Evans' paper starts with what the author calls "the second Cartan structure equation",

                R^a_b = D Ù ω^a_b ,                                                                 ((1))

and with the second Bianchi identity,

                D Ù R^a_b := 0 .                                                                 ((2))

The symbol DÙ stands, in Evans' notation, for the exterior covariant derivative, ω and R are the connection and the curvature forms, respectively. Eq.((1)) represents the definition of the curvature form. The second structure equation, which follows immediately from ((1)) and from the definition of D, is given as

                R^a_b = d Ù ω^a_b + ω^a_c Ù ω^c_b .                                                 ((5))

The second Bianchi identity follows from ((5)) by exterior differentiation:

                d Ù R^a_b + ω^a_c Ù R^c_b − R^a_c Ù ω^c_b = 0.                                 ((6))

Torsion is introduced according to

                T^a = d Ù q^a + ω^a_b Ù q^b ,                                                 ((7))

with the tetrad one-forms q^a, which we interpret, according to the context, as a local orthonormal coframe.

2.2 Objections to the 'derivation' of Eqs. ((11)) and ((13))

. . . Eq.((6)) can be rewritten as

                d Ù R^a_b = j^a_b ,                                                                 ((10))

                d Ù R^{~ a}_b = j^{~ a}_b ,                                                                 ((11))

where

                j^a_b = R^a_c Ù ω^c_b − ω^a_c Ù R^c_b ,                                                 ((12))

                j^{~ a}_b = R^{~ a}_c Ù ω^c_b − ω^a_c Ù R^{~ c}_b .                                         ((13))

The tilde denotes the Hodge dual [1-20] of the tensor valued two-form

                R^a_bμν = − R^a_bνμ , . . .                                                                 ((14))

While it is true that ((10)) and ((12)) are a rewriting of ((6)), this is false for ((11)) and ((13)). Eqs.((11)) and ((13)) do not follow from differential geometry. Especially the combination of ((11)) and ((13)), namely

                d Ù R^{~ a}_b = R^{~ a}_c Ù ω^c_b − ω^a_c Ù R^{~ c}_b ,

cannot be derived from the second Bianchi identity ((6)) and does not hold in general. Indeed, DÙR^a_b=0 does not imply DÙR^{~ a}_b=0 , since taking the Hodge dual doesn't commute with D.

2.3 The electromagnetic sector of Evans' theory, the index type mismatch

Eqs.((17)) and ((18)) relate, according to Evans, a generalized electromagnetic field strength F^a and a potential A^a to the torsion and the tetrad, respectively,

                F^a = A^(o) T^a ,                                                                                 ((17))

                A^a = A^(o) q^a ,                                                                                 ((18))

where A^(o) is, presumably, a universal constant. Evans' next but one equation is the first Bianchi identity,

                d Ù T^a = R^a_b Ù q^b − ω^a_b Ù T^b .                                                 ((20))

Let us look at Evans' motivation for his choices ((17)) and ((18)). Evans supposed an analogy of A^a and F^a with the Maxwellian potential one-form A and the field strength two-form F according to

                A → A^a ,                 F → F^a .                                                 (1)

In Maxwell's theory, F = dÙA is then put in analogy to Cartan's first structure equation (definition of the torsion) T^a = DÙq^a.

One serious objection is based on the fact that Evans has not given any information about the relations between the concrete electromagnetic fields F=(E,B) in physics and his quadruple of two-forms F⁰, F¹, F², F³ and the associated quadruple of one-forms A⁰, A¹, A², A³. Evans himself ignores that problem of attaching a superscript 'a' to all electromagnetic field quantities without giving a satisfying explanation of that index surplus.

Evans' attempts to interpret (1) appropriately doesn't even work in the case of a simple circularly polarized plane (cpp) wave. His considerations are contradictory and incomplete, and we see no way to define F⁰, F¹, F², F³ and A⁰, A¹, A², A³ even for a bit more complicated field as, e.g., a superposition of different cpp waves travelling in different directions. This is not a mathematical error, but a physical gap, and we doubt that one can find a general solution of that problem. Anyway, Evans never presented such a solution.

