普朗克尺度下量子场的引力自正则化

Zahid Zakir
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引用次数: 0

摘要

具有接近普朗克能量的环图产生了一个强大的外部引力场,这减缓了远处观察者的局部过程,直到他们冻结。由于普朗克长度是量子系统的引力半径,这个和更小尺度的事件不可能在有限的世界时间t中发生,也不会对s矩阵有贡献。因此,引力时间膨胀导致局域频率的强红移,提供了环图的引力自正则化。没有引力作用的环修正,在普朗克能量处被截断,给出了有引力作用的环修正的上界,这一事实导致了引力正则化的简单规则。规范场和引力子的量子修正很小,微扰理论级数收敛。在普朗克能量之前,单环引力子的贡献是足够的,因为多环引力子受到“能量/普朗克能量”关系的高度抑制。具有幂律增长修正的标量场应该是有效场。场的非线性增强了引力,加速了冻结,从而抑制了高能项。不可重整模型是有限的,但只有当它们的环修正在普朗克尺度上保持小时才会变得一致,这发生在量子引力中。引力正则化扩展标准模型(ESM)包括引力子和带有效标量的标准模型,它是可重整的和有限的,这简化了它的进一步推广。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Gravitational self-regularization of quantum fields at Planck scales
Loop diagrams with near-Planck energies create a strong external gravitational field, which slows down local processes for distant observers up to their freezing. Since Planck length is the gravitational radius of the system of quanta, the events of this and smaller scale cannot occur in finite world time t and do not contribute to the S-matrix. Consequently, gravitational time dilation, leading to a strong redshift of local frequencies, provides gravitational self-regularization of the loop diagrams. The loop corrections without gravity effects, cut off at Planck energy, give upper bounds for the corrections with gravity effects and this fact leads to simple rules of gravitational regularization. The corrections with quanta of gauge fields and gravitons are small, and the perturbation theory series converge. At pre-Planck energies, one-loop graviton contributions are sufficient, since the multi-loop ones are damped by high degrees of the relation “energy/Planck energy”. Scalar field with power-law growing corrections should be effective field. Non-linearity of fields enhances gravity and get faster freezing, which suppresses the high energy terms. Nonrenormalizable models are finite, but become consistent only when their loop corrections remain small on Planck scale and this occurs in quantum gravity. Gravitationally regularized Extended Standard Model (ESM), including gravitons and Standard Model with effective scalars, is renormalizable and finite, which simplifies its further generalization.
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