ar X iv : q ua nt - p h / 98 05 07 9 v 1 2 7 M ay 1 99 8 On Quantum Mechanics
نویسنده
چکیده
We discuss the aximatic basis of quantum mechanics and show that it is neither general nor consistent, since it does not incorporate the magnetic quantization as in the cyclotron motion and the flux quantization. A general and consistent system of axioms is conjectured which incorporates also the magnetic quanti-zation.
منابع مشابه
ar X iv : q ua nt - p h / 98 05 07 9 v 2 2 9 M ay 1 99 8 On Quantum Mechanics
We discuss the aximatic basis of quantum mechanics and show that it is neither general nor consistent, since it does not incorporate the magnetic quantization as in the cyclotron motion and the flux quantization. A general and consistent system of axioms is conjectured which incorporates also the magnetic quanti-zation.
متن کاملar X iv : q ua nt - p h / 98 05 07 9 v 3 2 J un 1 99 8 On Quantum Mechanics
We discuss the axiomatic basis of quantum mechanics and show that it is neither general nor consistent, since its axioms are incompatible with each other and moreover it does not incorporate the magnetic quantization as in the cyclotron motion. A general and consistent system of axioms is conjectured which incorporates also the magnetic quantization.
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The connection between the strictly isospectral construction in supersymmetric quantum mechanics and the general zero mode solutions of the Schroedinger equation is explained by introducing slightly generalized first-order intertwining operators. We also present a multiple-parameter generalization of the strictly isospectral construction in the same perspective.
متن کاملar X iv : q ua nt - p h / 02 05 05 2 v 1 1 0 M ay 2 00 2 ALTERNATIVE STRUCTURES AND BIHAMILTONIAN SYSTEMS
In the study of bi-Hamiltonian systems (both classical and quantum) one starts with a given dynamics and looks for all alternative Hamiltonian descriptions it admits. In this paper we start with two compatible Hermitian structures (the quantum analog of two compatible classical Poisson brackets) and look for all the dynamical systems which turn out to be bi-Hamiltonian with respect to them.
متن کاملar X iv : q ua nt - p h / 96 05 04 2 v 1 2 9 M ay 1 99 6 A generalized Pancharatnam geometric phase formula for three level quantum systems
We describe a recently developed generalisation of the Poincar ′ e sphere method, to represent pure states of a three-level quantum system in a convenient geometrical manner. The construction depends on the properties of the group SU(3) and its generators in the defining representation, and uses geometrical objects and operations in an eight dimensional real Euclidean space. This construction i...
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تاریخ انتشار 1998