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(50 points)The textarea shown to the left is named ta in a form named f1.It contains the top 10,000 passwords in order of frequency of use - each followed by a comma (except the last one). To model phase transition from Quark-Gluon Plasma to hadronic state of matter the Freeze-Out code (written in Fortran 90) is used. It is based on relativistic kinetic equation, which describes non-equilibrium dynamics of the freeze-out process. I am familiar with Linux, Mac OS X, Windows, Fortran, Pascal.

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  • Using 55.8 pb(-1) of e(+)e(-) collisions recorded at the psi(3770) resonance with the CLEO-c detector at CESR, we determine absolute hadronic branching fractions of charged and neutral D mesons using a double tag technique. Among measurements for three D-0 and six D+ modes, we obtain reference branching fractions B(D-0- K(-)pi(+))=(3.91 +/- 0.08 +/- 0.09)% and B(D+- K(-)pi(+)pi(+))=(9.5.

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Related to hadronic: quark

had·ron

(hăd′rŏn′)n.
Any of a class of subatomic particles that are composed of two or three quarks and participate in strong interactions. The class of hadrons is divided into the mesons and baryons.
[Greek hadros, thick; see sā- in Indo-European roots + -on.]
American Heritage® Dictionary of the English Language, Fifth Edition. Copyright © 2016 by Houghton Mifflin Harcourt Publishing Company. Published by Houghton Mifflin Harcourt Publishing Company. All rights reserved.

hadron

(ˈhædrɒn) n
(Nuclear Physics) any elementary particle capable of taking part in a strong nuclear interaction and therefore excluding leptons and photons
[C20: from Greek hadros heavy, from hadēn enough + -on]
Collins English Dictionary – Complete and Unabridged, 12th Edition 2014 © HarperCollins Publishers 1991, 1994, 1998, 2000, 2003, 2006, 2007, 2009, 2011, 2014

had•ron

Hadronic (ˈhæd rɒn)
n.
any of a group of elementary particles subject to the strong interaction, subdivided into baryons and mesons.
ha•dron′ic,adj.
Random House Kernerman Webster's College Dictionary, © 2010 K Dictionaries Ltd. Copyright 2005, 1997, 1991 by Random House, Inc. All rights reserved.
Noun1.hadron - any elementary particle that interacts strongly with other particles
antibaryon - the antiparticle of a baryon; a hadron with a baryon number of -1
antiquark - the antiparticle of a quark
baryon, heavy particle - any of the elementary particles having a mass equal to or greater than that of a proton and that participate in strong interactions; a hadron with a baryon number of +1
elementary particle, fundamental particle - (physics) a particle that is less complex than an atom; regarded as constituents of all matter
meson, mesotron - an elementary particle responsible for the forces in the atomic nucleus; a hadron with a baryon number of 0
quark - (physics) hypothetical truly fundamental particle in mesons and baryons; there are supposed to be six flavors of quarks (and their antiquarks), which come in pairs; each has an electric charge of +2/3 or -1/3; 'quarks have not been observed directly but theoretical predictions based on their existence have been confirmed experimentally'
Based on WordNet 3.0, Farlex clipart collection. © 2003-2012 Princeton University, Farlex Inc.

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Department of Physics and Astronomy Faculty Publications

Title

Authors

Published in:

Physical Review D 76,11 (2007)

Link to original published article:

http://dx.doi.org/10.1103/PhysRevD.76.112001

Abstract

Using 281 pb(-1) of e(+)e(-) collisions recorded at the psi(3770) resonance with the CLEO-c detector at CESR (Cornell Electron Storage Ring), we determine absolute hadronic branching fractions of charged and neutral D mesons using a double tag technique. Among measurements for three D-0 and six D+ modes, we obtain reference branching fractions B(D-0 -> K-pi(+))=(3.891 +/- 0.035 +/- 0.059 +/- 0.035)% and B(D+-> K-pi(+)pi(+))=(9.14 +/- 0.10 +/- 0.16 +/- 0.07)%, where the first uncertainty is statistical, the second is all systematic errors other than final-state radiation (FSR), and the third is the systematic uncertainty due to FSR. We include FSR in these branching fractions by allowing for additional unobserved photons in the final state. Using an independent determination of the integrated luminosity, we also extract the cross sections sigma(e(+)e(-)-> D-0(D) over bar (0))=(3.66 +/- 0.03 +/- 0.06) nb and sigma(e(+)e(-)-> D+D-)=(2.91 +/- 0.03 +/- 0.05) nb at a center-of-mass energy, E-cm=3774 +/- 1 MeV.

Keywords

Astronomy & Astrophysics;; Physics, Particles & Fields

Date of this Version

Hadronic Mac Os X

January 2007

Hadronic Mac Os Catalina

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