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Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto de Matemática Pura e Aplicada, Brazil www.impa.br/hossein/ Encontro conjunto CBPF-IMPA, 2011
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Page 1: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting problems in Number Theory andPhysics

Hossein Movasati

IMPA, Instituto de Matemática Pura e Aplicada, Brazilwww.impa.br/∼hossein/

Encontro conjunto CBPF-IMPA, 2011

Page 2: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

A documentary on string theory by Brian Greene:

Page 3: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting

Fibonacci numbers:

Fn = Fn−1 + Fn−2, F0 = 0, F1 = 1.

The Fibonacci numbers give the number of pairs of rabbits nmonths after a single pair begins breeding (and newly bornbunnies are assumed to begin breeding when they are twomonths old), as first described by Leonardo of Pisa (also knownas Fibonacci) in his book Liber Abaci (from mathworld).The generating function for Fibonacci numbers:

F =∞∑

n=0

Fnqn =q

1− q − q2

From this we get

Fn =αn − βn

α− β, α, β =

12

(1±√

5).

limn→∞

Fn

Fn−1= lim

n→∞F

1n

n =12

(1 +√

5)

Page 4: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

CountingFibonacci numbers:

Fn = Fn−1 + Fn−2, F0 = 0, F1 = 1.

The Fibonacci numbers give the number of pairs of rabbits nmonths after a single pair begins breeding (and newly bornbunnies are assumed to begin breeding when they are twomonths old), as first described by Leonardo of Pisa (also knownas Fibonacci) in his book Liber Abaci (from mathworld).The generating function for Fibonacci numbers:

F =∞∑

n=0

Fnqn =q

1− q − q2

From this we get

Fn =αn − βn

α− β, α, β =

12

(1±√

5).

limn→∞

Fn

Fn−1= lim

n→∞F

1n

n =12

(1 +√

5)

Page 5: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

CountingFibonacci numbers:

Fn = Fn−1 + Fn−2, F0 = 0, F1 = 1.

The Fibonacci numbers give the number of pairs of rabbits nmonths after a single pair begins breeding (and newly bornbunnies are assumed to begin breeding when they are twomonths old), as first described by Leonardo of Pisa (also knownas Fibonacci) in his book Liber Abaci (from mathworld).

The generating function for Fibonacci numbers:

F =∞∑

n=0

Fnqn =q

1− q − q2

From this we get

Fn =αn − βn

α− β, α, β =

12

(1±√

5).

limn→∞

Fn

Fn−1= lim

n→∞F

1n

n =12

(1 +√

5)

Page 6: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

CountingFibonacci numbers:

Fn = Fn−1 + Fn−2, F0 = 0, F1 = 1.

The Fibonacci numbers give the number of pairs of rabbits nmonths after a single pair begins breeding (and newly bornbunnies are assumed to begin breeding when they are twomonths old), as first described by Leonardo of Pisa (also knownas Fibonacci) in his book Liber Abaci (from mathworld).The generating function for Fibonacci numbers:

F =∞∑

n=0

Fnqn =q

1− q − q2

From this we get

Fn =αn − βn

α− β, α, β =

12

(1±√

5).

limn→∞

Fn

Fn−1= lim

n→∞F

1n

n =12

(1 +√

5)

Page 7: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

CountingFibonacci numbers:

Fn = Fn−1 + Fn−2, F0 = 0, F1 = 1.

The Fibonacci numbers give the number of pairs of rabbits nmonths after a single pair begins breeding (and newly bornbunnies are assumed to begin breeding when they are twomonths old), as first described by Leonardo of Pisa (also knownas Fibonacci) in his book Liber Abaci (from mathworld).The generating function for Fibonacci numbers:

F =∞∑

n=0

Fnqn =q

1− q − q2

From this we get

Fn =αn − βn

α− β, α, β =

12

(1±√

5).

limn→∞

Fn

Fn−1= lim

n→∞F

1n

n =12

(1 +√

5)

