Searcharxiv⌕ Search

arXiv subjects

Vu B Ho

Publications and source records attributed to Vu B Ho.

8 recordsLinked to original sources
arXiv1996

Spacetime Structures and Physical Theories

General relativity is applied to the strong interaction; the nexus between the two being arrived at by constructing a line element having the Yukawa form, which is used to describe geometrically the classical dynamics of a particle moving under the influence of the short-range strong interaction. It is shown that, with reasonable assumptions, the theory of general relativity can be made compatible with quantum mechanics by using the general relativistic field equations to construct a Robertson-Walker metric for a quantum particle. The resulting line element of the particle can be transformed entirely to that of a Minkowski spacetime, and the spacetime dynamics of the particle described by a Minkowski observer takes the form of quantum mechanics. It is also discussed the physical aspects of the affine connection in general relativity and its relationship with the field strength of the electromagnetic field and strong interaction. A heuristic geometric formulation of the electromagnetic field as an independent spacetime structure is presented.

hep-th↗
arXiv1996

Quantum mechanics in multiply connected spaces

This paper analyses quantum mechanics in multiply connected spaces. It is shown that the multiple connectedness of the configuration space of a physical system can determine the quantum nature of physical observables, such as the angular momentum. In particular, quantum mechanics in compactified Kaluza-Klein spaces is examined. These compactified spaces give rise to an additional angular momentum which can adopt half-integer values and, therefore, may be identified with the intrinsic spin of a quantum particle.

hep-th↗
arXiv1995

A discussion on a possibility to interpret quantum mechanics in terms of general relativity

It is shown that, with some reasonable assumptions, the theory of general relativity can be made compatible with quantum mechanics by using the field equations of general relativity to construct a Robertson-Walker metric for a quantum particle so that the line element of the particle can be transformed entirely to that of the Minkowski spacetime, which is assumed by a quantum observer, and the spacetime dynamics of the particle described by a Minkowski observer takes the form of quantum mechanics. Spacetime structure of a quantum particle may have either positive or negative curvature. However, in order to be describable using the familiar framework of quantum mechanics, the spacetime structure of a quantum particle must be "quantised" by an introduction of the imaginary number $i$. If a particle has a positive curvature then the quantisation is equivalent to turning the pseudo-Riemannian spacetime of the particle into a Riemannian spacetime. This means that it is assumed the particle is capable of measuring its temporal distance like its spatial distances. On the other hand, when a particle has a negative curvature and a negative energy density then quantising the spacetime structure of the particle is equivalent to viewing the particle as if it had a positive curvature and a positive energy density.

hep-th↗
arXiv1995

A geometric formulation of strong interaction

It is observed that, at short range, the field equations of general relativity admit a line element that takes the form of Yukawa potential. The result leads to the possibility that strong interaction may also be described by field equations that have the same form as that of general relativity. It is then shown how such field equations may arise from the coupling of two strong fields.

hep-th↗
arXiv1994

On the quantisation of the angular momentum

When a hydrogen-like atom is treated as a two dimensional system whose configuration space is multiply connected, then in order to obtain the same energy spectrum as in the Bohr model the angular momentum must be half-integral.

hep-th↗
arXiv1993

Spacetime structure and Quantum physics

A description of electromagnetism as four-dimensional spacetime structure leads to the dynamics of a charged particle being determined only by the four-vector potential and the existence of an electromagnetic field depending on the topological structure of the background spacetime. When the spacetime structure of electromagnetism is complex it is possible to connect spacetime structure and quantum physics via the method of path integration. (This paper is a consequence of an attempt to incorporate gravitation into electromagnetism by describing gravity as a coupling of two electromagnetic fields.)

gr-qc↗