In mathematics, the Arf invariant of a nonsingular quadratic form over a field of characteristic 2 was defined by Turkish mathematician Cahit Arf (1941) when he started the systematic study of quadratic forms over arbitrary fields of characteristic 2. The Arf invariant is the substitute, in characteristic 2, of the discriminant for quadratic forms in characteristic not 2. Arf used his invariant, among others, in his endeavor to classify quadratic forms in characteristic 2.
In the special case of the 2-element field F2 the Arf invariant can be described as the element of F2 that occurs most often among the values of the form. Two nonsingular quadratic forms over F2 are isomorphic if and only if they have the same dimension and the same Arf invariant. This fact was essentially known to Dickson (1901), even for any finite field of characteristic 2, and it follows from Arf's results for an arbitrary perfect field. An assessment of Arf's results in the framework of the theory of quadratic forms can be found in,
The Arf invariant is particularly applied in geometric topology, where it is primarily used to define an invariant of (4k+2)-dimensional manifolds (singly even-dimension manifolds: surfaces (2-manifolds), 6-manifolds, 10-manifolds, etc.) with certain additional structure called a framing, and thus the Arf–Kervaire invariant and the Arf invariant of a knot. The Arf invariant is analogous to the signature of a manifold, which is defined for 4k-dimensional manifolds (doubly even-dimensional); this 4-fold periodicity corresponds to the 4-fold periodicity of L-theory. The Arf invariant can also be defined more generally for certain 2k-dimensional manifolds.
The Arf invariant belongs to a quadratic form over a field K of characteristic 2. Any binary non-singular quadratic form over K is equivalent to a form with in K. The Arf invariant is defined to be the product . If the form is equivalent to , then the products and differ by an element of the form with in K. These elements form an additive subgroup U of K. Hence the coset of modulo U is an invariant of , which means that it is not changed when is replaced by an equivalent form.
Every nonsingular quadratic form over K is equivalent to a direct sum of nonsingular binary forms. This has been shown by Arf but it had been earlier observed by Dickson in the case of finite fields of characteristic 2. The Arf invariant Arf() is defined to be the sum of the Arf invariants of the . By definition, this is a coset of K modulo U. Arf  has shown that indeed Arf() does not change if is replaced by an equivalent quadratic form, which is to say that it is an invariant of .
The Arf invariant is additive; in other words, the Arf invariant of an orthogonal sum of two quadratic forms is the sum of their Arf invariants.
Arf's main results
If the field K is perfect then every nonsingular quadratic form over K is uniquely determined (up to equivalence) by its dimension and its Arf invariant. In particular this holds over the field F2. In this case U=0 and hence the Arf invariant is an element of the base field F2; it is either 0 or 1.
If the field is not perfect then the Clifford algebra is another important invariant of a quadratic form. For various fields Arf has shown that every quadratic form is completely characterized by its dimension, its Arf invariant and its Clifford algebra. Examples of such fields are function fields (or power series fields) of one variable over perfect base fields.
Quadratic forms over F2
Over F2 the Arf invariant is 0 if the quadratic form is equivalent to a direct sum of copies of the binary form , and it is 1 if the form is a direct sum of with a number of copies of .
William Browder has called the Arf invariant the democratic invariant because it is the value which is assumed most often by the quadratic form. Another characterization: q has Arf invariant 0 if and only if the underlying 2k-dimensional vector space over the field F2 has a k-dimensional subspace on which q is identically 0 – that is, a totally isotropic subspace of half the dimension; its isotropy index is k (this is the maximum dimension of a totally isotropic subspace of a nonsingular form).
The Arf invariant in topology
are both zero (e.g. if is closed). The intersection form
is non-singular. (Topologists usually write F2 as .) A quadratic refinement for is a function which satisfies
Let be any 2-dimensional subspace of , such that . Then there are two possibilities. Either all of are 1, or else just one of them is 1, and the other two are 0. Call the first case , and the second case . Since every form is equivalent to a symplectic form, we can always find subspaces with x and y being -dual. We can therefore split into a direct sum of subspaces isomorphic to either or . Furthermore, by a clever change of basis, . We therefore define the Arf invariant
- = (number of copies of in a decomposition Mod 2) .
