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Classically, this implies that the chiral current, is conserved, .
Quantum mechanically, the chiral current is not conserved: Jackiw discovered this due to the non-vanishing of a triangle diagram. Fujikawa reinterpreted this as a change in the partition function measure under a chiral transformation. To calculate a change in the measure under a chiral transformation, first consider the Dirac fermions in a basis of eigenvectors of the Dirac operator:
The transformation of the coefficients are calculated in the same manner. Finally, the quantum measure changes as
where the Jacobian is the reciprocal of the determinant because the integration variables are Grassmannian, and the 2 appears because the a's and b's contribute equally. We can calculate the determinant by standard techniques:
to first order in ?(x).
Specialising to the case where ? is a constant, the Jacobian must be regularised because the integral is ill-defined as written. Fujikawa employed heat-kernel regularization, such that
( can be re-written as , and the eigenfunctions can be expanded in a plane-wave basis)
after applying the completeness relation for the eigenvectors, performing the trace over ?-matrices, and taking the limit in M. The result is expressed in terms of the field strength 2-form,
This result is equivalent to Chern class of the -bundle over the d-dimensional base space, and gives the chiral anomaly, responsible for the non-conservation of the chiral current.
K. Fujikawa and H. Suzuki (May 2004). Path Integrals and Quantum Anomalies. Clarendon Press. ISBN0-19-852913-9.
S. Weinberg (2001). The Quantum Theory of Fields. Volume II: Modern Applications.. Cambridge University Press. ISBN0-521-55002-5.