Quadratic Forms Beyond Arithmetic

3 months ago 2

Alexander Merkurjev

Raman Parimala

Communicated by Notices Associate Editor Han-Bom Moon

1. Introduction

The concept of quadratic forms can be traced back to ancient civilizations such as the Babylonians and Greeks. The Greeks, particularly Euclid in his famous work Elements, presented geometric methods for solving quadratic equations. The Greeks’ focus on geometry and their methods continued to influence mathematicians for centuries. Rules for quadratic equations were also discussed in The Nine Chapters on the Mathematical Art, composed in China by 200 BCE. The general formula for solving a quadratic equation in one variable—equivalent to the modern symbolic formula—was first stated by the Indian mathematician Brahmagupta in his treatise Brāhmasphutasiddhānta in 628 CE.

A quadratic form over a commutative ring is a homogeneous polynomial of degree in variables with coefficients in . In particular, the sum of squares is a quadratic form defined over any .

The problem of representing integers as sums of squares dates back to ancient times. The Greeks, especially the Pythagoreans, were interested in the properties of numbers and their geometric interpretations. The concept of sums of squares is closely related to the Pythagorean theorem, conceived in Mesopotamia (1800 BC), first stated precisely in the Shulbha Sutra of Baudhayana (800 BC) and a statement of proof from China.

In the seventh century, the Indian mathematician Brahmagupta considered what is now called Pell’s equation, , and found a method for its solution.

One of the earliest and most significant results in the area of quadratic forms is Fermat’s theorem on sums of two squares. In the seventeenth century, Fermat stated that an odd prime number can be expressed as a sum of two squares if and only if is congruent to modulo .

Another milestone in the study of sums of squares is the four square theorem, proven by Lagrange in 1770. This theorem states that every positive integer can be represented as the sum of four squares.

Euler’s sums of two squares identity

shows that the set of sums of two squares in a commutative ring is closed under multiplication; this statement was generalized to the binary quadratic form by Brahmagupta. Similar formulas also exist for the sums of four and eight squares.

In the beginning of the nineteenth century Gauss completed the theory of composition of binary quadratic forms over the integers. Far-reaching generalizations in the twenty-first century are the higher composition laws of Bhargava leading to asymptotics for the number of number fields with bounded discriminant of degree at most 5 (see 1).

In the early twentieth century, the main focus of the study of quadratic forms is the arithmetic theory over the rings of algebraic integers and number fields. Witt in the 30s laid the foundation of the algebraic theory of quadratic forms that deals with the study of quadratic forms over arbitrary fields. There was great progress in this study initiated by Pfister’s theory of multiplicative forms in the 60s. Several open questions and conjectures were posed since then, a major one being the Milnor conjectures. Since the 80s, the introduction of powerful techniques from algebraic geometry transformed the study of quadratic forms, leading to great leaps like a solution of the Milnor conjecture.

In this article we trace the progress in the algebraic theory of quadratic forms over the last four decades. For simplicity we only consider fields of characteristic different from , although the theory of quadratic forms in characteristic is also well developed. We stay aside from the theory of quadratic forms over commutative rings such as rings of algebraic integers etc.

In Section 2 we briefly recall basic definitions. In the next section we introduce a method of the study of quadratic forms in the last four decades based on algebraic geometry. We introduce the quadric hypersurface (quadric) associated with a quadratic form and a tool based on the study of closed subvarieties (algebraic cycles) on the products of quadrics. In Section 4 we state two theorems on the proof of Milnor conjectures that compare the graded Witt ring and the graded mod 2 Galois cohomology via Milnor’s -theory of fields.

In the next section some discrete invariants of fields (the -invariant and the Pythagoras number) that are defined by means of quadratic forms are considered. Although these invariants were defined a while ago, the newly developed techniques allowed us to obtain recent results in this direction. There are big open questions concerning these invariants. The determination of the -invariant of function fields of curves over totally imaginary number fields is the ultimate goal while even the finiteness for remains open. Another big open question is the determination of the Pythagoras number of rational function fields over the field of real numbers and the question is open even for .

