Alternative tangent and cotangent structures and their physical applications
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arXiv
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| Format: | Preprint |
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2025
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| _version_ | 1866909998504738816 |
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| author | Cariñena, José F. Clemente-Gallardo, Jesús Marmo, Giuseppe |
| author_facet | Cariñena, José F. Clemente-Gallardo, Jesús Marmo, Giuseppe |
| contents | The conditions under which a given manifold $M$ may be given a tangent bundle or a cotangent bundle structure are analyzed. This is an important property arising in different contexts. For instance, in the study of integrability of a given dynamics the existence of alternative compatible structures is very relevant, as well as in the geometric approach to Classical Mechanics. On the other hand in the quantum-to-classical transition, a Weyl system plays an important role for it provides (within the so-called Weyl-Wigner formalism) a description of quantum mechanics on a (symplectic) phase-space $M$. A Lagrangian subspace $Q\subset M$ of the (linear) phase space determines thus a maximal set of pairwise commuting unitary operators, which is used to parametrize the quantum states. As the choice of this maximal Abelian set of observables is not unique, the different choices make the phase space to become diffeomorphic to different cotangent bundles $T^*Q$ corresponding to different choices for the base manifold (and hence the fibers). These motivating ideas are used to study how to define alternative tangent and/or cotangent bundle structures on a phase space. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2509_20855 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Alternative tangent and cotangent structures and their physical applications Cariñena, José F. Clemente-Gallardo, Jesús Marmo, Giuseppe Mathematical Physics 81Q10, 81Q15, 35J10 The conditions under which a given manifold $M$ may be given a tangent bundle or a cotangent bundle structure are analyzed. This is an important property arising in different contexts. For instance, in the study of integrability of a given dynamics the existence of alternative compatible structures is very relevant, as well as in the geometric approach to Classical Mechanics. On the other hand in the quantum-to-classical transition, a Weyl system plays an important role for it provides (within the so-called Weyl-Wigner formalism) a description of quantum mechanics on a (symplectic) phase-space $M$. A Lagrangian subspace $Q\subset M$ of the (linear) phase space determines thus a maximal set of pairwise commuting unitary operators, which is used to parametrize the quantum states. As the choice of this maximal Abelian set of observables is not unique, the different choices make the phase space to become diffeomorphic to different cotangent bundles $T^*Q$ corresponding to different choices for the base manifold (and hence the fibers). These motivating ideas are used to study how to define alternative tangent and/or cotangent bundle structures on a phase space. |
| title | Alternative tangent and cotangent structures and their physical applications |
| topic | Mathematical Physics 81Q10, 81Q15, 35J10 |
| url | https://arxiv.org/abs/2509.20855 |