- Let be a compact, connected, oriented 2-dimensional manifold, i.e. a surface, of genus such that the boundary is either empty or is connected. Embed in , where . Choose a framing of M, that is a trivialization of the normal (m-2)-plane vector bundle. (This is possible for , so is certainly possible for ). Choose a symplectic basis for . Each basis element is represented by an embedded circle . The normal (m-1)-plane vector bundle of has two trivializations, one determined by a standard framing of a standard embedding and one determined by the framing of M, which differ by a map i.e. an element of for . This can also be viewed as the framed cobordism class of with this framing in the 1-dimensional framed cobordism group , which is generated by the circle with the Lie group framing. The isomorphism here is via the Pontrjagin-Thom construction. Define to be this element. The Arf invariant of the framed surface is now defined
Note that , so we had to stabilise, taking to be at least 4, in order to get an element of . The case is also admissible as long as we take the residue modulo 2 of the framing.
- The Arf invariant of a framed surface detects whether there is a 3-manifold whose boundary is the given surface which extends the given framing. This is because does not bound. represents a torus with a trivialisation on both generators of which twists an odd number of times. The key fact is that up to homotopy there are two choices of trivialisation of a trivial 3-plane bundle over a circle, corresponding to the two elements of . An odd number of twists, known as the Lie group framing, does not extend across a disc, whilst an even number of twists does. (Note that this corresponds to putting a spin structure on our surface.) Pontrjagin used the Arf invariant of framed surfaces to compute the 2-dimensional framed cobordism group , which is generated by the torus with the Lie group framing. The isomorphism here is via the Pontrjagin-Thom construction.
- Let be a Seifert surface for a knot, , which can be represented as a disc with bands attached. The bands will typically be twisted and knotted. Each band corresponds to a generator . can be represented by a circle which traverses one of the bands. Define to be the number of full twists in the band modulo 2. Suppose we let bound , and push the Seifert surface into , so that its boundary still resides in . Around any generator , we now have a trivial normal 3-plane vector bundle. Trivialise it using the trivial framing of the normal bundle to the embedding for 2 of the sections required. For the third, choose a section which remains normal to , whilst always remaining tangent to . This trivialisation again determines an element of , which we take to be . Note that this coincides with the previous definition of .
- The Arf invariant of a knot is defined via its Seifert surface. It is independent of the choice of Seifert surface (The basic surgery change of S-equivalence, adding/removing a tube, adds/deletes a direct summand), and so is a knot invariant. It is additive under connected sum, and vanishes on slice knots, so is a knot concordance invariant.
- The intersection form on the 2k+1-dimensional -coefficient homology of a framed 4k+2-dimensional manifold M has a quadratic refinement , which depends on the framing. For and represented by an embedding the value is 0 or 1, according as to the normal bundle of is trivial or not. The Kervaire invariant of the framed 4k+2-dimensional manifold M is the Arf invariant of the quadratic refinement on . The Kervaire invariant is a homomorphism on the 4k+2-dimensional stable homotopy group of spheres. The Kervaire invariant can also be defined for a 4k+2-dimensional manifold M which is framed except at a point.
- In surgery theory, for any -dimensional normal map there is defined a nonsingular quadratic form on the -coefficient homology kernel
- refining the homological intersection form . The Arf invariant of this form is the Kervaire invariant of (f,b). In the special case this is the Kervaire invariant of M. The Kervaire invariant features in the classification of exotic spheres by Kervaire and Milnor, and more generally in the classification of manifolds by surgery theory. Browder defined using functional Steenrod squares, and Wall defined using framed immersions. The quadratic enhancement crucially provides more information than : it is possible to kill x by surgery if and only if . The corresponding Kervaire invariant detects the surgery obstruction of in the L-group .
- de Rham invariant, a mod 2 invariant of (4k+1)-dimensional manifolds
- Lorenz, Falko; Roquette (2010), "On the Arf invariant in historic perspective", Mathematische Semesterberichte 57: 73–102, doi:10.1007/s00591-010-0072-8.
- Lorenz, Falko; Roquette (2011), "On the Arf invariant in historical perspective, Part 2", Mathematische Semesterberichte 59.
- Arf (1941),
- Martino and Priddy, p.61
- Browder, Proposition III.1.8
- See Lickorish (1997) for the relation between the Arf invariant and the Jones polynomial.
- See Chapter 3 of Carter's book for another equivalent definition of the Arf invariant in terms of self-intersections of discs in 4-dimensional space.
- Arf, Cahit (1941), "Untersuchungen über quadratische Formen in Körpern der Charakteristik 2, I", J. Reine Angew. Math 183: 148–167
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- L. Pontrjagin, Smooth manifolds and their applications in homotopy theory American Mathematical Society Translations, Ser. 2, Vol. 11, pp. 1–114 (1959)
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