# On the vDVZ Discontinuity in Massive Conformal Gravity

Authors: F. F. Faria
Journal: Advances in High Energy Physics
 (2019)

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## Abstract

By taking the massless limit of linearized massive conformal gravity coupled to a source, we show that the theory is free from the vDVZ discontinuity. This result is confirmed when we take the massless limit of the gravitational potential of the theory, which is shown to be finite at the origin.


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## Body

## 1. Introduction

Recently, it has been explicitly shown that the classical theory of massive conformal gravity (MCG) has a negative energy massive tensor field [1], which is a common feature of theories of gravity with fourth-order derivative terms in their actions [2]. The problem with such field is that it can produce instabilities on the classical solutions of the theory [3]. In addition, the theory may present a discontinuity in the limit as the mass of the field goes to zero.At the quantum level, the corresponding quantum state of a negative energy field is taken to have negative energy or negative norm [4]. The requirement that the theory be renormalizable makes it necessary to choose the negative norm ghost state over the negative energy state. This choice spoils the unitarity of the S-matrix unless the position of the ghost pole is gauge-dependent [5].In quantum MCG, the negative energy massive tensor field gives rise to a massive spin-2 ghost state. The presence of this ghost state ensures the renormalizability of the theory [1, 6]. In addition, it has recently been shown that the position of the pole of the MCG ghost state depends on the conformal gauge [7], which means that the theory is not only renormalizable but also unitary. Hence, MCG is a consistent theory of quantum gravity.The aim of this work is to verify part of the consistency of classical MCG. Due to the extent and complexity of the calculations on the stability of the classical MCG solutions, we will leave them for future works. Here we focus on studying the continuity of the theory in the massless limit. In Section2 we describe MCG in the presence of matter fields. In Section 3 we analyze the particle content of the theory. In Section 4 we take the massless limit of the theory and check whether it is continuous or not. In Section 5 we evaluate the relation between the continuity of the theory and the behavior of its gravitational potential at the origin. Finally, in Section 6 we present our conclusions.


