The dark side of the moon - new connections in geometry, number theory and physics -

Similar documents
Moonshine: Lecture 3. Moonshine: Lecture 3. Ken Ono (Emory University)

Umbral Moonshine and String Theory

Mathieu Moonshine. Matthias Gaberdiel ETH Zürich. String-Math 2012 Bonn, 19 July 2012

Generalised Moonshine in the elliptic genus of K3

Mock Modular Mathieu Moonshine

1. Introduction and statement of results This paper concerns the deep properties of the modular forms and mock modular forms.

Generalized Mathieu Moonshine and Siegel Modular Forms

Borcherds proof of the moonshine conjecture

Symmetries of K3 sigma models

Ramanujan s Deathbed Letter. Larry Rolen. Emory University

Proof of the Umbral Moonshine Conjecture

Current algebras and higher genus CFT partition functions

A CHARACTERIZATION OF THE MOONSHINE VERTEX OPERATOR ALGEBRA BY MEANS OF VIRASORO FRAMES. 1. Introduction

Umbral Moonshine and K3 CFTs

Black Holes and Hurwitz Class Numbers

Representation theory of vertex operator algebras, conformal field theories and tensor categories. 1. Vertex operator algebras (VOAs, chiral algebras)

Umbral Moonshine and the Niemeier Lattices

Crystal Bases for Quantum Generalized Kac-Moody Algebras

Yasu Kawahigashi ( ) the University of Tokyo/Kavli IPMU (WPI) Kyoto, July 2013

Binary codes related to the moonshine vertex operator algebra

Three Projects Using Lattices, Modular Forms, String Theory & K3 Surfaces

arxiv: v3 [math.nt] 8 Aug 2018

Moonshine. John FR Duncan 1, Michael J Griffin 2 and Ken Ono 2*

Monstrous moonshine and monstrous Lie superalgebras.

Mock and quantum modular forms

Modular Moonshine II. 24 July 1994, corrected 19 Sept 1995

Conformal field theory, vertex operator algebras and operator algebras

Constructing Majorana representations

Periods and generating functions in Algebraic Geometry

The Leech Lattice. Balázs Elek. November 8, Cornell University, Department of Mathematics

Ramanujan s last prophecy: quantum modular forms

Dyon degeneracies from Mathieu moonshine

Quantum Black Holes, Localization & Mock Modular Forms

Quantum Black Holes, Localization & Mock Modular Forms

MOCK THETA FUNCTIONS OF ORDER 2 AND THEIR SHADOW COMPUTATIONS

Holomorphic symplectic fermions

INDEFINITE THETA FUNCTIONS OF MORE GENERAL TYPE: NEW RESULTS AND APPLICATIONS

Constructing Majorana representations

A PROOF OF THE THOMPSON MOONSHINE CONJECTURE

Vertex operator algebras as a new type of symmetry. Beijing International Center for Mathematical Research Peking Universty

Which supersymmetric CFTs have gravity duals?

Holomorphic Bootstrap for Rational CFT in 2D

Sporadic & Exceptional

Three-Charge Black Holes and ¼ BPS States in Little String Theory

Possible Advanced Topics Course

Three-Charge Black Holes and ¼ BPS States in Little String Theory I

Vertex operator algebras, the Verlinde conjecture and modular tensor categories

arxiv: v1 [math.qa] 17 Oct 2016

Counting problems in Number Theory and Physics

arxiv: v3 [math.rt] 20 Aug 2016

(τ) = q (1 q n ) 24. E 4 (τ) = q q q 3 + = (1 q) 240 (1 q 2 ) (1 q 3 ) (1.1)

arxiv:math/ v1 [math.nt] 6 Nov 2004

Local conformal nets arising from framed vertex operator algebras

Frames of the Leech lattice and their applications

Subfactors and Modular Tensor Categories

Chapter 25 Finite Simple Groups. Chapter 25 Finite Simple Groups

Mock modular forms and their shadows

On the representation theory of affine vertex algebras and W-algebras

NUMBER THEORY IN STRING THEORY: SKEW, MOCK, FALSE, AND QUANTUM

Modular Matrix Models & Monstrous Moonshine:

