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Magnetic Spherical PendulumYildirim, Selma 01 January 2003 (has links) (PDF)
The magnetic spherical pendulum is a mechanical system consisting of a
pendulum whereof the bob is electrically charged, moving under the influence
of gravitation and the magnetic field induced by a magnetic monopole deposited
at the origin. Physically not directly realizable, it turns out to be
equivalent to a reduction of the Lagrange top. This work is essentially the logbook
of our attempts at understanding the simplest contemporary approaches
to the magnetic spherical pendulum.
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Classification, Casimir invariants, and stability of lie-poisson systems /Thiffeault, Jean-Luc, January 1998 (has links)
Thesis (Ph. D.)--University of Texas at Austin, 1998. / Vita. Includes bibliographical references (leaves 148-158) and index. Available also in a digital version from Dissertation Abstracts.
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Some quantum mechanical applications of the theory of Lie algebrasWollenberg, L. S. January 1967 (has links)
No description available.
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Application of co-adjoint orbits to the loop group and the diffeomorphism group of the circleLano, Ralph Peter 01 May 1994 (has links)
No description available.
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Symetrie systémů v prostorech příbuzných prostoročasu vícedimenzionální černé díry / Symmetries of systems in spaces related to high-dimensional black hole spacetimeKolář, Ivan January 2014 (has links)
In this work we study properties of the higher-dimensional generally rotating black hole space-time so-called Kerr-NUT-(A)dS and the related spaces with the same explicit and hidden symetries as the Kerr-NUT-(A)dS spacetime. First, we search commuta- tivity conditions for classical (charged) observables and their operator analogues, then we investigate a fulfilment of these conditions in the metioned spaces. We calculate the curvature of these spaces and solve the charged Hamilton-Jacobi and Klein-Gordon equations by the separation of the variables for an electromagnetic field, which pre- serves integrability of motion of a charged particle and mutual commutativity of the corresponding operators.
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