Let $M$ be a Riemannian manifold with the Levi-Civita connection. For $x \in M$ and $X \in T_x(M)$ we can consider geodesic $\gamma$ with the properties that $\gamma(0)=x$ and $\gamma'(0)=X$. Such geodesic exists and is unique: existence is guaranteed provided we take vectors $X$ in some suitable neighborhood of $0$ in $T_x(M)$. If we define $y:=\gamma(1)$ we arrive at the definition of exponential map $\exp_x:T_xM \to M$ (defined only on some small neighborhood of $0$ in $T_xM$).
From the other hand, we can consider $GL(n,\mathbb{R})$ as an open set in $\mathbb{R}^{n^2}$: therefore it becomes manifold on its own right. I would like to understand why in this situation $\exp_{I}(A)=e^{A}$ where on the left hand side is the exponential map from riemannian manifold at identity matrix and the right hand side is just the exponential of the matrix. Here we identify $T_I(Gl(n))$ with $\mathbb{R}^{n^2}$.
2026-04-04 13:09:12.1775308152
Exponential map and matrices: comparison of two pictures
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You haven't specified which Riemannian metric you want to consider on $\operatorname{GL}_n(\mathbb{R})$. I don't know if you can put a Riemannian metric on $\operatorname{GL}_n(\mathbb{R})$ such that the corresponding geodesics are given by $\exp(tA)$ but you can show the following:
The problem with generalizing $(3)$ from $G$ to the whole of $\operatorname{GL}_n(\mathbb{R})$ is that $\operatorname{GL}_n(\mathbb{R})$ has no bi-invariant metric.