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Geometry of the State Space of Quantum Mechanics

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Classical Systems in Quantum Mechanics
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Abstract

A description of differential geometrical structure of the quantum pure-states space, the projective Hilbert space, is provided. It is shown that this space is endowed with a natural symplectic structure which allows us to reformulate quantum mechanics in classical mechanical language as a classical field theory.

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Notes

  1. 1.

    Another, more intuitive and more detailed approach to the structure of quantum state space can be found in [16]. For geometry and dynamics (also nonlinear) of general—not only pure—states see also [37, Sect. 2.1].

  2. 2.

    For an alternative proof valid also for unitary orbits of density matrices see [37, Theorem 2.1.19].

  3. 3.

    A brief review of the theory of unbounded operators is present in [37, C], or in [37, Textbook] in detail.

  4. 4.

    A certain, more detailed, account of the geometry and interpretation questions of the set of density matrices is given in [37, 2.1-e].

  5. 5.

    A core \(D\subset {\mathcal H}\) of a closable operator   C is such a subset \(D\subset D(C)\subset {\mathcal H}\), that the closure of the restriction \(\overline{C\upharpoonright D}=\overline{C}\), cf. also [37, C1].

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Correspondence to Pavel Bóna .

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Bóna, P. (2020). Geometry of the State Space of Quantum Mechanics. In: Classical Systems in Quantum Mechanics. Springer, Cham. https://doi.org/10.1007/978-3-030-45070-0_2

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