The Gravity Gauge Theory and Gravity Field Equation in Flat Space

In this paper, we have proposed the theory of ( ) 1 U gravity gauge, and the gravity theory has been introduced into quantum field theory. We have further given the tensor equation of gravity field in the flat space, and found the gravity field equation is the Lorentz covariant and gauge invariant. The gravity theory can be quantized and can be unified with the electroweak and strong interaction at a new gauge group ( ) ( ) ( ) 1 2 3 U SU SU ⊗ ⊗ .


Introduction
The Einstein's general theory of gravity (GR) is treated as geometry of curved space-time, which appears to provide a successful macroscopic description of all known gravitational phenomena; it is of interest to explore alternative theories that may provide a more fundamentally appealing description or suggest new experiments leading to the discovery of new phenomena [1] [2].As well known, most of the fundamental interactions in nature based on the gauge theory have been constructed to be physically sensible due to that they lead to the consistent quantum description.The gauge theories are in principle applicable up to arbitrarily high energy scales.Thus, it would be natural to seek a gauge theory structure for the gravitational interaction in which the general relativity is derived as the low energy limit.Quantum gauge theory of gravity is proposed in the framework of quantum field theory, the mathematical structures of GR in the first-order formalism and gauge theory appear very similar at classical level gauge transformation, the gravity gauge field should be introduced naturally.Otherwise, we give the equation of gravity tensor field at the flat Minkowski spacetime, and further prove the gravity field equation is the Lorentz covariant and gauge invariant.The gravity theory can be quantized and can be unified with the electroweak and strong interaction at a new gauge group ( ) ( ) ( )

The U(1) Gauge Field of Gravity
The Einstein gravitational field equation with matter is The gravitational field is the geometry field of spacetime, which is equivalent to the spacetime curve.The general theory of gravity can be reinterpreted as a field theory over flat Minkowski spacetime, the gravity can be taken as real matter field, produced by the matter motion and distribution.In the following, we shall introduce gravity field in the Minkowski spacetime, which is massless spin-2 field.In group theory, the representation of the rotation group and Lorentz group is described by a field with 2 1 s + independent components for a particle with spin 0,1, 2, s =  .For the massless spin-2 gravity field, it should be described by a tensor field ( ) In quantum field theory, the Lagrangean density of real field, complex field and Dirac spinor field are: ( ) ( ) At Equations ( 2), ( 3) and ( 4), if the local gauge is invariant, the gauge field should be introduced.We need form a gauge covariant derivation D µ to re- ( ) ( ) ( ) These gauge fields are the vector fields with spin s = 1, and corresponding to the particles , , and γ .
For the strong interaction theory of between quark and gluon, it has the ( ) gauge symmetry, and the gauge field are eight gluons vector fields ( ) In quantum gauge theory, the all gauge fields are vector fields with spin s = 1, which can only describe electromagnetic interaction, weak interaction and strong interaction, and cannot describe the gravity interaction with spin s = 2.Why the quantum gauge theory cannot describe the gravity interaction?From Equation (2) to (4), we can find the differential operator µ ∂ ap- pears alone in the Lagrangean density.When we make the ( ) the µ ∂ should be make the transformation as Equation ( 5), it only introduce the vector gauge field ( ) where ( ) is the vector gauge field with spin s = 1, and is the tensor gauge field with spin s = 2, i.e., the gravity gauge field.
For the Dirac equation we add the term µ ν ∂ ∂ , it becomes where ε is the dimensionless constant.Since the gravity is very weak, the con- the Lagrangean density of Equation ( 15) is ( ) substituting Equations ( 18) and ( 19) into the Lagrangean equation ( ) we can obtain the Equation (15).At the U(1) local gauge transformations (10) and (11), in order to make Equation ( 17) gauge invariant, we should introduce the gauge fields A µ and µν φ , they are where e and g are the coupling constants, and the Equation ( 17) becomes ( ) gauge transformations (10) and (11) the Lagrangean density L should be changed into L′ , it is ( ) ( ) the covariant derivatives D µ and D µν should be transformed as the local gauge invariance demand the Lagrangean density is invariable, i.e.,
At transformation ( ) these is then we require i.e., by Equation (34), we can give the gravity gauge transformation at ( ) the Equation (34) becomes by Equation (36), the gauge transformation of gravity is Multiplying Equation ( 15) by ( ) ) it becomes K-G equation.So, the Equation ( 15) is a relativistic field equation, and we can prove it is Lorentz covariant.
The Lorentz transformation is and its infinitesimal transformation is where µν ω is a infinitesimal parameter, the complete set of transformations µν Λ are called Lorentz group.At the Lorentz transformation (39), the transformation of Dirac spinor field ( ) where ( ) is the representation of the Lorentz group for the spinor field ( ) γ , ν γ are the Dirac matrices, and there are the following transformation relations: making the Lorentz transformation to Equation (15), it is It has the same equation form at the Lorentz transformation, i.e., Equation (15) is the Lorentz covariant.For the K-G particle of spin s = 0, its field equation is ( ) and its Lagrangean density is ( ) In order to describe the gravity interaction, the Equation ( 46) should be modified as ( ) where λ is the dimensionless constant, µ β and ν β are four-dimensional constant vectors.Since the gravity is very weak, the contribution of the new added term µ ν µ ν λβ β ∂ ∂ should be very small, there is ( ) the Lagrangean density (47) should be modified as substituting Equations ( 51) and (52) into Lagrangean equation We can obtain the Equation (48).At U(1) gauge transformations (10) and (11), the Equation (50) should be introduced the electromagnetism and gravity gauge fields (18) and ( 19), and the gravity gauge transformation (37).

