Abstract
We review some theoretical and phenomenological aspects of the scenario in which the spontaneous breaking of chiral symmetry is not triggered by a formation of a large condensate \(\left\langle {\bar qq} \right\rangle \). Emphasis is put on the resulting pattern of light quark masses, on the constraints arising from QCD sum rules and on forthcoming experimental tests.
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Stern, J. (1998). Light quark masses and condensates in QCD. In: Bernstein, A.M., Drechsel, D., Walcher, T. (eds) Chiral Dynamics: Theory and Experiment. Lecture Notes in Physics, vol 513. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0104896
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DOI: https://doi.org/10.1007/BFb0104896
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