I have been studying rudimentary gauge gravity, using the soldering equation to show how local P-translations can be related to global Lorentz and coordinate transformations. My question relates to the tangent space $T_{p}M$ at a point $p$ on a manifold $M$, and the properties of hypersurfaces (submanifolds) of $M$, which I'll denote $X$. Essentially, if $X$ and $M$ share a point $p$, then is the the exponential map $exp:T_{p}M\rightarrow{M}$ equivalent to $exp:T_{p}X\rightarrow{X}$?
2026-03-26 20:40:36.1774557636
Can a Riemannian submanifold effectively act as a local tangent space?
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I think this is what you are trying to ask: Suppose that $M$ is a Riemannian manifold, $X\subset M$ is a hypersurface equipped with the Riemannian metric induced from $M$. Fix a point $p\in X$. We then have two exponential maps: $\exp_p^M: T_pM\to M$ and $\exp_p^X: T_pX\to X$. (A caveat: The metrics might be incomplete and the exponential maps might be defined only on neighborhoods of $0$ in the respective tangent spaces. I will ignore this issue.) We have the natural inclusion $T_pX\subset T_pM$. Then your question is:
Since you do not seem to know what the word "restriction" means, here is a reformulation of the above question:
The answer to this question is in general negative. The reason is the failure of $X$ to be totally geodesic in $M$. (A submanifold $X$ of a Riemannian manifold $M$ is called totally geodesic if each geodesic in $X$, with respect to the metric of $X$, is also a geodesic in $M$.) As a concrete example, consider $M={\mathbb R}^n$ with the standard flat Riemannian metric (with the metric tensor $g_{ij}(x)=\delta_{ij}$). Let $X\subset M$ be a round sphere. Then for each point $p\in X$, $v\in T_pX$, $\exp^M_p(v)\ne \exp_p^X(v)$, unless $v=0$.
Addendum: Much of the trouble that physicists have with explaining themselves to mathematicians comes down to the matter of language, since mathematics is both science and language. Here is a fragment taken from Richard Feynman's book "Surely you are joking, Mr. Feynman." There, Feynman explains that he had invented alternatives to the standard math notation and what was the result: