In mathematics, a Witt vector is an infinite sequence of elements of a commutative ring. Ernst Witt showed how to put a ring structure on the set of Witt vectors, in such a way that the ring of Witt vectors over the finite field of order is isomorphic to , the ring of -adic integers. They have a highly non-intuitive structure[1] upon first glance because their additive and multiplicative structure depends on an infinite set of recursive formulas which do not behave like addition and multiplication formulas for standard p-adic integers.

The main idea[1] behind Witt vectors is instead of using the standard -adic expansion

to represent an element in , we can instead consider an expansion using the Teichmüller character

which sends each element in the solution set of in to an element in the solution set of in . That is, we expand out elements in in terms of roots of unity instead of as profinite elements in . We can then express a -adic integer as an infinite sum

which gives a Witt vector

Then, the non-trivial additive and multiplicative structure in Witt vectors comes from using this map to give an additive and multiplicative structure such that induces a commutative ring morphism.

History edit

In the 19th century, Ernst Eduard Kummer studied cyclic extensions of fields as part of his work on Fermat's Last Theorem. This led to the subject now known as Kummer theory. Let   be a field containing a primitive  -th root of unity. Kummer theory classifies degree   cyclic field extensions   of  . Such fields are in bijection with order   cyclic groups  , where   corresponds to  .

But suppose that   has characteristic  . The problem of studying degree   extensions of  , or more generally degree   extensions, may appear superficially similar to Kummer theory. However, in this situation,   cannot contain a primitive  -th root of unity. Indeed, if   is a  -th root of unity in  , then it satisfies  . But consider the expression  . By expanding using binomial coefficients we see that the operation of raising to the  -th power, known here as the Frobenius homomorphism, introduces the factor   to every coefficient except the first and the last, and so modulo   these equations are the same. Therefore  . Consequently, Kummer theory is never applicable to extensions whose degree is divisible by the characteristic.

The case where the characteristic divides the degree is today called Artin–Schreier theory because the first progress was made by Artin and Schreier. Their initial motivation was the Artin–Schreier theorem, which characterizes the real closed fields as those whose absolute Galois group has order two.[2] This inspired them to ask what other fields had finite absolute Galois groups. In the midst of proving that no other such fields exist, they proved that degree   extensions of a field   of characteristic   were the same as splitting fields of Artin–Schreier polynomials. These are by definition of the form   By repeating their construction, they described degree   extensions. Abraham Adrian Albert used this idea to describe degree   extensions. Each repetition entailed complicated algebraic conditions to ensure that the field extension was normal.[3]

Schmid[4] generalized further to non-commutative cyclic algebras of degree  . In the process of doing so, certain polynomials related to the addition of  -adic integers appeared. Witt seized on these polynomials. By using them systematically, he was able to give simple and unified constructions of degree   field extensions and cyclic algebras. Specifically, he introduced a ring now called  , the ring of  -truncated  -typical Witt vectors. This ring has   as a quotient, and it comes with an operator   which is called the Frobenius operator because it reduces to the Frobenius operator on  . Witt observes that the degree   analog of Artin–Schreier polynomials is

 

where  . To complete the analogy with Kummer theory, define   to be the operator   Then the degree   extensions of   are in bijective correspondence with cyclic subgroups   of order  , where   corresponds to the field  .

Motivation edit

Any  -adic integer (an element of  , not to be confused with  ) can be written as a power series  , where the   are usually taken from the integer interval  . It is hard to provide an algebraic expression for addition and multiplication using this representation, as one faces the problem of carrying between digits. However, taking representative coefficients   is only one of many choices, and Hensel himself (the creator of  -adic numbers) suggested the roots of unity in the field as representatives. These representatives are therefore the number   together with the   roots of unity; that is, the solutions of   in  , so that  . This choice extends naturally to ring extensions of   in which the residue field is enlarged to   with  , some power of  . Indeed, it is these fields (the fields of fractions of the rings) that motivated Hensel's choice. Now the representatives are the   solutions in the field to  . Call the field  , with   an appropriate primitive   root of unity (over  ). The representatives are then   and   for  . Since these representatives form a multiplicative set they can be thought of as characters. Some thirty years after Hensel's works Teichmüller studied these characters, which now bear his name, and this led him to a characterisation of the structure of the whole field in terms of the residue field. These Teichmüller representatives can be identified with the elements of the finite field   of order   by taking residues modulo   in  , and elements of   are taken to their representatives by the Teichmüller character  . This operation identifies the set of integers in   with infinite sequences of elements of  .

