On the Cosmic Evolution of the Quantum Vacuum Using Two Variable <i>G</i> Models and Winterberg’s Thesis

Christopher Pilot
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Abstract

We work within a Winterberg framework where space, i.e., the vacuum, consists of a two component superfluid/super-solid made up of a vast assembly (sea) of positive and negative mass Planck particles, called planckions. These material particles interact indirectly, and have very strong restoring forces keeping them a finite distance apart from each other within their respective species. Because of their mass compensating effect, the vacuum appears massless, charge-less, without pressure, net energy density or entropy. In addition, we consider two varying G models, where G, is Newton’s constant, and G-1, increases with an increase in cosmological time. We argue that there are at least two competing models for the quantum vacuum within such a framework. The first follows a strict extension of Winterberg’s model. This leads to nonsensible results, if G increases, going back in cosmological time, as the length scale inherent in such a model will not scale properly. The second model introduces a different length scale, which does scale properly, but keeps the mass of the Planck particle as, ± the Planck mass. Moreover we establish a connection between ordinary matter, dark matter, and dark energy, where all three mass densities within the Friedman equation must be interpreted as residual vacuum energies, which only surface, once aggregate matter has formed, at relatively low CMB temperatures. The symmetry of the vacuum will be shown to be broken, because of the different scaling laws, beginning with the formation of elementary particles. Much like waves on an ocean where positive and negative planckion mass densities effectively cancel each other out and form a zero vacuum energy density/zero vacuum pressure surface, these positive mass densities are very small perturbations (anomalies) about the mean. This greatly alleviates, i.e., minimizes the cosmological constant problem, a long standing problem associated with the vacuum.
利用双变量<i>G</i>模型和温特伯格的论文
我们在温特伯格框架内工作,其中空间,即真空,由双组分超流体/超固体组成,由大量正负质量普朗克粒子(称为普朗克粒子)组成。这些物质粒子之间的相互作用是间接的,并且具有很强的恢复力,使它们在各自的物种中彼此保持有限的距离。由于它们的质量补偿效应,真空显得无质量、无电荷、没有压力、净能量密度或熵。此外,我们考虑了两个变化的G模型,其中G是牛顿常数,G-1随着宇宙时间的增加而增加。我们认为,在这样一个框架内,至少有两个相互竞争的量子真空模型。第一种是对温特伯格模型的严格扩展。这将导致无意义的结果,如果G增加,回到宇宙时间,因为这种模型中固有的长度尺度将不能适当地缩放。第二个模型引入了一个不同的长度尺度,这个尺度是正确的,但保持普朗克粒子的质量为±普朗克质量。此外,我们建立了普通物质、暗物质和暗能量之间的联系,弗里德曼方程中的所有三种质量密度都必须被解释为剩余真空能,只有在聚合物质形成后,在相对较低的CMB温度下才会出现。从基本粒子的形成开始,由于不同的标度定律,真空的对称性将被打破。就像海洋中的波浪一样,正的和负的普朗克质量密度有效地相互抵消,形成零真空能量密度/零真空压力表面,这些正的质量密度是对平均值的非常小的扰动(异常)。这极大地缓解了,即最小化了宇宙常数问题,这是一个长期存在的与真空有关的问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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