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Self-field Theory, General Relativity and Quantum Theory

机译:自场论,广义相对论和量子论

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There are theoretical similarities between general relativity (GR) and quantum field theory (QFT). Among the most fundamental are that both are based on 2nd order wave equations and their associated potential theories and gauge considerations. In comparison SFT is based on the 1st order Maxwellian with its field variables that have a much reduced emphasis on gauge. Both GR and QFT are based around single particle analyses rather than the mutual effects that couple particles together studied in SFT. Finally both GR and quantum theory employ a metric that in the view of SFT serves to accommodate the over constraint of the basic equations. In both cases this is linked to a theoretical requirement for a zero-mass photon. Thus both quantum theory and GR depend upon a zero mass photon and hence from the point of view of SFT both quantum theory and GR are theoretical approximations. For quantum theory zero mass springs from the earliest observations of beta decay and again when a negligible rest mass of the photon could hardly be compared with the seemingly endless radiation from within the nucleus of the bombs dropped on Hiroshima and Nagasaki in 1945. The cosmological principle that had its genesis in the Vatican's unscientific and dogmatic dealings with Galileo was a way to avoid having any universal centre of gravity thus making the same mistake again. Nevertheless it is only an approximation in the light of SFT where it is seen that non-homogeneity and anisotropy are both present in the gravitational structure itself where space is divided into different gravitational regions. This structure depends on the composite nature and non-zero mass of the photon. The space within the Universe cannot be thought of as the surface of an expanding balloon other than as a theoretical approximation that holds for GR. It is known that at smaller than cosmological domains the cosmological principle does not hold for instance for any possible surviving location of the Big Bang. We may think of a biological tissue such as liver where the dielectric constant is averaged over the microstructure such as biological cells. While such an approximation is useful for numerical estimation it cannot be assumed to hold in any fine detail across smaller domains; this holds for both a homogenous isotropic model of liver and of the Cosmos.
机译:广义相对论(GR)与量子场论(QFT)之间在理论上有相似之处。两者中最基本的都是基于二阶波动方程及其相关的势能理论和量规考虑因素。相比之下,SFT基于一阶Maxwellian及其场变量,而对场规的重视程度大大降低。 GR和QFT都基于单个粒子分析,而不是基于SFT中研究的将粒子耦合在一起的相互作用。最后,遗传算法和量子理论都采用了一种度量,从SFT的角度来看,该度量可用来适应基本方程的过度约束。在这两种情况下,这都与零质量光子的理论要求有关。因此,量子理论和GR都依赖于零质量的光子,因此从SFT的角度来看,量子理论和GR都是理论上的近似。对于量子理论,零质量源自最早的β衰变观测结果,而且当光子的静止质量可忽略不计时,又很难与1945年在广岛和长崎投下的炸弹核内看似无休止的辐射相提并论。宇宙学原理起源于梵蒂冈与伽利略的不科学和教条式的交往是避免任何普遍的重心从而再次犯同样错误的一种方式。然而,从SFT的角度来看,这只是一个近似值,可以看到在空间划分为不同引力区域的引力结构本身中都存在非均质性和各向异性。这种结构取决于光子的复合性质和非零质量。除了作为GR的理论近似值之外,不能将宇宙中的空间视为膨胀气球的表面。众所周知,在小于宇宙学领域的领域,宇宙学原理并不适用于例如大爆炸的任何可能幸存地点。我们可能会想到生物组织(例如肝脏),其介电常数是在整个微观结构(例如生物细胞)上平均的。尽管这样的近似对数值估计很有用,但不能假定它在较小的域中具有任何精细的细节。这对于肝脏和宇宙的均质各向同性模型都成立。

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