Taking those representatives the expressions for addition and multiplication can be written in closed form. We now have the following problem (stated for the simplest case:  ): given two infinite sequences of elements of   describe their sum and product as  -adic integers explicitly. This problem was solved by Witt using Witt vectors.

Detailed motivational sketch edit

We derive the ring of  -adic integers   from the finite field   using a construction which naturally generalizes to the Witt vector construction.

The ring   of  -adic integers can be understood as the inverse limit of the rings   taken along the obvious projections. Specifically, it consists of the sequences   with   such that   for   That is, each successive element of the sequence is equal to the previous elements modulo a lower power of p; this is the inverse limit of the projections  

The elements of   can be expanded as (formal) power series in  

 

where the coefficients   are taken from the integer interval   Of course, this power series usually will not converge in   using the standard metric on the reals, but it will converge in   with the  -adic metric. We will sketch a method of defining ring operations for such power series.

Letting   be denoted by  , one might consider the following definition for addition:

 

and one could make a similar definition for multiplication. However, this is not a closed formula, since the new coefficients are not in the allowed set  

Representing elements in Fp as elements in the ring of Witt vectors W(Fp) edit

There is a better coefficient subset of   which does yield closed formulas, the Teichmüller representatives: zero together with the   roots of unity. They can be explicitly calculated (in terms of the original coefficient representatives  ) as roots of   through Hensel lifting, the  -adic version of Newton's method. For example, in   to calculate the representative of   one starts by finding the unique solution of   in   with  ; one gets   Repeating this in   with the conditions   and  , gives   and so on; the resulting Teichmüller representative of  , denoted  , is the sequence

 

The existence of a lift in each step is guaranteed by the greatest common divisor   in every  

This algorithm shows that for every  , there is exactly one Teichmüller representative with  , which we denote   Indeed, this defines the Teichmüller character   as a (multiplicative) group homomorphism, which moreover satisfies   if we let   denote the canonical projection. Note however that   is not additive, as the sum need not be a representative. Despite this, if   in   then   in  

Representing elements in Zp as elements in the ring of Witt vectors W(Fp) edit

Because of this one-to-one correspondence given by  , one can expand every  -adic integer as a power series in   with coefficients taken from the Teichmüller representatives. An explicit algorithm can be given, as follows. Write the Teichmüller representative as   Then, if one has some arbitrary  -adic integer of the form   one takes the difference   leaving a value divisible by  . Hence,  . The process is then repeated, subtracting   and proceed likewise. This yields a sequence of congruences

 

So that

 

and   implies:

 

for

 

Hence we have a power series for each residue of x modulo powers of p, but with coefficients in the Teichmüller representatives rather than  . It is clear that

 

since

 

for all   as   so the difference tends to 0 with respect to the  -adic metric. The resulting coefficients will typically differ from the   modulo   except the first one.

Additional properties of elements in the ring of Witt vectors motivating general definition edit

The Teichmüller coefficients have the key additional property that   which is missing for the numbers in  . This can be used to describe addition, as follows. Consider the equation   in   and let the coefficients   now be as in the Teichmüller expansion. Since the Teichmüller character is not additive,   is not true in  . But it holds in   as the first congruence implies. In particular,

 

and thus

 

Since the binomial coefficient   is divisible by  , this gives

 

This completely determines   by the lift. Moreover, the congruence modulo   indicates that the calculation can actually be done in   satisfying the basic aim of defining a simple additive structure.

For   this step is already very cumbersome. Write

 

Just as for   a single  th power is not enough: one must take

 

However,   is not in general divisible by   but it is divisible when   in which case   combined with similar monomials in   will make a multiple of  .

