Abstract
A couple of quantum gravity theories were proposed to make theoretical predictions about the behavior of gravity. The most recent approach to quantum gravity, called Etheory, is proposed mathematical, but there is not formulated much about what dynamics of gravity this theory proposes. This research paper treats the main results of the application of Etheory to General relativity involving conservation laws and scattering of particles in presence of gravity. Also the lowenergy limit of this theory is shown.1. Introduction
Quantum gravity theories focus on the concept of a quantization of General Relativity which has no UVdivergences. Such theories become relevant a few Planck lengths after the Big Bang due to the high energy densities that were present in this time period. Many approaches of quantum gravity were proposed in research literature. The most popular approach to renormalizable quantum gravity is String theory, which assumes that there are additional dimensions in the universe. Moreover, it uses the concept of supersymmetry. Elementary particles are not pointlike; they have a form of a string or membrane such that the momentum uncertainty remains finite independent on the backgrounds in which these objects are. However, these concepts are still not validated experimentally.
Recently, a new approach of quantum gravity was developed (Linker 2016). This approach uses a semigroup called “Esemigroup” to discretize the spacetime structure. By the introduction of a generalized curvature measure, the action of General Relativity can be rewritten. The key observation to do this is that the chain complex in differential geometry of smooth manifolds (the deRham complex on Riemannian manifolds or smooth fiber bundles) is losing the exactness if the space has nonvanishing curvature. Causal Dynamical Triangulation (CDT) has similarities with this theory (Ambjørn 2013). With CDT the spacetime structure is also formulated discrete (Loll 1998). Here, the key ingredient is the Regge calculus that provides a proper discretization of the spacetime (Immirzi 1997). Despite the large efforts of quantum gravity theories in the last decades it has to be made clear which quantum gravity theories predict regarding gravity on microscopic scales.
This research paper shows how Etheory can be applied to a scalar boson which underlies gravitational effects in 4dimensional spacetime. The lowenergy limit, conservation laws and the perturbative calculation of scattering amplitudes are shown. With these considerations the general procedure of an application of Etheory to gravitational physics called “Egravity” is made clear. Similarities between this quantum gravity theory and Topological Dipole Field Theory (Linker 2015) are also shown in this research paper. Topological Dipole Field Theory (TDFT) is a model that describes a modification of the dynamics of gauge bosons which implies distinct behavior of quantum fluctuations.
2. Theory
The basic concept of Egravity ist the Esemigroup . Assuming that the 4dimensional spacetime can be triangulated by simplices. Then, this Esemigroup has the generators for the 4dimensional spacetime. Here, the reason for the choice of exactly five generators is that 4dimensional simplices have five corners. When multiplying some generators one has elements
that represent lines between corners generated by in a geometrical sense. Similary, triangles and its higherdimensional generalizations can be realized by multiplying the corresponding generators (Property (i) of Esemigroups). Also, a simplex might not be welldefined (Property (ii) of Esemigroups). When a simplex is build up on two identical corners, it is not welldefined (Property (iii) of Esemigroups). Clearly, arbitrary simplex elements, where corners are labeled by numbers, are not changing when the labeling numbers are interchanged (Property (iv) of Esemigroups).
Curvature arises from simplices (or more general: subspaces of topological spaces) that are not welldefined; this leads to a loss of exactness in a chain complex. A very important function that is used in Egravity theory is the indicator function . This indicator function has the value 0 if it is applied on an empty set and 1 otherwise. It holds for the generalized curvature 2form on a simplex generated by the generators the formula
where is the corresponding coboundary operator. May be the set of all simplices, then the action of quantum General Relativity reads:
Here, is a coupling constant and the operation denotes the evaluation at the simplex . It is easy to prove the lowenergy limit of the action (2). Let be and with metric tensor and ist determinant . Then the expression denotes the average curvature measure; this measure can be identified with the Ricci scalar. Also the Ricci scalar can be regarded as proportional to the directionaveraged Riemann curvature tensor weighted with metric tensor, i.e. .
An example of a quantum gravity theory with matter sources is the gravitational theory. The action of the nongravitational theory has the form:
In this action, is a coupling constant and is the 0form scalar field. It is easy to include gravity in the action (3). Continuum integrals have to be replaced by a sum over a discrete set of simplices (similar to the discretization of integrals in finite element methods). It is obvious to set:
To rewrite the kinetic energy term of (3) one has to transform ordinary directional derivatives to derivatives in direction of outward normal vectors in simplices. From linear algebra it is known that a linear combination of field quantities on a simplex surface element (dependent on the triangulation that is used) yields a directional derivative. By using the relation , where the superscript denotes that the factor is omitted and are the transformation factors that depend on the triangulation, one obtains:
Because of the fact (field values are vanishing on empty sets) one can also write any quantum field as with , where the superscript denotes that this quantum field exists independent on the equaliser set (it exists even on empty sets). With this decomposition, one has the information about gravity included only in the indicator function. Finally, the action (3) in presence of gravity can be written as:
The term contains all information about the coupling of matter with the gravitational field, i.e. products of indicator functions with matter field. It is clear that the total action of Egravity with spin0 boson has the form: . Only the term includes boson selfinteractions and gravitational interactions.
May be the set of all equalizers that are possible in the set , one has the following path integral for Egravity:
The Feynman propagator (7) is a path integral over a set of inhomogenous spacetime strucutres. Local translations in space and time yield different structures of spacetime. This implies a nonconservation of energy and nonconservation of momentum by Noether’s theorem. Spinangularmomentum is also not conserved by Noether’s theorem, because local rotation of simplices also generate a different structure of spacetime in general. Only on length and time scales large in comparison with Planck length and Planck time, energymomentum and spinangularmomentum is covariantly conserved; by averaging up inhomogenities and anisotropies of spacetime, the effect of inhomogenity and anisotropy becomes smaller such that it can be assumed to be conserved in a covariant way.
Scattering amplitudes from Egravity can be computed by expanding the factor of the propagator (7) in Taylor series. One can perform the following decompositions:
While is a pure gravityboson coupling term, describes ordinary boson selfinteractions as well as gravitational effects. Since the gravity field is governed by a nongaussian distribution, nonvanishing higher stochastic moments are possible. Therefore, it is difficult to draw gravitational interactions in Feynman diagrams; these interactions have to be computed nonperturbatively. However, a perturbative expansion with gravitational effects contains also a vertex with only one ingoing boson and only one outgoing boson due to interactions generated by .
Such a type of interaction vertex also occurs in TDFT. In the case of TDFT, an interaction generated by a single gauge boson correspond to a quantum fluctuation occuring while the gauge boson propagates. Also in Egravity, a gravitational selfinteraction of a boson (or more general: a particle) is an interaction very similar to a quantum fluctuation in TDFT. Fluctuations in particle energy and particle momentum can be induced by TDFT interactions as well as by gravitational interactions.
3. Conclusions
Egravity is a quantum field theory, where basic integrals of motion like energy are not conserved in general. Only in the lowenergy regime these integrals of motions can exist. Scattering processes predicted by Egravity contain also selfinteractions of particles due to gravity. This modifies the behavior of quantum fluctuations in a similar way as TDFT does. Gravitational modifications of quantum fluctuations apply on all elementary particles and gauge bosons and not only on gauge bosons.
References
Linker, P. “Foundations of ETheory”. The Winnower, 2016, 3:e145350.06184. doi: 10.15200/winn.145350.06184. URL: https://www.thewinnower.com/papers/3339foundationsofetheory
Ambjørn, J. et al. “Trees and spatial topology change in CDT”. J. Phys. A: Math. Theor. ,2013, 46: 315201. doi: 10.1088/17518113/46/31/315201
Loll, R ."Discrete Approaches to Quantum Gravity in Four Dimensions". Living Reviews in Relativity, 1998, 1: 13. doi:10.12942/lrr199813. arXiv:grqc/9805049. Bibcode: 1998LRR.....1...13L
Immirzi, G. „Quantum Gravity and Regge calculus“. Nucl.Phys.Proc.Suppl. , 1997, 57: 6572. doi: 10.1016/S09205632(97)00354X
Linker, P. „Topological Dipole Field Theory“. The Winnower, 2015, 3:e144311.19292. DOI: 10.15200/winn.144311.19292
Showing 9 Reviews