The Equation of Gravity Field in Minkowski Spacetime
In Section 2, we introduce gravity field and gravity gauge transformation.In the following, we should give the equation of gravity field, which is spin s = 2 massless field.The spin s = 2 massless field µν φ generated by the energy momentum tensor T µν from a object, particle or a group of particles, they are symmetrical tensors T T We construct the following independent tensors for the spin s = 2 massless gravity field µν φ , they are where k is the gravitational constant, and g ρσ ρσ φ φ = . By derivative µ ∂ , we have ( ) , i.e., ( ) ( ) ( ) the source tensor T µν is conservative, it is by Equation ( 59) and (60), we get and Equation ( 57) becomes take 2 1 a = , we obtain ( ) if we choose the following gauge condition i.e., substituting Equations ( 66)-(69) into Equations (63), it becomes defining the new tensor µν Φ as the gravity field tensor, it is the Equation ( 64) and (70) become and the Equation ( 72) is the gravity field equation including source, and the gauge condition is (73).In the absence of sources, the free gravity field and the gauge condition become and the Lagrangean density of Equation ( 72) is then substituting Equations ( 77) and (78) into the Lagrangean equation we can obtain the free gravity field equation the Equation (80) has the plane wave solution, which is the gravitational wave, it is ( ) where 0 Φ is the amplitude, ( ) ω k is the wave vector (frequency), and e µν is the second order polarization tensor.The general solution of Equation ( 80) is ( ) In the Newton gravity, the Newtonian potential ϕ satisfies Poisson equation where G is the gravity constant, and 0 ρ is mass density, there is, the Equation (83) can be written as When 0 µ ρ = = , and a object or particle is at rest, the Equation (72) becomes comparing Equation ( 85) with (86), we have then the gravity field Equation (72) becomes with the gauge condition (75), there is For the closed system, the energy momentum tensor of the whole system satisfies the conservation law, it is The gravity field Equation (89) satisfies the condition of energy momentum conservation.
For a object or particle, its mass m, mass density ρ , velocity u µ , energy momentum tensor T u u µν µ ν ρ = , and its gravity field equation is when the object or particle is at rest, the velocity component ( ) and where 0 ρ is the rest mass density of object or particle, the solutions of Equa- tions (93) and (94) are where 1 c and 2 c are the constants, and 00 Φ is the Newtonian gravitational potential.In the nonrelativistic limit, the gravity field Equation (89) becomes the Journal of High Energy Physics, Gravitation and Cosmology Newtonian gravity equation.
For the spin Dirac field, the total Lagrangean density is For the spin s = 0, K-G field, the total Lagrangean density is, ( ) The Equations ( 98) and (99) can be described electroweak interaction, strong interaction and gravity interaction for spin s = 1/2 and s = 0 particle and field.
The free gravity field Equation ( 80) is a tensor equation, which is Lorentz covariant.In the following, we shall prove the Lagrangean density ( 76) is ( ) At the transformation (37), the gravity field gauge transformation is, where ( ) ( ) ( ) ( ) similarly, we have the gauge transformation of Lagrangean density is and the variation of action is

Conclusion
In this paper, we have proposed the gauge theory of gravity.In Dirac equation and K-G equation, they have introduced the vector gauge field, such as electroweak and strong interaction gauge field, which are vector gauge fields, and have not introduced the gravity gauge field.In order to introduce the gravity gauge metric tensor, G is Newton's gravitational constant and c is the speed of light.The energy-momentum tensor v T µ gives the motion and distribution of the matter in spacetime, producing the gravitation fieldtensor of Riemannian curved spacetime.The important properties of the Einstein gravitational field equation are: the distribution and motion of the matter determine the curved spacetime structure, and the distribution of matter can be determined by the X.Y. Wu et al. spacetime structure.

1 U
106), the variation is to field µν Φ , and the Lagrangean density is equivalent when it adds a term of four-dimension divergence.Since the variation of action is equivalent before and after the gauge invariant.By the Lagrangean density of gravity field (76) and the gravity field Equation (89), we can quantize the gravitational field with the canonical quantization or path integral quantization, which should be studied in the future.

1 U
field, we should add a term of partial derivative µ ν ∂ ∂ in Dirac equation and K-G equation.At the ( ) gauge transformation, the gravity gauge field should be introduced naturally.Otherwise, we give the equation of gravity tensor field at the flat Minkowski spacetime, and further prove the gravity field equation is the Lorentz covariant and gauge invariant.The gravity theory can be quantized and can be unified with the electroweak and strong interaction at a be studied in the future.