## 2. Massive Conformal Gravity

Let us consider the total MCG action (here we consider units in whichc=ħ=1) [8](1)Stot=1k2∫d4x-gφ2R+6∂μφ∂μφ-12m2CαβμνCαβμν+∫d4xLm,where k2 is a constant whose value will be determined in Section 5, m is a constant with dimension of mass, φ is a scalar field called dilaton,(2)CαβμνCαβμν=RαβμνRαβμν-4RμνRμν+R2+2RμνRμν-13R2is the Weyl tensor squared, Rαμβν is the Riemann tensor, Rμν=Rαμαν is the Ricci tensor, R=gμνRμν is the scalar curvature, and Lm=Lm(gμν,Ψ) is the Lagrangian density of the matter field Ψ. Besides being invariant under coordinate transformations, action (1) is also invariant under the conformal transformations(3)g~μν=e2θxgμν,φ~=e-θxφ,L~m=Lm,where θ(x) is an arbitrary function of the spacetime coordinates.It is worth noticing that under the transformations(4)g^μν=φ2gμν,φ^=1,action (1) takes the form(5)S^tot=1k2∫d4x-g^R^-12m2C^αβμνC^αβμν+∫d4xL^m.In addition, the MCG line element ds2=(φ2gμν)dxμdxν reduces to the general relativistic line element(6)ds^2=g^μνdxμdxν,and the MCG geodesic equation(7)d2xλdτ2+Γλμνdxμdτdxνdτ+1φ∂φ∂xρgλρ+dxλdτdxρdτ=0reduces to the general relativistic geodesic equation(8)d2xλdτ2+Γ^λμνdxμdτdxνdτ=0, where(9)Γλμν=12gλρ∂μgνρ+∂νgμρ-∂ρgμνis the Levi-Civita connection. Thus, in the absence of matter, MCG is equivalent to the Einstein-Weyl gravity. In the presence of matter, however, the two theories are not equivalent, since the dilaton field φ reappears in the transformed matter Lagrangian density L^m=Lm(φ-2g^μν,Ψ).Since the integral of the Euler density(10)E=RαβμνRαβμν-4RμνRμν+R2is topologically invariant, we can write (1) as(11)Stot=1k2∫d4x-gφ2R+6∂μφ∂μφ-1m2RμνRμν-13R2+∫d4xLm.By varying (11) with respect to gμν and φ, we obtain the MCG field equations(12)φ2Gμν+6∂μφ∂νφ-3gμν∂ρφ∂ρφ+gμν∇ρ∇ρφ2-∇μ∇νφ2-1m2Wμν=12k2Tμν,(13)∇μ∇μ-16Rφ=0,where(14)Wμν=∇α∇βCμανβ-12RαβCμανβis the Bach tensor,(15)Gμν=Rμν-12gμνRis the Einstein tensor,(16)∇ρ∇ρφ=1-g∂ρ-g∂ρφis the generally covariant d’Alembertian for a scalar field, and(17)Tμν=2-gδLmδgμνis the matter energy-momentum tensor.Taking the trace of (12), we find(18)6φ∇μ∇μ-16Rφ=12k2T,where T=gμνTμν. The field equations (13) and (18) require that T=0, which means that MCG couples consistently only to conformally invariant matter fields. This is not a problem because it is well known that all matter fields are conformally invariant in the Standard Model of particle physics. The massless matter fields are naturally conformally invariant whereas the massive matter fields become conformally invariant after the introduction of the Higgs field.


