Searcharxiv⌕ Search

arXiv subjects

Andrzej J. Staruszkiewicz

Publications and source records attributed to Andrzej J. Staruszkiewicz.

3 recordsLinked to original sources

De Sitter Invariant Vacuum States, Vertex Operators, and Conformal Field Theory Correlators

We show that there is only one physically acceptable vacuum state for quantum fields in de Sitter space-time which is left invariant under the action of the de Sitter-Lorentz group $SO(1,d)$ and supply its physical interpretation in terms of the Poincare invariant quantum field theory (QFT) on one dimension higher Minkowski spacetime. We compute correlation functions of the generalized vertex operator $:e^{i\hat{S}(x)}:$, where $\hat{S}(x)$ is a massless scalar field, on the $d$-dimensional de Sitter space and demonstrate that their limiting values at timelike infinities on de Sitter space reproduce correlation functions in $(d-1)$-dimensional Euclidean conformal field theory (CFT) on $S^{d-1}$ for scalar operators with arbitrary real conformal dimensions. We also compute correlation functions for a vertex operator $e^{i\hat{S}(u)}$ on the Łobaczewski space and find that they also reproduce correlation functions of the same CFT. The massless field $\hat{S}(u)$ is the nonlocal transform of the massless field $\hat{S}(x)$ on de Sitter space introduced by one of us.

hep-th↗

Quantum Mechanics of the Electric Charge

A simple argument against the existence of magnetic monopoles is given. The argument is an important part of the quantum theory of the electric charge developed by the author.

hep-th↗

An Infinite Lie Algebra Associated with the Quantum Coulomb Field

The theory of the quantum Coulomb field associates with each Lorentz frame, i. e., with each unit, future oriented time-like vector $u$, the operator of the number of transversal infrared photons $N(u)$ and the phase $S(u)$ which is the coordinate canonically conjugated with the total charge $Q: [Q, S(u)] = ie, e$ being the elementary charge. It is shown that the operators $N(u), Q/e S(u)$ and $Q^2$ form an infinite Lie algebra. One can conclude from this algebra that $\DeltaN(u) = (4/π) Q^2$, where $Δ$ is the Laplace operator in the Lobachevsky space of four-velocities $u$, thus relating the total charge $Q$ with the number of infrared photons.

hep-th↗