E. Barnes; F. Bedeschi; S. Behrends; S. Belforte; G. Bellettini; J. Bellinger; J. Bensinger; A. Beretvas; J. P. Berge; S. Bertolucci; S. Bhadra; M. Binkley; R. E. Blair; C. Blocker; A. W. Booth; G. Brandenburg; D. N. Brown; E. Buckley; A. Byon; K. L. Byrum; C. Campagnari; M. Campbell
An analysis of {ital W}- and {ital Z}-boson production using data from the Collider Detector at Fermilab at {radical}{ital s} =1.8 TeV yields {sigma}({ital W}{r arrow}{ital ev})/{sigma}({ital Z}{r arrow}{ital ee})=10.2{plus minus}0.8(stat){plus minus}0.4(syst). The width of the {ital W} boson, {Gamma}({ital W}), and a limit on the top-quark mass independent of decay mode are extracted from this measurement.
Physical Review D | 1990
F. Abe; D. Amidei; G. Apollinari; G. Ascoli; M. Atac; P. Auchincloss; A. Baden; A. Barbaro-Galtieri; V. E. Barnes; F. Bedeschi; S. Behrends; S. Belforte; G. Bellettini; J. Bellinger; J. Bensinger; A. Beretvas; P. Berge; S. Bertolucci; S. Bhadra; M. Binkley; R. E. Blair; C. Blocker; J. Bofill; A. W. Booth; G. Brandenburg; D. N. Brown; A. Byon; K. L. Byrum; M. Campbell; R. Carey
We present the dijet invariant-mass distribution in the region between 60 and 500 GeV, measured in 1.8-TeV {ital {bar p}p} collisions in the Collider Detector at Fermilab. Jets are restricted to the pseudorapidity interval {vert bar}{eta}{vert bar}{lt}0.7. Data are compared with QCD calculations; axigluons are excluded with 95% confidence in the region 120{lt}{ital M}{sub {ital A}}{lt}210 GeV for axigluon width {Gamma}{sub {ital A}}={ital N}{alpha}{sub s}{ital M}{sub {ital A}}/6, with {ital N}=5.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994
P. Auchincloss; P. de Barbaro; A. Bodek; H. S. Budd; M. Pillai; F. Qun; W. K. Sakumoto; F. S. Merritt; M. J. Oreglia; B.A. Schumm; T. Bolton; C. G. Arroyo; K.T. Bachmann; A.O. Bazarko; R.E. Blair; C. Foudas; B.J. King; W.C. Lefmann; W.C. Leung; S.R. Mishra; E. Oltman; P. Z. Quintas; S.A. Rabinowitz; F. Sciulli; W.G. Seligman; M. H. Shaevitz; R. H. Bernstein; F. Borcherding; H. E. Fisk; M.J. Lamm
Abstract We have extracted the momentum dependence of the mean, the truncated mean and the most probable value of the energy deposited in a segmented, iron-scintillator, hadron calorimeter by high-energy muons. Data were drawn from a sample of momentum-analyzed, high-energy muons produced in charged-current neutrino interactions. The truncated mean energy deposition of high-energy muons traversing 20 calorimeter segments increases by approximately 16% per 100 GeV c increase in muon momentum over the range 25−125 GeV c ; the most probable energy deposition increases by approximately 7%. These results are important for experiments at high-energy colliders (e.g., Tevatron, SSC and LHC) which use the d E d x of high-energy muons to calibrate the response of electromagnetic and hadron calorimeters with tower geometry. The data are in qualitative agreement with GEANT3 (v3.15/308a) simulations.
Physics Letters B | 1990
Gui Nyun Kim; R. Breedon; Winston Ko; R. Lander; K. Maeshima; R. Malchow; J. Smith; D. Stuart; R. Imlay; P. Kirk; J. Lim; R. R. McNeill; W. Metcalf; S. S. Myung; C.P. Cheng; P. Gu; J. Li; Y.K. Li; M.H. Ye; Y.C. Zhu; A. Abashian; K. Gotow; K.P. Hu; E.H. Low; M. E. Mattson; L. E. Piilonen; K.L. Sterner; S. Lusin; C. Rosenfeld; A.T.M. Wang
Abstract We report on a search for the pair production of leptoquarks and colored leptons in e + e − annihilations t center-of-mass energies from 50 to 60.8 GeV, using the AMY detector at TRISTAN. No evidence for such particles is found and 95% CL mass limits are given.
