2007
DOI: 10.1590/s0103-97332007000300006
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Derivative dispersion relations above the physical threshold

Abstract: We discuss some formal and practical aspects related to the replacement of Integral Dispersion Relations (IDR) by derivative forms, without high-energy approximations. We first demonstrate that, for a class of functions with physical interest as forward scattering amplitudes, this replacement can be analytically performed, leading to novel Extended Derivative Dispersion Relations (EDDR), which, in principle, are valid for any energy above the physical threshold. We then verify the equivalence between the IDR a… Show more

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Cited by 16 publications
(30 citation statements)
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References 23 publications
(66 reference statements)
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“…The use of prescriptions seem to us unjustified in the region of intermediate and low energy data, since they are asymptotic results [37]. By constrast, derivative dispersion relations allow an analytical approach and can be extended down to 4 -5 GeV [40,41] or even below (above the physical threshold) in the form of a double infinite series [42,43] or a single series [44]. However, and that is a crucial point in this work, we shall not consider simultaneus fits to total cross section data and ρ information for the six reasons that follows.…”
Section: B Data Ensemble and Critical Commentsmentioning
confidence: 99%
“…The use of prescriptions seem to us unjustified in the region of intermediate and low energy data, since they are asymptotic results [37]. By constrast, derivative dispersion relations allow an analytical approach and can be extended down to 4 -5 GeV [40,41] or even below (above the physical threshold) in the form of a double infinite series [42,43] or a single series [44]. However, and that is a crucial point in this work, we shall not consider simultaneus fits to total cross section data and ρ information for the six reasons that follows.…”
Section: B Data Ensemble and Critical Commentsmentioning
confidence: 99%
“…Equation (74) On the other hand, from the high-energy approximate result (75), for γ = 2, we obtain the triple pole contribution (68). Moreover, from (75), in the general case, σ(s) ≈ β ln γ (s), ρ(s) ≈ γπ 2 ln(s) .…”
Section: A Exact Resultsmentioning
confidence: 88%
“…The differences between the derivative representations by these authors and our final results are discussed in [6], as well as other formal aspects involved.…”
Section: Extended Derivative Dispersion Relationsmentioning
confidence: 78%