On Algebraic Independence of Special Zeta Values in Characteristic p
Jing Yu
National Taiwan University and TIMS, Taipei
July, 2010, Workshop on Arithmetic Geometry
t-motives
Let t, σ be variables independent of θ.
Let ¯k(t)[σ, σ−1] be noncommutative ring of Laurent polynomials in σ with coefficients in ¯k(t), subject to the relation
σf := f(−1)σ for all f ∈ ¯k(t).
Here f(−1) is the rational function obtained from f ∈ ¯k(t) by twisting all its coefficients a ∈ ¯k to a1q.
A pre-t-motive M over Fq is a left ¯k(t)[σ, σ−1]-module which is finite-dimensional over ¯k(t).
Let m ∈ Matr×1(M ) be a ¯k(t)-basis of M .
Multiplying by σ on M is represented by σ(m) = Φm for some matrix Φ ∈ GLr(¯k(t)).
The category of pre-t-motives over Fq forms a rigid abelian Fq(t)-linear tensor category.
t-motives
Let t, σ be variables independent of θ.
Let ¯k(t)[σ, σ−1] be noncommutative ring of Laurent polynomials in σ with coefficients in ¯k(t), subject to the relation
σf := f(−1)σ for all f ∈ ¯k(t).
Here f(−1) is the rational function obtained from f ∈ ¯k(t) by twisting all its coefficients a ∈ ¯k to a1q.
A pre-t-motive M over Fq is a left ¯k(t)[σ, σ−1]-module which is finite-dimensional over ¯k(t).
Let m ∈ Matr×1(M ) be a ¯k(t)-basis of M .
Multiplying by σ on M is represented by σ(m) = Φm for some matrix Φ ∈ GLr(¯k(t)).
The category of pre-t-motives over Fq forms a rigid abelian Fq(t)-linear tensor category.
Frobenius difference equations
From a pre-t-motive, one associates a “system of Frobenius difference equation”which has solutions in series of t.
Consider the operator on C∞ by x 7→ x1q. Then extend this operator to C∞((t)) as follows, for f =P
iaiti∈ C∞((t)) define f(−1) :=P
iaqi−1ti. More generally, for matrix B with entries in C∞((t)) define twisting B(−1) by the rule B(−1)ij = Bij(−1).
Let m ∈ Matr×1(M ) be a ¯k(t)-basis of M .
Multiplying by σ on M is represented by σ(m) = Φm for some matrix Φ ∈ GLr(¯k(t)).
Theequationto be solved in Ψ ∈ Matr(C∞((t)) is : Ψ(−1)= ΦΨ.
Frobenius difference equations
From a pre-t-motive, one associates a “system of Frobenius difference equation”which has solutions in series of t.
Consider the operator on C∞ by x 7→ x1q. Then extend this operator to C∞((t)) as follows, for f =P
iaiti∈ C∞((t)) define f(−1) :=P
iaqi−1ti. More generally, for matrix B with entries in C∞((t)) define twisting B(−1) by the rule B(−1)ij = Bij(−1).
Let m ∈ Matr×1(M ) be a ¯k(t)-basis of M .
Multiplying by σ on M is represented by σ(m) = Φm for some matrix Φ ∈ GLr(¯k(t)).
Theequationto be solved in Ψ ∈ Matr(C∞((t)) is : Ψ(−1)= ΦΨ.
Frobenius difference equations
From a pre-t-motive, one associates a “system of Frobenius difference equation”which has solutions in series of t.
Consider the operator on C∞ by x 7→ x1q. Then extend this operator to C∞((t)) as follows, for f =P
iaiti∈ C∞((t)) define f(−1) :=P
iaqi−1ti. More generally, for matrix B with entries in C∞((t)) define twisting B(−1) by the rule B(−1)ij = Bij(−1).
Let m ∈ Matr×1(M ) be a ¯k(t)-basis of M .
Multiplying by σ on M is represented by σ(m) = Φm for some matrix Φ ∈ GLr(¯k(t)).