## 3. The Particle Content

Using the weak-field approximations(19)gμν=ημν+khμν,(20)φ=1+kσ,and keeping only the terms of second order in the fields hμν and σ, we find that (11) reduces to the total linearized MCG action(21)S¯tot=∫d4xL¯EHhμν+2σR¯+6∂μσ∂μσ-1m2R¯μνR¯μν-13R¯2+∫d4x12khμνT∘μνT,where T∘μνT is the traceless part of the flat fermion energy-momentum tensor (see the appendix),(22)R¯μν=12∂μ∂ρhρν+∂ν∂ρhρμ-∂ρ∂ρhμν-∂μ∂νhis the linearized Ricci tensor,(23)R¯=∂μ∂νhμν-∂μ∂μhis the linearized scalar curvature, and(24)L¯EHhμν=-14∂ρhμν∂ρhμν-2∂μhνρ∂ρhμν+2∂μhμν∂νh-∂μh∂μhis the linearized Einstein-Hilbert Lagrangian density, with h=ημνhμν.In order to obtain a second-order derivative form, we choose the method of the decomposition into oscillator variables [9] and write (21) as(25)S¯tot=∫d4x14hμν□qμν-12hμν∂μ∂ρqρν+14hμν∂μ∂νq+14h∂μ∂νqμν-14h□q+m216hμνhμν-m28hμνqμν+m216qμνqμν-m216h2+m28hq-m216q2+2hμν∂μ∂νσ-h□σ-6σ□σ+12khμνT∘μνT,where □=ημν∂μ∂ν and q=ημνqμν. Varying this action with respect to qμν gives (the parentheses in the indices denote symmetrization)(26)qμν=hμν-2m2□hμν-2∂ρ∂(μhν)ρ+∂μ∂νh+13ημν∂ρ∂σhρσ-13ημν□h,and with this the field equations obtained from (25) are equivalent to the field equations obtained from (21). Finally, with the change of variables(27)hμν=Aμν+Bμν,(28)qμν=Aμν-Bμν,we find the action(29)S¯tot=∫d4xL¯EHAμν-L¯EHBμν+m24BμνBμν-B2+2Aμν∂μ∂νσ-A□σ+Bμν∂μ∂νσ-B□σ-6σ□σ+12kAμνT∘μνT+12kBμνT∘μνT,where A=ημνAμν and B=ημνBμν.In order to reveal the complete particle content of (29), we consider the transformations(30)Aμν=Aμν′+1m∂μVν+∂νVμ+2ημνσ,(31)Bμν=Bμν′-1m∂μVν+∂νVμ-2ημνσ,which gives(32)S¯tot=∫d4xL¯EHAμν′-L¯EHBμν′+m24B′μνBμν′-B′2+14FμνFμν+3m2B′σ-2mσ∂μVμ-mB′μν∂μVν-B′∂μVμ-6σ□+2m2σ+12kA′μνT∘μνT+12kB′μνT∘μνT,where Fμν=∂μVν-∂νVμ.Taking into account the conservation and the traceless condition ofT∘μνT, we can see that (32) is invariant under the gauge transformations(33)Aμν′→Aμν′+∂μξν+∂νξμ,(34)Bμν′→Bμν′+∂μχν+∂νχμ,Vμ→Vμ+mχμ,(35)Bμν′→Bμν′+2mζημν,Vμ→Vμ+∂μζ,σ→σ-mζ,where ξμ and χμ are arbitrary spacetime dependent vector fields, and ζ is an arbitrary spacetime dependent scalar field. Classically, we may impose the gauge conditions(36)∂μAμν′-12∂νA′=0,(37)∂μBμν′-12∂νB′-mVν=0,(38)∂μVμ-m12B′+3σ=0,which fix the gauge freedoms up to residual gauge parameters satisfying the subsidiary conditions(39)□ξμ=0,(40)□-m2χμ=0,(41)□-m2ζ=0.By substituting (36)-(38) into (32) and integrating by parts, we obtain the diagonalized action(42)S¯totd=∫d4x14A′μν□Aμν′-18A′□A′-14B′μν□-m2Bμν′+18B′□-m2B′-12Vμ□-m2Vμ-6σ□-m2σ+12kA′μνT∘μνT+12kB′μνT∘μνT,which is dynamically equivalent to action (21). This action contains a positive energy massless tensor field Aμν′, a negative energy massive tensor field Bμν′, a negative energy massive vector field Vμ, and a negative energy massive scalar field σ. In order to identify which of these fields have physical degrees of freedom, we note that Aμν′ has 10 degrees of freedom, Bμν′ has 10 degrees of freedom, Vμ has 4 degrees of freedom, and σ has 1 degree of freedom, giving a total of 25 (=10+10+4+1) degrees of freedom. Conditions (36)-(41) reduce the degrees of freedom by 18 (=4+4+1+4+4+1). Therefore, MCG has only 7 (=25-18) physical degrees of freedom, 2 for the massless field Aμν′ and 5 for the massive field Bμν′.


