東京理科大学 理工学部 加塩朋和
∗E-mail: kashio [email protected]
2018 年 2 月 26 日 ( 月 ) ∼ 3 月 1 日 ( 木 ) 坂内研究室 プロジェクト研究集会 会場:箱根太陽山荘 ( 箱根・強羅温泉 )
∗2010年2月1日〜3月31日 坂内研究室 所属
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 1 / 39
Definition (Euler’s Γ-function) Γ(z) :=
∫
∞0
t
z−1e
−tdt ( ℜ (z) > 0).
z Γ(z) =
∫
∞0
(t
z)
′e
−tdt = [
t
ze
−t]
∞0
−
∫
∞0
t
z(e
−t)
′dt = Γ(z + 1).
Γ(1) =
∫
∞0
e
−tdt = [
− e
−t]
∞0
= 1 ⇝ Γ(n) = (n − 1)!.
Γ(1/2) = 1.772453850 . . . .
Γ(1/3) = 2.678938534 . . . , Γ(2/3) = 1.354117939 . . . . Γ(1/4) = 3.625609908 . . . , Γ(3/4) = 1.225416702 . . . . Γ(1/2)
2= 3.141592653 · · · = π.
Γ(1/4)Γ(3/4)/π = 1.414213562 · · · = √ 2.
Γ(1/3)Γ(2/3)/π = 1.154700538 · · · = 2 √
3/3.
Theorem (Euler’s reflection formula) Γ(z)Γ(1 − z) = π
sin πz (
= 2πi
e
iπz− e
−iπz)
.
Theorem (Multiplication formula)
Γ(z)Γ(z +
12) = 2
12−2z√
2πΓ(2z).
d
∏
−1 k=0Γ(z +
kd) = d
12−dz√
2π
d−1Γ(dz).
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 3 / 39
Theorem (Euler’s reflection formula) Γ(z) √
2π
Γ(1 − z)
√ 2π = 1
2 sin πz = i e
iπz− e
−iπzz∈Q
≒ √
cyclotomic unit.
Theorem (Multiplication formula)
Γ(z) √ 2π
Γ(z +
12)
√ 2π = 2
12−2zΓ(2z)
√ 2π .
d
∏
−1 k=0Γ(z +
kd)
√ 2π = d
12−dzΓ(dz)
√ 2π .
⇒ Γ
1(z) := Γ(z)
√ 2π seems to be more important.
In fact, Γ
1(z)
Hurwitz-Lerch= exp (
dds
∑
∞k=0
(z + k)
−s|
s=0) (z > 0).
Problem
“How many” monomial relations of Γ
1(
Na) := Γ(
Na)/ √
2π are there?
e.g.,
∏
(a,N)=1
Γ
1(
Na) = √
N (“cyclotomic unit”) = 1 (N ̸ = p
r).
Γ
1(
181)
30Γ
1(
185)
9Γ
1(
186)
31Γ
1(
187)
21Γ
1(
188)
12Γ
1(
182)
18Γ
1(
183)
32Γ
1(
184)
21= 1.
⇝ seems to be irregular.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 5 / 39
Problem
“How many” relations of the form ∏
N−1a=1
Γ
1(
Na)
ka∈ Q
×are there?
In other words,
Consider the group (under the multiplication) G
N:= ⟨ Γ
1(
Na) | 1 ≤ a ≤ N ⟩
Q= {
N−1∏
a=1
Γ
1(
Na)
ra| r
a∈ Q }
⊂ C
×/ Q
×.
Then
N − 1 − (# of relations) = dim
QG
N= ? = ϕ(N )/2.
Theorem
G
N:= ⟨ Γ
1(
Na) | 1 ≤ a ≤ N ⟩
Q⊂ C
×/ Q
×. Then dim
QG
N≤ ϕ(N )/2.
