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Recently, there have been reports that the chirally restored phase of QCD iseffectively symmetric under $U(N_f) \times U(N_f)$ rather than $SU(N_f)\timesSU(N_f)$. We supplement their argument by including the contributions fromtopologically nontrivial gauge field configurations and discuss how theconclusions are modified. General statements are made concerning the particlespectrum of QCD with light $N_f$ flavors in the high temperature chirallyrestored phase.Comment: 6 pages, no figures, revte

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">U</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">A</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>(1) symmetry restoration in QCD with<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="italic">N</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">f</mml:mi></mml:mrow></…

UA(1) symmetry restoration in QCD withNf