Page 8: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Eisenstein series

E2k = 1 + (−1)k 4kBk

∑n≥1

σ2k−1(n)qn,

k = 1,2,3, q ∈ C, |q| < 1,

B1 =16, B2 =

130, B3 =

142, . . . ,

σi(n) :=∑d |n

d i ,

Page 9: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Eisenstein series

E2k = 1 + (−1)k 4kBk

∑n≥1

σ2k−1(n)qn,

k = 1,2,3, q ∈ C, |q| < 1,

B1 =16, B2 =

130, B3 =

142, . . . ,

σi(n) :=∑d |n

d i ,

Page 10: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Eisenstein series

E2k = 1 + (−1)k 4kBk

∑n≥1

σ2k−1(n)qn,

k = 1,2,3, q ∈ C, |q| < 1,

B1 =16, B2 =

130, B3 =

142, . . . ,

σi(n) :=∑d |n

d i ,

Page 11: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. The theory of modular forms over SL(2,Z): homogeneouspolynomials of the ring

C[E4,E6], deg(E4) = 4, deg(E6) = 6.

2. The theory of quasi/differential modular forms overSL(2,Z): homogeneous polynomials of the ring

C[E2,E4,E6], deg(E2) = 2, deg(E4) = 4, deg(E6) = 6

3. In general, a (quasi) modular form over a subgroup ofSL(2,Z) of finite rank is an element in the algebraic closureof C(E2,E4,E6).

Page 12: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. The theory of modular forms over SL(2,Z): homogeneouspolynomials of the ring

C[E4,E6], deg(E4) = 4, deg(E6) = 6.

2. The theory of quasi/differential modular forms overSL(2,Z): homogeneous polynomials of the ring

C[E2,E4,E6], deg(E2) = 2, deg(E4) = 4, deg(E6) = 6

3. In general, a (quasi) modular form over a subgroup ofSL(2,Z) of finite rank is an element in the algebraic closureof C(E2,E4,E6).

Page 13: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. The theory of modular forms over SL(2,Z): homogeneouspolynomials of the ring

C[E4,E6], deg(E4) = 4, deg(E6) = 6.

2. The theory of quasi/differential modular forms overSL(2,Z): homogeneous polynomials of the ring

C[E2,E4,E6], deg(E2) = 2, deg(E4) = 4, deg(E6) = 6

3. In general, a (quasi) modular form over a subgroup ofSL(2,Z) of finite rank is an element in the algebraic closureof C(E2,E4,E6).

Page 14: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented. J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjectureR. Borcherds 1992: Solved

Page 15: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented. J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjectureR. Borcherds 1992: Solved

Page 16: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented. J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjectureR. Borcherds 1992: Solved

Page 17: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented.

J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjectureR. Borcherds 1992: Solved

Page 18: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented. J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjecture

R. Borcherds 1992: Solved

Page 19: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monstrous moonshine conjecture,

The j-function

j = 1728E3

4

E34 − E2

6=

q−1 + 744 + 196884q + 21493760q2 + 864299970q3 + · · · .

196884 = 196883 + 1

MacKay 1978: 196883 is the number of dimensions in whichthe Monster group can be most simply represented. J.H.Conway, S.P. Norton 1979: Monstrous moonshine conjectureR. Borcherds 1992: Solved

Page 20: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monster group

I If normal subgroups of a group G are {1} and G then G iscalled a simple group.

I In the classification of all finite simple groups there appear26 sporadic groups. The Monster group M is the largest ofthe sporadic groups.

|M| = 246 ·320 ·59 ·76 ·112 ·133 ·17·19·23·29·31·41·47·59·71

I Dimensions of irreducible representations of M: 1, 196883,

21296876, 842609326, 18538750076, 19360062527, 293553734298, 3879214937598, 36173193327999,

125510727015275, 190292345709543, 222879856734249, 1044868466775133, 1109944460516150,

2374124840062976.

Page 21: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monster group

I If normal subgroups of a group G are {1} and G then G iscalled a simple group.

