Abstract
This chapter presents the most important notions and examples of the theory of operator algebras. These are then used to formulate the basic principles of quantum field theory and some examples of algebraic QFTs.
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Notes
- 1.
In general, a v. Neumann algebra is isomorphic to a v. Neumann algebra in standard form if it has a faithful representation which in turn is the case if it has a faithful normal state, i.e. a normal state such that \(\omega (a^*a) = 0\) implies \(a=0\). In the following, we will always assume that this is the case.
- 2.
It is understood here that b acts on \( \langle \psi |\) in \(\bar{\mathbb {C}}^N\) by \(b \langle \psi | \equiv \langle b^* \psi |\).
- 3.
As a vector space, the graded tensor product is first defined to be the usual (algebraic) tensor product. The product is defined as \((a_1 \hat{\otimes }b_1)(a_2 \hat{\otimes }b_2)= (-1)^{deg(a_2)deg(b_1)} \, a_1 a_2 \hat{\otimes }b_1 b_2\) and the *-operation is \((a \hat{\otimes }b)^* = (-1)^{deg(a)deg(b)} a^* \hat{\otimes }\ b^*\), where the degree is defined to be 0 resp. 1 for even resp. odd elements under \(\alpha \). It is then shown that a natural \(C^*\)-norm compatible with these relations and the above isomorphism can be defined which extends the \(C^*\)-norm of \({\mathfrak C}(K_i, \Gamma _i)\). The graded tensor product is the \(C^*\)-closure under this norm.
- 4.
The covering group is needed to describe non-integer spin.
- 5.
In terms of algebras:
$$ \pi _0(\mathfrak {A}) = \left( \bigcup _{x \in \mathbb {R}^{d,1}} \pi _0(\mathfrak {A}(O+x)) \right) '' $$for any causal diamond O.
- 6.
If there are none, then the norm is set to infinity.
- 7.
Here the braces denote “generated by, as a \(C^*\)-algebra”, and \(\mathrm{supp}(F)=\mathrm{supp}(q)\cup \mathrm{supp}(p)\), where the support \(\mathrm{supp}\) of a function is the closure of the set of all points where it does not vanish.
- 8.
Our convention for the Fourier transform in one dimension is \(\widetilde{f}(p) = \frac{1}{\sqrt{2\pi }} \int \mathrm{d}x f(x) e^{-ipx}\).
- 9.
In our setup, we arrive at the normalization
$$\begin{aligned}{}[a(\mathbf{k}), a^\dagger (\mathbf{k}')] = 2\omega (\mathbf{k}) \ \delta ^d(\mathbf{k}-\mathbf{k}') \cdot 1 \ , \quad [a(\mathbf{k}), a(\mathbf{k}')] = 0 . \end{aligned}$$(2.37) - 10.
The complex conjugate, \(\bar{V}\), of a vector space V is identical as a set, but has the scalar multiplication \(\lambda \cdot v \equiv \bar{\lambda } v\).
- 11.
Apart from the value m of the mass of the basic particle.
- 12.
I.e., it satisfies the relations of the permutation group.
- 13.
Informally, \(z^\dagger (\theta ) = z(\theta )^*\).
- 14.
J turns out to be equal to the modular conjugation associated with the algebra \(\mathfrak {R}\) defined below.
- 15.
- 16.
One sometimes requires that the symmetry algebra of the net is the full Virasoro algebra, i.e. that the net contains the algebra of quantized diffeomorphisms as a subnet. Then the split property is automatic [43].
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Hollands, S., Sanders, K. (2018). Formalism for QFT. In: Entanglement Measures and Their Properties in Quantum Field Theory. SpringerBriefs in Mathematical Physics, vol 34. Springer, Cham. https://doi.org/10.1007/978-3-319-94902-4_2
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