25,231 research outputs found
Top quark production cross-section at the Tevatron Run 2
The top quark pair production cross-section has been
measured in collisions at center of mass energies of 1.96 TeV using
Tevatron Run 2 data. In the begining of Run 2 both CDF and D\O\
measurements in the {\it dilepton} channel
$t\bar{t}{\to}WbW\bar{b}{\to}\bar{\ell}{\nu}_{\ell}b{\ell}^{'}\
bar{\nu}_{{\ell}^{'}}\bar{b}t\bar{t}{\to}WbW\bar{b}{\to}q\bar{q}^{'}b{\ell}\bar{\nu}_{\ell
}\bar{b}+\bar{\ell}{\nu}_{\ell}bq\bar{q}^{'}\bar{b}$ agree with the NLO
(Next-to-Leading-Order) theoretical predictions. The presence of a top signal
in Tevatron data has been reestablished.Comment: 4 pages, 3 figure
On a static charged fluid around a magnetized mass
We show that any magnetostatic axially symmetric solution of the
Einstein-Maxwell equations can be endowed with a specific charged fluid source
of the Polanco et al type via a simple procedure requiring the knowledge of
exclusively the magnetostatic seed spacetime. Using this procedure we construct
yet another exact solution for a massive magnetic dipole surrounded by a static
charged fluid which is different from the Polanco et al metric.Comment: 5 pages, no figures, submitted to Physical Review
Remarks on the mass-angular momentum relations for two extreme Kerr sources in equilibrium
The general analysis of the relations between masses and angular momenta in
the configurations composed of two balancing extremal Kerr particles is made on
the basis of two exact solutions arising as extreme limits of the well-known
double-Kerr spacetime. We show that the inequality M^2 >= |J| characteristic of
an isolated Kerr black hole is verified by all the extremal components of the
Tomimatsu and Dietz-Hoenselaers solutions. At the same time, the inequality can
be violated by the total masses and total angular momenta of these binary
systems, and we identify all the cases when such violation occurs.Comment: 11 pages, 4 figure
A combined Majumdar-Papapetrou-Bonnor field as extreme limit of the double-Reissner-Nordstrom solution
The general extreme limit of the double-Reissner-Nordstrom solution is worked
out in explicit analytical form involving prolate spheroidal coordinates. We
name it the combined Majumdar-Papapetrou-Bonnor field to underline the fact
that it contains as particular cases the two-body specialization of the
well-known Majumdar-Papapetrou solution and Bonnor's three-parameter
electrostatic field. To the latter we give a precise physical interpretation as
describing a pair of non-rotating extremal black holes with unequal masses and
unequal opposite charges kept apart by a strut, the absolute values of charges
exceeding the respective (positive) values of masses.Comment: 10 pages, 3 figures, title changed, the result extended, matching the
published versio
Utility analysis : current trends and future directions.
Utility analysis procedures offer organizational decision-makers useful information regarding the relative values of different interventions. Years of research have resulted in a number of practically viable utility models and extensions. There is a continued need for research to examine the accuracy of utility estimates and to further compare the different models. A more recent research concern is that of low levels of acceptance of utility analysis results by practitioners. Many researchers are turning their attention to ways in which this acceptance may be increased. This article reviews different utility models as well as a number of important extensions. It then discusses current utility analysis issues, such as the aforementioned acceptance problem and the introduction of a multi-attribute utility model. The article concludes with suggestions for future utility analysis researchUtility theory; Mathematical models; Decision making;
Experimental determination of the b quark mass in DELPHI
The running mass of the b quark as defined in the MS-bar renormalization
scheme, m_b, was measured at the M_Z scale using 2.8 million hadronic Z^0
decays collected by the DELPHI experiment at LEP. The result is m_b(M_Z) = 2.67
+- 0.25 (stat.) +- 0.34 (frag.) +- 0.27(theo.) GeV/c^2 which differs from that
obtained at the Upsilon scale, by m_b(M_\Upsilon/2)-m_b(M_Z) = 1.49 +- 0.52
GeV/c^2. This measurement, performed far from the production
threshold, provides the first experimental observation of the running of the
quark masses.Comment: Talk given at the QCD 97 conference held in Montpellier, July 1997.
Also available here http://hep.ph.liv.ac.uk/~martis
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