Tensor categories and the mathematics of rational and logarithmic conformal field theory

N = 2 supersymmetric gauge theory and Mock theta functions

Analytic Number Theory

Superconformal Field Theory and Operator Algebras

Simple groups and the classification of finite groups

Quantum Mock Modular Forms Arising From eta-theta Functions

Arithmetic properties of harmonic weak Maass forms for some small half integral weights

On the zeros of certain modular forms

Three-dimensional imprimitive representations of PSL 2 (Z) and their associated vector-valued modular forms

On classification of rational vertex operator algebras of central charge 1

(1 e r ) p24(1 r 2 /2) = det(w)τ(n)e w(nρ) e ρ

N = 2 heterotic string compactifications on orbifolds of K3 T 2

Vertex Operator Algebra Structure of Standard Affine Lie Algebra Modules

Representation theory of W-algebras and Higgs branch conjecture

LMS SW&SW Regional Meeting and Workshop on Algebraic Structures and Quantum Physics Cardiff, December 2017

EXERCISES IN MODULAR FORMS I (MATH 726) (2) Prove that a lattice L is integral if and only if its Gram matrix has integer coefficients.

Some open problems in mathematical two-dimensional conformal field theory

Knot Homology from Refined Chern-Simons Theory

REGULARIZED INNER PRODUCTS AND WEAKLY HOLOMORPHIC HECKE EIGENFORMS

On vertex operator algebras as sl 2 -modules

Vertex algebras, chiral algebras, and factorisation algebras

arxiv:math/ v1 [math.qa] 4 Dec 2003

THE REPRESENTATION THEORY, GEOMETRY, AND COMBINATORICS OF BRANCHED COVERS

Ramanujan s first letter to Hardy: 5 + = 1 + e 2π 1 + e 4π 1 +

PARITY OF THE COEFFICIENTS OF KLEIN S j-function

Eric Perlmutter, DAMTP, Cambridge

Knots and Mirror Symmetry. Mina Aganagic UC Berkeley

Cubic curves: a short survey

TRIPLE GENERATIONS OF THE LYONS SPORADIC SIMPLE GROUP MALEBOGO JOHN MOTALANE MASTER OF SCIENCE MATHEMATICS UNIVERSITY OF SOUTH AFRICA

THE MASTER SPACE OF N=1 GAUGE THEORIES

Elliptic Cohomology. Prospects in Mathematics Durham, December Sarah Whitehouse. University of Sheffield

Conference on Infinite Dimensional Lie Theory and its Applications (15-20 December, 2014) Title & Abstract

Vertex Algebras and Geometry

Virasoro hair on locally AdS 3 geometries

Supported by a Royal Society professorship and by NSF grant DMS

Analytic number theory for probabilists

On some conjectures on VOAs

One-loop Partition Function in AdS 3 /CFT 2

Topics in Geometry: Mirror Symmetry

Three-Dimensional Gravity Reconsidered

Transcription:

The dark side of the moon - new connections in geometry, number theory and physics - Daniel Persson Mathematical Sciences Colloquium January 29, 2018

Symmetries Transformations that leave a geometric object invariant A circle has infinitely many rotational symmetries

Symmetries Transformations that leave a geometric object invariant A circle has infinitely many rotational symmetries

Infinite rotational symmetry Finite reflection symmetry

Symmetry groups The set of symmetries of an object form a mathematical structure called a group. Two consecutive transformations is also a symmetry There exists an identity transformation Each transformation has an inverse Consecutive transformations are associative

Permutation symmetries The set {1,2,3} has 6 permutations (1,2,3) (1,3,2) (2,1,3) (2,3,1) (3,1,2) (3,2,1) These belong to the permutation group of 3 elements.