Example (N = 6)
Write α ∼ β if α ≡ β mod Q
×.
duplication: Γ
1(a/6)Γ
1(a/6 + 1/2) ∼ Γ
1(2a/6) (a = 1, 2, 3)
triplication: Γ
1(a/6)Γ
1(a/6 + 1/3)Γ
1(a/6 + 2/3) ∼ Γ
1(3a/6) (a = 1, 2)
1 − 1 0 1 0 0 1 0 − 1 1
0 0 1 0 0
1 0 0 0 1
0 1 0 1 0
| {z }
rank=4
Γ
1(1/6) Γ
1(2/6) Γ
1(3/6) Γ
1(4/6) Γ
1(5/6)
=
Γ
1(1/6)Γ
1(2/6)
−1Γ
1(4/6) Γ
1(2/6)Γ
1(4/6)
−1Γ
1(5/6)
Γ
1(3/6) Γ
1(1/6)Γ
1(5/6) Γ
1(2/6)Γ
1(4/6)
∼
1 1 1 1 1
⇒ dim G
6≤ 5 − 4 = 1.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 7 / 39
⇝ Shimura’s period symbol p
K(σ, τ ) ∈ C
×/ Q
×is characterized by p
K(σ, Ξ) := ∏
τ∈Ξ
p
K(σ, τ ) ≡
{ π
−1∫
γ
ω
σ(σ ∈ Ξ)
∫
γ
ω
σ(σ / ∈ Ξ) mod Q
×for abelian variety A of CM-type (K, Ξ), “K -eigen” differential form ω
σ:
A/ Q : abelian variety with K = End(A) ⊗
ZQ . Ξ = Ξ
Ais a half of Hom(K, C ) defined by
K ↷ H
dR1(A, C ) ∼ = C
[K:C]via ⊕
σ∈Hom(K,C)
σ
∪ ∪
K ↷ H
0(A, Ω
1A) ∼ = C
[K:C]/2via ⊕
σ∈Ξ
σ.
K ↷ C · ω
σ⊂ H
dR1(A, C ) via σ ∈ Hom(K, C ): k
∗(ω
σ) = σ(k)ω
σ. γ: arbitrary closed path with ∫
γ
ω
σ̸= 0.
p
K(σ, Ξ) ≡
{ π
−1∫
γ
ω
σ(σ ∈ Ξ)
∫
γ
ω
σ(σ / ∈ Ξ) mod Q
×Example
-2 -1 0 1 2 3
-2 -1 0 1 2
γ
K = Q ( √
− 1), Hom(K, C ) = { id, ρ } , E : y
2= x
3− x, End(E) = Z[“ √
−1”], “ √
−1” : (x, y) 7→ (−x, iy).
⇝ ω
id=
dxy, ω
ρ=
xdxy, Ξ = { id } :
“ √
− 1”
∗dxy=
−iydx= i
dxy, “ √
− 1”
∗xdxy=
xdxiy= − i
xdxy. p
Q(√−1)(id, id) = π
−1∫
γ
dx
y = 2π
−1∫
0−1
√ dx x
3− x
x=−√
=
tπ
−1∫
10
dt
t
34(1 − t)
12= π
−1B (
14,
12) = π
−21Γ(
14) Γ(
34) .
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 9 / 39
Shimura’s period symbol p
K(σ, τ ) ( ≒ CM-periods) provides the transcendental pars of
critical values of L-functions of algebraic Hecke characters.
special values of Hilbert modular forms at CM-points.
the exponentials of the derivative values of partial zeta functions of totally real fields at s = 0
(Yoshida’s conjecture on “absolute CM-periods”).
Enjoys some “nice” properties:
For ι: K
′∼ = K, p
K(σ, τ ) = p
K′(σ ◦ ι, τ ◦ ι).
For K ⊂ L, σ ˜ ∈ Hom(L, C ), τ ∈ Hom(K, C ), p
K(˜ σ|
K, τ ) = p
L(˜ σ, Inf(τ )) := ∏
˜
τ∈Hom(L,C),˜τ|K=τ
p
L(˜ σ, τ ˜ ).
For the complex conjugation ρ, p
K(σ, τ )p
K(σ, ρ ◦ τ ) = 1.