I In the classification of all finite simple groups there appear26 sporadic groups. The Monster group M is the largest ofthe sporadic groups.

|M| = 246 ·320 ·59 ·76 ·112 ·133 ·17·19·23·29·31·41·47·59·71

I Dimensions of irreducible representations of M: 1, 196883,

21296876, 842609326, 18538750076, 19360062527, 293553734298, 3879214937598, 36173193327999,

125510727015275, 190292345709543, 222879856734249, 1044868466775133, 1109944460516150,

2374124840062976.

Page 22: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monster group

I If normal subgroups of a group G are {1} and G then G iscalled a simple group.

I In the classification of all finite simple groups there appear26 sporadic groups. The Monster group M is the largest ofthe sporadic groups.

|M| = 246 ·320 ·59 ·76 ·112 ·133 ·17·19·23·29·31·41·47·59·71

I Dimensions of irreducible representations of M: 1, 196883,

21296876, 842609326, 18538750076, 19360062527, 293553734298, 3879214937598, 36173193327999,

125510727015275, 190292345709543, 222879856734249, 1044868466775133, 1109944460516150,

2374124840062976.

Page 23: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Monster group

I If normal subgroups of a group G are {1} and G then G iscalled a simple group.

I In the classification of all finite simple groups there appear26 sporadic groups. The Monster group M is the largest ofthe sporadic groups.

|M| = 246 ·320 ·59 ·76 ·112 ·133 ·17·19·23·29·31·41·47·59·71

I Dimensions of irreducible representations of M: 1, 196883,

21296876, 842609326, 18538750076, 19360062527, 293553734298, 3879214937598, 36173193327999,

125510727015275, 190292345709543, 222879856734249, 1044868466775133, 1109944460516150,

2374124840062976.

Page 24: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Modularity theorem

An elliptic curve over Z:

E : y2 = 4x3 − a2x − a3,

a2,a3 ∈ Z,∆ := a32 − 27a2

3 6= 0.

Let p be a prime and Np be the number of solutions of Eworking modulo p

ap(E) := p − Np

A version of modularity theorem says that there is modular formof weight 2 associated to some congruence group, namelyf =

∑∞n=0 anqn, such that

ap = ap(E)

for all primes p 6 |∆.

Page 25: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Modularity theorem

An elliptic curve over Z:

E : y2 = 4x3 − a2x − a3,

a2,a3 ∈ Z,∆ := a32 − 27a2

3 6= 0.

Let p be a prime and Np be the number of solutions of Eworking modulo p

ap(E) := p − Np

A version of modularity theorem says that there is modular formof weight 2 associated to some congruence group, namelyf =

∑∞n=0 anqn, such that

ap = ap(E)

for all primes p 6 |∆.

Page 26: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Modularity theorem

An elliptic curve over Z:

E : y2 = 4x3 − a2x − a3,

a2,a3 ∈ Z,∆ := a32 − 27a2

3 6= 0.

Let p be a prime and Np be the number of solutions of Eworking modulo p

ap(E) := p − Np

A version of modularity theorem says that there is modular formof weight 2 associated to some congruence group, namelyf =

∑∞n=0 anqn, such that

ap = ap(E)

for all primes p 6 |∆.

Page 27: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Modularity theorem

An elliptic curve over Z:

E : y2 = 4x3 − a2x − a3,

a2,a3 ∈ Z,∆ := a32 − 27a2

3 6= 0.

Let p be a prime and Np be the number of solutions of Eworking modulo p

ap(E) := p − Np

A version of modularity theorem says that there is modular formof weight 2 associated to some congruence group, namelyf =

∑∞n=0 anqn, such that

ap = ap(E)

for all primes p 6 |∆.

Page 28: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Example:E : y2 + y = x3 − x2

The corresponding modular form is

η(q)2η(q11)12 = q−2q2−q3 +2q4 +q5 +2q6−2q7−2q9−2q10

+q11 − 2q12 + 4q13 + · · · ,

where

η(q) = ∆1

24 = q1

24

∞∏n=1

(1− qn)

is the Dedekind eta function and

∆ =1

1728(E3

4 − E26 ).