Ile de feu 2 (Island of fire) M12 Olivier Messiaen 1949 This piece of music has the symmetry group of a 45-dim algebraic structure

Ile de feu 2 Olivier Messiaen 1949 M 12 (Island of fire) This piece of music has the symmetry group of a 45-dim algebraic structure

This corresponds to the following permutation: P 1 =(1, 7, 10, 2, 6, 4, 5, 9, 11, 12)(3, 8)

This corresponds to the following permutation: P 1 =(1, 7, 10, 2, 6, 4, 5, 9, 11, 12)(3, 8) Messiaen also uses the following permutation in another part: P 2 =(1, 6, 9, 2, 7, 3, 5, 4, 8, 10, 11)(12)

This corresponds to the following permutation: P 1 =(1, 7, 10, 2, 6, 4, 5, 9, 11, 12)(3, 8) Messiaen also uses the following permutation in another part: P 2 =(1, 6, 9, 2, 7, 3, 5, 4, 8, 10, 11)(12) Theorem (Diaconis, Graham, Kantor 1985): M 12 = hp 1,P 2 i Of course, Messiaen did not use all 95040 permutations in the Mathieu group!

Finite simple groups Finite groups that can not be divided into smaller pieces are called simple. These are like building blocks of symmetries

Finite simple groups Finite groups that can not be divided into smaller pieces are called simple. These are like building blocks of symmetries Prime numbers Elementary particles 2, 3, 5, 7, 11, 13, 17, 19, 23, 29, 31, 37, 41, 43, 47, 53, 59, 61, 67, 71, 73, 79, 83, 89, 97

Classification of finite simple groups 1832: Galois discovers the first infinite family (alternating groups)

Classification of finite simple groups 1832: Galois discovers the first infinite family (alternating groups) 1861-1873: Mathieu discovers M 11,M 12,M 22,M 23,M 24

Classification of finite simple groups 1832: Galois discovers the first infinite family (alternating groups) 1861-1873: Mathieu discovers M 11,M 12,M 22,M 23,M 24

Classification of finite simple groups 1832: Galois discovers the first infinite family (alternating groups) 1861-1873: Mathieu discovers M 11,M 12,M 22,M 23,M 24 1972-1983: Gorenstein program to classify all finite simple groups

The monster

Conjecture (Fischer & Griess, 1973): There exists a huge finite simple group of order The monster

Conjecture (Fischer & Griess, 1973): There exists a huge finite simple group of order The monster Theorem (Griess 1982): The monster group exists. It is the symmetry group of a certain 196884-dimensional algebraic structure. (commutative, non-associative algebra)

Conjecture (Fischer & Griess, 1973): There exists a huge finite simple group of order The monster Theorem (Griess 1982): The monster group exists. It is the symmetry group of a certain 196884-dimensional algebraic structure. (commutative, non-associative algebra) 1983: The classification program is completed! This was a heroic joint effort of 100 s of mathematicians.

[https://irandrus.files.wordpress.com/2012/06/periodic-table-of-groups.pdf]

Classification Several infinite families: cyclic, alternating, Lie type 26 sporadic cases

Classification Several infinite families: cyclic, alternating, Lie type 26 sporadic cases Monster M

Classification Several infinite families: cyclic, alternating, Lie type 26 sporadic cases The happy family (all related to the monster)

Classification Several infinite families: cyclic, alternating, Lie type 26 sporadic cases The happy family (all related to the monster) Pariah groups (not related to the monster)

Classification Several infinite families: cyclic, alternating, Lie type 26 sporadic cases The happy family (all related to the monster) Pariah groups (not related to the monster) Why do these groups exist?

The first hints of moonshine

The first hints of moonshine In 1978 John McKay was taking a break from the classification program of finite groups and was doing some recreational reading in number theory.