Theorem (Rohrlich, Bannai-Otsubo, Yoshida) Γ
1(
Na) ∼ π
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩,
where [σ
b: ζ
N7→ ζ
Nb] ∈ Gal( Q (ζ
N)/ Q ), ⟨ α ⟩ ∈ (0, 1] denotes the fraction part of α ∈ Q .
sketch of proof.
Explicit computation of ∫
γ
x
r−1y
s−Ndx on the N th Fermat curve F
N: x
N+ y
N= 1:
∫
γ
x
r−1y
s−Ndx ≒
∫
10
t
Nr(1 − t)
Nsdt = B (
Nr,
Ns) = Γ(
Nr)Γ(
Ns) Γ(
r+sN) .
& linear algebra using “nice” properties.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 11 / 39
Γ
1(
Na) ∼ π
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩.
proof of dim
QG
N≤ ϕ(N )/2.
G
N:= ⟨ Γ
1(
Na) | 1 ≤ a ≤ N − 1 ⟩
= ⟨π
δb2p
Q(ζN)(id, σ
b) | (b, N ) = 1⟩ (δ
b:= 1, −1, 0 if b ≡ 1, −1,otherwise)
pK(σ,τ)pK(σ,ρ◦τ)=1
= ⟨ π
δb2p
Q(ζN)(id, σ
b) | (b, N ) = 1, 1 ≤ b ≤ N/2 ⟩ .
Γ
1(
Na) ∼ π
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩.
“Multiplication formula”
d
∏
−1 k=0Γ
1(
Na+
kd) ∼ Γ
1(
daN).
also follows: may assume that d | N (due to p
K(˜ σ|
K, τ ) = p
L(˜ σ, Inf(τ ))).
d−1
∏
k=0
Γ
1(
Na+
kd) ∼ π
∑dk=0−1 12−⟨Na+kd⟩p
Q(ζN)(id, σ
b)
∑
(b,N)=1
∑d−1 k=0 1
2−⟨abN+kbd⟩
= π
12−⟨adN⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abdN ⟩∼ Γ
1(
adN) by multiplication formula ∑
d−1k=0
B
1(x +
kd) = B
1(dx) for B
1(x) = x −
12.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 13 / 39
Γ
1(
Na) ∼ π
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩.
“Reflection formula”
Γ
1(
Na)Γ
1(1 −
Na) ∈ Q
×follows from p
K(σ, τ )p
K(σ, ρ ◦ τ ) = 1.
Moreover the “reciprocity law”
˜ σ
b( Γ
1(⟨
Na⟩)Γ
1(1 − ⟨
Na⟩) )
≡ Γ
1(⟨
abN⟩)Γ
1(1 − ⟨
abN⟩) mod µ
∞for any lift σ ˜
b∈ Gal( Q / Q ) of σ
b: ζ
N7→ ζ
Nb, follows from Coleman’s
formula on the absolute Frobenius action on F
N: x
N+ y
N= 1.
For simplicity, assume that p ∤ 2N. Let B
cris⊂ B
dRbe Fontaine’s period rings, Φ
cris↷ B
cristhe absolute Frobenius action. Similarly to
∫
: H
1sing(F
N( C )) × H
dR1(F
N, Q ) → C ⇝ p
Q(ζN)(σ, τ ) ∈ C
×/ Q
×, we can define the p-adic period symbol
∫
p
: H
1sing(F
N(C)) × H
dR1(F
N, Q) → B
cris⇝ p
Q(ζN),p(σ, τ ) ∈ (B
cris− { 0 } )
Q/( Q ∩ Q
urp)
×Q.
(Note that F
Nhas good reduction at p ∤ N .) By Complex Multiplication, the ratio [ ∫
γ
ω
σ: ∫
p,γ
ω
σ] depends only on Ξ, σ, i.e.,
∫
γωσ
∫γ′ωσ′
=
∫
p,γωσ
∫p,γ′ωσ′
∈ Q .
