空间点不是点:它们的波函数消除了量子场论的紫外发散性

Kevin Cahill
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引用次数: 0

摘要

空间的点 $p(x)$ 是服从量子力学的观测值,其平均值 $\langle p(x) \rangle$ 则服从广义相对论。在空平三维空间中,一个点 $p(x)$ 可以表示为其平均值 $langle \boldsymbol p(x) \rangle+ \boldsymbol \epsilon(x)$ 与其量子余数 $\boldsymbol p(x) \rangle = \boldsymbol x 的和。无处不在的傅立叶指数 $\exp( i\boldsymbol k \cdot \boldsymbol p(x))$ 就是 $\exp( i \boldsymbol k \cdot (\boldsymbol x + \boldsymbol \epsilon))$。如果量子余数 $ \boldsymbol \epsilon(x)$ 的概率分布是正态分布且宽度为 $\sigma$、那么指数平均值$ \exp(i \boldsymbol k ( \boldsymbolx + \boldsymbol \epsilon ) \rangle$ 包含一个高斯因子$ \exp( -\sigma^2 \boldsymbol k^2/2 ) $ ,它使得自能、费曼图和暗能紫外有限。这种复杂的想法需要新的玻色子,并表明超对称性是软破坏的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The points of space are not points: their wavefunctions remove the ultraviolet divergences of quantum field theory
The points $p(x)$ of space are observables that obey quantum mechanics with average values $\langle p(x) \rangle$ that obey general relativity. In empty flat 3-space, a point $p(x)$ may be represented as the sum $ \boldsymbol p(x) = \langle \boldsymbol p(x) \rangle+ \boldsymbol \epsilon(x)$ of its average value $\langle \boldsymbol p(x) \rangle = \boldsymbol x$ and its quantum remainder $ \boldsymbol \epsilon(x)$. The ubiquitous Fourier exponential $\exp( i \boldsymbol k \cdot \boldsymbol p(x))$ is then $\exp( i \boldsymbol k \cdot ( \boldsymbol x + \boldsymbol \epsilon))$. If the probability distribution of the quantum remainders $ \boldsymbol \epsilon(x)$ is normal and of width $\sigma$, then the average of the exponential $\langle \exp(i \boldsymbol k ( \boldsymbol x + \boldsymbol \epsilon ) \rangle$ contains a gaussian factor $ \exp( - \sigma^2 \boldsymbol k^2/2 ) $ which makes self-energies, Feynman diagrams and dark energy ultraviolet finite. This complex of ideas requires new bosons and suggests that supersymmetry is softly broken.
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