Gauge by a Hessian potential of is NG and obeys Poisson
OpenNewtonCartan.gauge_NG_poisson_of_hessFLet be a classical Newton–Cartan connection on satisfying CurvConds for a smooth density , and suppose its Riemann tensor has the Trautman form
Let be a smooth potential whose raised gradient reproduces this field:
Then the gauge-transformed connection
is flat and compatible (hence an object of NG), and obeys Poisson's equation with respect to .
The flatness computation uses the classical Christoffel reduction together with the Hessian identity to cancel all components of ; Poisson follows by tracing CurvConds (1) against the same identity.
Formalization Note. gaugeΓ, IsNG, Poisson, and CurvConds are as in Def_NewtonCartan_defs.
DEPRECATED: required ∂_d(∇^a φ) = R^a_00d for temporal d as well, which is stronger than needed for gauge flatness. Replaced by NewtonCartan.gauge_NG_poisson_of_spatial_hess.
import Definitions.Def_NewtonCartan_defs open scoped ContDiff
namespace NewtonCartan
/-- If $\partial_d(\nabla^a\varphi)=R^a{}_{00d}$ and $\Gamma t$ is classical with Trautman $t_b$-form curvature and CurvConds, then `gaugeΓ Γt φ` is NG and satisfies Poisson. -/
theorem gauge_NG_poisson_of_hessF (Γt : Conn) (ρ : E → ℝ) (φ : E → ℝ)
(hΓt : IsClassical Γt) (hρ : ContDiff ℝ ∞ ρ) (hcurv : CurvConds Γt ρ)
(hφ : ContDiff ℝ ∞ φ)
(hform : ∀ x a b c d,
riem Γt x a b c d =
tt b * (tt c * riem Γt x a 0 0 d - tt d * riem Γt x a 0 0 c))
(hhess : ∀ x a d, pd (fun y => gradUp φ y a) d x = riem Γt x a 0 0 d) :
IsNG (gaugeΓ Γt φ) φ ∧ Poisson (gaugeΓ Γt φ) φ ρ := by sorry
end NewtonCartan