For a finite-dimensional nonsingular quadratic form over a field of characteristic different from two, a Witt decomposition is an orthogonal splittingwhere is a hyperbolic plane of a quadratic form and is an anisotropic quadratic form. The integer is the Witt index. Both and the isometry class of the anisotropic part are determined by , although the particular subspaces realizing the splitting need not be unique.[ref]
Over , take . Set , and . Thenso . The one-dimensional remainder is anisotropic and the Witt index is one. This is an isometry of quadratic spaces, stronger than merely expressing the underlying vector space as a direct sum.
The construction starts from an isotropic vector, finds a partner with nonzero polar pairing, and splits off the hyperbolic plane they generate. Repeating the process ends when no nonzero isotropic vector remains. The decomposition makes the isotropic directions and the residual arithmetic obstruction visible separately.
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