Page 29: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Example:E : y2 + y = x3 − x2

The corresponding modular form is

η(q)2η(q11)12 = q−2q2−q3 +2q4 +q5 +2q6−2q7−2q9−2q10

+q11 − 2q12 + 4q13 + · · · ,

where

η(q) = ∆1

24 = q1

24

∞∏n=1

(1− qn)

is the Dedekind eta function and

∆ =1

1728(E3

4 − E26 ).

Page 30: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Example:E : y2 + y = x3 − x2

The corresponding modular form is

η(q)2η(q11)12 = q−2q2−q3 +2q4 +q5 +2q6−2q7−2q9−2q10

+q11 − 2q12 + 4q13 + · · · ,

where

η(q) = ∆1

24 = q1

24

∞∏n=1

(1− qn)

is the Dedekind eta function and

∆ =1

1728(E3

4 − E26 ).

Page 31: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. Taniyama-Shimura conjecture.

2. A. Weils proved for semistable elliptic curves: This was anessential part of the proof of the Fermat last theorem

3. R. Taylor, C. Breuil, B. Conrad, F.Diamond: Modulartiytheorem

Page 32: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. Taniyama-Shimura conjecture.2. A. Weils proved for semistable elliptic curves: This was an

essential part of the proof of the Fermat last theorem

3. R. Taylor, C. Breuil, B. Conrad, F.Diamond: Modulartiytheorem

Page 33: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. Taniyama-Shimura conjecture.2. A. Weils proved for semistable elliptic curves: This was an

essential part of the proof of the Fermat last theorem3. R. Taylor, C. Breuil, B. Conrad, F.Diamond: Modulartiy

theorem

Page 34: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting holomorphic maps from curves to anelliptic curve

1. Let E be a complex elliptic curve and let p1, . . . ,p2g−2 bedistinct points of E , where g ≥ 2.

2. The set Xg(d) of equivalence classes of holomorphic mapsφ : C → E of degree d from compact connected smoothcomplex curves C to E , which have only one doubleramification point over each point pi ∈ E and no otherramification points, is finite. By the Hurwitz formula thegenus of C is equal to g.

3. Define

Fg :=∑d≥1

∑[φ]∈Xd (d)

1|Aut (φ) |

qd .

4. R. Dijkgraaf, M. Douglas, D. Zagier, M. Kaneko:

Fg ∈ Q[E2,E4,E6].

Page 35: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting holomorphic maps from curves to anelliptic curve

1. Let E be a complex elliptic curve and let p1, . . . ,p2g−2 bedistinct points of E , where g ≥ 2.

2. The set Xg(d) of equivalence classes of holomorphic mapsφ : C → E of degree d from compact connected smoothcomplex curves C to E , which have only one doubleramification point over each point pi ∈ E and no otherramification points, is finite. By the Hurwitz formula thegenus of C is equal to g.

3. Define

Fg :=∑d≥1

∑[φ]∈Xd (d)

1|Aut (φ) |

qd .

4. R. Dijkgraaf, M. Douglas, D. Zagier, M. Kaneko:

Fg ∈ Q[E2,E4,E6].

Page 36: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting holomorphic maps from curves to anelliptic curve

1. Let E be a complex elliptic curve and let p1, . . . ,p2g−2 bedistinct points of E , where g ≥ 2.

2. The set Xg(d) of equivalence classes of holomorphic mapsφ : C → E of degree d from compact connected smoothcomplex curves C to E , which have only one doubleramification point over each point pi ∈ E and no otherramification points, is finite. By the Hurwitz formula thegenus of C is equal to g.

3. Define

Fg :=∑d≥1

∑[φ]∈Xd (d)

1|Aut (φ) |

qd .

4. R. Dijkgraaf, M. Douglas, D. Zagier, M. Kaneko:

Fg ∈ Q[E2,E4,E6].