Another discrete invariant, the dimension of a quadratic form, is discussed in Section 6. One of the old intriguing questions on the determination of all possible splitting patterns of quadratic forms of given dimension is still unsolved.

In the last section we introduce the Chow motives technique. Indecomposable direct summands of the motives of quadrics can be visualized in the diagrams defined in this section.

2. Definitions

Basic references are 13 and 2.

Let be a field of characteristic not , that is in . We write for the multiplicative group of nonzero elements in .

A quadratic form on a finite dimensional vector space over is a map such that

1)

for all and and

2)

the map defined by the formula is a (symmetric) bilinear form.

Note that the bilinear form reconstructs by the equality . Thus, to give a quadratic form on a vector space is the same as to give a symmetric bilinear form on .

The integer is called the dimension of the form . Let be a basis for . If with is an arbitrary vector in , we have

where . Thus is given by a quadratic homogeneous polynomial over . We say that is nondegenerate if the (symmetric) matrix is nondegenerate. This is equivalent to the nondegeneracy of the bilinear form . Below we will consider nondegenerate quadratic forms only.

The determinant of is well defined modulo the subgroup of squares in . The discriminant of is in .

Two quadratic forms and are isomorphic if there is an -linear isomorphism such that for all . The forms and are isomorphic if and only if they are given by the same quadratic polynomial in some bases for and .

Let be nonzero elements in . We write for the quadratic form on the space of -columns . It is called the diagonal form and it has a diagonal matrix in the standard basis for . Every quadratic form over is isomorphic to a diagonal form for some (not uniquely determined) .

If is a quadratic from over and is a field extension, one can define a quadratic form on the -space over with the associated bilinear form on defined by for all and .

The orthogonal sum of two forms and is the quadratic form on defined by .

The form is the hyperbolic plane. A quadratic form is hyperbolic if it is isomorphic to the orthogonal sum of copies of .

A quadratic form is called isotropic if there is a nonzero vector such that ; otherwise, is called anisotropic. Every form is isomorphic to , where is an anisotropic form and . The integer is called the Witt index of . It is equal to if and only if is anisotropic.

Two quadratic forms and are Witt equivalent if the forms and are isomorphic. The set of equivalence classes of quadratic forms over is the Witt ring of with respect to the orthogonal sum and tensor product of forms. For example, is isomorphic to : an integer corresponds to the form under the isomorphism.

One of the most important properties of the Witt ring: two quadratic forms and are isomorphic if and only if in and .

The ideal of even dimensional forms in is called the fundamental ideal. The quotient is isomorphic to . The powers of the fundamental ideal form a filtration on . The discriminant yields an isomorphism between and . The determination of all the quotients is one of the fundamental problems of the algebraic theory of quadratic forms (see Section 4 below).

Let . The -dimensional quadratic form

is called an -fold Pfister form. The th power of the fundamental ideal in the Witt ring is generated by the -fold Pfister forms as an abelian group. An -fold Pfister form is either anisotropic or hyperbolic.

Example 2.1.
1)

Let be a quadratic field extension of . The norm form defined by is the -fold Pfister form .

2)

Let and let be a quaternion -dimensional (associative noncommutative) -algebra with basis and multiplication table , and . The reduced norm form defined by is the -fold Pfister form .

3)

For a triple of elements there is an octonian (nonassociative noncommutative) -dimensional algebra that admits a norm quadratic form that is the -fold Pfister form .

Note that norm forms in all the examples are multiplicative, i.e., the product of two values of is a value of . By the Hurwitz theorem, there are no algebras of dimensions not 1, 2, 4, and 8 with the multiplicative norm. Nevertheless, the set of nonzero values of an -fold Pfister form is closed under multiplication for every . In particular, the sum of squares is a multiplicative quadratic form over any field.