The first hints of moonshine In 1978 John McKay was taking a break from the classification program of finite groups and was doing some recreational reading in number theory. He then stumbled upon the following series expansion: J(q) = 1 q + 196884q + 21493760q2 + 864299970q 3 + 20245856256q 4 +

The first hints of moonshine In 1978 John McKay was taking a break from the classification program of finite groups and was doing some recreational reading in number theory. He then stumbled upon the following series expansion: J(q) = 1 q + 196884q + 21493760q2 + 864299970q 3 + 20245856256q 4 + Being a finite group theorist he immediately opened up the Atlas

196884 = 1 + 196883 McKay s equation

196884 = 1 + 196883 McKay s equation 21493760 = 1 + 196883 + 21296876 Thompson s equation

196884 = 1 + 196883 McKay s equation 21493760 = 1 + 196883 + 21296876 Thompson s equation What does this really mean?

Fun with the monster 196884 = 1 + 196883 21493760 = 1 + 196883 + 21296876 We can think of 196883 as the dimension of a vector space on which the monster acts This is the smallest non-trivial irreducible representation of M The factor 1 then corresponds to the trivial reps.

Fun with the monster 196884 = 1 + 196883 21493760 = 1 + 196883 + 21296876 We can think of 196883 as the dimension of a vector space on which the monster acts This is the smallest non-trivial irreducible representation of M The factor 1 then corresponds to the trivial reps. 1! V 1 dim R V 1 =1 196883! V 2 dim R V 2 = 196883 21296876! V 3 dim R V 3 = 21296876

Fun with the monster 196884 = 1 + 196883 21493760 = 1 + 196883 + 21296876 We can think of 196883 as the dimension of a vector space on which the monster acts This is the smallest non-trivial irreducible representation of M The factor 1 then corresponds to the trivial reps. 1! V 1 dim R V 1 =1 196883! V 2 dim R V 2 = 196883 21296876! V 3 dim R V 3 = 21296876 =Tr e V 1 =Tr e V 2 =Tr e V 3

Fun with the monster 196884 = 1 + 196883 21493760 = 1 + 196883 + 21296876 We can think of 196883 as the dimension of a vector space on which the monster acts This is the smallest non-trivial irreducible representation of M The factor 1 then corresponds to the trivial reps. 1! V 1 dim R V 1 =1 196883! V 2 dim R V 2 = 196883 21296876! V 3 dim R V 3 = 21296876 =Tr e V 1 =Tr e V 2 =Tr e V 3 characters of the identity element e 2 M

McKay and Thompson conjectured that there exists an infinite-dimensional, graded monster module, called V \, such that V \ = 1M n= 1 V (n)

McKay and Thompson conjectured that there exists an infinite-dimensional, graded monster module, called V \, such that V \ = 1M n= 1 V (n) V ( 1) = V 1 V (0) =0 V (1) = V 1 V 2 V (2) = V 1 V 2 V 3 and the J-function is the graded dimension 1X J(q) = Tr(e V (n) )q n n= 1

McKay and Thompson conjectured that there exists an infinite-dimensional, graded monster module, called V \, such that V \ = 1M n= 1 V (n) V ( 1) = V 1 V (0) =0 V (1) = V 1 V 2 V (2) = V 1 V 2 V 3 and the J-function is the graded dimension 1X J(q) = Tr(e V (n) )q n n= 1 This suggests to also consider for each g 2 M the McKay-Thompson series T g (q) = 1X n= 1 Tr(g V (n) )q n

Modular forms J(q) = 1 q + 196884q + 21493760q2 + 864299970q 3 + 20245856256q 4 +

Modular forms J(q) = 1 q + 196884q + 21493760q2 + 864299970q 3 + 20245856256q 4 + The J-function has a very special invariance property. If we set q = e 2 i 2 H = {z 2 C =(z) > 0} then we have f a + b c + d = f( ) a c b d 2 SL(2, Z)

Modular forms J(q) = 1 q + 196884q + 21493760q2 + 864299970q 3 + 20245856256q 4 + The J-function has a very special invariance property. If we set q = e 2 i 2 H = {z 2 C =(z) > 0} then we have f a + b c + d = f( ) a c b d 2 SL(2, Z) This is a modular form of weight 0 (or a modular function). Up to a constant there is a unique such function which is holomorphic away from a simple pole at the cusp =( )!1