Page 37: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting holomorphic maps from curves to anelliptic curve

1. Let E be a complex elliptic curve and let p1, . . . ,p2g−2 bedistinct points of E , where g ≥ 2.

2. The set Xg(d) of equivalence classes of holomorphic mapsφ : C → E of degree d from compact connected smoothcomplex curves C to E , which have only one doubleramification point over each point pi ∈ E and no otherramification points, is finite. By the Hurwitz formula thegenus of C is equal to g.

3. Define

Fg :=∑d≥1

∑[φ]∈Xd (d)

1|Aut (φ) |

qd .

4. R. Dijkgraaf, M. Douglas, D. Zagier, M. Kaneko:

Fg ∈ Q[E2,E4,E6].

Page 38: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Counting holomorphic maps from curves to anelliptic curve

1. Let E be a complex elliptic curve and let p1, . . . ,p2g−2 bedistinct points of E , where g ≥ 2.

2. The set Xg(d) of equivalence classes of holomorphic mapsφ : C → E of degree d from compact connected smoothcomplex curves C to E , which have only one doubleramification point over each point pi ∈ E and no otherramification points, is finite. By the Hurwitz formula thegenus of C is equal to g.

3. Define

Fg :=∑d≥1

∑[φ]∈Xd (d)

1|Aut (φ) |

qd .

4. R. Dijkgraaf, M. Douglas, D. Zagier, M. Kaneko:

Fg ∈ Q[E2,E4,E6].

Page 39: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

For instance,

F2(q) =1

103680(10E3

2 − 6E2E4 − 4E6),

F3(q) =1

35831808(−6E6

2 + 15E42 E4 − 12E2

2 E34 + 7E3

4 +

4E32 E6 − 12E2E4E6 + 4E2

6 ).

Page 40: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Number of rational curves on K 3 surfaces

1. K3 surface: simply connected+trivial canonical bundle2. In an (n + g)-dimensional linear system |L| the generic

fiber is of genus n + g.3. Let Nn(g) be the number of geometric genus g curves in|L| passing through g points (so that n is the number ofnodes).

4. Yau-Zaslow (1996), Beauville(1999), Göttsche(1994),Bryan-Leung(1999): For generic (X ,L) we have

∞∑n=0

Nn(g)qn = (−124

∂E2

∂q)g 1728q

E34 − E2

6.

Page 41: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Number of rational curves on K 3 surfaces

1. K3 surface: simply connected+trivial canonical bundle

2. In an (n + g)-dimensional linear system |L| the genericfiber is of genus n + g.

3. Let Nn(g) be the number of geometric genus g curves in|L| passing through g points (so that n is the number ofnodes).

4. Yau-Zaslow (1996), Beauville(1999), Göttsche(1994),Bryan-Leung(1999): For generic (X ,L) we have

∞∑n=0

Nn(g)qn = (−124

∂E2

∂q)g 1728q

E34 − E2

6.

Page 42: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Number of rational curves on K 3 surfaces

1. K3 surface: simply connected+trivial canonical bundle2. In an (n + g)-dimensional linear system |L| the generic

fiber is of genus n + g.

3. Let Nn(g) be the number of geometric genus g curves in|L| passing through g points (so that n is the number ofnodes).

4. Yau-Zaslow (1996), Beauville(1999), Göttsche(1994),Bryan-Leung(1999): For generic (X ,L) we have

∞∑n=0

Nn(g)qn = (−124

∂E2

∂q)g 1728q

E34 − E2

6.

Page 43: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Number of rational curves on K 3 surfaces

1. K3 surface: simply connected+trivial canonical bundle2. In an (n + g)-dimensional linear system |L| the generic

fiber is of genus n + g.3. Let Nn(g) be the number of geometric genus g curves in|L| passing through g points (so that n is the number ofnodes).

4. Yau-Zaslow (1996), Beauville(1999), Göttsche(1994),Bryan-Leung(1999): For generic (X ,L) we have

∞∑n=0

Nn(g)qn = (−124

∂E2

∂q)g 1728q

E34 − E2

6.