3. Algebro-Geometric Methods

During the last three decades the methods of algebraic geometry interfaced algebraic theory of quadratic forms. One can associate to every quadratic form over the quadric hypersurface (simply called the quadric of ) given by the equation in the projective space . The quadric has dimension and it is smooth if is nondegenerate. The variety is integral if . By definition, has a point over if and only if the form is isotropic. More generally, has a point over a field extension if and only if is isotropic over . For example, the quadric , where , has no points over , but it has points over .

The two quadrics and are isomorphic if and only if the quadratic forms and are similar, that is each of the forms and is an -multiple of the other.

We write for the function field . Note that is isotropic over . Indeed, if are homogeneous coordinates in , we can view the rational functions as the elements in satisfying in . Thus, the equation has a nonzero solution over the field .

The field is a generic splitting field of : the form is isotropic over a field extension if and only if there is an -place from to , that is an -algebra homomorphism of a valuation -subalgebra to .

Consider the following example of an application of the theory of algebraic cycles. Let be an anisotropic quadratic form over and let be a field extension. We would like to know when is isotropic over , i.e., the equation has a nonzero solution over . Typically, the extension is finitely generated, so we can choose an integral variety over such that is isomorphic to the function field of over . By the main property of the quadric, has a point over if and only if there is a morphism or, equivalently, a rational morphism defined on a nonempty open subset . The closure of the graph of in the product yields a cycle class of dimension in the Chow group of rational equivalence classes of cycles of dimension on .

Conversely, a prime algebraic cycle on of dimension that is birational when projecting to yields a rational morphism and therefore a point of over .

Thus, one can use the machinery of algebraic cycles. In particular, one can obtain new cycles by intersecting with other cycles (for example, with the Chern classes of the vector bundles such as the tangent bundle), by considering pull-backs and push-forwards with respect to certain morphisms and also applying the Steenrod operations modulo .

4. Milnor Conjectures

The most spectacular achievement in the algebraic theory of quadratic forms is the solution of the Milnor conjectures.

The Milnor -theory of a field is the (graded) quotient ring of the tensor -algebra of the multiplicative group by the ideal generated by the tensors , where with . In particular, and . The group is generated by the symbols , where , that are multiplicative with respect to every variable (when the other variables are fixed) and satisfy the Steinberg relation if for some . The assignment

yields a well-defined graded ring homomorphism

Let be the absolute Galois group of a field , i.e., is the Galois group of a separable closure of over . We write for the graded cohomology ring of with coefficients in . The multiplication in is given by the cup-product . In particular, and . For every write for the corresponding cohomology class in . The assignment

yields a well-defined graded ring homomorphism

called the norm residue homomorphism modulo . Thus, we have the following diagram of graded ring homomorphisms.

Milnor has conjectured in the 70s that both maps and are isomorphisms for all fields. This conjecture for was settled by the first author in the 80s leading to a solution of the longstanding question on the generation of the -torsion in the Brauer group of a field by quaternion algebras.

Voevodsky in 24 proved one of the Milnor conjectures.

Theorem 4.1.

The graded ring homomorphism is always an isomorphism.

In the proof Voevodsky introduces a number of revolutionary ideas and tools. The main tool is the motivic cohomology defined by Voevodsky. Another tool is the motivic Steenrod operations defined by Voevodsky in analogy with the classical topological operations. The motivic analogs of some of the basic operations, the Milnor operations, played an essential role in the proof.

Enriching Voevodsky’s methods, Orlov, Vishik, and Voevodsky proved in 16 another Milnor conjecture.

Theorem 4.2.

The graded ring homomorphism is always an isomorphism.

In particular, for every , we get a group isomorphism

We can call the maps the cohomological invariants of quadratic forms. These invariants determine anisotropic quadratic forms up to isomorphism as follows. Suppose we are given two anisotropic quadratic forms and and we want to decide whether and are isomorphic, or, equivalently, that the form is hyperbolic. We compute the cohomological invariants of one by one starting with . Note that the next invariant is defined if the previous one vanishes.

The invariant takes to its dimension modulo in . If this invariant vanishes, i.e., has even dimension, then . The invariant is equal to the discriminant of in . If the discriminant of is trivial, the form belongs to and we can compute . This is the class of the Clifford algebra of in the subgroup of the Brauer group of classes of exponent . If this vanishes, then and so on. If , i.e., and , then is hyperbolic (19, p. 33) and the form and are isomorphic.