Therefore, Evans' analogy F ↔ T^a, for a=0,1,2,3, causes a type mismatch between the vector valued torsion two-form T^a and the scalar valued electromagnetic field strength two-form F. The analogous holds for A ↔ q^a , for a=0,1,2,3 as well.

Evans' whole SCR paper is based on the dubious assumption that (1), and thus ((17)) and ((18)), make sense in physics. Without a concrete physical interpretation of (1), Evans' whole SCR paper is null and void, regardless whether there are other (mathematical) errors or not.

Moreover, as it was with the second Bianchi identity, so here, Evans' equations ((23)), ((16)), and ((17)), if combined, lead to

                d Ù T^~a = R^~a_b Ù q^b − ω^a_b Ù T^~b,.                                                 (2)

Eq.(2), contrary to Evans' statement, is not a consequence of the first Bianchi identity and does not hold in Cartan's differential geometry. It represents an additional ad hoc assumption.

2.4 The gravitational sector of Evans' theory, objections to Eq. ((30))

Eq.((29)) is the field equation of Einstein's general relativity theory,

                G^μν = k T^μν ,                                                                                 ((29))

after which Evans writes:

. . . Eq.(29) is well known, but much less transparent than the equivalent Cartan equation

                D Ù ω^a_b = k D Ù T^a_b := 0 . . .                                                                 ((30))

Eq.((30)) is certainly not equivalent to ((29)), and it cannot be a part of general relativity theory, be it tensorial or in Cartan form. The reason is very simple: T^a_b in ((30)) has to be a one-form. Therefore it should be integrated over a world-line and not over a hypersurface of four-dimensional spacetime, as it is done with the energy-momentum tensor. In other words, Eq.((30)) is simply incorrect since the energy-momentum in exterior calculus is a covector-valued three-form (or, if its Hodge dual is taken, a covector-valued one-form).

2.5 The wrong `curvature vector' and the dubious potential equation

Now Evans turns to the combined equation ((5)) and ((10)),

                d Ù (d Ù ω^a_b + ω^a_c Ù ω^c_b) = j^a_b ,                                                                 ((31))

with his comment that in vector notation it gives, in particular,

                Ñ · R(orbital) = J⁰ ,                                                                                 ((32))

with

                R(orbital) = R⁰₁⁰¹ i + R⁰₂⁰¹ j + R⁰₃⁰¹ k                                                 ((33))

It is evident that ((32)) is not equivalent to ((31)), if only for the simple reason that ((31)) involves a three-form, where all indices must be different from each other, while ((32)), with the divergence operator, involves summation over repeated indices. In ((37)), Evans evidently attempts to calculate the (0i) component of the curvature form:

                R^a_b = − ¹/_c ^∂ωa_b/_∂t − Ñω^0a_b − ω^0a_c ω^c_b + ω^a_c ω^0c_b .                                 ((37))

This is again incorrect. In fact, starting from ((5)), the calculation of the components (R_0i)^a_b , for i=1,2,3 , yields

                (R_0i)^a_b = ∂_b(ω_i)^a_b − ∂_i(ω₀)^a_b + (ω₀)^a_c (ω_i)^c_b − (ω_i)^a_c (ω₀)^c_b .                 (3)

Raising the index 0 of ω₀ in the term ∂_i(ω₀)^a_b, as Evans does, is illegitimate, because the metric component g⁰⁰ of the Schwarzschild metric, which Evans considers, is not a constant function of the variables xⁱ. The sign in front of the time derivative in ((37)) is also wrong.