Physical Review Letters | 1990
F. Abe; D. Amidei; G. Apollinari; G. Ascoli; M. Atac; P. Auchincloss; A. Baden; A. Barbaro-Galtieri; V. E. Barnes; F. Bedeschi; S. Behrends; S. Belforte; G. Bellettini; J. Bellinger; J. Bensinger; A. Beretvas; P. Berge; S. Bertolucci; S. Bhadra; M. Binkley; R. E. Blair; C. Blocker; J. Bofill; A. W. Booth; G. Brandenburg; D. N. Brown; A. Byon; K. L. Byrum; M. Campbell; R. Carey
The production rate of charged {ital D}{sup *} mesons in jets has been measured in 1.8-TeV {ital {bar p}p} collisions at the Fermilab Tevatron with the Collider Detector at Fermilab. In a sample of approximately 32 300 jets with a mean transverse energy of 47 GeV obtained from an exposure of 21.1 nb{sup {minus}1}, a signal corresponding to 25.0{plus minus}7.5(stat){plus minus}2.0(syst) {ital D}{sup *{plus minus}}{r arrow}K{sup {minus plus}}{pi}{sup {plus minus}}{pi}{sup {plus minus}} events is seen above background. This corresponds to a ratio {ital N}({ital D}{sup *+}+D{sup *{minus}})/N(jet) =0.10{plus minus}0.03{plus minus}0.03 for {ital D}{sup *} mesons with fractional momentum {ital z} greater than 0.1.
Journal of Physics G | 1996
U.K. Yang; P. Auchincloss; P. de Barbaro; A. Bodek; H. S. Budd; D. A. Harris; W. K. Sakumoto; W C Lefmann; R. Steiner; M. J. Oreglia; B.A. Schumm; R. A. Johnson; M. Nussbaum; L Perera; M. Vakili; G Arroyo; A.O. Bazarko; J. M. Conrad; J.H. Kim; B.J. King; S. Koutsoliotas; C. McNulty; S.R. Mishra; P. Z. Quintas; A. Romosan; F. Sciulli; W.G. Seligman; M. H. Shaevitz; P. Spentzouris; E. G. Stern
Measurements of neutrino - nucleon and antineutrino - nucleon differential cross sections using the CCFR neutrino detector at Fermilab have been used to extract preliminary values of in the kinematic region 0.01 < x < 0.6 and . The new data provide the first measurements of R in the region x < 0.1. The x and dependence of R is compared with a QCD-based fit to previous data. The QCD fit, which provides an estimate of R in the small-x region where R has not been previously measured, is in good agreement with the new CCFR data.
Physical Review Letters | 1995
F. Abe; H. Akimoto; A. Akopian; M. Albrow; Amendolia; D. Amidei; J. Antos; C. Anway-Wiese; S. Aota; G. Apollinari; T. Asakawa; W. Ashmanskas; M. Atac; P. Auchincloss; F. Azfar; P. Azzi-Bacchetta; N. Bacchetta; W. Badgett; S. Bagdasarov; M. W. Bailey; J. Bao; de Barbaro P; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Bartalini; G. Bauer; T. Baumann; F. Bedeschi; S. Behrends
We establish the existence of the top quark using a 67pb{sup {minus}1} data sample of {ital p}{ovr bar}{ital p} collisions at {radical}{ital s}=1.8TeV collected with the Collider Detector at Fermilab (CDF). Employing techniques similar to those we previously published, we observe a signal consistent with {ital tb}{ovr bar}, but inconsistent with the background prediction by 4.8{sigma}. Additional evidence for the top quark is provided by a peak in the reconstructed mass distribution. We measure the top quark mass to be 176{plus_minus}8(stat){plus_minus}10(syst)GeV/{ital c}{sup 2}, and the {ital tt}{ovr bar} production cross section to be 6.8{sub {minus}2.4}{sup +3.6}pb.We establish the existence of the top quark using a 67 pb^-1 data sample of Pbar-P collisions at Sqrt(s) = 1.8 TeV collected with the Collider Detector at Fermilab (CDF). Employing techniques similar to those we previously published, we observe a signal consistent with t-tbar decay to WW b-bbar, but inconsistent with the background prediction by 4.8 sigma. Additional evidence for the top quark is provided by a peak in the reconstructed mass distribution. We measure the top quark mass to be 176 +/-8(stat) +/- 10(sys.) GeV/c^2, and the t-tbar production cross section to be 6.8 +3.6 -2.4 pb.