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Forward muon production in proton-antiproton collisions at [square root of] s=1.8 TeVSkarha, John Erwin. January 1989 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1989. / Cover title. On t.p. "[square root of]" appears as the square root symbol. Includes bibliographical references (p. 255-262).
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A search for the Higgs boson in proton-antiproton collisions at [center-of-mass energy] = 1.8 TeVNeu, Christopher Carl, January 2003 (has links)
Thesis (Ph. D.)--Ohio State University, 2003. / Title from first page of PDF file. Document formatted into pages; contains xxii, 166 p.; also includes graphics (some col.) Includes bibliographical references (p. 163-166). Available online via OhioLINK's ETD Center
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Measurement of the top quark mass with neural networks /Sánchez, Carlos Andrés. January 2002 (has links)
No description available.
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Relative transverse momentum distributions of bottom hadrons produced in 1.96 TeV proton-antiproton collisionsRoy, Philippe, 1983- January 2008 (has links)
Fragmentation is the process by which bare quarks dress themselves up as hadrons. Since we cannot get reliable calculations of this process using perturbative quantum chromodynamics, the fragmentation properties of quarks must be obtained empirically. We report on the signal extraction and relative transverse momentum (pT) spectrum determination that will lead to a high precision measurement of relative fragmentation fractions of b quarks into B hadrons, in 1.96 TeV pp¯ collisions. Using 1.9 fb-1 of data taken with the CDF-II detector, we fully reconstruct 473 +/- 42 B0s→D-sp + , 15206 +/- 203 B0 → D-pi+, 1483 +/- 45 B0 → D*-pi + and 4444 +/- 297 L0b→L+ cp- candidate decays. In order to reduce systematic uncertainties, ratios of pT spectra are reported. We find that Bs and B0 mesons are produced with similar pT and Λb baryons are produced with lower pT than B0 mesons. Our results are consistent with previous CDF measurements suggesting a difference between fragmentation processes observed at lepton and hadron colliders.
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Measurement of Z + [gamma] Production and Search for Anomalous Triple Gauge Couplings in Proton-antiproton Collisions at [radical symbol]S = 1.96 TevDeng, Jianrong, January 2008 (has links)
Thesis (Ph. D.)--Duke University, 2008.
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Measurement of the top pair production cross section at CDF using neural networksMarginean, Radu. January 2004 (has links)
Thesis (Ph. D.)--Ohio State University, 2004. / Title from first page of PDF file. Document formatted into pages; contains xiii, 110 p.; also includes graphics (some col.). Includes bibliographical references (p. 106-110).
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Srch for charged Higgs bosons decaying to top and bottom quarks in proton-antiproton collisionsKertzscher, Gustavo, January 1900 (has links)
Thesis (M.Sc.). / Written for the Dept. of Physics. Title from title page of PDF (viewed 2009/06/25). Includes bibliographical references.
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Relative transverse momentum distributions of bottom hadrons produced in 1.96 TeV proton-antiproton collisionsRoy, Philippe, 1983- January 2008 (has links)
No description available.
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Transverse and longitudinal Bose-Einstein correlations in antiproton-proton reactions at centre-of-mass energy 630 GeVOctober, Faith Joy 03 1900 (has links)
Thesis (MSc)--Stellenbosch University, 2002. / ENGLISH ABSTRACT: We use Hanbury-Brown Twiss interferometry to determine Bose-Einstein correlations in the
transverse and longitudinal directions. By using these two directions, we are able to determine
the shape of the pion emitting source. The analysis is done with the UA1 (1985) data for pp
collisions at Vs = 630 GeV. Two frames of reference, namely the laboratory frame and the
Longitudinal Center-of-Mass System (LCMS) are used. A fit to a two-dimensional Gaussian
parametrization yields good results.
In the laboratory frame, an oblate form of the source is observed, with the value of the
transverse radius (rt) larger than the longitudinal (rL) one. The LCMS analysis finds a prolate
form of the source (rt < rL). A few reasons are discussed for the difference in the shape between
the different reference frames. Our results are also compared with other hadron-hadron and
e+ e: experiments. / AFRIKAANSE OPSOMMING: Hanbury-Brown Twiss interferometrie was gebruik om Bose-Einstein korrelasies in die transversale
en longitudinale rigtings te bepaal. Deur hierdie twee rigtings te gebruik, kan die vorm van
die pion-bron bepaal word. Die UA1 (1985) datastel van die pp botsings by Vs = 630 GeV is
gebruik om die analise uit te voer. Twee verwysingstelsels, naamlik die laboratorium stelsel en
die Longitudinale Massamiddelpunt-stelsel is aangewend. 'n Passing met 'n twee-dimensionele
Gaussiese parametrisering het goeie resultate opgelewer.
In die laboratorium stelsel, is 'n ovaalvormige vorm vir die bron waargeneem, met die transversale
radius (rt) groter as die longitudinale radius (rl)' Die Longitudinale Massamiddelpunt stelsel
het 'n prolate vorm vir die bron voorspel, met rt < ri, 'n Paar redes vir die verskil in die vorm
van die pion-bron vir die verskillende verwysingstelsels word bespreek. Ons resultate word ook
met ander hadron-hadron en e+e- eksperimente vergelyk.
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Search for large extra dimensions in the exclusive photon + missing energy channel in PP collisionsLazoflores, Jose A. Hagopian, V. Hagopian, Sharon. January 2006 (has links)
Thesis (Ph. D.)--Florida State University, 2006. / Advisors: Vasken Hagopian, Sharon Hagopian, Florida State University, College of Arts and Sciences, Dept. of Physics. Title and description from dissertation home page (viewed Sept. 15, 2005). Document formatted into pages; contains xiv, 155 pages. Includes bibliographical references.
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