Then in ((42)), when restricting to the static case, Evans 'forgets' one of the quadratic terms of his erroneous ((37)):

                R^a_b = − Ñω^0a_b + ω^a_c ω^0c_b .                                                                 ((42))

Again, this is wrong, since now R^a_b is not in the Lie algebra of the Lorentz group. The same error applies to ((44)), where ω^0a_b is substituted by Φ^a_b ,

                R^a_b = − ÑΦ^a_b + ω^a_c Φ^c_b .                                                                 ((44))

Then Evans adds:

. . . It is convenient to use a negative sign for the vector part of the spin connection, so

                R^a_b = − (Ñ Φ^a_b + ω^a_c Φ^c_b) ...                                                                 ((45))

This is another evident and grave error. Since the sign of the connection form is not a question of 'convenience' in the theory of gravity, where the curvature tensor contains both linear and quadratic terms in the connection. Changing the sign of the connection forms changes its curvature in an essential way.

Using incomprehensible and sometimes evidently wrong reasonings, such as skipping one term when going from ((37)) to ((42)), as we saw above, Evans postulates a potential equation ((63)) for an unidentified variable Φ for the case of the Schwarzschild geometry. We shall discuss the "electromagnetic analogue of Eq.(63)", namely Eq. ((65)), in the following section.

3. The Resonance Catastrophe

"It is shown in this section that Eq.(31) produces an infinite number of resonance peaks of infinite amplitude in the gravitational potential [2-20]. To show this numerically, Eq.(31) is developed in vector notation . . . "

This is an unfounded claim followed by no proof and no numerical results either. In addition the claim is erroneous as we shall see below. At the very end of his article Evans at last arrives at the topic `resonance' that is already announced in the title of his paper. He reports:

. . . The electromagnetic analogue of Eq. (63) is

                ^∂²φ/_∂r² − ¹/_r ^∂φ/_∂r + ¹/_r² φ = − ^ρ(0)/_εo cos(κ r)                                                 ((65))

which has been solved recently using analytical and numerical methods [2-20]. These solutions for φ and Φ show the presence of an infinite number of resonance peaks, each of which become infinite in amplitude at resonance.

Evans' efforts (together with H. Eckardt) with respect to the resonance of ((65)) are available on his website. He attempts to find values of the parameter κ that yield resonances of the right hand side of ((65)) with the eigensolutions of this Euler type ordinary differential equation (ODE). However, the eigensolutions of the associated homogeneous ODE are well-known. The eigenspace is spanned by the special solutions

                φ₁ = r         and         φ₁ = r log r .                                                                 (4)

Resonance means that the driving term cos(κ r) belongs to the eigenspace, i.e., is a linear combination, with constant coefficients, of the functions φ₁ and φ₂ for any value of the parameter κ. Obviously this is not the case.

Moreover, the general solution of ((65)) can be calculated. With the help of Mathematica, we obtain

                φ(r) = c₁ r + c₂ r log r − ^ρ(0)/_εo ^r/_κ Si(κr) ,                                                 (5)

where Si( ) denotes the sine integral function defined by

                Si(z) := ∫_o^{z sin t}/_t dt                                                                                 (6)

for real z satisfying the estimate

                | Si(z) | ≤ min(|z|,2) .                                                                                 (7)

The graph of Si(z) is displayed in Fig.1, Graph of the sine integral Si(z)

Thus, the κ dependent part of the solution (5) satisfies the estimate

                | ^ρ(0)/_εo ^r/_κ Si(κr)| ≤ ^ρ(0)/_εo min (r², ^2r/_κ) .                                                 (8)

Consequently, the general solution of ((65)) is bounded for all real values of κ and r. For no value of κ, we will have a resonance of the right-hand-side of ((65)) with the eigensolutions (4).

However, Evans & Eckardt apply a lot of their specific 'new math': an inadmissible rotation of the complex plane of eigenvalues by an angle of 90° and multiplication by the imaginary unit i, among other peculiarities, see [3] for details. Evans & Eckardt succeed in detecting resonance peaks, unattainable to all who are using standard mathematics only.

There are no resonance peaks at all, quite apart from the errors
in Evans' theory previous to his equations ((63)) and ((65)).