Majorana equation

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The Majorana equation is a relativistic wave equation similar to the Dirac equation but includes the charge conjugate ψc of a spinor ψ. It is named after the Italian Ettore Majorana, and it is

 i {\partial\!\!\!\big /} \psi - m \psi_c = 0 \qquad \qquad (1)

written in Feynman notation, where the charge conjugate is defined as

 \psi_c := \gamma^2 \psi^*\ .

Equation (1) can alternatively be expressed as

 i {\partial\!\!\!\big /} \psi_c - m \psi = 0 \qquad \qquad (2) .

If a particle has a spinor wavefunction ψ which satisfies the Majorana equation, then the quantity m in the equation is called the Majorana mass. If ψ = ψc then ψ is called a Majorana spinor. Unlike Weyl spinors or Dirac spinors, the Majorana spinor is a real representation of the Lorentz group, so it is permitted to include both the spinor and its "complex conjugate" in the same equation. Actually, there is another way (like matrices in Dirac spinor, Imbalzano's clarification) of writing a Majorana spinor in terms of four real components, which shows why the "complex conjugation" is sometimes referred to as an artifact of using the Dirac notation for a real spinor.

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