Date: Thu, 25 Dec 08 01:00:24 GMT
Subject: hep-ex daily 4 new + 2 crosses received   by eprepget 

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received   by eprepget from  Tue 23 Dec 08 21:00:01 GMT  to  Wed 24 Dec 08 21:00:01 GMT
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arXiv:0812.4458
Date: Tue, 23 Dec 2008 22:29:57 GMT   (60kb)

Title: Measurement of Cross Sections for $b$ Jet Production in Events with a
  $Z$ Boson in $p\bar{p}$ Collisions at $\sqrt{s}=1.96$ TeV
Authors: CDF collaboration: T. Aaltonen, et al
Categories: hep-ex
Comments: submitted to Phys. Rev. D
Report-no: FERMILAB-PUB-08-576-E
\\
  A measurement of the $\bjet$ production cross section is presented for events
containing a $Z$ boson produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$
TeV, using data corresponding to an integrated luminosity of 2 fb$^{-1}$
collected by the CDF II detector at the Tevatron. $Z$ bosons are selected in
the electron and muon decay modes. Jets are considered with transverse energy
$E_T>20$ GeV and pseudorapidity $|\eta|<1.5$ and are identified as $\bjets$
using a secondary vertex algorithm. The ratio of the integrated $Z+\bjet$ cross
section to the inclusive $Z$ production cross section is measured to be $3.32
\pm 0.53 {\rm (stat.)} \pm 0.42 {\rm (syst.)}\times 10^{-3}$. This ratio is
also measured differentially in jet $E_T$, jet $\eta$, $Z$-boson transverse
momentum, number of jets, and number of $\bjets$. The predictions from leading
order Monte Carlo generators and next-to-leading-order QCD calculations are
found to be consistent with the measurements within experimental and
theoretical uncertainties.
\\ ( http://arxiv.org/abs/0812.4458 ,  60kb)
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arXiv:0812.4469
Date: Wed, 24 Dec 2008 01:21:08 GMT   (236kb)

Title: Top Quark Mass Measurement in the Lepton plus Jets Channel Using a
  Modified Matrix Element Method
Authors: CDF Collaboration, T. Aaltonen, et al
Categories: hep-ex
Comments: 46 pages, 16 figures. Submitted to Phys. Rev. D
Report-no: FERMILAB-PUB-08-574-E
\\
  We report a measurement of the top quark mass, m_t, obtained from ppbar
collisions at sqrt(s) = 1.96 TeV at the Fermilab Tevatron using the CDF II
detector. We analyze a sample corresponding to an integrated luminosity of 1.9
fb^-1. We select events with an electron or muon, large missing transverse
energy, and exactly four high-energy jets in the central region of the
detector, at least one of which is tagged as coming from a b quark. We
calculate a signal likelihood using a matrix element integration method, with
effective propagators to take into account assumptions on event kinematics. Our
event likelihood is a function of m_t and a parameter JES that determines /in
situ/ the calibration of the jet energies. We use a neural network discriminant
to distinguish signal from background events. We also apply a cut on the peak
value of each event likelihood curve to reduce the contribution of background
and badly reconstructed events. Using the 318 events that pass all selection
criteria, we find m_t = 172.7 +/- 1.8 (stat. + JES) +/- 1.2 (syst.) GeV/c^2.
\\ ( http://arxiv.org/abs/0812.4469 ,  236kb)
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arXiv:0812.4527
Date: Wed, 24 Dec 2008 12:29:50 GMT   (176kb)

