By Konrad Rudnicki
This quantity, dedicated to the issues of relativity, gravitation and similar matters in physics, offers papers introduced and/or mentioned throughout the convention "Redshifts and Gravitation in a Relativistic Universe" held in Cesena on September 17-20th 1999. In a fashion, this convention represents a reaction to Zwicky's strategy, defined above. Its major objective was once to function a discussion board for concepts and theories that pass opposed to the mainstream of technology. the various theories are already solid of their ultimate shape; a few are only tough rules nonetheless present process improvement.
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Additional resources for Gravitation, Electromagnetism and Cosmology : Toward a New Synthesis
This makes the following two expressions identical: ⎧Ψ = R0 RG ( sin ϕ − i cos ϕ ) ⎪ ⎛ ⎞ . ⎨ RG −1⎟ ⎪ ΔR = R0 ⎜⎜ 1 − i ⎟ R0 ⎝ ⎠ ⎩ We also have, therefore, the complex conjugate function Ψ = R0 RG ( sin ϕ + i cos ϕ ) The displacement velocity In the complex framework, we can now develop the expression for the velocity differential Δυ pertinent to the vacuum displacement as acceleration in general, or more particularly in the case of gravitation, from the preceding: Geometry of Acceleration in Space-Time ⎛ R Δυ = c ⋅ ⎜1 − 1 − G ⎜ R0 ⎝ ⎛ R ≡ c ⋅ ⎜⎜1 − i G ⋅ R0 ⎝ ⎞ ⎟⎟ ⎠ R 1− 0 RG ⎞ ⎟⎟ ⎠ 21 .
Our model may be thought of as a starting point for more detailed investigations of the non-baryonic dark matter scenario. As we see here, the dilaton (massless scalar field) may act dynamically in the same way as massive bodies. In this way the dilaton can become another candidate for the cold dark matter. On the galactic scale, however, where dilatonic configurations could be invoked to explain the central engine for AGNs and quasars, our model does not solve the flat rotation curve problem. In this aspect it would be very interesting to extend the model discussed in this paper by inclusion of an axion field.
It contains 16 independent components. The remaining 4 functions allowed by the general form of the material tensor density η μνλρ ( x ) are provided by the 4 independent components of the totally antisymmetric G tensor jμνλ ( x ) formed from ρ M ( x ) and jM ( x ) . It is erroneous to try to relate this antisymmetric tensor to the external current, as in (21), because this will introduce an additional 16 new functions. It is also erroneous to treat this tensor as any kind of current, because it is not a tensor density.
Gravitation, Electromagnetism and Cosmology : Toward a New Synthesis by Konrad Rudnicki