It generates the field of rational functions on the sphere (Hauptmodul) SL(2, Z)\H any modular function = polynomial in J( ) polynomial in J( )

It generates the field of rational functions on the sphere (Hauptmodul) SL(2, Z)\H any modular function = polynomial in J( ) polynomial in J( ) Monstrous moonshine conjecture (Conway-Norton 1979): For all elements g 2 M The McKay-Thompson series T g ( ) are hauptmoduls with respect to some genus zero g SL(2, R) g genus zero g\h

The stuff we were getting was not supported by logical argument. It had the feeling of mysterious moonbeams lighting up dancing Irish leprechauns. Moonshine can also refer to illicitly distilled spirits, and it seemed almost illicit to be working on this stuff. - John Conway

Monster group M???? Modular function J( )

Monster group Enter physics! M 2d conformal field theory (vertex operator algebra) Modular function J( )

1988: Frenkel, Lepowsky, Meurman constructed the moonshine module V \ It is a 2-dimensional orbifold conformal field theory (string theory), a. k. a. vertex operator algebra, whose automorphism group is M A quantum field theory with conformal symmetry defined on a Riemann surface

1988: Frenkel, Lepowsky, Meurman constructed the moonshine module V \ It is a 2-dimensional orbifold conformal field theory (string theory), a. k. a. vertex operator algebra, whose automorphism group is M A quantum field theory with conformal symmetry defined on a Riemann surface To explain moonshine we need a special class of CFT s: holomorphic CFT = self-dual Vertex Operator Algebra (VOA) In general a VOA describes only part of a CFT

1988: Frenkel, Lepowsky, Meurman constructed the moonshine module V \ It is a 2-dimensional orbifold conformal field theory (string theory), a. k. a. vertex operator algebra, whose automorphism group is M A quantum field theory with conformal symmetry defined on a Riemann surface To explain moonshine we need a special class of CFT s: holomorphic CFT = self-dual Vertex Operator Algebra (VOA) In general a VOA describes only part of a CFT 1992: Borcherds proved the full moonshine conjecture, earning him the Fields medal

Do we understand everything now? Why genus zero? Proven by Borcherds but no understanding of its origin. 2016: Explanation proposed by Paquette-D.P.-Volpato using T-duality in string theory. (part of which is a mathematical proof using VOAs)

Do we understand everything now? Why genus zero? Proven by Borcherds but no understanding of its origin. 2016: Explanation proposed by Paquette-D.P.-Volpato using T-duality in string theory. (part of which is a mathematical proof using VOAs) Long-standing conjecture by Frenkel-Lepowsky-Meurman: The moonshine module V \ is unique. Partial results by Dong-Li-Mason, Tuite, Paquette-D.P.-Volpato, Carnahan-Komuro-Urano,

Do we understand everything now? Why genus zero? Proven by Borcherds but no understanding of its origin. 2016: Explanation proposed by Paquette-D.P.-Volpato using T-duality in string theory. (part of which is a mathematical proof using VOAs) Long-standing conjecture by Frenkel-Lepowsky-Meurman: The moonshine module V \ is unique. Partial results by Dong-Li-Mason, Tuite, Paquette-D.P.-Volpato, Carnahan-Komuro-Urano, Generalized moonshine conjecture by Norton in 1987: Moonshine for orbifolds of V \ Given as a PhD project by Borcherds to his student Carnahan around 2005. Complete proof announced by Carnahan in 2017.

Generalized moonshine includes several more of the sporadic groups occurring as centralizers of elements in the monster. Frenkel-Lepowsky-Meurman: The sporadic groups exist because of moonshine.

What does the future have in store? New moonshine!

New moonshine!

