Isotropic quadratic form
In mathematics, a quadratic form over a field F is said to be isotropic if there is a non-zero vector on which the form evaluates to zero. Otherwise the quadratic form is anisotropic. More precisely, if q is a quadratic form on a vector space V over F, then a non-zero vector v in V is said to be isotropic if q(v)=0. A quadratic form is isotropic if and only if there exists a non-zero isotropic vector for that quadratic form.
Suppose that (V,q) is quadratic space and W is a subspace. Then W is called an isotropic subspace of V if some vector in it is isotropic, a totally isotropic subspace if all vectors in it are isotropic, and an anisotropic subspace if it does not contain any (non-zero) isotropic vectors. The isotropy index of a quadratic space is the maximum of the dimensions of the totally isotropic subspaces.
1. The hyperbolic plane is a two-dimensional isotropic quadratic space with the form xy.
2. A quadratic form q on a finite-dimensional real vector space V is anisotropic if and only if q is a definite form:
- either q is positive definite, i.e. q(v)>0 for all non-zero v in V ;
- or q is negative definite, i.e. q(v)<0 for all non-zero v in V.
More generally, if the quadratic form is non-degenerate and has the signature (p,q), then its isotropy index is the minimum of p and q.
4. If F is a finite field and (V,q) is a quadratic space of dimension at least three, then it is isotropic.
5. If F is the field Qp of p-adic numbers and (V,q) is a quadratic space of dimension at least five, then it is isotropic.
Split quadratic space 
A space with quadratic form is split (or metabolic) if there is a subspace which is equal to its own orthogonal complement: equivalently, the index of isotropy is equal to half the dimension. The hyperbolic plane is an example, and over a field of characteristic not equal to 2, every split space is a direct sum of hyperbolic planes.
Relation with classification of quadratic forms 
From the point of view of classification of quadratic forms, anisotropic spaces are the basic building blocks for quadratic spaces of arbitrary dimensions. For a general field F, classification of anisotropic quadratic forms is a nontrivial problem. By contrast, the isotropic forms are usually much easier to handle. By Witt's decomposition theorem, every inner product space over a field is an orthogonal direct sum of a split space and an anisotropic space.
See also 
- Null vector
- Witt group
- Witt ring (forms)
- Witt's theorem
- Symmetric bilinear form
- Universal quadratic form
- Milnor & Husemoller (1973) p.57
- Milnor & Husemoller (1973) pp.9,12
- Milnor & Husemoller (1973) pp.12–13
- Milnor & Husemoller (1973) p.56
- Lam, T.Y. (1973). The Algebraic Theory of Quadratic Forms. Mathematics Lecture Note Series. Reading, MA: W. A. Benjamin Publishers. §1.3 Hyperbolic plane and hyperbolic spaces. ISBN 0-805-35664-3 Check
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- Milnor, J.; Husemoller, D. (1973). Symmetric Bilinear Forms. Ergebnisse der Mathematik und ihrer Grenzgebiete 73. Springer-Verlag. ISBN 3-540-06009-X. Zbl 0292.10016.
- O'Meara, O.T (1963). Introduction to Quadratic Forms. Springer-Verlag. p. 94 §42D Isotropy. ISBN 3-540-66564-1.
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