<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Ricci on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/ricci/</link><description>Recent content in Ricci on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Sun, 21 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/ricci/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (11): Curvature in Riemannian Geometry — Riemann, Ricci, and Scalar</title><link>https://www.chenk.top/en/differential-geometry/11-curvature-on-manifolds/</link><pubDate>Sun, 21 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/11-curvature-on-manifolds/</guid><description>&lt;p>Curvature is the central concept of Riemannian geometry. Intuitively, it measures how much a space deviates from being flat — how parallel lines converge or diverge, how triangles have angle excess or deficit, how volumes grow differently from Euclidean expectations. In the previous article we saw that the path-dependence of parallel transport signals the presence of curvature: a vector carried around a closed loop on &lt;span class="math-inline">$S^2$&lt;/span>
 returns rotated, while on &lt;span class="math-inline">$\mathbb{R}^n$&lt;/span>
 it does not. The next step is to make this precise, to extract a tensor that exactly captures this rotation, and to understand its various contractions.&lt;/p></description></item></channel></rss>