⇝ [p
Q(ζN)(σ, τ ) : p
Q(ζN),p(σ, τ )] ∈ (C
×× B
Qcris)/(µ
∞× µ
∞)(Q ∩ Q
urp)
×Q.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 15 / 39
Theorem (Coleman, p ∤ 2N for simplicity)
G(
Na) :=
Γ
1(
Na) · (2πi)
1 2−⟨Na⟩ p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩∈ B
crisQ/µ
∞.
⇝ Γ
p( ⟨
paN⟩ ) ≡ p
12−⟨Na⟩G( ⟨
paN⟩ )
Φ
cris(G( ⟨
Na⟩ )) mod µ
∞with Morita’s Γ
p: Z
p→ Z
×p, Γ
p(n) := (−1)
n∏
1≤k≤n−1 p∤k
k.
sketch of proof.
Explicit computation of Φ
crison H
cris1(F
N) by the following lemma
& linear algebra using “nice” properties.
Lemma
Let C/ Q
pbe a projective smooth connected algebraic curve having good (or arboreal) reduction,
ω =
∑
∞ n=1a
nt
n dtt, η =
∑
∞ n=1b
nt
n dtts.t. Φ
cris(ω) = αη.
Then
α = lim
k→∞
pσ
p(a
nk) b
pnkwhen lim
k→∞
n
ka
nk= 0.
Note that
x
r−1y
s−Ndx = x
r(1 − x
N)
s−NNdx x =
∑
∞ n=0( − 1)
n(
s−NN
n )
x
r+nNdx x .
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 17 / 39
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩
p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩, Γ
p( ⟨
paN⟩ ) ≡ p
12−⟨Na⟩G( ⟨
paN⟩ )
Φ
cris(G(⟨
Na⟩)) mod µ
∞implies the “reciprocity law on cyclotomic units”
˜ σ
p( Γ
1( ⟨
Na⟩ )Γ
1(1 − ⟨
Na⟩ ) )
≡ Γ
1( ⟨
abN⟩ )Γ
1(1 − ⟨
abN⟩ ) mod µ
∞since
G(⟨
Na⟩)G(1 − ⟨
Na⟩) ≡ Γ
1(⟨
Na⟩)Γ
1(1 − ⟨
Na⟩) mod µ
∞, Γ
p(z)Γ
p(1 − z) ∈ µ
∞,
Φ
cris= ˜ σ
pon Q
urp∩ Q .
Coleman’s formula
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩
p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩,
Γ
p(⟨
paN⟩) ≡ p
12−⟨Na⟩G(⟨
paN⟩)
Φ
cris(G( ⟨
Na⟩ )) mod µ
∞also implies the “Anderson-Gross-Koblitz formula”
d−1
∏
k=0
Γ
p(⟨
pNka⟩) ≡ “Gauss sum” := ∏
(b,N)=1
π
1
h(⟨abN⟩−12)·σb−1
P
mod µ
∞for d := order of p ∈ ( Z /N Z )
×, the maximal subfield H ⊂ Q (ζ
N) where p splits completely, the prime ideal P corresponding to id : H , → Q
p,
P
h= (π
P) with h := h
H.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 19 / 39
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩ p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩, Γ
p( ⟨
paN⟩ ) ≡ p
12−⟨Na⟩G( ⟨
paN⟩ )
Φ
cris(G(⟨
Na⟩)) mod µ
∞sketch of proof of ∏
d−1k=0
Γ
p( ⟨
pNka⟩ ) ≡ ∏
(b,N)=1
π
1
h(⟨abN⟩−12)·σ−1b
P
.
Note that d = deg P
Q(ζN). Hence, for an algebraic Hecke character χ of Q (ζ
N) whose infinity type is the “reflex of the CM-type”,
d−1
∏
k=0
Γ
p( ⟨
pNka⟩ ) ≒ “Φ
dcris↷ H
cris(M (χ))” ≒ χ(P
Q(ζN)).
Morita’s Γ
p: Z
p→ Z
×pis the unique continuous function satisfying Γ
p(0) = 1, Γ
p(z + 1) = z
∗Γ
p(z), z
∗:=
{ −z (z ∈ Z
×p),
− 1 (z ∈ p Z
p).
Proposition (for the proof, see Koblitz, Robert, Schikhof, etc.) Γ
p(z) mod µ
∞satisfies “multiplication formula”:
d
∏
−1 k=0Γ
p(z +
kd) ≡ d
1−dz+(dz)1Γ
p(dz) mod µ
∞(p ∤ d ∈ N ), where z
1∈ Z
pis defined by z = z
0+ pz
1with z
0∈ { 1, 2, . . . , p } . Note that z +
kp∈ / Z
pwhen z ∈ Z
p.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 21 / 39
Definition
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩ p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩, Γ
period( ⟨
paN⟩ ) := p
12−⟨Na⟩G( ⟨
paN⟩ )
Φ
cris(G( ⟨
Na⟩ )) on Z
(p)∩ (0, 1).
We can derive “multiplication formula”:
d
∏
−1 k=0Γ
period(z +
kd) ≡ d
1−dz+(dz)1Γ
period(dz) mod µ
∞(p ∤ d ∈ N ),
from properties of classical Γ-function or period symbols, independently of
Coleman’s formula Γ
p(z) ≡ Γ
period(z).
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩ p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩, Γ
period( ⟨
paN⟩ ) := p
12−⟨Na⟩G( ⟨
paN⟩ )
Φ
cris(G( ⟨
Na⟩ )) on Z
(p)∩ (0, 1).
Proof of “multiplication formula” for period symbols.
z := ⟨ px ⟩ (x ∈ Z
(p)∩ (0, 1)) ⇒ z = px − n (0 ≤ n ≤ p − 1)
⇒ Z
(p)∋ x =
z+np⇒ n = p − z
0(z = z
0+ pz
1, 1 ≤ z
0≤ p) ⇒ x = z
1+ 1 i.e., Γ
period(z) = p
12−(z1+1)Φ G(z)cris(G(z1+1))
(z ∈ Z
(p)∩ (0, 1)) z ∈ (0,
1d) ⇒
∏dk=0−Γ1periodΓperiod(dz)(z+kd)=
∏d−1
k=0Γ1(z+kd)
Γ1(dz)
·
∏d−1Γ1((dz)1+1)k=0Γ1((z+kd)1+1)
·
“p-power” · “period symbols” ≡ d
12−dz· d
(dz)1+1−12≡ d
1−dz+(dz)1.
Note { (z +
kd)
1+ 1 | k = 0, · · · , d − 1 } = {
(dz)d1+1+
kd| k = 0, · · · , d − 1 } since both sets are contained in d
−1Z ∩ [
zp,
zp+ 1 −
pd1].
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 23 / 39
Definition
G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩
p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩, Γ
period(z) := p
12−(z1+1)G(z)
Φ
cris(G(z
1+ 1)) on z ∈ Z
(p)∩ (0, 1).
Remark
p-adic continuity of Γ
period( ⟨
paN⟩ ) follows from the facts that We can take γ so that ∫
γ
x
r−1y
s−Ndx = B(
Nr,
Ns) (Bannai-Otsubo).
Coefficients of x
r−1y
s−Ndx = ∑
∞n=0
(−1)
n(
s−N Nn) x
r+nN dxxare
“continuous” on
Nr,
Ns∈ Z
p.
Then we can define Γ
period(z) on Z
p.
Problem
Is Γ
p(z) mod µ
∞characterized by “multiplication formula”
d−1
∏
k=0
Γ
p(z +
kd) ≡ d
1−dz+(dz)1Γ
p(dz) mod µ
∞(p ∤ d ∈ N )?
⇝ ? ⇝ an alternative proof for Coleman’s formula without explicit calculation.
