ε-quadratic form

In mathematics, specifically the theory of quadratic forms, an ε-quadratic form is a generalization of quadratic forms to skew-symmetric settings and to *-rings; \epsilon = \pm 1, accordingly for symmetric or skew-symmetric. They are also called (-)^n-quadratic forms, particularly in the context of surgery theory.

There is the related notion of ε-symmetric forms, which generalizes symmetric forms, skew-symmetric forms (= symplectic forms), Hermitian forms, and skew-Hermitian forms. More briefly, one may refer to quadratic, skew-quadratic, symmetric, and skew-symmetric forms, where "skew" means (-) and the * (involution) is implied.

The theory is 2-local: away from 2, ε-quadratic forms are equivalent to ε-symmetric forms: half the symmetrization map (below) gives an explicit isomorphism.

Contents

Definition

ε-symmetric forms and ε-quadratic forms are defined as follows.[1]

Given a module M over a *-ring R, let B(M) be the space of bilinear forms on M, and let T\colon B(M) \to B(M) be the "conjugate transpose" involution B(u,v) \mapsto B(v,u)^*. Let \epsilon=\pm 1; then \epsilon T is also an involution. Define the ε-symmetric forms as the invariants of \epsilon T, and the ε-quadratic forms are the coinvariants.

As a short exact sequence,

Q^\epsilon(M) \to B(M) \stackrel{1-\epsilon T}{\longrightarrow} B(M) \to Q_\epsilon(M)

As kernel (algebra) and cokernel,

Q^\epsilon(M)�:= \mbox{ker}\,(1-\epsilon T)
Q_\epsilon(M)�:= \mbox{coker}\,(1-\epsilon T)

The notation Q^\epsilon(M), Q_\epsilon(M) follows the standard notation M^G, M_G for the invariants and coinvariants for a group action, here of the order 2 group (an involution).

We obtain a homomorphism (1 %2B \epsilon T)\colon Q_\epsilon(M) \to Q^\epsilon(M) which is bijective if 2 is invertible in R. (The inverse is given by multiplication with 1/2.)

An ε-quadratic form \psi \in Q_\epsilon(M) is called non-degenerate if the associated ε-symmetric form (1 %2B \epsilon T)(\psi) is non-degenerate.

Generalization from *

If the * is trivial, then \epsilon=\pm 1, and "away from 2" means that 2 is invertible: \frac{1}{2} \in R.

More generally, one can take for \epsilon \in R any element such that \epsilon^*\epsilon=1.\epsilon=\pm 1 always satisfy this, but so does any element of norm 1, such as complex numbers of unit norm.

Similarly, in the presence of a non-trivial *, ε-symmetric forms are equivalent to ε-quadratic forms if there is an element \lambda \in R such that \lambda^* %2B \lambda = 1. If * is trivial, this is equivalent to 2\lambda=1 or \lambda = \frac{1}{2}.

For instance, in the ring R=\mathbf{Z}\left[\textstyle{\frac{1%2Bi}{2}}\right] (the integral lattice for the quadratic form 2x^2-2x%2B1), with complex conjugation, \lambda=\textstyle{\frac{1%2Bi}{2}} is such an element, though \frac{1}{2} \not\in R.

Intuition

In terms of matrices, (we take V to be 2-dimensional):

ax^2 %2B bxy%2Bcyx %2B dy^2 = ax^2 %2B (b%2Bc)xy %2B dy^2\, ,
which is a quotient map with kernel \begin{pmatrix}0 & b\\-b & 0\end{pmatrix}.

Refinements

An intuitive way to understand an ε-quadratic form is to think of it as a quadratic refinement of its associated ε-symmetric form.

For instance, in defining a Clifford algebra over a general field or ring, one quotients the tensor algebra by relations coming from the symmetric form and the quadratic form: vw%2Bwv=2B(v,w) and v^2=Q(v). If 2 is invertible, this second relation follows from the first (as the quadratic form can be recovered from the associated bilinear form), but at 2 this additional refinement is necessary.

Examples

An easy example for an ε-quadratic form is the standard hyperbolic ε-quadratic form H_\epsilon(R) \in Q_\epsilon(R \oplus R^*). (Here, R^*�:= hom_R(R,R) denotes the dual of the R-module R.) It is given by the bilinear form ((v_1,f_1),(v_2,f_2)) \mapsto f_2(v_1). The standard hyperbolic ε-quadratic form is needed for the definition of L-theory.

For the field of two elements R={\mathbf F}_2 there is no difference between (+1)-quadratic and (-1)-quadratic forms, which are just called quadratic forms. The Arf invariant of a nonsingular quadratic form over \mathbf{F}_2 is an {\mathbf F}_2-valued invariant with important applications in both algebra and topology.

Given an oriented surface \Sigma embedded in \mathbf{R}^3, the middle homology group H_1(\Sigma) carries not only a skew-symmetric form (via intersection), but also a skew-quadratic form, which can be seen as a quadratic refinement, via self-linking. The skew-symmetric form is an invariant of the surface \Sigma, whereas the skew-quadratic form is an invariant of the embedding \Sigma \subset \mathbf{R}^3, e.g. for the Seifert surface of a knot. The Arf invariant of the skew-quadratic form is a framed cobordism invariant generating the first stable homotopy group \pi^s_1.

For the standard embedded torus, the skew-symmetric form is given by \begin{pmatrix}0 & 1\\-1 & 0\end{pmatrix} (with respect to the standard symplectic basis), and the skew-quadratic refinement is given by xy with respect to this basis: Q(1,0)=Q(0,1)=0: the basis curves don't self-link; and Q(1,1)=1: a (1,1) self-links, as in the Hopf fibration. (This form has Arf invariant 0, and thus this embedded torus has Kervaire invariant 0.)

Applications

A key application is in algebraic surgery theory, where even L-groups are defined as Witt groups of ε-quadratic forms, by C.T.C.Wall

References

  1. ^ Foundations of algebraic surgery, by Andrew Ranicki, p. 6