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I'm reading the book Basics of Thermal Field Theory also available on the authors webpage http://www.laine.itp.unibe.ch/basics.pdf

In the section 4.1 (Path integral for the partition function of a fermionic oscillator) they introduce Grassmann variables $c$ and $c^*$ that satisfy several properties, in particular

  • $c$, $c^*$ are treated as independent variables, like $x$, $p$.
  • $c^2=(c^*)^2$, $cc^*=-c^*c$
  • $c$, $c^*$ are defined to anticommute with $\hat a$, $\hat a ^\dagger$ as well.

These are classical analogs of fermionic creation and annihilation operators $\hat a$ and $\hat a ^\dagger$. To define the path integral (using classical fields $c(\tau)$ and $c^*(\tau)$) $$ \int \mathcal{D}c(\tau) \mathcal{D} c^*(\tau)e^{-\frac{1}{h}S} $$ of the fermionic harmonic oscillator they introduce coherent states $$ |c\rangle = e^{-c\hat a^\dagger} |0>. $$

So here $c$ plays a role of a "number". The only way I see how to make sense of this definition is to extend scalars of the Hilbert space: instead of two dimensional Hilbert space $H$ we consider Hilbert space over Grassmann algebra $A=\mathbb{C}<c, c^*>$ i.e. tensor product $H_A=A \otimes_\mathbb{C} H$, then fermionic coherent state is an element of $H_A$, but not an element of $H$.

So, for quantisation of fermions we need to extend scalars of the Hilbert space from $\mathbb{C}$ to Grassmann numbers $A$. Is that correct?

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    $\begingroup$ Related: physics.stackexchange.com/q/40746/2451 and links therein. $\endgroup$ – Qmechanic Nov 19 '16 at 20:49
  • $\begingroup$ Hi Alex, I removed your last resource recommendation subquestion, cf. this meta post. $\endgroup$ – Qmechanic Nov 19 '16 at 20:51
  • $\begingroup$ They certainly insist that the cs are not operators (matrices); they do not envision them as 2x2 matrices! $\endgroup$ – Cosmas Zachos Nov 19 '16 at 21:26
  • $\begingroup$ Not sure; see if it is consistent, i.e. picking up a - sign when slipping past the matrix. It is evident they are replicating coherent states of sorts, so the eigenvalue of a fermion annihilation op has to be fermionic, and the two fermionic objects must anti commute. $\endgroup$ – Cosmas Zachos Nov 19 '16 at 21:49
  • $\begingroup$ I do not imply that. My comment about division ring was a response to an earlier version of the post. $\endgroup$ – Qmechanic Nov 20 '16 at 17:37
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I know nothing about supernumbers, but the construction that you mention for the Fermi oscillator looks easy to formalize.

On the wikipedia page, they say that the set of polynomials in $n$ Grassmann generators can be identified with the exterior algebra of a linear space, and in the case of complex Grassmann number we should take a space on the complex one. Actually, I think that this is a bit imprecise, since in quantum field theory we want the $\theta$'s and $\theta^*$ 's to be two independent set of Grassmann generators. In fact, everything works out if we identify the set of Grassmann polynomials with the covariant exterior algebra: $$\Lambda _{\bullet}(V\oplus V^*),$$ where $V$ and $V^*$ are two complex anti-isomorphic vector spaces (I have worked out this by myself, so please correct me if I'm wrong).

In any case, this is not the real point of the question. Suppose that you have a set of Grassmann numbers $\mathscr G$ generated by two elements $\lbrace \theta,\theta ^* \rbrace$. We want to make sense of an expression such as $P(\theta,\theta ^*) \vert \alpha \rangle$, and we can do this in the same way which allows us to multiply a real vector by a complex scalar: tensor product.

If the "physical" Hilbert $\mathcal H$ space consists of vectors: $$\vert \rangle = \alpha \vert 0 \rangle + \beta \vert 1\rangle,$$where $\alpha,\beta$ are ordinary complex numbers, we define a vector space $\mathcal H' =\mathscr G \otimes \mathcal H $. The multiplication by Grassmann numbers can be defined on decomposable tensors by: $$Q (P \otimes \vert \rangle)=(QP )\otimes \vert \rangle$$and extended by linearity on the whole space $\mathcal H '$. In particular, the old $\mathcal H$ can be seen as the subspace spanned by the elements $1\otimes \vert \rangle$, and the multiplication by the scalar $\lambda$ in $\mathcal H$ agrees with the multiplication by the "Grassmann number" $\lambda$ on $\mathcal H '$.

All other things are just formal manipulations, plus some ad-hoc definition, for example to make sense of the conjugation $P\vert \rangle \to \langle \vert P^*$. For example, you can introduce the "coherent state" $$\vert \theta \rangle = \vert 0\rangle + \theta \vert 1\rangle,$$ which is an eigenvector of $a\equiv\text {id}_{\mathscr G} \otimes a$ :$$a\vert \theta \rangle = \theta \vert \theta \rangle,$$ which may be the reason why your book is introducing Grassmann numbers.

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  • $\begingroup$ In the comments I proposed the same idea: Hilbert spaces for fermions are not over $\mathbb{C}$, but over Grassman algebra by extension of scalars. It looks like a reasonable interpretation, but I be happier if I see a reference with clear explanation of this point as "standard" for quantisation of fermi fields. $\endgroup$ – Alex Nov 19 '16 at 22:46
  • $\begingroup$ Hi Alex, all the books I have seen intuitively multiply vectors by anticommuting numbers without any further comment, so I can't help you. This is my personal way of making sense of it, and I can't see any difficulty with it, but I understand that you'd like to see a "standardized" treatment. You might try to read Swanson, "Path integrals and quantum processes", which has a quite extensive section on the subject, but doesn't go into these (a bit tedious) details. Hope this helps $\endgroup$ – pppqqq Nov 19 '16 at 22:54

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