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Is the classical action for fermions grassman valued or real valued?

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Consider the classical action which appears in the exponent when calculating the amplitude of some scattering process using the path integral approach. For a theory with fermions, the fields are treated as classical anti-commuting variables: All fermionic terms in the action are constructed as the product of an even number of grassman variables in such a way that the action is a hermitian commuting number.

My question is the following: The product of an even number of grassman variables is never valued in the reals $\mathbb{R}$ (unless of course it is identically zero). It is valued in the grassman algebra. Does this mean that the action itself is valued in the grassman algebra? If so, then it seems to cause a problem in any theory which couples fermions to bosons: When extreemizing the action one would obtain equations of motion which involve both real valued terms as well as terms valued in the grassman algebra, and these terms must surely decouple from one another. As an example, consider a theory of gravity coupled to Dirac spinors. Varying the classical action with respect to the vierbein, one would obtain an Einstein equation with a stress energy tensor constructed from spinor bilinears. In other words, the left hand side of the Einstein equation would be real valued, while the right hand side would be valued in the grassman algebra. This doesn't seem to make sense so I must be misunderstanding something, but I don't quite see where.

1. Is my understanding correct that the classical action is constructed using grassman valued numbers, and is therefore valued in the grassman algebra and not the reals?

2. If the action is grassman valued, then what about the classical equations of motion? Are these grassman valued as well, and if so do the `grassman' and `real' parts necessarily decouple from one another? 

Any help you could give me would be greatly appreciated as I am pretty confused by this!

asked 5 days ago in Theoretical Physics by anonymous [ no revision ]
recategorized 4 days ago by Dilaton

1 Answer

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I don't fully understand Grassmann variables myself, but I think I can answer your question:

1. Yes, the action itself is Grassmann-valued. This is not as bad as it sounds, because in the path integral, we integrate over them, and we know how to do that with Grassmann variables. The action does not have to be real for the path integral to make sense.

In fact, bosonic fields take values in the Grassmann algebra as well. Bosonic values are always even elements of the algebra. For instance, when doing a Hubbard-Stratonovich transformation, we shift e.g. $\phi \to \phi + \overline{\psi}\psi$ where $\phi$ is a bosonic field and $\overline{\psi},\psi$ are fermionic fields. Clearly, this only makes sense when the field $\phi$ takes values in the Grassmann algebra, and is not just a real number.

For a mathematically precise review of Grassmann variables and integration, I found Terence Tao's blog post "Supercommutative gaussian integration, and the gaussian unitary ensemble" extremely helpful. This question is answered there as well.

2. In a path integral setting, the classical equations of motion are obtained by looking at the stationary points of the exponent. This makes sense when the exponent is real-valued, because we can argue that the integral is dominated by the contributions from the stationary points. Unfortunately, I don't know whether this argument still makes sense for Grassmann fields! After all, we cannot argue that the integrand has a maximum, because that assumes that the integrand is a real number which can be compared with other real numbers. I don't know how to justify it.

Of course, we can still formally write down the Euler-Lagrange equations. They now take values in the Grassmann algebra as well, and would need to be solved with this in mind. This has been done to obtain a classical variant of spin, e.g. in F.A. Berezin and S. Marinov, "Particle spin dynamics as the grassmann variant of classical mechanics" (1977). I am not sure how far this has been developed, I am unaware of any "serious" applications (and would love to be corrected on this).

answered 4 days ago by Greg Graviton (665 points) [ revision history ]
edited 1 hour ago by Greg Graviton

Just one small remark. The article about spin dynamics was written by Berezin and Marinov.

@DavidBarMoshe Corrected, thanks! I had copied the author information from the Springer page, but the latter was apparently not complete.

Two small comments:

1. The Lagrangian density and the action are even Grassmann valued, hence live in a commutative subalgebra of the noncommutative Grassmann algebra. This is conceptually important.

2. The concept of a stationary point still makes sense mathematically as it only requires a notion of differentiation with respect to a field, and not an order relation.

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