5. Field Invariants

We discuss two integer invariants of fields associated to quadratic forms, namely the -invariant and the Pythagoras numbers.

5.1. -invariant

The -invariant of a field is the largest dimension of an anisotropic quadratic form over . For example and . The -invariant of a finite field is . The -invariant of a local field is equal to . The Hasse-Minkowski theorem implies that the -invariant of a totally imaginary number field is 4. The formula shows that every power of is the -invariant of some field. Breaking the myth that all invariants of fields associated to quadratic forms are a power of 2, it was shown in 15, that every even integer is the -invariant of some field. On the other hand, it is known that the -invariant is not equal to 3,5 or 7 (19, Proposition 1.3, p. 111). It is expected that every odd integer is the value of the -invariant. Izhboldin has shown in 7 that there are fields of -invariant . In 22 Vishik proved that every integer of the form for can be the -invariant of a field.

The behavior of the -invariant of finite field extensions has been studied extensively. We have the following theorem of Leep for finite field extensions.

Theorem 5.1 (19, Theorem 3.1, p. 120).

Let be an extension of degree . Then .

There may be bounds for the -invariants of finite extensions independent of the degree of the extensions.

The behavior of the -invariant under rational function field extensions is not well understood.

Question 5.2.

If , is

If this question has an affirmative answer, then it follows that there are bounds independent of the degree for the -invariant of finite field extensions. In fact the above question is wide open if is a totally imaginary number field. Even for the function fields of -adic curves, the question remained open until the late 90s when the first finiteness results emerged from Merkurjev and Hoffmann-Van Geel. A theorem of Saltman on bounding indices of elements in the 2-torsion of the Brauer group was pivotal to this theorem. We have the following theorem for function fields of -adic curves.

Theorem 5.3 (17, 18).

Let be a -adic field and the function field of a curve over . Then .

We have the following more general extension of the above theorem which fundamentally uses a theorem of Heath-Brown on the zeros of systems of -adic quadratic forms.

Theorem 5.4 (14).

Let be a -adic field and the function field of a variety of dimension over . Then .

We also have the following theorem extending to general complete discretely valued fields, which uses the patching techniques of Harbater-Hartmann-Krashen.

Theorem 5.5 (4).

Let be a complete discretely valued field with residue field . Let be the function field of a curve over . Suppose that char and there exists an integer such that for all finitely generated extensions of of transcendence degree at most 1. Then .

5.2. Pythagoras number

The Pythagoras number of a field is the smallest integer such that every sum of squares in is a sum of at most squares in .

For example . If is a real number field, then (cf. 19, p. 95). The study of the Pythagoras number of fields which are formally real, i.e., is not a sum of squares in the field, is interesting. The following theorem answers a question of Pfister.

Theorem 5.6 (6).

Every positive integer is the Pythagoras number of a formally real field.

The determination of Pythagoras numbers of rational function fields has a long history. Pfister theory leads to (cf. 19, p. 95). We have and (19, p. 96). We have bounds (19, p. 97). One has the following sharper bound for if is a formally real field of transcendence degree over a subfield, namely (3).

A major open question in this area is the following.

Question 5.7.

What is ?

More on the arithmetic side, interesting questions arise concerning the Pythagoras number of a formally real function field over the field of rational numbers. The inequality goes back to Landau (1906) and we have for real number fields (19, Theorem 1.9, p. 100). Conjecturally for a function field in one variable over a number field, (19, Conjecture 1.10, p. 100). The estimate is due to Colliot-Thélène and a sharper estimate is due to Pop (20). One has the following general result for a function field in variables over a number field, namely (cf. 19, p. 100/101). This combines the Milnor conjecture and a local-global principle for the Galois cohomology of higher-dimensional function fields due to Jannsen in 8.

6. Dimensions of Quadratic Forms

In this section we discuss results on the dimension of quadratic forms satisfying certain conditions.

