Time Dilation as Field

Ogonowski, Piotr

doi:10.4236/jmp.2012.32027

Cited by 2 publications

(2 citation statements)

References 6 publications

(4 reference statements)

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“…However, we have shown in section 2.3 that scalar field Φ = 1/γ r may serve us to describe gravity on flat manifold. Therefore we will start with such scalar field and following [18] we will consider some Maxwelllike equations on flat manifold. It is known, that Special Relativity was invented as consequence of Maxwell rights analysis.…”

Section: Gravity As Wave Equation In Minkowski Spacetimementioning

confidence: 99%

Maxwell-like picture of General Relativity and its Planck limit

Ogonowski¹,

Skindzier²

2013

Preprint

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We show that Geroch decomposition leads us to Maxwell-like representation of gravity in (3 + 1) metrics decomposition that may be perceived as Lorentz invariant version of GEM. For such decomposition we derive four-potential V µ and gravitational field tensor F µν that is associated with gravitational interaction. Next we show that gravitational four-current J µ derived for introduced four-potential produce energystress tensor and reproduce main General Relativity formula. Next we introduce valid Lagrangian and equations of motion that explains obtained results. At the end we introduce new approach to quantization of gravity that results in proper quantum values and is open to further generalization.

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Section: Gravity As Wave Equation In Minkowski Spacetimementioning

confidence: 99%

Maxwell-like picture of General Relativity and its Planck limit

Ogonowski¹,

Skindzier²

2013

Preprint

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“…The annihilation of an electron and a positron could then be deemed to jump rest mass instantaneously to an infinite speed through time. Recent results from Ogonowski [4] suggest all this could also have implications for gravity.…”

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confidence: 97%

Dark Experiments: From Black Holes to Cosmic Rays

Allen¹

2012

JMP

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Some nagging questions in modern physics can be resolved rigorously using a basic mathematical formalism, albeit with the need to admit that non-isomorphic realities arise to various degrees in a given universe. Let U=(m', m") be an unordered pair of distinct massive objects in different reference frames. A dark experiment is an ordering <mu, mv> of the elements of U, either <m', m"> or, exclusively, <m", m'> , where the left-hand member of the ordered pair is called the observer, and where there exists a 1-to-1 mapping f:{<mu}→{events}, mv> , such that both elements of an ordered pair in a dark experiment agree on the events that unfold in the experiment. However, since <m', m">≠ <m", m'>, it follows that f(<m', m">)≠f(<m", m'>). This describes non-isomorphic realities where in both elements of each ordered pair mapping two distinct sets of unfolding events will agree on their respective events. Consequently, there is an inherent limitation on what can be determined directly from experimentation. Examples arise in the context of the Hawking information paradox, relativistic time travel, and cosmic ray experiments

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Time Dilation as Field

Cited by 2 publications

References 6 publications

Maxwell-like picture of General Relativity and its Planck limit

Maxwell-like picture of General Relativity and its Planck limit

Dark Experiments: From Black Holes to Cosmic Rays

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