## 4. The Massless Limit

In the massless limitm→0, action (32) reduces to(43)S¯tot=∫d4xL¯EHAμν′-L¯EHBμν′-6σ□σ+14FμνFμν+12kA′μνT∘μνT+12kB′μνT∘μνT.It is not difficult to see that this action is invariant under the gauge transformations(44)Aμν′→Aμν′+∂μξν+∂νξμ,(45)Bμν′→Bμν′+∂μχν+∂νχμ,(46)Vμ→Vμ+∂μζ.Thus, by imposing the gauge conditions(47)∂μAμν′-12∂νA′=0,(48)∂μBμν′-12∂νB′=0,(49)∂μVμ=0to (43) and integrating by parts, we obtain the diagonalized action(50)S¯totd=∫d4x14A′μν□Aμν′-18A′□A′-14B′μν□Bμν′+18B′□B′-12Vμ□Vμ-6σ□σ+12kA′μνT∘μνT+12kB′μνT∘μνT,which contains a positive energy massless tensor field Aμν′ with 10 degrees of freedom, a negative energy massless tensor field Bμν′ with 10 degrees of freedom, a negative energy massless vector field Vμ with 4 degrees of freedom, and a negative energy massless scalar field σ with 1 degree of freedom.The gauge conditions (47)-(49) fix the gauge freedoms up to residual gauge parameters satisfying the subsidiary conditions(51)□ξμ=0,(52)□χμ=0,(53)□ζ=0.Conditions (47)-(49) and (51)-(53) reduce the 25 degrees of freedom of the MCG massless limit by 18, giving a total of 7 physical degrees of freedom, 2 for the massless tensor field Aμν′, 2 for the massless tensor field Bμν′, 2 for the massless vector field Vμ, and 1 for the massless scalar field σ. Hence, the number of physical degrees of freedom is preserved in the massless limit of the theory. Two of the five degrees of freedom of the massive tensor field go into the massless vector field, and one goes into the massless scalar field. Since the scalar and vector fields do not couple to the source, MCG is free of the van Dam-Veltman-Zakharov (vDVZ) discontinuity [10, 11].It is worth noticing that MCG differs from theories of gravity with only a massive tensor field, for which general relativity (GR) should be recovered in the massless limit. Usually it is the absence of this recovery that is associated with the vDVZ discontinuity. However, the real meaning of the vDVZ discontinuity is that the massless limit of a massive theory is not equivalent to the massless theory, which violates the physical continuity principle [12]. That is why it is so important for a massive theory to be free from the vDVZ discontinuity.Recently, it was proposed that the vDVZ discontinuity of a local gravitational theory is closely related to the finiteness of the gravitational potential at the origin [13]. If this proposal is valid, then the MCG potential should have a singularity at the origin, which we will show to be not true in the next section.


## 5. The Newtonian Singularity

The variation of (42) with respect to A′μν and B′μν gives the field equations(54)□Aμν′-12ημνA′=-kT∘μνT,(55)□-m2Bμν′-12ημνB′=kT∘μνT.Taking the traces of (54) and (55) and replacing them back, we obtain(56)□Aμν′=-kT∘μνT,(57)□-m2Bμν′=kT∘μνT,whose general solutions are given by(58)Aμν′=k∫d4p2π4eip·xp2T∘μνTp,(59)Bμν′=-k∫d4p2π4eip·xp2+m2T∘μνTp,where(60)T∘μνTp=∫d4xe-ip·xT∘μνTxis the Fourier transform of the traceless part of the source.In the case of a point particle source with massM at rest at the origin, for which T∘μνf(x)=Mδμ0δν0δ3(x), we have(61)T∘μνT=Mδμ0δν0+14ημνMδ3x,where we consider ημν=diag(-1,+1,+1,+1). Substituting the 00 component of (61) into (58) and (59), we find the general solutions(62)A00′=k3M4∫d3p2π4eip·xp2=k3M414πr,(63)B00′=-k3M4∫d3p2π4eip·xp2+m2=-k3M4e-mr4πr.It then follows from (27), (30), and (31) that(64)h00=A00′+B00′=k3M16πr1-e-mr.Finally, noting that 2ϕ=-kh00, we find the MCG potential(65)ϕr=-GMr1-e-mr,where we chose k2=32πG/3 in order for (65) to agree with the Newtonian potential in the limit where m tends to infinity. It is not difficult to see that (65) is finite at the origin, which is a necessary condition for the renormalizability of the theory [14]. In addition, the massless limit provides a zero-order term of e-mr≈1 in the MCG potential, which confirms that the theory is free of the vDVZ discontinuity.


## 6. Final Remarks

We have found that MCG contains only two linearized fields with physical degrees of freedom: the usual positive energy massless tensor field and a negative energy massive tensor field. In the massless limit, the number of physical degrees of freedom of the theory remains the same, with the massive tensor field being decomposed into massless tensor, vector, and scalar fields. The absence of coupling between the vector and scalar fields and the source makes the theory free of the vDVZ discontinuity. In addition, it was shown that the MCG potential is singularity free, which indicates that the vDVZ discontinuity is not directly related to the finiteness of the gravitational potential at the origin.



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*Source: 7013012-2019-03-05.xml*