IndisputableMonolith.Relativity.Geometry.Curvature
This module supplies the Christoffel symbols and the standard curvature tensors derived from a metric tensor. It is cited by any construction that needs the Levi-Civita connection, covariant derivatives, or the lattice-to-curvature bridge. The module consists of explicit definitions together with immediate algebraic identities and Minkowski-space special cases.
claimThe Christoffel symbols are given by $Γ^λ_{μν} = ½ g^{λσ}(∂_μ g_{νσ} + ∂_ν g_{μσ} - ∂_σ g_{μν})$, from which the Riemann tensor $R^ρ{}_{σμν}$, Ricci tensor $R_{μν}$, Ricci scalar $R$, and Einstein tensor $G_{μν}$ are constructed by the usual contractions and commutators.
background
The module rests on the Metric and Tensor modules for the pseudo-Riemannian metric $g_{μν}$ and on the Derivatives module for the partial derivative operator on tensor components. It introduces the standard objects of local Riemannian geometry: the Christoffel symbols as connection coefficients, the Riemann curvature tensor measuring non-commutativity of covariant derivatives, and the successive contractions that yield the Ricci tensor and scalar. The setting is four-dimensional pseudo-Riemannian geometry with the Minkowski metric as the flat reference case.
proof idea
This is a definition module. The central definition extracts the Christoffel symbols directly from first derivatives of the metric. Symmetry of the lower indices follows at once from the definition. The Riemann tensor is assembled from derivatives of the symbols plus quadratic terms; the Ricci tensor and scalar are obtained by contraction. Minkowski specializations are verified by direct substitution of the flat metric and its vanishing derivatives.
why it matters in Recognition Science
The module is required by LeviCivitaTheorem for the uniqueness of the torsion-free metric-compatible connection, by DiscreteBridge for mapping lattice J-cost defects onto the Ricci scalar and Einstein tensor, and by CovariantDerivative, ParallelTransport, and RiemannSymmetries for all subsequent differential operations. It closes the passage from the RS-derived metric in MetricUnification to the curvature terms that enter the Einstein field equations.
scope and limits
- Does not derive the Einstein field equations.
- Does not treat non-metric or torsionful connections.
- Does not address global topology or manifold completeness.
- Does not compute curvature for arbitrary non-flat metrics beyond Minkowski space.
used by (7)
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IndisputableMonolith.Relativity.Geometry -
IndisputableMonolith.Relativity.Geometry.CovariantDerivative -
IndisputableMonolith.Relativity.Geometry.DiscreteBridge -
IndisputableMonolith.Relativity.Geometry.LeviCivitaTheorem -
IndisputableMonolith.Relativity.Geometry.MetricUnification -
IndisputableMonolith.Relativity.Geometry.ParallelTransport -
IndisputableMonolith.Relativity.Geometry.RiemannSymmetries
depends on (3)
declarations in this module (13)
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def
christoffel -
theorem
christoffel_symmetric -
def
riemann_tensor -
def
ricci_tensor -
theorem
riemann_antisymmetric_last_two -
def
ricci_scalar -
def
einstein_tensor -
lemma
eta_deriv_zero -
theorem
minkowski_christoffel_zero_proper -
theorem
minkowski_riemann_zero -
theorem
minkowski_ricci_zero -
theorem
minkowski_ricci_scalar_zero -
theorem
minkowski_einstein_zero