TY - JOUR
T1 - Gravitational anomalies
AU - Alvarez-Gaumé, Luis
AU - Witten, Edward
N1 - Funding Information:
1 Research supported in part by the National Science Foundation under grant no. PHY-82-15249. 2 Research supported in part by the National Science Foundation under grant no. PHY-80-19754.
PY - 1984/4/2
Y1 - 1984/4/2
N2 - It is shown that in certain parity-violating theories in 4k+2 dimensions, general covariance is spoiled by anomalies at the one-loop level. This occurs when Weyl fermions of spin- 1 2 or -3 2 or self-dual antisymmetric tensor fields are coupled to gravity. (For Dirac fermions there is no trouble.) The conditions for anomaly cancellation between fields of different spin is investigated. In six dimensions this occurs in certain theories with a fairly elaborate field content. In ten dimensions there is a unique theory with anomaly cancellation between fields of different spin. It is the chiral n = 2 supergravity theory, which is the low-energy limit of one of the superstring theories. Beyond ten dimensions there is no way to cancel anomalies between fields of different spin.
AB - It is shown that in certain parity-violating theories in 4k+2 dimensions, general covariance is spoiled by anomalies at the one-loop level. This occurs when Weyl fermions of spin- 1 2 or -3 2 or self-dual antisymmetric tensor fields are coupled to gravity. (For Dirac fermions there is no trouble.) The conditions for anomaly cancellation between fields of different spin is investigated. In six dimensions this occurs in certain theories with a fairly elaborate field content. In ten dimensions there is a unique theory with anomaly cancellation between fields of different spin. It is the chiral n = 2 supergravity theory, which is the low-energy limit of one of the superstring theories. Beyond ten dimensions there is no way to cancel anomalies between fields of different spin.
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U2 - 10.1016/0550-3213(84)90066-X
DO - 10.1016/0550-3213(84)90066-X
M3 - Article
AN - SCOPUS:0010190678
SN - 0550-3213
VL - 234
SP - 269
EP - 330
JO - Nuclear Physics, Section B
JF - Nuclear Physics, Section B
IS - 2
ER -