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Majorana and Majorana-Weyl fermions in lattice gauge theory

Teruaki Inagaki1 and Hiroshi Suzuki2

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In various dimensional euclidean lattice gauge theories, we examine a compatibility of the Majorana decomposition and the charge conjugation property of lattice Dirac operators. In 8n and 1+8n dimensions, we find a difficulty to decompose a classical lattice action of the Dirac fermion into a system of the Majorana fermion and thus to obtain a factrized form of the Dirac determinant. Similarly, in 2+8n dimensions, there is a difficulty to decompose a classical lattice action of the Weyl fermion into a system of the Majorana-Weyl fermion and thus to obtain a factrized form of the Weyl determinant. Prescriptions based on the overlap formalism do not remove these difficulties. We argue that these difficulties are reflections of the global gauge anomaly associated to the real Weyl fermion in 8n dimensions. For this reason (besides other well-known reasons), a lattice formulation of the N = 1 super Yang-Mills theory in these dimensions is expected to be extremely difficult to find.


Keywords

Lattice Gauge Field Theories

Anomalies in Field and String Theories

Field Theories in Lower Dimensions

Field Theories in Higher Dimensions

 

E-print Number: hep-lat/0406026

Cited: by |

Refers: to

PACS

11.15.Ha Lattice gauge theory

11.10.Kk Field theories in dimensions other than four

11.30.Er Charge conjugation, parity, time reversal, and other discrete symmetries

11.25.-w Strings and branes

Subjects

Particle physics and field theory

Dates

Issue 07 (July 2004)

Received 17 June 2004, accepted for publication 16 July 2004

Published 11 August 2004



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