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Part of the book series: Latin American Mathematics Series ((LAMSUFSC))

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Abstract

Chapter 2 explains the algebraic approach to quantum statistical mechanics in the (very) simple case of finite quantum systems. Here, we extend this approach to a large class of infinitely extended (infinite-dimensional) quantum systems that are homogeneous in space. The physical interactions considered in this chapter are short-range, in a sense, that is, they do not contain additional mean-field interaction terms, this kind of long-range interactions being the subject of Chap. 6. Crucial phenomenological aspects of thermodynamic equilibrium of infinite systems, like existence of first-order phase transitions and spontaneous symmetry breaking, can be derived in the short-range setting, as simple corollaries of classical (deep) results of convex analysis. In this chapter, we additionally contribute a brief introduction to the mathematical foundations of the Hartree-Fock theory, which is very popular in molecular and condensed matter physics.

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Notes

  1. 1.

    We adopt this terminology, because of the formal analogy to the classical case: Recall that the invariant probability measures of a given classical dynamical systems are ergodic, in the usual sense, iff they are extreme in the convex set of all invariant measures of the system.

  2. 2.

    In the present construction, one may even take the group U(N) of all unitary N × N matrices. However, we restrict ourselves to the so-called special unitary matrices, because this case is the most relevant one in physics.

  3. 3.

    Recall that a homeomorphism is a bijection (one-to-one and onto) such that both the function and its inverse are continuous.

  4. 4.

    By definition, Ξ is a mapping \(\mathcal {A}\rightarrow C(E(\mathcal {A}); \mathbb {C})\). It is naturally seen here as a mapping \(\mathcal {A}\rightarrow C(E;\mathbb {C})\), by restriction of continuous functions on \(E(\mathcal {A})\) to E.

  5. 5.

    That is, \(\mathrm {e}_{\mathrm {s},x}(\tilde {\mathrm {s}},\tilde {x})=1\) if \(( \mathrm {s},x)=(\tilde {\mathrm {s}},\tilde {x})\) and \(\mathrm {e}_{\mathrm {s},x}( \tilde {\mathrm {s}},\tilde {x})=0\), else.

  6. 6.

    In some papers, only (approximating) Slater determinants are considered.

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Correspondence to Jean-Bernard Bru or Walter de Alberto Siqueira Pedra .

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Bru, JB., Alberto Siqueira Pedra, W.d. (2023). Thermodynamic Equilibrium in Infinite Volume. In: C*-Algebras and Mathematical Foundations of Quantum Statistical Mechanics. Latin American Mathematics Series(). Springer, Cham. https://doi.org/10.1007/978-3-031-28949-1_5

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