Geodesic
Chiral bosonization of $U_A(1)$-currents and the energy-momentum tensor in quantum chromodynamics
Zapiski Nauchnykh Seminarov POMI, Questions of quantum field theory and statistical physics. Part 13, Tome 224 (1995), pp. 55-67 
A. A. Andrianov; V. A. Andrianov; V. L. Yudichev. Chiral bosonization of $U_A(1)$-currents and the energy-momentum tensor in quantum chromodynamics. Zapiski Nauchnykh Seminarov POMI, Questions of quantum field theory and statistical physics. Part 13, Tome 224 (1995), pp. 55-67. http://geodesic.mathdoc.fr/item/ZNSL_1995_224_a5/
@article{ZNSL_1995_224_a5,
     author = {A. A. Andrianov and V. A. Andrianov and V. L. Yudichev},
     title = {Chiral bosonization of $U_A(1)$-currents and the energy-momentum tensor in quantum chromodynamics},
     journal = {Zapiski Nauchnykh Seminarov POMI},
     pages = {55--67},
     year = {1995},
     volume = {224},
     language = {ru},
     url = {http://geodesic.mathdoc.fr/item/ZNSL_1995_224_a5/}
}
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Voir la notice du chapitre de livre provenant de la source Math-Net.Ru

A generalization of the chiral Lagrangian is obtained by extended low-temperature bosonization of vector, axial vector, scalar, and pseudoscalar $U(3)$ quark currents. Estimates for its structural constants are given in accordance with the developed AANN model of QCD-bosonization. Following the ideology of chiral perturbation theory, we transform the bosonized chiral Lagrangian into the phenomenological form. Relations of Zweig-rule type are established. This enables us to express the new structural constants in terms of the given constants. The correspondence between the predictions obtained by the low-temperature bosonozation method and available phenomenological estimates are discussed. Bibliography: 9 titles.