Title: A High Resolution Neutrino Experiment in a Magnetic Field for Project-X
  at Fermilab
Authors: S. R. Mishra, R. Petti, C. Rosenfeld
Categories: hep-ex
Comments: 6 pages, 2 figures
\\
  We propose a new high-resolution neutrino experiment within a dipole magnetic
field, HiResM$\nu$. This experiment will run along with long-baseline neutrino
oscillation experiments (LBL$\nu$) such as NO$\nu$A, a large-cavity detector at
DUSEL, or a Liquid-Argon detector in the Medium-Energy (ME) configuration of
the NuMI-beam. Assuming the 120 GeV Main Injector proton intensities we
anticipate 140(50) million $\nu_\mu$ ($\overline{\nu}_\mu$) Charged-Current
(CC) events in the fiducial volume, for 3(4)-year run with the ME
(anti)neutrino beam. Alternatively, the same statistics could be collected in
just 1(1.5) year with the High Energy (HE) beam configuration. The goals of
HiResM$\nu$ are twofold. It will measure the relative abundance and the energy
spectrum of $\nu_\mu$, $\overline{\nu}_\mu$, $\nu_e$ and $\overline{\nu}_e$
CC-interactions, which are directly relevant to LBL$\nu$. It will serve as an
`Event-Generator' of real neutrino interactions to estimate backgrounds and
efficiencies in LBL$\nu$. As such, it will provide a quantitative determination
of the overall energy-scale of neutrino CC interactions and of hadronic
multiplicities for all CC and Neutral-Current (NC) event topologies. In
addition, it will perform precise measurements of electroweak parameters, of
(semi)exclusive processes such as quasi-elastic, resonance, $\pi^0$ / $K^0_S$ /
$\Lambda$/charm-hadron production, as well as of the hadronic structure of
nucleons and nuclei. We expect to reach a sensitivity of about 0.2% on the weak
mixing angle by combining different channels. The new experiment will also
perform searches for new physics beyond the Standard Model.
\\ ( http://arxiv.org/abs/0812.4527 ,  176kb)
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arXiv:0812.4543
Date: Wed, 24 Dec 2008 15:58:50 GMT   (222kb)

Title: A study of quasi-elastic muon neutrino and antineutrino scattering in
  the NOMAD experiment
Authors: NOMAD Collaboration
Categories: hep-ex
Comments: 26 pages, 18 figures, to be submitted to Eur.Phys.J.C
\\
  We have studied the muon neutrino and antineutrino quasi-elastic (QEL)
scattering reactions using a set of experimental data collected by the NOMAD
collaboration. We have performed measurements of the cross-section of these
processes on a nuclear target (mainly Carbon) normalizing it to the total
(anti)neutrino charged current cross-section. The axial mass parameter was
extracted from the measured quasi-elastic neutrino cross-section. It is
consistent with the axial mass values recalculated from the antineutrino
cross-section and extracted from the pure Q^2 shape analysis of the high purity
sample of neutrino quasi-elastic 2-track events, but has smaller systematic
error. Our measured M_A mass is found to be in good agreement with the world
average value obtained in previous deuterium filled bubble chamber experiments.
The NOMAD measurement of M_A is lower than those recently published by K2K and
MiniBooNE collaborations. However, within the large errors quoted by these
experiments on M_A, these results are compatible with the more precise NOMAD
value.
\\ ( http://arxiv.org/abs/0812.4543 ,  222kb)
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arXiv:0812.4092 (*cross-listing*)
Date: Mon, 22 Dec 2008 04:51:12 GMT   (39kb)

Title: Further insights into the "$\rho\pi$ puzzle"
Authors: Qiang Zhao, Gang Li, and Chao-Hsi Chang
Categories: hep-ph hep-ex
Comments: 7 pages, 2 figures, proceeding of "The Conference on
  Interdisciplinary Fields of Particle Physics, Nuclear Physics and Cosmology",
  Aug. 2-4, 2008, Yunnan, China
\\
  Based on a systematic investigation of $J/\psi(\psi^\prime)\to VP$, where $V$
and $P$ stand for light vector and pseudoscalar mesons, we identify the role
played by the electromagnetic (EM) transitions and intermediate meson loop
transitions, which are essential ingredients for understanding the $J/\psi$ and
$\psi^\prime$ couplings to $VP$. We show that on the one hand, the EM
transitions have relatively larger interferences in $\psi^\prime\to \rho\pi$
and $K^*\bar{K}+c.c.$ as explicitly shown by vector meson dominance (VMD). On
the other hand, the strong decay of $\psi^\prime$ receives relatively larger
destructive interferences from the intermediate meson loop transitions. By
identifying these mechanisms in an overall study of $J/\psi(\psi^\prime)\to
VP$, we provide a coherent understanding of the so-called "$\rho\pi$ puzzle".
\\ ( http://arxiv.org/abs/0812.4092 ,  39kb)
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arXiv:0812.4260 (*cross-listing*)
Date: Mon, 22 Dec 2008 18:04:24 GMT   (199kb)

Title: Can universality of the QCD evolution be checked in W boson decays into
  hadrons?
Authors: A.V. Kisselev and V.A. Petrov
Categories: hep-ph hep-ex
Comments: 14 pages, 7 figures
\\
  Hadron multiplicity from $W$ boson is calculated in pQCD. The agreement of
our theoretical predictions with the LEP data says in favor of universality of
the QCD evolution in hard processes.
\\ ( http://arxiv.org/abs/0812.4260 ,  199kb)
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