2020
DOI: 10.1088/1674-1137/ababf8
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Logarithmic Regge pole

Abstract: This work presents the subtraction procedure and the Regge cut in the logarithmic Regge pole approach. The subtraction mechanism leads to the same asymptotic behavior as previously obtained in the non-subtraction case. The Regge cut, in contrast, introduces a clear role to the non-leading contributions for the asymptotic behavior of the total cross-section. From these results, some simple parameterization is introduced to fit the experimental data for the proton-proton and antiproton-proton total cross-section… Show more

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Cited by 5 publications
(12 citation statements)
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References 39 publications
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“…For the results expressed by (ii), on the other hand, one has that ∆ tot (s) does not obey the Pomeranchuk theorem, unless c p = c p . The last results given by (iii) seems to be reasonable under the lights of the experimental data, representing a Pomeron intercept α P = 1 [8].…”
Section: Asymptotic Behavior Of Total Cross Section and ρ-Parametersupporting
confidence: 68%
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“…For the results expressed by (ii), on the other hand, one has that ∆ tot (s) does not obey the Pomeranchuk theorem, unless c p = c p . The last results given by (iii) seems to be reasonable under the lights of the experimental data, representing a Pomeron intercept α P = 1 [8].…”
Section: Asymptotic Behavior Of Total Cross Section and ρ-Parametersupporting
confidence: 68%
“…where f ± (s, 0) ≡ f ± (s), and k is the subtraction constant. Without loss of generality, one adopts k = 0 since the influence of such parameter is restricted to the low energy domain [8]. Notice the addition of high-order derivative terms in equations (2) may turn this representation more sensitive to describe high-energy experimental data.…”
Section: Asymptotic Behavior Of Total Cross Section and ρ-Parametermentioning
confidence: 99%
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“…Recently, a novel theoretical approach for the leading Regge pole was introduced [65,66]. In that approach, the leading Regge pole can be represented by the logarithmic of the collision energy, which means this representation agrees with the Froissart-Martin bound.…”
Section: Total Cross Sectionmentioning
confidence: 91%
“…Now, one needs the input for the total cross section. In the intermediate energy range, one can use the following simple parameterization for the total cross section [27] σ tot (s) = a 1 (s/s 0 ) a2 + a 3 ln α P (0) (s/s 0 ),…”
Section: Total Cross Sectionmentioning
confidence: 99%