where the last addend corresponds to the Wilson term again. It modifies the mass of the doublers to
where is the number of momentum components with . In the continuum limit
the doublers become very heavy and decouple from the theory.
Wilson fermions do not contradict the Nielsen–Ninomiya theorem because they explicitly violate chiral symmetry since the Wilson term does not anti-commute with .
↑
Rothe, Heinz J. (2005). "4 Fermions on the lattice". Lattice Gauge Theories: An Introduction. World Scientific Lecture Notes in Physics (3rded.). World Scientific Publishing. pp.56–57. ISBN978-9814365857.
↑
Gattringer, C.; Lang, C.B. (2009). "5 Fermions on the lattice". Quantum Chromodynamics on the Lattice: An Introductory Presentation. Lecture Notes in Physics. Vol.788. Springer. pp.112–114. doi:10.1007/978-3-642-01850-3. ISBN978-3642018497.