Theequationto be solved in Ψ ∈ Matr(C∞((t)) is : Ψ(−1)= ΦΨ.
Let t = θ
We view Ψ as giving a “fundamental”solution of the system of Frobeniusdifference equations described by the algebraic matrix Φ coming from M .
Note that if Ψ0∈ Matr(C∞((t))) is also a solution of the Frobenius system from Φ, then Ψ0−1Ψ ∈ GLr(Fq(t)).
A power series f =P∞
i=0aiti ∈ C∞[[t]] that converges everywhere and satisfies
[k∞(a0, a1, a2, . . . ) : k∞] < ∞
is called an entire power series. As a function of t it takes values in k∞, when restricted to k∞. The ring of the entire power series is denoted by E.
If all entries of a solution Ψ of the Frobenius system in question are in E, one canspecializ Ψ to Ψ(θ).
Let t = θ
We view Ψ as giving a “fundamental”solution of the system of Frobeniusdifference equations described by the algebraic matrix Φ coming from M .
Note that if Ψ0∈ Matr(C∞((t))) is also a solution of the Frobenius system from Φ, then Ψ0−1Ψ ∈ GLr(Fq(t)).
A power series f =P∞
i=0aiti ∈ C∞[[t]] that converges everywhere and satisfies
[k∞(a0, a1, a2, . . . ) : k∞] < ∞
is called an entire power series. As a function of t it takes values in k∞, when restricted to k∞. The ring of the entire power series is denoted by E.
If all entries of a solution Ψ of the Frobenius system in question are in E, one canspecializ Ψ to Ψ(θ).
Rigid analytic trivialization
| · |∞:= a fixed absolute value for the completed field C∞. T := {f ∈ C∞[[t]] | f converges on |t|∞≤ 1}.
L := the fraction field of T.
Pre t-motive M is called rigid analytically trivial if there exists Ψ ∈ GLr(L) such that
Ψ(−1)= ΦΨ.
Such matrix Ψ is called a rigid analytic trivialization of the pre t-motive in question.
The category R of rigid analytically trivial pre-t-motives over Fq
forms a neutral Tannakian category over Fq(t).
Rigid analytic trivialization
| · |∞:= a fixed absolute value for the completed field C∞. T := {f ∈ C∞[[t]] | f converges on |t|∞≤ 1}.
L := the fraction field of T.
Pre t-motive M is called rigid analytically trivial if there exists Ψ ∈ GLr(L) such that
Ψ(−1)= ΦΨ.
Such matrix Ψ is called a rigid analytic trivialization of the pre t-motive in question.
The category R of rigid analytically trivial pre-t-motives over Fq
forms a neutral Tannakian category over Fq(t).
Tannakian duality
Given object M in R and let TM be the strictly full Tannakian subcategory of R generated by M . That is, TM consists of all objects of R isomorphic to subquotients of finite direct sums of
M⊗u⊗ (M∨)⊗v for various u, v,
where M∨ is the dual of M . By Tannakianduality, TM is representable by an affine algebraic group scheme ΓM over Fq(t).
Such ΓM is called the motivic Galois groupof M .
Given rigid analytically trivial pre-t-motive M , the motivic Galois group ΓM is isomorphic over Fq(t) to the linear algebraic Galois group ΓΨ of the associated Frobenius difference equation.
Tannakian duality
Given object M in R and let TM be the strictly full Tannakian subcategory of R generated by M . That is, TM consists of all objects of R isomorphic to subquotients of finite direct sums of
M⊗u⊗ (M∨)⊗v for various u, v,
where M∨ is the dual of M . By Tannakianduality, TM is representable by an affine algebraic group scheme ΓM over Fq(t).
Such ΓM is called the motivic Galois groupof M .
Given rigid analytically trivial pre-t-motive M , the motivic Galois group ΓM is isomorphic over Fq(t) to the linear algebraic Galois group ΓΨ of the associated Frobenius difference equation.