Moonshine revolution 2010: New moonshine for M 24 conjectured by Eguchi, Ooguri, Tachikawa The role of the J-function is now played by the elliptic genus of string theory on a K3-surface (weak Jacobi form)

Moonshine revolution 2010: New moonshine for M 24 conjectured by Eguchi-Ooguri-Tachikawa 2012: Proven by Gannon But no analogue of the monster module is constructed! 2013: Generalized Mathieu moonshine established by Gaberdiel-D.P.-Volpato The role of the J-function is now played by the elliptic genus of string theory on a K3-surface (weak Jacobi form)

Moonshine revolution 2010: New moonshine for M 24 conjectured by Eguchi-Ooguri-Tachikawa 2012: Proven by Gannon But no analogue of the monster module is constructed! 2013: Generalized Mathieu moonshine established by Gaberdiel-D.P.-Volpato But why?? The role of the J-function is now played by the elliptic genus of string theory on a K3-surface (weak Jacobi form) There is no string theory on K3 with Mathieu symmetry (Gaberdiel-Hohenegger-Volpato) Also a mathematical formulation of no-go theorem by Huybrechts using autoequivalences of derived categories of coherent sheaves on K3-surfaces.

But it doesn t stop there! 2012: Umbral moonshine proposed by Cheng-Duncan-Harvey A class of 23 moonshines, including Mathieu moonshine. Classified by Niemeier lattices. Involves also non-sporadic groups!

But it doesn t stop there! 2012: Umbral moonshine proposed by Cheng-Duncan-Harvey A class of 23 moonshines, including Mathieu moonshine. Classified by Niemeier lattices. Involves also non-sporadic groups! 2015: Umbral moonshine conjecture proven by Duncan-Griffin-Ono 2016: Generalized Umbral moonshine established by Cheng-de Lange-Whalen

But it doesn t stop there! 2012: Umbral moonshine proposed by Cheng-Duncan-Harvey A class of 23 moonshines, including Mathieu moonshine. Classified by Niemeier lattices. Involves also non-sporadic groups! 2015: Umbral moonshine conjecture proven by Duncan-Griffin-Ono 2016: Generalized Umbral moonshine established by Cheng-de Lange-Whalen Naturally formulated using mock modular forms This goes back to Ramanujan s last letter to Hardy

The Last Letter... Towards the end of his stay in England, Ramanujan fell very ill and he returned to India in 1919 3 months before his death, Ramanujan wrote a final letter to Hardy, including a list of 17 mysterious functions: Mock Theta Functions It took nearly 100 years, and the efforts of generations of mathematicians before Ramanujan s theory was finally understood... (Zwegers)

The Last Letter... Towards the end of his stay in England, Ramanujan fell very ill and he returned to India in 1919 3 months before his death, Ramanujan wrote a final letter to Hardy, including a list of 17 mysterious functions: Mock Theta Functions The mock theta functions arise as McKay-Thompson series in Umbral moonshine!

So what are mock modular forms? Def (Zwegers, Zagier): A mock modular form of weight k is the first member of a pair (h, g) h : H! C is holomorphic with at most exponential growth at cusps g : H! C is a holomorphic cusp form with weight 2 k (the shadow)

So what are mock modular forms? Def (Zwegers, Zagier): A mock modular form of weight k is the first member of a pair (h, g) h : H! C is holomorphic with at most exponential growth at cusps g : H! C is a holomorphic cusp form with weight 2 k (the shadow) The completion h + g with g =(4i) k 1 Z 1 (z + ) k g( z)dz is a non-holomorphic modular form (harmonic Maass form) of weight k

So what are mock modular forms? Def (Zwegers, Zagier): A mock modular form of weight k is the first member of a pair (h, g) h : H! C is holomorphic with at most exponential growth at cusps g : H! C is a holomorphic cusp form with weight 2 k (the shadow) The completion h + g with g =(4i) k 1 Z 1 (z + ) k g( z)dz is a non-holomorphic modular form (harmonic Maass form) of weight k Umbral moonshine arises for weight k =1/2 Note: modular forms are mock modular forms with zero shadow g =0

