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Related papers: K3 Elliptic Genus and an Umbral Moonshine Module

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Monstrous moonshine relates distinguished modular functions to the representation theory of the monster. The celebrated observations that 196884=1+196883 and 21493760=1+196883+21296876, etc., illustrate the case of the modular function…

Representation Theory · Mathematics 2015-12-31 John F. R. Duncan , Michael J. Griffin , Ken Ono

A map between string junctions in the affine 7-brane backgrounds and vector bundles on del Pezzo surfaces is constructed using mirror symmetry. It is shown that the lattice of string junctions with support on an affine 7-brane configuration…

High Energy Physics - Theory · Physics 2014-11-18 Tamas Hauer , Amer Iqbal

The anomaly for the Monster group $\mathbb{M}$ acting on its natural (aka moonshine) representation $V^\natural$ is a particular cohomology class $\omega^\natural \in \mathrm{H}^3(\mathbb{M},\mathrm{U}(1))$ that arises as a conformal field…

Quantum Algebra · Mathematics 2019-11-05 Theo Johnson-Freyd

Given a holomorphic $C_2$-cofinite vertex operator algebra $V$ with graded dimension $j-744$, Borcherds's proof of the monstrous moonshine conjecture implies any finite order automorphism of $V$ has graded trace given by a "completely…

Representation Theory · Mathematics 2018-10-29 Scott Carnahan , Takahiro Komuro , Satoru Urano

We study M-theory and D-brane quantum partition functions for microscopic black hole ensembles within the context of the AdS/CFT correspondence in terms of highest weight representations of infinite-dimensional Lie algebras, elliptic…

High Energy Physics - Theory · Physics 2013-08-12 A. A. Bytsenko , M. Chaichian , R. J. Szabo , A. Tureanu

The word moonshine refers to unexpected relations between the two distinct mathematical structures: finite group representations and modular objects. It is believed that the key to understanding moonshine is through physical theories with…

High Energy Physics - Theory · Physics 2018-07-03 Vassilis Anagiannis , Miranda C. N. Cheng

Using the geometry of the projective plane over the finite field F_q, we construct a Hermitian Lorentzian lattice L_q of dimension (q^2 + q + 2) defined over a certain number ring $\cO$ that depends on q. We show that infinitely many of…

Representation Theory · Mathematics 2012-10-10 Tathagata Basak

In these notes, based on lectures given in Istanbul, we give an introduction both to Monstrous Moonshine and to the classification of rational conformal field theories, using this as an excuse to explore several related structures and go on…

Quantum Algebra · Mathematics 2007-05-23 Terry Gannon

We study the moduli dependence of the chiral ring in N = (4,4) superconformal field theories, with special emphasis on those CFTs that are dual to type IIB string theory on AdS3xS3xX4. The chiral primary operators are sections of vector…

High Energy Physics - Theory · Physics 2009-03-27 Jan de Boer , Jan Manschot , Kyriakos Papadodimas , Erik Verlinde

We study two-dimensional (4,4) superconformal field theories of central charge c=6, corresponding to nonlinear sigma models on K3 surfaces, using the superconformal bootstrap. This is made possible through a surprising relation between the…

High Energy Physics - Theory · Physics 2015-11-13 Ying-Hsuan Lin , Shu-Heng Shao , David Simmons-Duffin , Yifan Wang , Xi Yin

In this note we consider smooth elliptic Calabi-Yau four-folds whose fiber ceases to be flat over compact Riemann surfaces of genus $g$ in the base. These non-flat fibers contribute Kaehler moduli to the four-fold but also add to the…

High Energy Physics - Theory · Physics 2021-09-15 Paul-Konstantin Oehlmann

We discuss the possibility of Mathieu group M24 acting as symmetry group on the K3 elliptic genus as proposed recently by Ooguri, Tachikawa and one of the present authors. One way of testing this proposal is to derive the twisted elliptic…

High Energy Physics - Theory · Physics 2011-06-27 Tohru Eguchi , Kazuhiro Hikami

We study the problem of identifying the moduli fields in fermionic four-dimensional string models. We deform a free-fermionic model by introducing exactly marginal operators in the form of Abelian Thirring interactions on the world-sheet,…

High Energy Physics - Theory · Physics 2011-07-19 Jorge L. Lopez , D. V. Nanopoulos , Kajia Yuan

We explicitly determine the locations of G orbifold conformal field theories, G=Z_M, M=2,3,4,6, G=\hat D_n, n=4,5, or G the binary tetrahedral group \hat T, within the moduli space M^{K3} of N=(4,4) superconformal field theories associated…

High Energy Physics - Theory · Physics 2007-05-23 Katrin Wendland

We present evidence that the CHL string in eight dimensions is dual to F-theory compactified on an elliptic K3 with a $\Gamma_{0}(2)$ monodromy group. The monodromy group $\Gamma_{0}(2)$ allows one to turn on the flux of an antisymmetric…

High Energy Physics - Theory · Physics 2007-05-23 Michael Bershadsky , Tony Pantev , Vladimir Sadov

Mathieu Moonshine, the observation that the Fourier coefficients of the elliptic genus on K3 can be interpreted as dimensions of representations of the Mathieu group M24, has been proven abstractly, but a conceptual understanding in terms…

High Energy Physics - Theory · Physics 2018-01-24 Matthias R. Gaberdiel , Christoph A. Keller , Hynek Paul

We discuss spectra of $AdS_3$ supergravities, arising in the near horizon geometry of D1/D5 systems in orbifolds/orientifolds of type IIB theory with 16 supercharges. These include models studied in a recent paper (hep-th/0012118), where…

High Energy Physics - Theory · Physics 2016-09-06 E. Gava , A. B. Hammou , J. F. Morales , K. S. Narain

An asymptotically flat spacetime in $D=4$ can be mapped via Couch-Torrence conformal inversion to the geometry around an extremal non-expanding and non-rotating horizon. At the linearized level, an infinite tower of conserved Newman-Penrose…

High Energy Physics - Theory · Physics 2026-05-01 Mohammad Akhond , Massimo Bianchi , Antonio Cristofaro , Fabio Riccioni

In the Mathur-Mukhi-Sen (MMS) classification scheme for rational conformal field theories (RCFTs), a RCFT is identified by a pair of non-negative integers $\mathbf{[n, \ell]}$, with $\mathbf{n}$ being the number of characters and…

High Energy Physics - Theory · Physics 2023-08-03 Chethan N. Gowdigere , Sachin Kala , Jagannath Santara

We construct a Borcherds Kac-Moody (BKM) superalgebra on which the Conway group Co$_0$ acts faithfully. We show that the BKM algebra is generated by the BRST-closed states in a chiral superstring theory. We use this construction to produce…

High Energy Physics - Theory · Physics 2019-09-04 Sarah M. Harrison , Natalie M. Paquette , Roberto Volpato
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