At this step, it becomes clear that one is actually working with addition of the form

 

This motivates the definition of Witt vectors.

Construction of Witt rings edit

Fix a prime number p. A Witt vector[5] over a commutative ring   (relative to the prime  ) is a sequence   of elements of  . Define the Witt polynomials   by

  1.  
  2.  
  3.  

and in general

 

The   are called the ghost components of the Witt vector  , and are usually denoted by  ; taken together, the   define the ghost map to  . If   is p-torsionfree, then the ghost map is injective and the ghost components can be thought of as an alternative coordinate system for the  -module of sequences (though note that the ghost map is not surjective unless   is p-divisible).

The ring of (p-typical) Witt vectors   is defined by componentwise addition and multiplication of the ghost components. That is, that there is a unique way to make the set of Witt vectors over any commutative ring   into a ring such that:

  1. the sum and product are given by polynomials with integral coefficients that do not depend on  , and
  2. projection to each ghost component is a ring homomorphism from the Witt vectors over  , to  .

In other words,

  •   and   are given by polynomials with integral coefficients that do not depend on R, and
  •   and  

The first few polynomials giving the sum and product of Witt vectors can be written down explicitly. For example,

 
 

These are to be understood as shortcuts for the actual formulas. If for example the ring   has characteristic  , the division by   in the first formula above, the one by   that would appear in the next component and so forth, do not make sense. However, if the  -power of the sum is developed, the terms   are cancelled with the previous ones and the remaining ones are simplified by  , no division by   remains and the formula makes sense. The same consideration applies to the ensuing components.

Examples of addition and multiplication edit

As would be expected, the unit in the ring of Witt vectors   is the element

 

Adding this element to itself gives a non-trivial sequence, for example in  ,

 

since

 

which is not the expected behavior, since it doesn't equal  . But, when we reduce with the map  , we get  . Note if we have an element   and an element   then

 

showing multiplication also behaves in a highly non-trivial manner.

Examples edit

  • The Witt ring of any commutative ring   in which   is invertible is just isomorphic to   (the product of a countable number of copies of  ). In fact the Witt polynomials always give a homomorphism from the ring of Witt vectors to  , and if   is invertible this homomorphism is an isomorphism.
  • The Witt ring   of the finite field of order   is the ring of  -adic integers written in terms of the Teichmüller representatives, as demonstrated above.
  • The Witt ring   of a finite field of order   is the ring of integers of the unique unramified extension of degree   of the ring of  -adic numbers  . Note   for   the  -th root of unity, hence  .

Universal Witt vectors edit

The Witt polynomials for different primes   are special cases of universal Witt polynomials, which can be used to form a universal Witt ring (not depending on a choice of prime  ). Define the universal Witt polynomials   for   by

  1.  
  2.  
  3.  
  4.  

and in general

 

Again,   is called the vector of ghost components of the Witt vector  , and is usually denoted by  .

We can use these polynomials to define the ring of universal Witt vectors or big Witt ring of any commutative ring   in much the same way as above (so the universal Witt polynomials are all homomorphisms to the ring  ).

Generating Functions edit

Witt also provided another approach using generating functions.[6]

Definition edit

Let   be a Witt vector and define

 

For   let   denote the collection of subsets of   whose elements add up to  . Then

 

We can get the ghost components by taking the logarithmic derivative:

 

Sum edit

Now we can see   if  . So that

 

if   are the respective coefficients in the power series  . Then

 

Since   is a polynomial in   and likewise for  , we can show by induction that   is a polynomial in  

Product edit

If we set   then

 

But

 .

Now 3-tuples   with   are in bijection with 3-tuples   with  , via   (  is the least common multiple), our series becomes

 

So that

 

where   are polynomials of   So by similar induction, suppose

 

then   can be solved as polynomials of  

Ring schemes edit

The map taking a commutative ring   to the ring of Witt vectors over   (for a fixed prime  ) is a functor from commutative rings to commutative rings, and is also representable, so it can be thought of as a ring scheme, called the Witt scheme, over   The Witt scheme can be canonically identified with the spectrum of the ring of symmetric functions.

