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arXiv 0801.2307gr-qc
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爱因斯坦-薛定谔理论的一种修正,包含了广义相对论和电动力学

A modification of Einstein-Schrodinger theory that contains both general relativity and electrodynamics

J. A. Shifflett

摘要:

我们修改爱因斯坦薛定谔理论,包括宇宙学常数$Λ_z$乘以对称度规,我们展示了如何理论可以很容易地耦合到额外的领域。假设宇宙学常数$Λ_z$几乎被薛定谔的宇宙学常数$Λ_b$抵消,后者乘以非对称基本张量,使得总的$Λ=Λ_z+Λ_b$与测量相匹配。由此产生的理论在极限下精确地成为爱因斯坦-麦克斯韦理论,即$|Λ_z|\to\infty$。对于$|Λ_z|\sim 1/(Planck length)^2$,场方程与普通爱因斯坦方程和麦克斯韦方程组相匹配,除了额外的项,这些额外的项是最坏情况场强和可测量的变化率的常用项中的$<10^{-16}$。拉格朗日量中可以包含额外的场,这些场可以耦合到对称度规和电磁矢量势,就像爱因斯坦-麦克斯韦理论一样。当包含源时,通过取爱因斯坦方程的散度,得到了常洛仑兹力方程。爱因斯坦-因菲尔德-霍夫曼(EIH)运动方程将爱因斯坦-麦克斯韦理论的运动方程与牛顿/库仑阶相匹配,这证明了洛伦兹力的存在,而无需来源。这解决了原来的爱因斯坦-薛定谔理论的一个问题,它未能预测洛伦兹力。精确的带电解与Reissner-Nordstrom解匹配,除了附加项是可测量的最坏情况半径的常用项的$\sim 10^{-66}$。一个精确的电磁平面波解与爱因斯坦-麦克斯韦理论中的对应解是相同的。

英文摘要:

We modify the Einstein-Schrodinger theory to include a cosmological constant $Λ_z$ which multiplies the symmetric metric, and we show how the theory can be easily coupled to additional fields. The cosmological constant $Λ_z$ is assumed to be nearly cancelled by Schrodinger's cosmological constant $Λ_b$ which multiplies the nonsymmetric fundamental tensor, such that the total $Λ=Λ_z+Λ_b$ matches measurement. The resulting theory becomes exactly Einstein-Maxwell theory in the limit as $|Λ_z|\to\infty$. For $|Λ_z|\sim 1/(Planck length)^2$ the field equations match the ordinary Einstein and Maxwell equations except for extra terms which are $<10^{-16}$ of the usual terms for worst-case field strengths and rates-of-change accessible to measurement. Additional fields can be included in the Lagrangian, and these fields may couple to the symmetric metric and the electromagnetic vector potential, just as in Einstein-Maxwell theory. The ordinary Lorentz force equation is obtained by taking the divergence of the Einstein equations when sources are included. The Einstein-Infeld-Hoffmann (EIH) equations of motion match the equations of motion for Einstein-Maxwell theory to Newtonian/Coulombian order, which proves the existence of a Lorentz force without requiring sources. This fixes a problem of the original Einstein-Schrodinger theory, which failed to predict a Lorentz force. An exact charged solution matches the Reissner-Nordstrom solution except for additional terms which are $\sim 10^{-66}$ of the usual terms for worst-case radii accessible to measurement. An exact electromagnetic plane-wave solution is identical to its counterpart in Einstein-Maxwell theory.

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