Abstract

In a previous paper it was shown that it is possible to construct some tests of forward dispersion relations which are independent of the high-energy behaviour of the total cross-sections. The present paper contains an investigation of the dependence of these tests on the threshold parameters (f2 and the scattering lengths). It is well known that the threshold parameters are not very well determined experimentally. Therefore, in order that our tests are reliable, it is necessary that they are practically independent of the threshold parameters. It turns out that there exist two tests of the forward dispersion relations which are practically independent of the actual values of the threshold parameters. This result yields the most critical test of forward dispersion relations (i.e. essentially local commutativity, Lorentz invariance and unitarity) proposed up to now. In the spirit of the previous work it is then shown that the two threshold parametersf2 andTS(m) can be determined by a method which is independent of the high-energy behaviour of the total cross-sections. Finally, it is shown that the existing experimental data indicate thatσA(E)=1/2(σ−(E)−σ+(E)) might change its sign somewhere between 20 GeV and 50 GeV. In an Appendix a discussion of the comparison of sum rules of the Khuri-Kinoshita-Martin type with experiments is given. It turns out that the sum rules of this type are much weaker than the tests discussed in the present paper.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.