1970
DOI: 10.1002/prop.19700180104
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πN Partial Wave Relations from Fixed-t Dispersion Relations

Abstract: Starting from fixed‐t dispersion relations we derive a set of relations for the πN partial wave amplitudes, generalizing previous work of OEHME [1], CAPPS and TAKEDA [2], and CHEW, GOLDBERGER, LOW and NAMBU [3]. Our relations contain a single integral kernel, which is agiven in a closed form valid for arbitrary angular momentum. This kernel correlates the imaginary parts of all partial wave amplitudes with the partial wave amplitude under consideration. The partial wave relations give the correct threshold beh… Show more

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Cited by 38 publications
(13 citation statements)
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“…Even more, HDRs are the unique choice if one demands that the curves pass through all kinematic channels, avoid double-spectral regions, do not introduce ostensible kinematic cuts into the partial-wave amplitudes, and still yield manageable kernel functions[107]. In view of the efforts[107,[189][190][191]] that led to s-channel PWDRs for πN scattering and thus provided the first step towards the construction of a Roy-equation analog for processes with πN crossing properties, the resulting full system of partial-wave hyperbolic dispersion relations is referred to as Roy-Steiner equations.…”
mentioning
confidence: 99%
“…Even more, HDRs are the unique choice if one demands that the curves pass through all kinematic channels, avoid double-spectral regions, do not introduce ostensible kinematic cuts into the partial-wave amplitudes, and still yield manageable kernel functions[107]. In view of the efforts[107,[189][190][191]] that led to s-channel PWDRs for πN scattering and thus provided the first step towards the construction of a Roy-equation analog for processes with πN crossing properties, the resulting full system of partial-wave hyperbolic dispersion relations is referred to as Roy-Steiner equations.…”
mentioning
confidence: 99%
“…Similar dispersive analyses have also been carried out for πN [124,149,150,[155][156][157], γ ( * ) γ ( * ) → ππ [158][159][160][161][162], e + e − → π + π − [163], γπ → ππ [164,165] and γK → πK [166]. The approach for obtaining rigorous and precise poles from dispersively constrained data fits, is also well-suited for the recent lattice calculations that we hope may shed further light on these issues.…”
Section: Cfd I=1 P-wavementioning
confidence: 84%
“…2.2. For the sake of completeness and convenience, in Appendix A the different contributions to (3.4) will be discussed along the lines of [21,[46][47][48] (correcting several typographical errors, adjusting the conventions, and partially extending the presentation therein at the same time).…”
Section: Partial-wave Hyperbolic Dispersion Relationsmentioning
confidence: 99%