Page 44: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Number of rational curves on K 3 surfaces

1. K3 surface: simply connected+trivial canonical bundle2. In an (n + g)-dimensional linear system |L| the generic

fiber is of genus n + g.3. Let Nn(g) be the number of geometric genus g curves in|L| passing through g points (so that n is the number ofnodes).

4. Yau-Zaslow (1996), Beauville(1999), Göttsche(1994),Bryan-Leung(1999): For generic (X ,L) we have

∞∑n=0

Nn(g)qn = (−124

∂E2

∂q)g 1728q

E34 − E2

6.

Page 45: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

For the case g = 0 (counting rational curves):

∞∑n=0

Nn(0)qn =1728q

E34 − E2

6= 1 + 24q + 324q2 + 3200q3

+25650q4 + 176256q5 + 1073720q6 + · · ·

(by definition N0(0) = 1). For instance, a smooth quadric X inP3 is K 3 and for such a generic X the number of planes tangentto X in three points is 3200.

Page 46: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

For the case g = 0 (counting rational curves):

∞∑n=0

Nn(0)qn =1728q

E34 − E2

6= 1 + 24q + 324q2 + 3200q3

+25650q4 + 176256q5 + 1073720q6 + · · ·

(by definition N0(0) = 1).

For instance, a smooth quadric X inP3 is K 3 and for such a generic X the number of planes tangentto X in three points is 3200.

Page 47: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

For the case g = 0 (counting rational curves):

∞∑n=0

Nn(0)qn =1728q

E34 − E2

6= 1 + 24q + 324q2 + 3200q3

+25650q4 + 176256q5 + 1073720q6 + · · ·

(by definition N0(0) = 1). For instance, a smooth quadric X inP3 is K 3 and for such a generic X the number of planes tangentto X in three points is 3200.

Page 48: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Beyond classical modular forms and ellipticcurves?!?

Page 49: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Clemens conjecture:

There exits a finite number of rational curves of a fixed degreein a generic quintic in P4.

Page 50: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Clemens conjecture:

There exits a finite number of rational curves of a fixed degreein a generic quintic in P4.

Page 51: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Candelas, de la Ossa, Green, Parkes (1991), in the frameworkof mirror symmetry calculates a quantity Y called Yukawacoupling:

Y = 5 + 2875q

1− q+ 609250 · 23 q2

1− q2 +

317206375 · 33 q3

1− q3 + · · ·+ ndd3 qd

1− qd + · · ·

They claimed that nd is the number of rational curves of degreed in a generic quintic in P4.

Page 52: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Candelas, de la Ossa, Green, Parkes (1991), in the frameworkof mirror symmetry calculates a quantity Y called Yukawacoupling:

Y = 5 + 2875q

1− q+ 609250 · 23 q2

1− q2 +

317206375 · 33 q3

1− q3 + · · ·+ ndd3 qd

1− qd + · · ·

They claimed that nd is the number of rational curves of degreed in a generic quintic in P4.

Page 53: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Candelas, de la Ossa, Green, Parkes (1991), in the frameworkof mirror symmetry calculates a quantity Y called Yukawacoupling:

Y = 5 + 2875q

1− q+ 609250 · 23 q2

1− q2 +

317206375 · 33 q3

1− q3 + · · ·+ ndd3 qd

1− qd + · · ·

They claimed that nd is the number of rational curves of degreed in a generic quintic in P4.