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Hi Patrick, usually elements of the group SU(2) are used to label the vertices of simplexes within the context of Quantum Gravity. Why use a semisimple group S? In what way does this alter the results compared with SU(2) labels?

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Its good paper but I do not understand perfictly why Only in the lowenergy regime these integrals of motions can exist and why not conserved ?

The general theory has not the ordinary continuous spacetime. Quantum field theory is reformulated to a discrete theory in this case.
Note that Noether's Theorem states: For every continuous(!) symmetry a conserved quantity exists.
Even because of this discrete System, translations and rotations can be performed also only discrete, not continuous. Every simplex that builds up the spacetime Looks different in general. Therefore spacetime is inhomogenous.
In continuum Limit one can indeed find continuous symmetries and therefore quantities like energy and momentum are conserved.

This theory has no gravitons. There is simply the nonhomogenous spacetime which mediates gravitational interaction. Therefore, (gravitational) energy is coming from the spacetime which can be "elastically compressed".



0
Being a Private Pilot, Commercial Student and Aerobatic Course Student, I am particularly mindful of the energy of gravity.
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, there are some of my kindred Christians who deny its reality? 
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The author claims a quantum theory of gravity. If this were even close to being correct, the article would be published in Nature. The author makes no attempt to connect these thoughts to anything that can be measured, or really any attempt to write a full theory. It would be wise that he first begins with demonstrating how it makes the all same predictions as general relativity in the classical limit, before trying to invent a new theory

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It is a wonderful paper. I liked your connection to E Theory to Topological Dipole Field Theory and Quantum Gravity (space time structure).

0
Nice Patric but i have a doubt , how the gravity will behave in extra dimensions time ?

If Etheory is applied to a spacetime with more than 3+1 dimensions, gravity does not behave much different than in the 3+1 dimensional case. But theoretically, in additional dimensions, the probability of wormholes might increase.

yeah , i met a community in my journeys they are handling more than four thousands time dimensions and its mathematics ,entirely different ,not only that but also the higher dimensional aspect of relativity and its explanation...really i was stunned ..

hi Patric i think quantum gravity is related to distributed time..

hi Patric i think quantum gravity is related to distributed time..



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It's really a good approach and interesting paper but I couldn't understand that why basic integrals of motion are not conserved. Hoping for more work from you. Best of luck. :)

Integrals of motions are conserved (covariantly) on large length and time scales (lowenergy limit). The nonconservation of energy and momentum is caused by the inhomogenity of spacetime on small length and time scales (Noether's theorem).


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An interesting work by Patrick Linker

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Good,i hope you can do much better than this.
The world need people like you.
License
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I don't use a semisimple Group; I am using a semigroup. A semigroup is a Group without identity and inverse element property.
The SU(2) Group appears in Loop Quantum gravity to describe spin Networks. It can also describe some simplex structures, but my Approach with a semigroup is a new one. The Esemigroup covers General simplices that also lead to loss of exactness in chain complexes (most chain complexes treating simplexlike structures). Exactly the loss of exactness allows to define curvature.