We present a two-part investigation of wormhole solutions in four-dimensional conformal (Weyl) gravity. Part I: We compute the Bach tensor B⏛⏜ for the Morris–Thorne wormhole metric with zero tidal force (Φ=0) and constant shape function b (r) =r₀, using a two-step covariant divergence method implemented in Python/SymPy. The result is verified to satisfy the tracelessness identity g^μνB⏛⏜=0. All four diagonal components are proportional to r₀² and vanish only when r₀=0 (flat Minkowski space). Hence the simplest Morris–Thorne wormhole is not a vacuum solution of pure conformal gravity. Part II: We show that Hamada's radial running coupling, which replaces the constant coupling t² by the running quantity t̄² (r) =1/β₀ ln (r²/r₀²), modifies the Bach equation to α (r) B⏛⏜+D⏛⏜=0 with α (r) =β₀ ln (r²/r₀²). Near the throat (r→r₀⁺) the effective coefficient α→0⁺ and the induced quantum stress-energy diverges, automatically satisfying the flare-out condition b' (r₀) <1. A linearised boundary value problem confirms the existence of a non-trivial shape function perturbation. Thus conformal gravity à la Hamada admits traversable wormholes without exotic matter, with the throat radius r₀∼ξ_Λ=1/ΛQG∼10⁻³⁵ m.
Yuri N. Berdinsky (Tue,) studied this question.