Page 54: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

The main ingredient of the theory of modular forms attached tomirror quintic Calabi-Yau varieties is a particular solution of thedifferential equation Ra1:

t0 = 1t5

(3750t50 + t0t3 − 625t4)

t1 = 1t5

(−390625t60 + 3125t4

0 t1 + 390625t0t4 + t1t3)

t2 = 1t5

(−5859375t70 − 625t5

0 t1 + 6250t40 t2 + 5859375t2

0 t4 + 625t1t4 + 2t2t3)

t3 = 1t5

(−9765625t80 − 625t5

0 t2 + 9375t40 t3 + 9765625t3

0 t4 + 625t2t4 + 3t23 )

t4 = 1t5

(15625t40 t4 + 5t3t4)

t5 = 1t5

(−625t50 t6 + 9375t4

0 t5 + 2t3t5 + 625t4t6)

t6 = 1t5

(9375t40 t6 − 3125t3

0 t5 − 2t2t5 + 3t3t6)

Page 55: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

The main ingredient of the theory of modular forms attached tomirror quintic Calabi-Yau varieties is a particular solution of thedifferential equation Ra1:

t0 = 1t5

(3750t50 + t0t3 − 625t4)

t1 = 1t5

(−390625t60 + 3125t4

0 t1 + 390625t0t4 + t1t3)

t2 = 1t5

(−5859375t70 − 625t5

0 t1 + 6250t40 t2 + 5859375t2

0 t4 + 625t1t4 + 2t2t3)

t3 = 1t5

(−9765625t80 − 625t5

0 t2 + 9375t40 t3 + 9765625t3

0 t4 + 625t2t4 + 3t23 )

t4 = 1t5

(15625t40 t4 + 5t3t4)

t5 = 1t5

(−625t50 t6 + 9375t4

0 t5 + 2t3t5 + 625t4t6)

t6 = 1t5

(9375t40 t6 − 3125t3

0 t5 − 2t2t5 + 3t3t6)

Page 56: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

q-expansion:

Taket = 5q

∂t∂q

and write each ti as a formal power series in q, ti =∑∞

n=0 ti,nqn

and substitute in the above differential equation. We see that itdetermines all the coefficients ti,n uniquely with the initialvalues:

t0,0 =15, t0,1 = 24, t4,0 = 0, t5,0 6= 0

Page 57: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

q-expansion:

Taket = 5q

∂t∂q

and write each ti as a formal power series in q, ti =∑∞

n=0 ti,nqn

and substitute in the above differential equation. We see that itdetermines all the coefficients ti,n uniquely with the initialvalues:

t0,0 =15, t0,1 = 24, t4,0 = 0, t5,0 6= 0

Page 58: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

124 t0 = 1

120 + q + 175q2 + 117625q3 + 111784375q4 +

1269581056265 + 160715581780591q6 +218874699262438350q7 + 314179164066791400375q8 +469234842365062637809375q9+722875994952367766020759550q10 + O(q11)

−1750 t1 = 1

30 + 3q + 930q2 + 566375q3 + 526770000q4 +

592132503858q5 + 745012928951258q6 +1010500474677945510q7 + 1446287695614437271000q8 +2155340222852696651995625q9+3314709711759484241245738380q10 + O(q11)

−150 t2 = 7

10 + 107q + 50390q2 + 29007975q3 +

26014527500q4 + 28743493632402q5+35790559257796542q6 + 48205845153859479030q7 +68647453506412345755300q8+101912303698877609329100625q9 +156263153250677320910779548340q10 + O(q11)

Page 59: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

−15 t3 = 6

5 + 71q + 188330q2 + 100324275q3 +

86097977000q4 + 93009679497426q5+114266677893238146q6 + 152527823430305901510q7 +215812408812642816943200q8+318839967257572460805706125q9 +487033977592346076373921829980q10 + O(q11)

−t4 =0− 1q1 + 170q2 + 41475q3 + 32183000q4 + 32678171250q5 +38612049889554q6 + 50189141795178390q7 +69660564113425804800q8 + 101431587084669781525125q9

153189681044166218779637500q10 + O(q11)

Page 60: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1125 t5 = −1

125 + 15q + 938q2 + 587805q3 + 525369650q4 +

577718296190q5 + 716515428667010q6 +962043316960737646q7 + 1366589803139580122090q8 +2024744003173189934886225q9+3099476777084481347731347688q10 + O(q11)

t6 = · · ·

ConjectureAll q-expansions of

124

t0 −1

120,−1750

t1 −130,−150

t2 −7

10,−15

t3 −65, −t4,

1125

t5 +1

125, · · ·

have positive integer coefficients.