6.1. Possible dimensions of anisotropic quadratic forms in

An anisotropic -fold Pfister form over belongs to and has dimension . By an Arason-Pfister theorem, every nonzero anisotropic form in is of dimension at least . Are there other restrictions on the dimensions of anisotropic quadratic forms in ?

Karpenko proved in 11 the following general result.

Theorem 6.1.

Let be an anisotropic quadratic form such that for some . If , then for some . All other even degrees at least are possible.

For example, the possible dimensions of anisotropic quadratic forms in are

6.2. Hoffmann’s separation theorem

Let and be two anisotropic quadratic forms over . When is isotropic over the field ? Equivalently, is there a rational morphism ? If is hyperbolic over , then (13, Ch. X, Theorem 4.5). This inequality does not hold in general if is just isotropic over .

Example 6.2.

Let be a general -fold Pfister form (i.e., is similar to an -fold Pfister form) and a subform of of dimension . Over the field the Pfister form is isotropic and hence hyperbolic. Therefore, is isotropic over .

Note that the numbers and in the example are not separated by a power of . The following result proved by Hoffmann in 5 (known as the separation theorem) explains this observation.

Theorem 6.3.

Let and be two anisotropic quadratic forms over . Suppose that for some . Then is anisotropic over .

6.3. The first Witt index

Let be an anisotropic quadratic form of dimension at least over . The form is isotropic. Its Witt index is then positive, denoted , and is called the first Witt index of . The “typical” value of the first Witt index is equal to . If is a “generic” form, e.g., over the field of rational functions, then . On the other hand, if is an anisotropic -fold Pfister form, then since is hyperbolic over .

All possible values of the first Witt index of all quadratic forms of given dimension were determined by Karpenko in 9.

Theorem 6.4.

Let be an anisotropic quadratic form of dimension . Write in base :

with . Then

for some .

In other words, is the remainder upon dividing by some power of less than . In fact, all values of given in the theorem are attained by some forms over appropriate fields. In particular, the number of possible values of is equal to the number of ’s in the base expression of the integer .

Example 6.5.
1)

If , then . This can also be deduced from Hoffmann’s separation theorem.

2)

All possible values of the first Witt index of an anisotropic form of dimension are the -powers . The largest value is the first Witt index of an -fold Pfister form.

6.4. Splitting patterns of quadratic forms

Let be a quadratic form of dimension over and let

denote all Witt indices of quadratic forms over all field extensions of . The tuple of strictly increasing integers is called the splitting pattern of . The smallest integer is the Witt index of . If is anisotropic, i.e., , the integer is the first Witt index .

All possible splitting patterns of quadratic forms of small dimension are determined by Vishik in 21. For example, the splitting patterns of anisotropic -dimensional forms are and . For arbitrary , it is unknown which splitting patterns of -dimensional forms occur.

Example 6.6.

(Excellent form) We employ the following inductive definition. An anisotropic quadratic form of dimension is called excellent if either or there is an excellent form such that and is a general Pfister form. Quadratic forms of dimension up to are excellent. A form of dimension is excellent if and only if it has trivial discriminant. The splitting pattern of an excellent form is determined inductively as follows: if in the definition, , then

In particular, the splitting pattern of an excellent form depends just on the dimension of . For example, if is an excellent form of dimension , then .

6.5. Izhboldin dimension

Let be a quadratic form over . Izhboldin defined an integer associated with the quadric , called the Izhboldin dimension:

where is the first Witt index of .

Example 6.7.

Let and be as in Example 6.2. Then . Note that is isotropic over and is isotropic over .

Theorem 6.8 (10).

Let be a quadratic form and let be a complete (possibly singular) algebraic variety over with all closed points of even degree and such that has a closed point of odd degree over (this holds, for example, if has a point over ). Then and in the case the form is isotropic over .

The following corollary can be viewed as a variant of the Separation Theorem.

Corollary 6.9.

Let and be anisotropic quadratic forms. If is isotropic over , then and in the case the form is isotropic over .

