Definition

Let MM be a finite-dimensional . A Riemannian metric on MM is a smooth symmetric covariant 22-tensor gg such that gpg_p is a positive-definite on TpMT_pM for every pMp\in M. Equivalently, gg is a on the TMTM. A Riemannian manifold is a pair (M,g)(M,g). In local coordinates, g=gijdxidxjg=g_{ij}\,dx^i\otimes dx^j, where the matrix (gij(p))(g_{ij}(p)) is symmetric positive definite at every point and each coefficient gijg_{ij} is smooth.

Metric and volume constructions

The metric assigns each tangent vector a length vg=g(v,v)\lVert v\rVert_g=\sqrt{g(v,v)} and each piecewise smooth curve γ\gamma a length

Lg(γ)=gγ(t)(γ˙(t),γ˙(t))dt.L_g(\gamma)=\int \sqrt{g_{\gamma(t)}(\dot\gamma(t),\dot\gamma(t))}\,dt.

Taking the infimum of curve lengths gives the Riemannian distance on each . The metric also identifies TMTM with the and determines a canonical volume density; an orientation turns this density into a volume form.

Canonical connection and curvature

Every Riemannian metric has a unique torsion-free, metric-compatible connection, the . It determines geodesics, parallel transport, and . These structures depend on derivatives of gg, whereas lengths and angles are pointwise data. Their construction and uniqueness are treated in Lee, Chapters 2–5.

Examples and scope

The Euclidean metric idxidxi\sum_i dx^i\otimes dx^i is the standard example on Rn\mathbb R^n. An immersion into pulls this metric back to a Riemannian metric when its differential is injective. Positive definiteness distinguishes Riemannian metrics from pseudo-Riemannian metrics, whose nondegenerate symmetric forms may have mixed signature. Smoothness is essential: an arbitrary choice of an inner product on each does not necessarily define a Riemannian metric.

References
  1. John M. Lee, Introduction to Riemannian Manifolds, 2nd ed., Graduate Texts in Mathematics 176, Springer, 2018. Publisher record. Relevant: Chapters 2–5.
  2. Manfredo P. do Carmo, Riemannian Geometry, Mathematics: Theory & Applications, Birkhäuser, 1992. Publisher record. Relevant: Chapters 0–3.