Stochastical Mechanics of Particle Systems in Clifford-Analytical Formulation Related to Hurwitz Pairs of Bidimension (8,5)
Stochastical Mechanics of Particle Systems in Clifford-Analytical Formulation Related to Hurwitz Pairs of Bidimension (8,5)
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与二维 Hurwitz 对相关的 Clifford 解析公式中粒子系统的随机力学 (8,5)
DOI:
10.1007/978-94-011-1896-5_10
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发表时间:
1994
期刊:
影响因子:
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通讯作者:
O. Suzuki
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文献类型:
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作者:
J. Ławrynowicz;L. Wojtczak;S. Koshi;O. Suzuki
A particle system is considered a system of interacting particles embedded in a many-dimensional space. The usual one-particle space-time may then be treated as a projection of an at least five-dimensional space, where the fifth dimension is of stochastic character. A formulation of the clasical mechanics infivedimensions is proposed, which is a non-trivial generalization of the relativistic forces as a result of the appearance of the fifth dimension. — The five-dimensional geometry introduced simplifies a more sophisticated Grauert geometry and assures the proper Clifford algebras and analyses of the corresponding Dirac-like equations according to the solvabilty of the generalized Hurwitz problems for the pseudo-euclidean Hurwitz pairs of dimensions five and eight. Therefore the corresponding holomorphic mappings enable us to construct spinors which describe the behaviour of particles as needed in the classical, quantum and statistical mechanics. — In the statistical mechanics the description in terms of a many-dimensional geometry leads in a natural way to the appearance of fluctuations of thermodynamical variables. Our formulation of the problem is based on Dirac-like equations extended to many-body forms, i.e. the Breit construction generalized to the generations of Hurwitz pairs starting from the pairs of spaces of dimensions five and eight. The construction leads to the hamiltonian in the representation of second quantization whose coefficients contain the stochastical parameters. — The usual diagonalization procedure allows us to find the energy eigenvalues and amplitudes of electronic or atomic eigenvectors. The direction perperdicular to the surface is then distinguished and the eigenvectors are of standing-wave character. The stability of the system is assured by a proper choice of boundary conditions. An illustrative example is given in the paper by B. Gaveau, J. Ławrynowicz and L. Wojtczak, published in this volume.
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