If you mean by "nD rotation" an orthogonal transformation with unit determinant, here is a simple recipe with a low computational complexity.
a) Principle: obtain it by a composition of two hyperplane reflections (aka symmetries) with rather close normal vectors (see remark 1).
b) Matrix version: You probably know that reflection with respect to an hyperplane with unit normal (column) vector $N$ is rendered by a Householder matrix $I_n-2NN^T$ (https://en.wikipedia.org/wiki/Householder_transformation). Thus, the rotation matrix is $$(I_n-2N_1N_1^T)(I_n-2N_2N_2^T)$$ where $N_2$ for example is a perturbation of $N_1$.
Remark 1: As remarked by @Rahul, this leaves a $(n-2)$ hyperplane invariant. In order to obviate this lack of generality, it suffices to apply again and again transformations $$(I_-2N_{2k+1}N_{2k+1}^T)(I_n-2N_{2k+2}N_{2k+2}^T)$$ for $k=1\cdots [n/2]$.
Remark 2: Principle a) generalizes a well known property of planar geometry (Composition of two reflections is a rotation): the composition of a reflection with respect to line $y=\tan(\alpha)x$, with a reflection with respect to line $y=\tan(\beta)x$ is a rotation with angle $2(\beta-\alpha)$.
Remark 3: in 3D, one can also consider Rodrigues' formula (https://en.wikipedia.org/wiki/Rodrigues%27_rotation_formula).
Remark 4: Vector $N$ is an eigenvector associated to the Householder matrix with eigenvalue $-1$.