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 25 / 39
Problem
d
∏
−1 k=0f (z +
kd) ≡ f (dz) (p ∤ d) ⇒ ? ⇒ f (z) ≡ 1
∏
d−1k=0
f (z +
kd) ≡ f (dz)
⇒ ∏
dk=1
f (z +
kd) ≡ f (dz + 1) (replace z with z +
1d)
⇒
f(z+1)f(z)≡
f(dz+1)f(dz)⇒ g(z) :=
f(z+1)f(z)≡ g(dz) (p ∤ d ∈ N )
⇒ g(z) ≡ c
n( ∃ c
ndepends only on n := ord
pz)
Problem
d−1
∏
k=0
f (z +
kd) ≡ f (dz) (p ∤ d)
⇒ g(z) :=
f(z+1)f(z)≡ c
n(n := ord
pz)
⇒ ? ⇒ f (z) ≡ 1
Write z − 1 = x
0+ x
1p + · · · + x
np
n+ · · · ∈ Z
p(0 ≤ x
n≤ p − 1)
⇒ f (z) ≡ lim
n→∞f (1)g(1)g(2) · · · g(x
0+ x
1p + · · · + x
np
n)
≡ lim
n→∞f(1)α
x00α
1x1· · · α
xnn(α
k:= c
p0k−1(p−1)c
p1k−2(p−1)· · · c
pk−−11c
k)
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 27 / 39
Problem
d−1
∏
k=0
f (z +
kd) ≡ f (dz) (p ∤ d)
⇒ f (1 +
∑
∞ k=0x
kp
k) ≡ f (1)
∏
∞ k=0α
xkk(c
k:=
f(pf(pk+1)k), α
k:= c
p0k−1(p−1)· · · c
pk−−11c
k→ 1)
⇒ ? ⇒ f (z) ≡ 1
Consider the case d = 2, z =
12: f (
12)f (1) ≡ f (1)
⇒ f (
12) = f (1 +
−21) = f(1 + ∑
∞k=0 p−1
2
p
k) ≡ f (1) ∏
∞k=0
α
p−1 2
k
≡ 1
⇒ f (1) ≡ ∏
∞k=0
α
−p−1 2
k
⇒ f (1 + ∑
∞k=0
x
kp
k) ≡ ∏
∞k=0
α
xk−p−1 2
k
Proposition
A continuous function f (z) on Z
psatisfies
d
∏
−1 k=0f(z +
kd) ≡ f (dz) (p ∤ d)
⇔ ∃ α
ksatisfying f(1 +
∑
∞ k=0x
kp
k) ≡
∏
∞ k=0α
xk−p−1 2
k
(0 ≤ x
k≤ p − 1).
In particular, there exist infinitely many parameters.
sketch of proof.
z+z′= 1⇒xk+x′k=p−1⇒f(z)f(z′)≡∏∞
k=0
α0k≡1⇒the casez= 0:
d∏−1
k=1
f(kd)≡1.
Then “mathematical induction” by
d−1∏
k=0
f(z+ 1 +kd)≡
d−1∏
k=0
f(z+kd)g(z+kd), f(dz+d)≡f(dz)g(dz)· · ·g(dz+d−1)andg(dz+k)≡g(z+kd)(k= 0, . . . , d−1).
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 29 / 39
Proposition
Assume a continuous function f (z) on Z
psatisfies
d−1
∏
k=0
f (z +
kd) ≡ f (dz) (p ∤ d) and put c
n:=
f(pf(pn+1)n). Then
1
c
0≡ c
1≡ · · · ⇔ f (z) ≡ c
z−1 2
0
.
2
c
1≡ c
2≡ · · · ⇔ f (z) ≡ c
z−1 2
0
(c
1/c
0)
z1+12(z = z
0+ pz
1, 1 ≤ z
0≤ p).
Proof.
1
α
k= c
p0k−1(p−1)· · · c
pk−−11c
k= c
p0k⇒ f (1 + ∑
∞k=0
x
kp
k) ≡ ∏
∞k=0
α
xk−p−1 2
k
= c
∑∞
k=0xkpk−p−21pk
0
= c
z−1 2
0
.
