A division algebra over a field is a division ring equipped with a unital algebra structure over , with mapping into its center of an associative algebra. Every nonzero element is invertible; it need not be finite-dimensional over .
A finite-dimensional associative division algebra over is one of the three displayed algebras. A nonreal element has an irreducible quadratic minimal polynomial and yields . Its centralizer is a division algebra over central , hence is by splitting minimal polynomials. Decompose the whole algebra into the plus and minus eigenspaces of conjugation by . If the minus space is zero, the algebra is ; otherwise it is , since multiplying by takes that space into the centralizer. One has and . Division forces , which can be rescaled to , yielding . Of these, only have center .
Let be a finite-dimensional division algebra over an algebraically closed field . Left multiplication by has an eigenvalue and a nonzero eigenvector . Thus ; multiplying by gives . Every element is scalar, so .
A quaternion is with real coefficients, where . They form a noncommutative real division algebra. The norm squared is , and every nonzero quaternion has inverse its conjugate divided by that squared norm. The unit quaternions form the Lie group .
The displayed complex matrices, with real coefficients, form a four-dimensional real associative algebra. Their three imaginary basis matrices square to minus the identity and satisfy , , , with the reversed products negative. For , quaternionic conjugation gives . Every nonzero matrix therefore has inverse inside this algebra. This realizes the real division algebra of quaternions within ; it is not a complex vector subspace.
A quaternion of norm is a unit quaternion. They form the topological group and identify with the sphere . Multiplication and inversion preserve the norm. The Hurewicz theorem identifies with ; hence homotopy-group addition in a topological group shows that has mapping degree , rather than .

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Division algebra is a type of algebraic structure where division is possible, except by zero. More formally, a division algebra is a vector space over a field \( F \) equipped with a bilinear multiplication operation that satisfies the following conditions: 1. **Non-Associativity or Associativity**: In a general division algebra, multiplication can be either associative or non-associative. If it is associative, the algebra is called an associative division algebra.