Main article: 8-polytope
A polytope in eight dimensions is called an 8-polytope. The most studied are the regular polytopes, of which there are only three in eight dimensions: the 8-simplex, 8-cube, and 8-orthoplex. A broader family are the uniform 8-polytopes, constructed from fundamental symmetry domains of reflection, each domain defined by a Coxeter group. Each uniform polytope is defined by a ringed Coxeter-Dynkin diagram. The 8-demicube is a unique polytope from the D8 family, and 421, 241, and 142 polytopes from the E8 family.
The 7-sphere or hypersphere in eight dimensions is the seven-dimensional surface equidistant from a point, e.g. the origin. It has symbol S7, with formal definition for the 7-sphere with radius r of S 7 = { x ∈ R 8 : ‖ x ‖ = r } . {\displaystyle S^{7}=\left\{x\in \mathbb {R} ^{8}:\|x\|=r\right\}.}
The volume of the space bounded by this 7-sphere is V 8 = π 4 24 R 8 {\displaystyle V_{8}\,={\frac {\pi ^{4}}{24}}\,R^{8}} which is 4.05871 × r8, or 0.01585 of the 8-cube that contains the 7-sphere.
Main article: Kissing number problem
The kissing number problem has been solved in eight dimensions, thanks to the existence of the 421 polytope and its associated lattice. The kissing number in eight dimensions is 240.
Main article: Octonion
The octonions are a normed division algebra over the real numbers, the largest such algebra. Mathematically they can be specified by 8-tuplets of real numbers, so form an 8-dimensional vector space over the reals, with addition of vectors being the addition in the algebra. A normed algebra is one with a product that satisfies
for all x and y in the algebra. A normed division algebra additionally must be finite-dimensional, and have the property that every non-zero vector has a unique multiplicative inverse. Hurwitz's theorem prohibits such a structure from existing in dimensions other than 1, 2, 4, or 8.
The complexified quaternions C ⊗ H {\displaystyle \mathbb {C} \otimes \mathbb {H} } , or "biquaternions," are an eight-dimensional algebra dating to William Rowan Hamilton's work in the 1850s. This algebra is equivalent (that is, isomorphic) to the Clifford algebra C ℓ 2 ( C ) {\displaystyle C\ell _{2}(\mathbb {C} )} and the Pauli algebra. It has also been proposed as a practical or pedagogical tool for doing calculations in special relativity, and in that context goes by the name Algebra of physical space (not to be confused with the Spacetime algebra, which is 16-dimensional.)