TL;DR: Inspired by the renormalizability of the non-commutative Phi^4 model with added oscillator term, the authors formulate a non-Commutative gauge theory, where the oscillator enters as a gauge fixing term in a BRST invariant manner.
Abstract: Inspired by the renormalizability of the non-commutative Phi^4 model with added oscillator term, we formulate a non-commutative gauge theory, where the oscillator enters as a gauge fixing term in a BRST invariant manner. All propagators turn out to be essentially given by the Mehler kernel and the bilinear part of the action is invariant under the Langmann-Szabo duality. The model is a promising candidate for a renormalizable non-commutative U(1) gauge theory.
TL;DR: In this paper, strong and weak type estimates for the Mehler kernel operator with respect to the region of holomorphy of the Ornstein-Uhlenbeck semigroup were obtained.
Abstract: For each p in [1, ∞) let Ep denote the closure of the region of holomorphy of the Ornstein-Uhlenbeck semigroup {Ht : t> 0} on L p with respect to the Gaussian measure. We prove sharp weak type and strong type estimates for the maximal operator f �→ H ∗ f = sup{|Hzf | : z ∈ Ep} and for a class of related operators. As a consequence of our methods, we give a new and simpler proof of the weak type 1 estimate for the maximal operator associated to the Mehler kernel.
TL;DR: Inspired by the renormalizability of the non-commutative Phi^4 model with added oscillator term, the authors formulate a non-Commutative gauge theory, where the oscillator enters as a gauge fixing term in a BRST invariant manner.
Abstract: Inspired by the renormalizability of the non-commutative Phi^4 model with added oscillator term, we formulate a non-commutative gauge theory, where the oscillator enters as a gauge fixing term in a BRST invariant manner. All propagators turn out to be essentially given by the Mehler kernel and the bilinear part of the action is invariant under the Langmann-Szabo duality. The model is a promising candidate for a renormalizable non-commutative U(1) gauge theory.
TL;DR: In this article, the generalized Mehler kernel formulas for conditional Wiener integrals are derived up to arbitrarily high orders in powers of ℏ, for exp{−TH(ℏ)/℈}(x, y), T>0, where H(ϵ)=[(−ℎ2/2)Δ1+V], Δ1 being the one-dimensional Laplacian, V being a real-valued potential V∈C∞(R), bounded below, together with its second derivative.
Abstract: Imitating Schilder’s results for Wiener integrals rigorous Laplace asymptotic expansions are proven for conditional Wiener integrals. Applications are given for deriving generalized Mehler kernel formulas, up to arbitrarily high orders in powers of ℏ, for exp{−TH(ℏ)/ℏ}(x, y), T>0 where H(ℏ)=[(−ℏ2/2)Δ1+V], Δ1 being the one‐dimensional Laplacian, V being a real‐valued potential V∈C∞(R), bounded below, together with its second derivative.