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arXiv 1003.0743quant-ph
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出现量子现象的广义分析力学

A Generalized Analytical Mechanics in which Quantum Phenomena Appear

Masao Yasuda

摘要:

目前,大质量宏观粒子的动力学是由经典分析力学(CM)给出,而大质量微观粒子的动力学是由量子力学(QM)给出。我们提出了一个力学有效的:我们变换,坐标变换下,协变张量的二阶下的动能项的Hamilton-Jacobi(H-J)方程。CM的作用,而不是与复同态群的作用,而是与一个扩展的复同态群的作用。然后,H-J方程,一阶偏微分方程,被修改为三阶。Euler-Lagrange方程CM,一个二阶常微分方程,与H-J方程相关。将最小作用量原理的直通作用量积分相应地修正为四阶积分。因此,我们得到一种力学,由于高阶方程,容纳了与量子现象相对应的现象。在限制势中粒子的能量被量子化到与量子力学相同的值。粒子在系综中的分布与量子力学不一致,但在实验不确定度范围内与实验一致。因此,该机制是QM的可测试替代方案。

英文摘要:

Currently, dynamics of a massive macroparticle is given by classical analytical mechanics (CM), while that of a massive micro one is given by quantum mechanics (QM). We propose a mechanics effective for both: We transform, under coordinate transformation, the covariant tensor of order two underlying the kinetic energy term of the Hamilton-Jacobi (H-J) eq. of CM, not with the action of the diffeomorphism group, but with an action of an extended diffeomorphism group. Then, the H-J eq., a first-order partial differential eq., is modified to a third-order one. The Euler-Lagrange eq. of CM, a second-order ordinary differential eq., related to the H-J eq. through action integral of the least action principle is accordingly modified to a fourth-order one. We thus obtain a mechanics which, because of the higher-order eqs., accommodates phenomena corresponding to quantum phenomena. Energy of a particle in a confining potential is quantized to the same values as those of QM. Particle distribution in an ensemble disagrees with that of QM, but agrees with experiments within experimental uncertainty. The mechanics therefore is a testable alternative to QM.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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