Yang-Mills theory in three dimensions as a quantum gravity theory

We perform the dual transformation of theYang-Mills theory in three dimensions using the Wilson action on the cubic lattice. The dual lattice is made of tetrahedra triangulating a 3-dimensional curved manifold but which is embedded into a flat 6-dimensional space [for the SU(2) gauge group]. In the continuum limit, the theory can be reformulated in terms of 6-component gauge-invariant scalar fields having the meaning of the external coordinates of the dual lattice sites. These 6-component fields induce a metric and a curvature of the 3-dimensional dual-color space. The Yang-Mills theory can also be rewritten as a quantum gravity theory with the Einstein-Hilbert action but with a purely imaginary Newton constant plus a homogeneous “ether” term. The theory can be formulated in a gauge-invariant and local form without explicit color degrees of freedom.     

Vacuum effects in quantum field theory

We discuss some consequences of applying a procedure developed in a previous paper, to implement the conformal and general invariance of the functional integral. It is shown that spontaneous breaking of those symmetries is unavoidable; we consider in particular the linear σ-model, in the conformal limit, and the Einstein gravitation and derive some simple relations among the vacuum expectation value, a phenomenological cut-off and the Lagrangian constants.     

Spontaneous quantum compactification in a d = 10 supersymmetric Yang-Mills theory

It is shown that an N = 1, d = 10 supersymmetric Yang-Mills theory admits a spontaneous quantum compactification of the form M₄ × S₆, where M₄, and S₆ are the Minkowski space and the 6-sphere, accordingly. The radius of S₆ is of the order of the Planck length L_Pl.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 1, pp. 77–83, January, 1990.The authors thank I. L. Bukhbinder for his help in our work.     

Yang-Mills theory and uniformization

We define a notion of a stable system of Hodge bundles. A stable system of Hodge bundles has a Hermitian-Yang-Mills metric and, if certain Chern classes vanish, this gives a complex variation of Hodge structure. We use these ideas to obtain a criterion for a variety to be uniformized by a bounded symmetric domain.     

Vacuum Cherenkov effect in logarithmic nonlinear quantum theory

We describe the radiation phenomena which can take place in the physical vacuum such as Cherenkov-type shock waves. Their macroscopical characteristics - cone angle, flash duration, radiation yield and spectral distribution - are computed. It turns out that the radiation yield is proportional to the square of the proper energy scale of the vacuum which serves also as the vacuum instability threshold and the natural ultraviolet cutoff. While the analysis is mainly based on the theory engaging the logarithmic nonlinear quantum wave equation, some of the obtained results must be valid for any Lorentz-invariance violating theory describing the vacuum by (effectively) continuous medium in the long-wavelength approximation.     

Vacuum degeneration in the quasiclassical approximation in non-Abelian quantum theory

In this paper we construct quasiclassical wave packets for a non-Abelian particle in an external chromomagnetic field and field-averaged coordinates and color vector. In this case the average color vector is found not to satisfy the quasiclassical Wong equations and vacuum degeneration is noted in such a field. The choice of the vacuum leads to spontaneous breakdown of the initial symmetry of the Hamiltonian.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 1, pp. 106–111, January, 1990.     

Half-monopoles in the Yang-Mills theory

Using a gauge-invariant characterization of monopoles defined via their centres, we investigate the generic topological field pattern for the three-dimensional Yang-Mills theory. This leads to field patterns with one-half winding number. After presenting the main features through the simpler case of half-vortices, we consider half-monopoles in detail.     

Yang-Mills gauge theory and gravitation

We point out that Yang's and Einstein's gravitational equations can be obtained from a geometric approach of Yang-Mills gauge theory in a sourceless case, under a decomposition of the Poincaré algebra. Otherwise, Einstein's equations cannot be derived from a Yang-Mills gauge equation when sources are inserted in the rotational sector of that algebra. A gauge Lagrangian structure is also discussed.     

A new quantum representation for canonical gravity and SU(2) Yang-Mills theory

Starting from Rovelli-Smolin's infinite-dimensional graded Poisson-bracket algebra of loop variables, we propose a new way of constructing a corresponding quantum representation. After eliminating certain quadratic constraints, we “integrate” an infinite-dimensional subalgebra of loop variables, using a formal group law expansion. With the help of techniques from the representation theory of semidirect-product groups, we find an exact quantum representation of the full classical Poisson-bracket algebra of loop variables, without any higher-order correction terms. This opens new ways of tackling the quantum dynamics for both canonical gravity and Yang-Mills theory.     

Exposition of magnetostatics based on the special theory of relativity

We present the division Magnetostatics in the course of general physics, with the treatment based on the deductions of the special theory of relativity, the invariance of the electric charge, Coulomb's law, and the superposition principle of fields. The exposition begins with the analysis of the interaction of two point electric charges with arbitrary orientations of their velocities.Translated from Izvestiya Vysshikh Uchenbnykh Zavedenii, Fizika, No. 4, pp. 61–65, April, 1985.     

Topological aspects of Yang-Mills theory

The space of mapsS ³ G has components which give the topological quantum number of Yang-Mills theory for the groupG. Each component of the space has further topological invariants. WhenG=SU(2) we show that these invariants (the homology groups) are captured by the space of instantons. Using these invariants we show that potentials must exist for which the massless Dirac equation (in Euclidean 4-space) has arbitrarily many independent solutions (for fixed instanton number).     

Gravity as Yang-Mills gauge theory

We propose a Yang-Mills field theory of gravity based on a unitary phase-gauge-invariance of the lagrangian where the gauge transformations are those of the SU(2) × U(1) symmetry of the 2-spinors. In the classical limit this microscopic theory results in Einstein's metrical theory of gravity, where we restrict ourselves in a first step to its linearized version.     

Integrable model of Yang-Mills theory and quasi-instantons

Within the framework of Euclidean conformal invariant Yang-Mills theory with a scalar field, a two-dimensional Hamiltonian system integrable for a definite relation between the coupling constants is considered. A particular solution of the Hamilton-Jacobi equation leads to a system of first-order equations providing a nonself-dual instanton-like solution of the model concerned. As a generalization of the system, a quasi-self-duality equation is suggested which is integrated by means of the 't Hooft ansatz and results in quasi-self-dual instantons (quasi-instantons).     

Two-loop diagrams in Yang-Mills theory

A calculation of the renormalisation constants of the Yang-Mills field to O(g⁴) is presented. The function β(g) is hence evaluated to O(g⁵) and possible implications for gauge theories of the strong interactions discussed.     

String-like phase in Yang-Mills theory

A dynamical mechanism is discussed leading to the phase where the string of the color flux tube is formed in Yang-Mills theory. The pairing force between massless gauge fields in the color single channel forms a tachyon or a Cooper state and leads to the instability of the normal vacuum. A stable vacuum is required to remain massless after the condensation of pairs. Then the stability of the new vacuum leads to the condition on the 't Hooft index α which is equivalent to the condition of the existence of the string solutions.