Since a reparamteization of a curve does not change its length, we can assume that the curve of length $L$ is parametrized by the constant speed which makes the curve $L/(2\pi)$-Lipschitz as a mapping from $\mathbb{S}^1$ (with arc-length distance) to $(M,g)$. Now the following result is a straightforward consequence of Theorem 5.1 in [1].

> **Theorem.** If $M$ is a compact connected and simply-connected  Riemannian manifold, then there is $\gamma>0$ such that every
> $L$-Lipschitz mapping $\alpha:\mathbb{S}^1\to M$ admits a $\gamma
 L$-Lipschitz extension $A:\overline{\mathbb{B}}^2(0,1)\to M$.

Indeed, using terminology from [1], $M$ is $1$-Lipschitz connected in the small, because it has a finite covering by balls that are bi-Lipschitz homeomorphic to Euclidean balls.

Now, as we pointed out at the beginning, we can assume that $\alpha_0$ is $L/(2\pi)$-Lipschitz. Therefore the extension $A$ is $\gamma L/(2\pi)$ Lipschitz and restrictions of $A$ to circles of radii $0\leq t\leq 1$ will give us a desired homotopy: the restriction to the circle of radius $t$ will have length at most $\gamma Lt\leq \gamma L$.



**[1] Lang, U., Schlichenmaier, T.,**
Nagata dimension, quasisymmetric embeddings, and Lipschitz extensions.