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QJT is considered as a regularization of QFT, where the fields are replacedby finite $p$-jets. The regularized phase space is infinite-dimensional,because not all histories are determined by initial conditions. Gaugesymmetries are not fully preserved by the regularization, and gauge anomaliesarise. These anomalies are of a new type, not present in QFT. They genericallydiverge when the regulator is removed, but can be made finite with a particularchoice of field content, provided that spacetime has at most four dimensions.The field content appears to include unphysical fields that violate thespin-statistics theorem.

QJT as a Regularization: Origin of the New Gauge Anomalies