Noncommutative momentum and torsional regularization
Nikodem Pop{\l}awski

TL;DR
This paper introduces a torsion-based noncommutative momentum space framework that regularizes divergent integrals in quantum field theory, leading to finite physical quantities like the electron's bare charge.
Contribution
It proposes a novel regularization method using torsion-induced noncommutative momentum relations, replacing traditional divergent integrals with finite summations.
Findings
Regularizes ultraviolet divergences in loop integrals.
Derives a finite, gauge-invariant vacuum polarization tensor.
Calculates a finite bare electron charge of approximately -1.22 times e.
Abstract
We show that in the presence of the torsion tensor , the quantum commutation relation for the four-momentum, traced over spinor indices, is given by . In the Einstein--Cartan theory of gravity, in which torsion is coupled to spin of fermions, this relation in a coordinate frame reduces to a commutation relation of noncommutative momentum space, , where is a constant on the order of the squared inverse of the Planck mass. We propose that this relation replaces the integration in the momentum space in Feynman diagrams with the summation over the discrete momentum eigenvalues. We derive a prescription for this summation that agrees with convergent integrals: \[ \int\frac{d^4p}{(p^2+\Delta)^s}\rightarrow 4\pi U^{s-2}\sum_{l=1}^\infty \int_0^{\pi/2} d\phi…
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