Warped anti-de Sitter (WAdS)/warped conformal field theory (WCFT) correspondence is an interesting realization of non-AdS holography. It relates three-dimensional warped anti-de Sitter (

{WAdS}_{3}

) spaces to a special class of two-dimensional quantum field theory with chiral scaling symmetry that acts only on right-moving modes. The latter are often called warped conformal field theories (

{WCFT}_{2}

), and their existence makes WAdS/WCFT particularly interesting as a tool to investigate a new type of two-dimensional conformal structure. Besides, WAdS/WCFT is interesting because it enables one to apply holographic techniques to the microstate counting problem of non-AdS, nonsupersymmetric black holes. Asymptotically

{WAdS}_{3}

black holes (

{WBH}_{3}

) appear as solutions of topologically massive theories, Chern-Simons theories, and many other models. Here, we explore

{WBH}_{3} \times Σ_{D - 3}

solutions of

D

-dimensional higher-curvature gravity, with

Σ_{D - 3}

being different internal manifolds, typically given by products of deformations of hyperbolic spaces, although we also consider warped products with time-dependent deformations. These geometries are solutions of the second order higher-curvature theory at special (critical) points of the parameter space, where the theory exhibits a sort of degeneracy. We argue that the dual (W)CFT at those points is actually trivial. In many respects, these critical points of

{WAdS}_{3} \times Σ_{D - 3}

vacua are the squashed/stretched analogs of the

{AdS}_{D}

Chern-Simons point of Lovelock gravity.

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