Similarly, the rings of truncated Witt vectors, and the rings of universal Witt vectors correspond to ring schemes, called the truncated Witt schemes and the universal Witt scheme.

Moreover, the functor taking the commutative ring   to the set   is represented by the affine space  , and the ring structure on   makes   into a ring scheme denoted  . From the construction of truncated Witt vectors, it follows that their associated ring scheme   is the scheme   with the unique ring structure such that the morphism   given by the Witt polynomials is a morphism of ring schemes.

Commutative unipotent algebraic groups edit

Over an algebraically closed field of characteristic 0, any unipotent abelian connected algebraic group is isomorphic to a product of copies of the additive group  . The analogue of this for fields of characteristic   is false: the truncated Witt schemes are counterexamples. (We make them into algebraic groups by forgetting the multiplication and just using the additive structure.) However, these are essentially the only counterexamples: over an algebraically closed field of characteristic  , any unipotent abelian connected algebraic group is isogenous to a product of truncated Witt group schemes.

Universal property edit

André Joyal explicated the universal property of the (p-typical) Witt vectors.[7] The basic intuition is that the formation of Witt vectors is the universal way to deform a characteristic   ring to characteristic 0 together with a lift of its Frobenius endomorphism.[8] To make this precise, define a  -ring   to consist of a commutative ring   together with a map of sets   that is a  -derivation, so that   satisfies the relations

  •  ;
  •  ;
  •  .

The definition is such that given a  -ring  , if one defines the map   by the formula  , then   is a ring homomorphism lifting Frobenius on  . Conversely, if   is  -torsionfree, then this formula uniquely defines the structure of a  -ring on   from that of a Frobenius lift. One may thus regard the notion of  -ring as a suitable replacement for a Frobenius lift in the non  -torsionfree case.

The collection of  -rings and ring homomorphisms thereof respecting the  -structure assembles to a category  . One then has a forgetful functor

 
whose right adjoint identifies with the functor   of Witt vectors. In fact, the functor   creates limits and colimits and admits an explicitly describable left adjoint as a type of free functor; from this, it is not hard to show that   inherits local presentability from   so that one can construct the functor   by appealing to the adjoint functor theorem.

One further has that   restricts to a fully faithful functor on the full subcategory of perfect rings of characteristic p. Its essential image then consists of those  -rings that are perfect (in the sense that the associated map   is an isomorphism) and whose underlying ring is  -adically complete.[9]

See also edit

References edit

  1. ^ a b Fisher, Benji (1999). "Notes on Witt Vectors: a motivated approach" (PDF). Archived (PDF) from the original on 12 January 2019.
  2. ^ Artin, Emil and Schreier, Otto, Über eine Kennzeichnung der reell abgeschlossenen Körper, Abh. Math. Sem. Hamburg 3 (1924).
  3. ^ A. A. Albert, Cyclic fields of degree   over   of characteristic  , Bull. Amer. Math. Soc. 40 (1934).
  4. ^ Schmid, H. L., Zyklische algebraische Funktionenkörper vom Grad pn über endlichen Konstantenkörper der Charakteristik p, Crelle 175 (1936).
  5. ^ Illusie, Luc (1979). "Complexe de de Rham-Witt et cohomologie cristalline". Annales scientifiques de l'École Normale Supérieure (in French). 12 (4): 501–661. doi:10.24033/asens.1374.
  6. ^ Lang, Serge (September 19, 2005). "Chapter VI: Galois Theory". Algebra (3rd ed.). Springer. pp. 330. ISBN 978-0-387-95385-4.
  7. ^ Joyal, André (1985). "δ-anneaux et vecteurs de Witt". C.R. Math. Rep. Acad. Sci. Canada. 7 (3): 177–182.
  8. ^ "Is there a universal property for Witt vectors?". MathOverflow. Retrieved 2022-09-06.
  9. ^ Bhatt, Bhargav (October 8, 2018). "Lecture II: Delta rings" (PDF). Archived (PDF) from the original on September 6, 2022.

Introductory edit

Applications edit

References edit