2
α
0= c
0, α
k= c
p0k(c
1/c
0)
pk−1(k ≥ 1)
⇒ f (1 + ∑
∞k=0
x
kp
k) ≡ c
∑∞
k=0xkpk−p−21pk
0
(c
1/c
0)
∑∞k=1xkpk−1−p−21pk−1.
Compare
ccnn+1
of Γ
period(z), Γ
p(z).
Idea:
Γperiod(pz)Γperiod(z+1)
Γperiod(pz+1)Γperiod(z)
= ? ≡
ΓΓpp(pz)Γ(pz+1)Γp(z+1)p(z)= {
1 (p | z) z (p ∤ z)
⇑
Γperiod(z)ΓperiodΓperiod(z+1p(pz))···Γperiod(z+p−p1)= ?
⇑ Γ
period(z) := p
12−z1Φ G(z)cris(G(z1+1))
(z ∈ Z
(p)∩ (0, 1), z = z
0+ pz
1) G(
Na) := Γ
1(
Na) · (2πi)
1 2−⟨Na⟩ p
∏
(b,N)=1
p
Q(ζN),p(id, σ
b)
12−⟨abN⟩(2πi)
12−⟨Na⟩∏
(b,N)=1
p
Q(ζN)(id, σ
b)
12−⟨abN⟩. Seems to be natural to put Γ
period(z) := p
???Φ G(z)cris(G(???))
even for z ∈ p
−1Z
×(p)∩ (0, 1).
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 31 / 39
When p | N , J (F
N) has potentially good reduction
⇝ [p
Q(ζN)(σ, τ ) : p
Q(ζN),p(σ, τ )] ∈ ( C
×× (B
crisQ
p)
Q)/(µ
∞× µ
∞) Q
×. for the composite ring B
crisQ
pof B
crisand Q
pin B
dR.
The action of the Weil group:
W
Qp:= { τ ∈ Gal( Q
p/ Q
p) | τ |
Qurp= Frob
degp τwith deg τ ∈ Z} , τ ∈ W
Qp⇝
{
Φ
τ:= Φ
degcrisτ⊗ τ ↷ B
crisQ
p= B
cris⊗
QurpQ
p, τ ↷ Q ∩ (0, 1) by τ (ζ
Na) = ζ
Nb⇒ τ (
Na) :=
Nb. Define p-adic gamma function on z ∈ ( Q − Z
(p)) ∩ (0, ∞ ) by
Γ
p(z) := exp
p(
dds
p-adic interpolation of ∑
∞k=0
(z + k)
−s|
s=0) .
[p
Q(ζN)(σ, τ ) : p
Q(ζN),p(σ, τ )] ∈ ( C
×× (B
crisQ
p)
Q)/(µ
∞× µ
∞) Q
×. τ ∈ W
Qp⇝ Φ
τ↷ (B
crisQ
p)
Q/µ
∞, τ ↷ Q ∩ (0, 1).
Γ
p(z) := exp
p(
dds
p-adic interpolation of ∑
∞k=0
(z + k)
−s|
s=0) . Theorem (Coleman, p ̸ = 2,
Na∈ ( Q − Z
(p)) ∩ (0, 1))
G(
Na) :=
Γ1(a N)(2πi)
1 2−⟨a
N⟩
p ∏
pQ(ζN),p(id,σb)12−⟨abN⟩ (2πi)12−⟨Na⟩∏
pQ(ζN)(id,σb)12−⟨abN⟩
⇒ Φ
τ(
G(Na) Γp(Na)pe( 12−Na))
≡
G(τ(Na))Γp(τ(Na))pe( 12−τ(Na))
(e := ord
pN ). As a result, Γ
period,τ(z) := p
e(z−τ−1(z))G(z)
Φ
τ(τ
−1(z)) (z ∈ ( Q − Z
(p)) ∩ (0, 1)) is “continuous” at (z, τ
−1(z)).
We need only the continuity!
東京理科大学 理工学部 加塩朋和 On special values ofΓ-function 2月27日15:20–16:20 33 / 39