1997
DOI: 10.1103/physrevd.55.5295
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Analytic perturbation theory in QCD and Schwinger’s connection between theβfunction and the spectral density

Abstract: We argue that a technique called analytic perturbation theory leads to a well-defined method for analytically continuing the running coupling constant from the spacelike to the timelike region, which allows us to give a selfconsistent definition of the running coupling constant for timelike momentum.The corresponding β-function is proportional to the spectral density, which confirms a hypothesis due to Schwinger.

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Cited by 128 publications
(243 citation statements)
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“…(11) hereinafter, which makes Eq. (10) identical to that of both the foregoing DPT [31][32][33][34] and the so-called analytic perturbation theory 2 (APT) [54][55][56][57]. It has to be noted that, in general, the perturbative spectral function at small values of its argument may be altered by the terms of an intrinsically nonperturbative nature.…”
Section: R-ratio Of Electron-positron Annihilation Into Hadronsmentioning
confidence: 99%
See 1 more Smart Citation
“…(11) hereinafter, which makes Eq. (10) identical to that of both the foregoing DPT [31][32][33][34] and the so-called analytic perturbation theory 2 (APT) [54][55][56][57]. It has to be noted that, in general, the perturbative spectral function at small values of its argument may be altered by the terms of an intrinsically nonperturbative nature.…”
Section: R-ratio Of Electron-positron Annihilation Into Hadronsmentioning
confidence: 99%
“…[120] and only afterwards was derived in Refs. [9,10,12,54,55]. Figure 3A displays the one-loop "timelike" effective couplant a (1) TL (s) (17) and the "naive" continuation of the oneloop perturbative couplant a (1) s (Q 2 ) (13) into the timelike domain (12).…”
Section: Figmentioning
confidence: 99%
“…We emphasize that in this approach, the higher order quantities A k (µ 2 ) (k ≥ 2) are not as basic, they are defined via Eqs. (26) for convenience of having closer notational analogy with pQCD formulas (and a k ↔ A k ). In these definitions (26), as well as in β j -running Eqs.…”
Section: Analytization Of Higher Powers Of the Coupling Parametermentioning
confidence: 99%
“…(27) are, in contrast to Eqs. (26), not definitions, but in general approximations for the evolution under RSch-changes. The RSch-dependence of A 1 (µ 2 ) is treated in more detail later in this work.…”
Section: Analytization Of Higher Powers Of the Coupling Parametermentioning
confidence: 99%
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