To explain my question I need to discuss two notions from differential geometry (the Riemann curvature tensor and sectional curvature), but this is really a linear algebra / Euclidean geometry question, so I will provide background material.
The Riemann curvature tensor is a certain linear function $R(u,v,w,z)$ with four vector inputs and one real output: $$R:\Bbb R^n\times\Bbb R^n\times\Bbb R^n\times\Bbb R^n\to\Bbb R.$$ Such a function has, a priori, $n^4$ degrees of freedom (one for every choice of four basis vectors). However, the Riemann tensor is required to satisfy a few requirements:
$R(u,v,w,z)=R(w,z,u,v)$ (interchange symmetry)
$R(v,u,w,z)=-R(u,v,w,z)$ and $R(u,v,z,w)=-R(u,v,w,z)$ (antisymmetry)
$R(u,v,w,z)+R(v,w,u,z)+R(w,u,v,z)=0$ (cyclic relation)
These symmetries end up bringing the number of degrees of freedom of $R$ from $n^4$ down to $\frac{n^2(n^2-1)}{12}$.
We can also define something called the sectional curvature $K$, defined as follows. Suppose $\sigma$ is a plane through the origin, and let $u$ and $v$ be orthonormal vectors spanning $\sigma$. Then $K(\sigma)$, also denoted $K(u,v)$, is defined to be $R(u,v,u,v)$. In general, if $u$ and $v$ span $\sigma$ but are not necessarily orthonormal, then $$K(\sigma)=\frac{R(u,v,u,v)}{(\|u\|\|v\|\sin\theta)^2}=\frac{R(u,v,u,v)}{\|u\|^2\|v\|^2-(u\cdot v)^2}$$ where $\theta$ is the angle between $u$ and $v$. It is an algebraic fact that $K(\sigma)$ does not depend on the choice of two generators of the plane $\sigma$. It is also an algebraic fact that $K$ determines $R$: if you know the sectional curvature of all planes, then you know all values of the curvature tensor.
(The underlying differential geometry idea is that $R$ is used to describe the curvature at a point in curved high-dimensional space, and $K$ relates it to two-dimensional Gaussian curvature.)
This raises the following natural question. Can one choose $\frac{n^2(n^2-1)}{12}$ planes in $\Bbb R^n$ in a natural way such that the sectional curvatures $K$ of these planes determine the Riemann tensor $R$? If these planes are chosen generically or randomly, then they will almost surely determine $R$. However, is there a particularly symmetric way to do this? Note that, since the degrees of freedom match exactly, the sectional curvatures of these planes will be independent.
When $n=3$, we need $6$ planes through the origin. I believe may select the planes connecting opposite edges of the cube. When $n=4$, we need $20$ planes. I believe we may select the planes through the centers of the Boerdijk–Coxeter helix rings of the $600$-cell. (Take care that these are planes, not hyperplanes, so they each intersect the hypersphere in a circle.) Does this generalize somehow?