Standard

Hadronic string, conformal invariance and chiral symmetry. / Alfaro, J.; Balart, L.; Andrianov, A. A.; Espriu, D.

In: International Journal of Modern Physics A, Vol. 18, No. 14, 10.06.2003, p. 2501-2539.

Research output: Contribution to journalArticlepeer-review

Harvard

Alfaro, J, Balart, L, Andrianov, AA & Espriu, D 2003, 'Hadronic string, conformal invariance and chiral symmetry', International Journal of Modern Physics A, vol. 18, no. 14, pp. 2501-2539. https://doi.org/10.1142/S0217751X03013922

APA

Alfaro, J., Balart, L., Andrianov, A. A., & Espriu, D. (2003). Hadronic string, conformal invariance and chiral symmetry. International Journal of Modern Physics A, 18(14), 2501-2539. https://doi.org/10.1142/S0217751X03013922

Vancouver

Alfaro J, Balart L, Andrianov AA, Espriu D. Hadronic string, conformal invariance and chiral symmetry. International Journal of Modern Physics A. 2003 Jun 10;18(14):2501-2539. https://doi.org/10.1142/S0217751X03013922

Author

Alfaro, J. ; Balart, L. ; Andrianov, A. A. ; Espriu, D. / Hadronic string, conformal invariance and chiral symmetry. In: International Journal of Modern Physics A. 2003 ; Vol. 18, No. 14. pp. 2501-2539.

BibTeX

@article{0f1671b7a51a4062933d23d98dc9775a,
title = "Hadronic string, conformal invariance and chiral symmetry",
abstract = " While it is clear that in some kinematic regime QCD can be described by an effective (as opposed to fundamental) string theory, it is not at all clear how this string theory should be. The {"}natural{"} candidate, the bosonic string, leads to amplitudes with the usual problems related to the existence of the tachyon, the absence of the adequate Adler zero, and massless vector particles, not to mention the conformal anomaly. The supersymmetric version does not really solve most of these problems. For a long time it has been believed that the solution of at least some of these difficulties is associated to a proper identification of the vacuum, but this program has remained elusive. We show in this work how the first three problems can be avoided, by using a sigma model approach where excitations above the correct (chirally noninvariant) QCD vacuum are identified. At the leading order in a derivative expansion we recover the nonlinear sigma model of pion interactions. At the next-to-leading order the O(p 4 ) Lagrangian of Gasser and Leutwyler is obtained, with values for the coefficients that match the observed values. We also discuss some issues related to the conformal anomaly. ",
keywords = "Chiral symmetry breaking, Conformal invaxiance, Effective chiral Lagrangian, Hadronic string",
author = "J. Alfaro and L. Balart and Andrianov, {A. A.} and D. Espriu",
year = "2003",
month = jun,
day = "10",
doi = "10.1142/S0217751X03013922",
language = "English",
volume = "18",
pages = "2501--2539",
journal = "International Journal of Modern Physics A",
issn = "0217-751X",
publisher = "WORLD SCIENTIFIC PUBL CO PTE LTD",
number = "14",

}

RIS

TY - JOUR

T1 - Hadronic string, conformal invariance and chiral symmetry

AU - Alfaro, J.

AU - Balart, L.

AU - Andrianov, A. A.

AU - Espriu, D.

PY - 2003/6/10

Y1 - 2003/6/10

N2 - While it is clear that in some kinematic regime QCD can be described by an effective (as opposed to fundamental) string theory, it is not at all clear how this string theory should be. The "natural" candidate, the bosonic string, leads to amplitudes with the usual problems related to the existence of the tachyon, the absence of the adequate Adler zero, and massless vector particles, not to mention the conformal anomaly. The supersymmetric version does not really solve most of these problems. For a long time it has been believed that the solution of at least some of these difficulties is associated to a proper identification of the vacuum, but this program has remained elusive. We show in this work how the first three problems can be avoided, by using a sigma model approach where excitations above the correct (chirally noninvariant) QCD vacuum are identified. At the leading order in a derivative expansion we recover the nonlinear sigma model of pion interactions. At the next-to-leading order the O(p 4 ) Lagrangian of Gasser and Leutwyler is obtained, with values for the coefficients that match the observed values. We also discuss some issues related to the conformal anomaly.

AB - While it is clear that in some kinematic regime QCD can be described by an effective (as opposed to fundamental) string theory, it is not at all clear how this string theory should be. The "natural" candidate, the bosonic string, leads to amplitudes with the usual problems related to the existence of the tachyon, the absence of the adequate Adler zero, and massless vector particles, not to mention the conformal anomaly. The supersymmetric version does not really solve most of these problems. For a long time it has been believed that the solution of at least some of these difficulties is associated to a proper identification of the vacuum, but this program has remained elusive. We show in this work how the first three problems can be avoided, by using a sigma model approach where excitations above the correct (chirally noninvariant) QCD vacuum are identified. At the leading order in a derivative expansion we recover the nonlinear sigma model of pion interactions. At the next-to-leading order the O(p 4 ) Lagrangian of Gasser and Leutwyler is obtained, with values for the coefficients that match the observed values. We also discuss some issues related to the conformal anomaly.

KW - Chiral symmetry breaking

KW - Conformal invaxiance

KW - Effective chiral Lagrangian

KW - Hadronic string

UR - http://www.scopus.com/inward/record.url?scp=0037502733&partnerID=8YFLogxK

U2 - 10.1142/S0217751X03013922

DO - 10.1142/S0217751X03013922

M3 - Article

AN - SCOPUS:0037502733

VL - 18

SP - 2501

EP - 2539

JO - International Journal of Modern Physics A

JF - International Journal of Modern Physics A

SN - 0217-751X

IS - 14

ER -

ID: 39933456