7. Chow Motives of Quadrics

The constructions and results in this section are due to Vishik (see 21). There is a functor from the category of smooth projective varieties to the additive category of Chow Motives taking a variety to its motive and a morphism of varieties to the class of the graph of in the Chow group of the classes of algebraic cycles in . The motive of the projective space decomposes into a direct sum , where are the Tate motives.

Let be a quadric of dimension over an algebraically closed field. Then

Note that the motive appears in the decomposition twice if .

We introduce the set of symbols

where and a bijection between and the set of Tate motives in the decomposition of as follows: and for .

Over an arbitrary field the motive is a direct sum of indecomposable motives. The collection of indecomposable motives in the direct sum is unique up to isomorphism. Over an algebraic closure of , every motive is the sum of certain Tate motives. Thus, the set is the disjoint union of subsets so that for every the elements of correspond to the Tate motives in the decomposition of over an algebraic closure. The motive is indecomposable if and only if .

We will consider the diagrams (graphs) with vertices given by the set . A connection is an edge in the diagram such that both ends of the edge belong to the same subset . (But we don’t necessarily connect every two vertices in the same subset .) We will draw vertices horizontally in the order they appear in the definition of with one exception: if is even we draw the vertices and one under the other to indicate that they correspond to the same Tate motive . Below are the diagrams for a -dimensional hyperbolic (respectively, -dimensional generic) quadrics.

Graphic without alt text Graphic without alt text
Example 7.1.

Let be a subform of dimension of a general anisotropic -fold Pfister form . Rost proved that there is a direct summand of the motive such that over an algebraic closure is isomorphic to . This motive depends on only (not on the choice of ); it is called the Rost motive of and denoted .

The motive of the Pfister quadric is isomorphic to . For example, if , the diagram of looks as follows.

Graphic without alt text
Example 7.2.

Let be an excellent quadratic form of dimension . The motive is a direct sum of twists of Rost motives of the general Pfister forms appearing in the definition of an excellent form. For example, the diagram of the motive of the -dimensional excellent form is as follows.

Graphic without alt text

The shape of the diagram depends only on . All connections in the diagram for an excellent form are called the excellent connections.

Let be an anisotropic form with the splitting pattern and , . There are the following standard connections in the diagram of .

Proposition 7.3.

Let be such that , where , and . Then the symbols and are connected in the diagram of .

The standard connections for an excellent form coincide with excellent connections. Vishik proved in 23 that for an arbitrary form excellent connections also appear in the diagram:

Theorem 7.4.

Let be an anisotropic quadratic form of dimension at least and let be an excellent form of the same dimension. Identify canonically and . If two symbols are connected in , then they are also connected in .

The theorem shows that the diagram of is contained in the diagram of . In particular, the diagram of an excellent form contains the smallest number of connections among the diagram of forms of the same dimension.

Example 7.5.

Let be an anisotropic Albert form, i.e., is a -dimensional quadratic form with trivial discriminant. Its splitting pattern is . Below are the two diagrams with the standard and excellent connections respectively.

Graphic without alt text Graphic without alt text

Combining these diagrams we see that all vertices are connected, hence the motive is indecomposable.

Indecomposability of the motive of a quadric is used in the following application due to Izhboldin and Karpenko in 12.

Theorem 7.6.

Let and be two anisotropic quadratic forms of the same odd dimension. Suppose that is isotropic over and is isotropic over . If in addition at least one of the two motives and is indecomposable, then the forms and are similar.

Acknowledgments

We are grateful to Nikita Karpenko, Alexander Vishik, and Venapally Suresh for the useful comments. We thank Manjul Bhargava for pointing out to us the contributions from ancient civilizations.

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Alexander Merkurjev is a professor of mathematics at the University of California, Los Angeles. His email address is [email protected].

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Raman Parimala is a professor in the department of mathematics at Emory University. Her email address is [email protected].

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Article DOI: 10.1090/noti3192

Credits

Photo of Alexander Merkurjev is courtesy of Alexander Merkurjev.

Photo of Raman Parimala is courtesy of Raman Parimala.

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