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Advances in High Energy Physics
Volume 2015 (2015), Article ID 803232, 4 pages
http://dx.doi.org/10.1155/2015/803232
Research Article

Scalar Form Factor of the Pion in the Kroll-Lee-Zumino Field Theory

1Centre for Theoretical & Mathematical Physics and Department of Physics, University of Cape Town, Rondebosch 7700, South Africa
2Instituto de Física, Pontificia Universidad Católica de Chile, Casilla 306, 22 Santiago, Chile

Received 28 August 2014; Accepted 4 January 2015

Academic Editor: Alexey A. Petrov

Copyright © 2015 C. A. Dominguez et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The publication of this article was funded by SCOAP3.

Abstract

The renormalizable Kroll-Lee-Zumino field theory of pions and a neutral rho-meson is used to determine the scalar form factor of the pion in the space-like region at next-to-leading order. Perturbative calculations in this framework are parameter-free, as the masses and the rho-pion-pion coupling are known from experiment. Results compare favorably with lattice QCD calculations.

1. Introduction

The scalar form factor of the pion [1, 2], and particularly its quadratic radius, plays an important role in chiral perturbation theory (CHPT) [3, 4]. This form factor is defined as the pion matrix element of the QCD scalar current ; that is, where . The associated quadratic scalar radius is given by where is the pion sigma term

The scalar radius fixes , one of the low energy constants of CHPT, through the relation where  MeV is the physical pion decay constant [5]. The low energy constant , in turn, determines the leading contribution in the chiral expansion of the pion decay constant; that is, where is the pion decay constant in the chiral limit.

This scalar form factor is not accessible experimentally, but it has been determined from lattice QCD (LQCD) [68], or hadronic models [9, 10].

Theoretically, the ideal tool to study this form factor, independently from LQCD, is the Kroll-Lee-Zumino Abelian renormalizable field theory of pions and a neutral -meson [11, 12]. This provides the appropriate field theory platform for the phenomenological vector meson dominance (VMD) model [13, 14], allowing for a systematic calculation of higher order quantum corrections ([15], this paper, has a misprint in equation (15) (the sign of the first term in curly brackets should be negative), with the remaining equations being correct. The electromagnetic square radius of the pion quoted in the paper is incorrect; the correct value is  fm2, in much better agreement with data than naive (single ) VMD.) [16]. Due to the renormalizability of the theory, predictions are parameter-free, as the strong coupling, , is known from experiment. In spite of this coupling being a strong interaction quantity, perturbative calculations in the scheme make sense because the effective expansion parameter turns out to be .

The KLZ theory has been used to compute the next-to-leading order (NLO) correction to the tree level (VMD) electromagnetic form factor of the pion in the space-like region with very good results [15]. In fact, it agrees with data up to  GeV2 with a chi-squared per degree of freedom , as opposed to VMD which gives . In addition, the mean-squared radius at NLO is  fm2, compared with the experimental result [5]  fm2, and the VMD value  fm2.

In this note we compute in this framework the scalar form factor of the pion at NLO in the space-like region and compare with current results from LQCD.

The KLZ Lagrangian is given by where is a vector field describing the meson (), is a complex pseudoscalar field describing the mesons, is the usual field strength tensor: , and is the current: . In spite of the explicit presence of the mass term in the Lagrangian, the theory is renormalizable because the neutral vector meson is coupled to a conserved current [11, 12]. Figures 1 and 2 show, respectively, the LO and the NLO diagrams, where the cross indicates the coupling of the current to the two pions. Notice that while the Lagrangian (6) contains a quartic coupling, this term only contributes in this application at NNLO and beyond.

Figure 1: Leading order (LO) contribution to the scalar form factor of the pion. The cross indicates the coupling of the scalar current to two pions.
Figure 2: Next-to-leading order (NLO) contribution to the scalar form factor.

Using the Feynman propagator for the -meson, and in dimensions, the unrenormalized vertex function in Figure 2 in dimensional regularization is given by where is defined as

In the scheme and renormalizing the vertex function at the point , the NLO contribution in Figure 2 is [16] with

For details on the renormalization procedure for the fields, masses, and coupling, see [15]. The result of a numerical evaluation of (9), using from the measured width of the -meson [5], is shown in Figure 3. Regarding the scalar radius, defined in (2), we confirm the NLO result obtained in [16] with a negligible error due to the strong coupling.

Figure 3: The normalized scalar form factor (8), to NLO in the space-like region.

This value is smaller than typical values in the literature [610]. However, it must be kept in mind that the NLO result is expected to be a lower bound; that is, with , the NNLO would reduce , thus increasing the radius. A rough order of magnitude estimate of the size of the NNLO contribution suggests a correction of some 20% to the NLO term (the NNLO calculation is quite formidable and beyond the scope of this note). This is obtained by estimating a typical two-loop diagram, for example, the -meson propagator at NNLO and comparing it with the NLO result. The Feynman integrals in the variables at NLO and NNLO are of order in the range explored here. We find the total contribution from this diagram to be over 20% of the NLO, thus increasing the radius to  fm2. It should be clear that this result (11) would be affected by (unknown) systematic uncertainties arising, for example, from hadronic contributions from fields absent from the KLZ Lagrangian (6).

A comparison of the KLZ form factor itself at low  GeV2 with LQCD results read from figures in [6, 8] shows good agreement. It should be mentioned, though, that LQCD results from [6] are for light-quark masses in the range from to , while those from [8] are for  MeV. These LQCD determinations find values for the scalar radius higher than in this analysis (11); that is,  fm2 from [6] and  fm2 from [8]. These results for the radius are determined from, for example, chiral extrapolations to the physical pion mass. Our results for the form factor are also in agreement within less than 10% with a CHPT calculation [17] in the range  GeV2. Regarding potential contributions to the form factor and its radius, for example, from other scalar degrees of freedom absent from the KLZ Lagrangian, they should be understood as part of the systematic uncertainties. The excellent agreement with data of KLZ results for the electromagnetic pion form factor [15] might be a result of the absence of other hadronic contributions with the same quantum numbers as the neutral -meson. In the case of the scalar form factor, these additional contributions are potentially present, and thus could become part of the systematic uncertainties.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was supported in part by FONDECyT (Chile) under Grants 1130056 and 1120770, by NRF (South Africa), and by the University of Cape Town URC. The authors wish to thank Gary Tupper for valuable discussions on KLZ and Hartmut Wittig for enlightening exchanges on LQCD.

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