Tannakian duality
Given object M in R and let TM be the strictly full Tannakian subcategory of R generated by M . That is, TM consists of all objects of R isomorphic to subquotients of finite direct sums of
M⊗u⊗ (M∨)⊗v for various u, v,
where M∨ is the dual of M . By Tannakianduality, TM is representable by an affine algebraic group scheme ΓM over Fq(t).
Such ΓM is called the motivic Galois groupof M .
Given rigid analytically trivial pre-t-motive M , the motivic Galois group ΓM is isomorphic over Fq(t) to the linear algebraic Galois group ΓΨ of the associated Frobenius difference equation.
Papanikolas theory 2008
This algebraic Galois group ΓΨ from solution Ψ has the key property
dim ΓΨ = tr.degk(t) k(t)(Ψ).
If furthermore Ψ ∈ Matr(E) and satisfies
tr.deg¯k(t)¯k(t)(Ψ) = tr.deg¯k¯k(Ψ(θ)), then we say that M has the GP property. It follows that
dim ΓM = tr.deg¯k ¯k(Ψ(θ)).
Pre-t-motives having the GP property first come from
Anderson-Brownawell-Papanikolas 2004, through reformulating the submodule theorem of Yu 1997 which plays the role of W¨ustholz subgroup theorem (1989).
Papanikolas theory 2008
This algebraic Galois group ΓΨ from solution Ψ has the key property
dim ΓΨ = tr.degk(t) k(t)(Ψ).
If furthermore Ψ ∈ Matr(E) and satisfies
tr.deg¯k(t)¯k(t)(Ψ) = tr.deg¯k¯k(Ψ(θ)), then we say that M has the GP property. It follows that
dim ΓM = tr.deg¯k ¯k(Ψ(θ)).
Pre-t-motives having the GP property first come from
Anderson-Brownawell-Papanikolas 2004, through reformulating the submodule theorem of Yu 1997 which plays the role of W¨ustholz subgroup theorem (1989).
The Carlitz motive
The Carlitz motive C. Let C = ¯k(t) with σ-action:
σf = (t − θ)f(−1), f ∈ C.
Here Φ = (t − θ). Analytic solution Ψ of the equation Ψ(−1) = (t − θ)Ψ is given by
ΨC(t) = (−θ)−q/(q−1)
∞
Y
i=1
(1 − t/θqi).
Note Galois group here is ΓC = Gm which has dimension 1.
Therefore ΨC(θ) = −1π˜ is transcendental over ¯k,
Motivic Galois theory
We are interested in finitely generated extension of ¯k = Fq(θ) generated by a set S of special values, denoted by KS. In particular we want to determine all algebraic relations among elements of S.
From known algebraic relations, we can guess the transcendence degree of KS over ¯k, and the goal is to prove that is indeed the specific degree in question.
To proceed, we construct a t-motive MS for this purpose, so that it has the GP property and its “periods”ΨS(θ) from rigid analytic trivialization generate also the field KS, then computing the dimension of this motivic Galois group ΓMS.
Motivic Galois theory
We are interested in finitely generated extension of ¯k = Fq(θ) generated by a set S of special values, denoted by KS. In particular we want to determine all algebraic relations among elements of S.
From known algebraic relations, we can guess the transcendence degree of KS over ¯k, and the goal is to prove that is indeed the specific degree in question.
To proceed, we construct a t-motive MS for this purpose, so that it has the GP property and its “periods”ΨS(θ) from rigid analytic trivialization generate also the field KS, then computing the dimension of this motivic Galois group ΓMS.
Motivic Galois games
Suppose we have pre-t-motive M1 (M2) with GP property for set of values S1 (S2 respectively), and we are able to determine the Galois group ΓM1 (ΓM2 respectively). To handle the set S1∪ S2, we form the direct sum of pre-t-motive M = M1⊕ M2. Then the dimension of the Galois group ΓM equals to the transcendence degree over ¯k of the compositum of the field KS1 and KS2 which is KS1∪S2. We have surjective morphisms from ΓM onto both ΓM1 and ΓM2. On many occasions this makes it possible to deduce the dimension of ΓM from the algebraic group structures of ΓM1 and ΓM2. As an example