Pseudo-Complex General Relativity - download pdf or read online

By Peter O. Hess, Mirko Schäfer, Walter Greiner

ISBN-10: 3319250604

ISBN-13: 9783319250601

ISBN-10: 3319250612

ISBN-13: 9783319250618

This booklet explores the position of singularities in most cases relativity (GR): the idea predicts that after a enough huge mass collapses, no identified strength is ready to cease it till all mass is targeted at some extent. The query arises, even if a suitable actual concept must have a singularity, no longer even a coordinate singularity. the looks of a singularity indicates the restrictions of the speculation. In GR this challenge is the powerful gravitational strength performing close to and at a super-massive focus of a critical mass. First, a old evaluate is given, on former makes an attempt to increase GR (which contains Einstein himself), all with particular motivations. it will likely be proven that the single attainable algebraic extension is to introduce pseudo-complex (pc) coordinates, another way for vulnerable gravitational fields non-physical ghost ideas seem. hence, the necessity to use pc-variables. we'll see, that the speculation incorporates a minimum size, with very important effects. After that, the pc-GR is formulated and in comparison to the previous makes an attempt. a brand new variational precept is brought, which calls for within the Einstein equations an extra contribution. however, the traditional variational precept should be utilized, yet one has to introduce a constraint with an analogous former effects. the extra contribution can be linked to hoover fluctuation, whose dependence at the radial distance should be nearly bought, utilizing semi-classical Quantum Mechanics. the most aspect is that pc-GR predicts that mass not just curves the distance but in addition adjustments the vacuum constitution of the gap itself. within the following chapters, the minimum size may be set to 0, as a result of its smallness. however, the pc-GR will preserve a remnant of the pc-description, particularly that the looks of a time period, which we may possibly name "dark energy", is inevitable. the 1st program might be mentioned in bankruptcy three, specifically ideas of significant mass distributions. For a non-rotating big item it's the pc-Schwarzschild answer, for a rotating gigantic item the pc-Kerr resolution and for a charged great item it is going to be the Reissner-Nordström resolution. This bankruptcy serves to get to grips on the way to unravel difficulties in pc-GR and on the right way to interpret the implications. one of many major results is, that we will put off the development horizon and therefore there'll be no black holes. the massive immense gadgets within the heart of approximately any galaxy and the so-called galactic black holes are inside of pc-GR nonetheless there, yet with the absence of an occasion horizon! bankruptcy four offers one other program of the idea, particularly the Robertson-Walker answer, which we use to version diversified results of the evolution of the universe. ultimately the potential of this thought to foretell new phenomena is illustrated.

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Sample text

R. Caianiello investigated the properties of the length element dω2 = gμν d x μ d x ν + dy μ dy ν . 4) where he identified the components y μ with the four-velocity, The four-velocity u μ μ xμ is defined here as ddsx = dcdτ , with τ denoting the eigentime. This definition is due to the common notation in literature. y μ = lu μ → dy μ = ldu μ . 5) The parameter l is introduced in order to maintain the units of length. That is, differently to the approach by Einstein, he did not consider some extended algebraic (complex) structure on real coordinates, but rather extended the coordinates to eight dimensions, with the new coordinates given by the respective four-velocities.

The length element square is defined as (use the rules explained in Chap. 52) with 1 + − g + gμν , 2 μν 1 + − g − gμν . 53) I When a pseudo-real metric is used (gμν = 0), this simplifies to R R d x μ d x ν + dy μ dy ν + I gμν d x μ dy ν + dy μ d x ν . 54) The first term has the same form as the length element squared proposed by M. Born and the last term corresponds to the dispersion relation, when the dy μ is identified with cl u μ . For the motion of a real particle, this term has to vanish, in order that the dω2 remains real.

38) ∗ ¯ and ν¯ also run in the with G μν ¯ = (G μν¯ ) . The indices μ and ν run from 1 to 4 and μ same interval. The α and β run from 1 to 8. 4 Hermitian Gravity 25 μ and using the definition of X μ and X we obtain 1 R μ μ μ μ I g + igμν d X R d X νR − id X R d X νI + id X I d X νR + d X I d X νI 2 μν 1 R μ μ μ μ I + gμν d X R d X νR + id X R d X νI − id X R d X νI + d X I d X νI − igμν 2 μ μ μ μ R I = gμν d X R d X νR + d X I d X νI + gμν d X R d X νI − d X I d X νR . 41) dω2 = Using the symmetries G ν¯ μ = G μν¯ and G μν ¯ = G ν μ¯ we can write I I = i G ν¯ μ − G ν μ¯ = i G μν¯ − G μν .

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Pseudo-Complex General Relativity by Peter O. Hess, Mirko Schäfer, Walter Greiner


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