10,903 research outputs found
Baryons made of heavy quarks at the LHC
Baryons made of heavy quarks are extremely interesting and could be seen at
the LHC.Comment: 1 pag
The Froissart bound for inelastic cross-sections
We prove that while the total cross{}-section is bounded by , where is the square of the c.m. energy and the mass of
the pion, the total inelastic cross{}-section is bounded by , which is 4 times smaller. We discuss the implications of this result
on the total cross{}-section itself.Comment: 9 pages. Corrected minor typo
Froissart Bound on Total Cross-section without Unknown Constants
We determine the scale of the logarithm in the Froissart bound on total
cross-sections using absolute bounds on the D-wave below threshold for
scattering. E.g. for scattering we show that for c.m. energy
, where .Comment: 6 page
Froissart Bound on Inelastic Cross Section Without Unknown Constants
Assuming that axiomatic local field theory results hold for hadron
scattering, Andr\'e Martin and S. M. Roy recently obtained absolute bounds on
the D-wave below threshold for pion-pion scattering and thereby determined the
scale of the logarithm in the Froissart bound on total cross sections in terms
of pion mass only. Previously, Martin proved a rigorous upper bound on the
inelastic cross-section which is one-fourth of the
corresponding upper bound on , and Wu, Martin,Roy and Singh
improved the bound by adding the constraint of a given . Here we
use unitarity and analyticity to determine, without any high energy
approximation, upper bounds on energy averaged inelastic cross sections in
terms of low energy data in the crossed channel. These are Froissart-type
bounds without any unknown coefficient or unknown scale factors and can be
tested experimentally. Alternatively, their asymptotic forms,together with the
Martin-Roy absolute bounds on pion-pion D-waves below threshold, yield absolute
bounds on energy-averaged inelastic cross sections. E.g. for
scattering, defining ,we show that for c.m. energy ,
where . This bound is
asymptotically one-fourth of the corresponding Martin-Roy bound on the total
cross section, and the scale factor is one-fourth of the scale factor in
the total cross section bound. The average over the interval (s,2s) of the
inelastic cross section has a bound of the same form with
replaced by .Comment: 9 pages. Submitted to Physical Review
The Corporate Bond Market in Canada
The Canadian corporate bond market has experienced a renaissance, in recent years, against a background of low inflation, reduced public borrowing, and the lowest levels of long-term interest rates in a generation. The authors examine the influences shaping the market and also compare the Canadian market with those of other countries. The increased level of activity in the market has been accompanied by the development of new products and by greater investor interest in instruments with higher returns and higher credit risk. A more dynamic Canadian corporate bond market is a welcome development since it offers borrowers an alternative source of funds, especially companies that have typically relied on the banking system and on the U.S. corporate bond market for financings involving higher levels of credit risk.
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