MOND has limelighted the fact that Newtonian dynamics and general relativity (GR) have not been verified to any accuracy at very low accelerations -at or below the MOND acceleration a0: Without invoking made-to-measure "dark matter", Newtonian dynamics (and hence general relativity) fail in accounting for galactic dynamics at such low accelerations. In particular, we do not have evidence that all the cherished, underlying principles of Newtonian dynamics or GR, such as locality or Lorentz invariance, still apply in the MOND limit. I discuss the possibility that the principle of general covariance might not apply in this limit. This would be in line with suggestions that general covariance, where it does hold, is only an emergent, hence approximate, property of relativistic dynamics. This idea also resonates well with MOND, which hinges on accelerations, for example because the existence of an effective absolute inertial frame is natural in MOND. Relaxing general covariance affords more freedom in constructing candidate MOND theories. For example, it may permit constructing pure-metric, local MOND theories, which is thought impossible with general covariance. I exemplify this with a MOND-oriented, oversimplified, noncovariant theory, where the gravitational Lagrangian isνγ )/2 is the (nonscalar) first-derivative part of the Ricci scalar R. Γ γ µν is the Levi-Civita connection of a metric, gµν, which couples minimally to matter, and ℓM = c 2 /a0 is the MOND length, which is of cosmological magnitude, being, e.g., of the order of the de Sitter radius of our Universe. This LM gives a covariant theory in the high-acceleration limit by requiring that F(z) → z + ζ, for z ≫ 1, which gives GR with a cosmological constant ζc −4 a 2 0 . In the MOND limit F ′ (z ≪ 1) ∝ z 1/2 . In the nonrelativistic limit the metric has a solution of the form gµν ≈ ηµν − 2φδµν, as in GR, but the potential φ solves a MOND, nonlinear Poisson analog. This form of gµν also produces gravitational lensing as in GR, only with the MOND potential. I show that this theory is a fixed-gauge expression of bimetric MOND (BIMOND), with the auxiliary metric constrained to be flat. The latter theory is thus a covariantized version of the formerá-la Stückelberg. This theory is also a special case of so-called f (Q) theories -aquadratic generalizations of "symmetric, teleparallel GR", which are, in turn, also equivalent to constrained BIMOND-type theories.
PACS numbers:where a H ≡ cH is the acceleration associated with the cosmological expansion rate, H (the Hubble-Lemaitre constant), and a H (0) is its present-day value, and ℓ Λ = (Λ/3) −1/2 is the radius associated with Λ -the observed equivalent of a cosmological constant. Defining the MOND length asgalactic dynamics and cosmology tell us that ℓ M ∼ ℓ Λ ∼ ℓ H , where ℓ H ≡ c/H 0 is the Hubble distance today. This numerical "coincidence", if fundamental, may have far-reaching ramifications for MOND, and for gravity in general (e.g., Ref.[10]). Unless one invokes large quantities of "dark matter" in galactic ...