Page 61: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1125 t5 = −1

125 + 15q + 938q2 + 587805q3 + 525369650q4 +

577718296190q5 + 716515428667010q6 +962043316960737646q7 + 1366589803139580122090q8 +2024744003173189934886225q9+3099476777084481347731347688q10 + O(q11)

t6 = · · ·

ConjectureAll q-expansions of

124

t0 −1

120,−1750

t1 −130,−150

t2 −7

10,−15

t3 −65, −t4,

1125

t5 +1

125, · · ·

have positive integer coefficients.

Page 62: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. We get the Yukawa coupling calculated by Candelas, de laOssa, Green, Parkes (1991):

−511(t4 − t50 )2

t35

= 5 + 2875q

1− q+ 609250 · 23 q2

1− q2 +

317206375 · 33 q3

1− q3 + · · ·+ ndd3 qd

1− qd + · · ·

2. Using a result of Yamaguchi and Yau (1994) we get alsogenus g topological string partition functions.

Page 63: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

1. We get the Yukawa coupling calculated by Candelas, de laOssa, Green, Parkes (1991):

−511(t4 − t50 )2

t35

= 5 + 2875q

1− q+ 609250 · 23 q2

1− q2 +

317206375 · 33 q3

1− q3 + · · ·+ ndd3 qd

1− qd + · · ·

2. Using a result of Yamaguchi and Yau (1994) we get alsogenus g topological string partition functions.

Page 64: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Darboux-Halphen-Ramanujan:

Ra2 :

t1 = t2

1 −1

12 t2t2 = 4t1t2 − 6t3t3 = 6t1t3 − 1

3 t22

t = 12q∂

∂q

Write each ti as a formal power series in q, ti =∑∞

n=0 ti,nqn andsubstitute in the above differential equation. We see that itdetermines all the coefficients ti,n uniquely with the initialvalues:

t1,0 = 1, t1,1 = −24

Page 65: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Darboux-Halphen-Ramanujan:

Ra2 :

t1 = t2

1 −1

12 t2t2 = 4t1t2 − 6t3t3 = 6t1t3 − 1

3 t22

t = 12q∂

∂q

Write each ti as a formal power series in q, ti =∑∞

n=0 ti,nqn andsubstitute in the above differential equation. We see that itdetermines all the coefficients ti,n uniquely with the initialvalues:

t1,0 = 1, t1,1 = −24

Page 66: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

In fact we have explicit formulas for ti . They are the well-knownEisenstein series:

ti = aiE2i = ai

(1 + bi

∞∑d=1

d2i−1 qd

1− qd

), i = 1,2,3, (1)

where

(b1,b2,b3) = (−24,240,−504), (a1,a2,a3) = (1,12,8).

Page 67: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Mirror quintic Calabi-Yau varieties:

Let Wψ be the variety obtained by the resolution of singularitiesof the following quotient:

{x ∈ P4 | Q = 0}/G,

Q = x50 + x5

1 + x52 + x5

3 + x54 − 5ψx0x1x2x3x4

where G is the group

G := {(ζ1, ζ2, · · · , ζ5) | ζ5i = 1, ζ1ζ2ζ3ζ4ζ5 = 1}

acting in a canonical way.

Page 68: Counting problems in Number Theory and Physicsw3.impa.br/~hossein/talks/talks/IMPA-CBPF-2011.pdf · Counting problems in Number Theory and Physics Hossein Movasati IMPA, Instituto

Mirror quintic Calabi-Yau varieties:

Let Wψ be the variety obtained by the resolution of singularitiesof the following quotient:

{x ∈ P4 | Q = 0}/G,

Q = x50 + x5

1 + x52 + x5

3 + x54 − 5ψx0x1x2x3x4

where G is the group

G := {(ζ1, ζ2, · · · , ζ5) | ζ5i = 1, ζ1ζ2ζ3ζ4ζ5 = 1}

acting in a canonical way.