Pariah moonshine 2017: Duncan, Mertens, Ono proposes moonshine for two of the Pariahs

Pariah moonshine 2017: Duncan, Mertens, Ono proposes moonshine for two of the Pariahs F ( ) = q 4 + 2 + 26752q 3 + 143376q 4 + 8288256q 7 + Mock modular form of weight k =3/2

Pariah moonshine 2017: Duncan, Mertens, Ono proposes moonshine for two of the Pariahs F ( ) = q 4 + 2 + 26752q 3 + 143376q 4 + 8288256q 7 + Mock modular form of weight k =3/2 New connections to number theory F ( ) = q 4 +2+ X D<0 a(d)q D a(d) The coefficients encode information about elliptic curves of discriminant D Implications for the Birch-Swinnerton-Dyer conjecture on the asymptotics of L-functions?

So what is moonshine, really?

So what is moonshine, really? Moonshine is not a well defined term, but everyone in the area recognizes it when they see it. Richard E. Borcherds

So what is moonshine, really?

Roles of vertex operator algebras/cft? M Monstrous Moonshine J( ) =q 1 + 196884q + modular function holomorphic VOA V \ monster Lie algebra (Borcherds algebra) m

Roles of vertex operator algebras/cft? M 24 Mathieu Moonshine mock modular forms string theory on K3? VOA? chiral de Rham complex? (Song) Borcherds Lie algebra???

Roles of vertex operator algebras/cft? The fact that generalized moonshine holds for Umbral moonshine strongly suggest some kind of underlying VOA structure (Gaberdiel-D.P.-Volpato, Cheng-de Lange-Whalen)

Rigidity (Harvey) Consider the case of the J-function: w =0 modular form for SL(2, Z) If it had a shadow it would have weight 2. But there are no weight 2 holomorphic modular forms for. This is due to the genus zero property. SL(2, Z)

Rigidity (Harvey) Consider the case of the J-function: w =0 modular form for SL(2, Z) If it had a shadow it would have weight 2. But there are no weight 2 holomorphic modular forms for. This is due to the genus zero property. SL(2, Z) Umbral moonshine Thompson moonshine Pariah moonshine weight 1/2 mock modular forms weight 3/2 mock modular forms no genus zero property

Rigidity (Harvey) Consider the case of the J-function: w =0 modular form for SL(2, Z) If it had a shadow it would have weight 2. But there are no weight 2 holomorphic modular forms for. This is due to the genus zero property. SL(2, Z) Umbral moonshine Thompson moonshine Pariah moonshine weight 1/2 mock modular forms weight 3/2 mock modular forms no genus zero property What is the analogue of genus zero? A consequence of T-duality in string theory (Paquette-D.P.-Volpato) McKay-Thompson series should be Rademacher summable (Duncan-Frenkel, Cheng-Duncan)

Quantum black holes? Witten proposed that the monster VOA describes the quantum properties of black holes in 3d gravity (via the AdS/CFT correspondence) McKay-Thompson series are partition functions of black hole microstates

Quantum black holes? Witten proposed that the monster VOA describes the quantum properties of black holes in 3d gravity (via the AdS/CFT correspondence) McKay-Thompson series are partition functions of black hole microstates A similar statement holds for Mathieu moonshine (Dabholkar-Murthy-Zagier) (Cheng, Raum, D.P.-Volpato) Black hole microstates organized into conjugacy classes of the sporadic group

Freeman Dyson in 1987: The mock theta-functions give us tantalizing hints of a grand synthesis still to be discovered. Somehow it should be possible to build them into a coherent group-theoretical structure, analogous to the structure of modular forms... This remains a challenge for the future. My dream is that I will live to see the day when our young physicists, struggling to bring the predictions of superstring theory into correspondence with the facts of nature, will be led to enlarge their analytic machinery to include mock theta-functions...

What else will we discover on the dark side of the moon?