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It is well known that anomaly cancellations for D_16 Lie algebra are at the root of the first string revolution. For E_8 Lie algebra, cancellation of anomalies is the principal fact leading to the existence of heterotic string. They are in…

High Energy Physics - Theory · Physics 2008-02-03 H. R. Karadayi , M. Gungormez

The SL(2,Z) anomaly recently derived for type IIB supergravity in 10 dimensions is shown to be a consequence of T-duality with the type IIA string, after compactification to 2 dimensions on an 8-fold. This explains the identity of the…

High Energy Physics - Theory · Physics 2016-09-06 Sunil Mukhi

We display the full anomaly structure of supergravity, including new D-term contributions to the conformal anomaly. This expression has the super-Weyl and chiral U(1)_K transformation properties that are required for implementation of the…

High Energy Physics - Theory · Physics 2009-09-28 Daniel Butter , Mary K. Gaillard

We present a theory of reduction of binary quadratic forms with coefficients in Z[lambda], where lambda is the minimal translation in a Hecke group. We generalize from the modular group Gamma(1) = SL(2,Z) to the Hecke groups and make…

Number Theory · Mathematics 2007-05-23 Wendell Culp-Ressler

The problem of the M5 brane anomaly cancellation is addressed. We reformulate FHMM construction making explicit the relation with the M5 brane SUGRA solution. We suggest another solution to the magnetic coupling equation which doesn't need…

High Energy Physics - Theory · Physics 2009-11-07 A. Boyarsky , B. Kulik

We study the normal bundles of the exceptional sets of isolated simple small singularities in the higher dimension when the Picard group of the exceptional set is $\mathbb{Z}$ and the normal bundle of it has some good filtration. In…

Algebraic Geometry · Mathematics 2018-12-31 Rong Du , Xinyi Fang

We describe the first order moduli space of heterotic string theory compactifications which preserve $N=1$ supersymmetry in four dimensions, that is, the infinitesimal parameter space of the Strominger system. We establish that if we…

High Energy Physics - Theory · Physics 2014-12-02 Xenia de la Ossa , Eirik E. Svanes

We use methods of arithmetic geometry to find solutions to the abelian local anomaly cancellation equations for a four-dimensional gauge theory whose Lie algebra has a single $\mathfrak{u}_1$ summand, assuming that a non-trivial solution…

High Energy Physics - Theory · Physics 2025-09-10 Ben Gripaios , Khoi Le Nguyen Nguyen

A notion of local section of the determinant line bundle is defined giving necessary and suficient conditions for anomaly cancellation compatible with locality. This definition gives an intrinsic geometrical interpretation of the local…

Mathematical Physics · Physics 2019-07-02 Roberto Ferreiro Pérez

Reductive W-algebras which are generated by bosonic fields of spin-1, a single spin-2 field and fermionic fields of spin-3/2 are classified. Three new cases are found: a `symplectic' family of superconformal algebras which are extended by…

High Energy Physics - Theory · Physics 2009-10-22 P. Bowcock

We introduce a new method to study mixed characteristic deformation of line bundles. In particular, for sufficiently large smooth projective families $f : \mathscr{X} \to \mathscr{S}$ defined over the ring of $N$-integers…

Algebraic Geometry · Mathematics 2026-02-11 David Urbanik , Ziquan Yang

The moduli stack M_X(E_8) of principal E_8-bundles over a smooth projective curve X carries a natural divisor Delta. We study the pull-back of the divisor Delta to the moduli stack M_X(P), where P is a semi-simple and simply connected group…

Algebraic Geometry · Mathematics 2009-09-14 Arzu Boysal , Christian Pauly

We first consider M-theory formulated on an open eleven-dimensional spin-manifold. There is then a potential anomaly under gauge transformations on the E_8 bundle that is defined over the boundary and also under diffeomorphisms of the…

High Energy Physics - Theory · Physics 2009-10-30 M. Henningson

We give a conceptual explanation of universal deformation formulas for unital associative algebras and prove some results on the structure of their moduli spaces. We then generalize universal deformation formulas to other types of algebras…

Algebraic Topology · Mathematics 2013-08-19 Elisabeth Remm , Martin Markl

We obtain several estimates for bilinear form with exponential sums with binomials $mx^k + nx^\ell$. In particular we show the existence of nontrivial cancellations between such sums when the coefficients $m$ and $n$ vary over rather sparse…

Number Theory · Mathematics 2016-11-29 Kui Liu , Igor E. Shparlinski , Tianping Zhang

Three exceptional modular invariants of SU(4) exist at levels 4, 6 and 8. They can be obtained from appropriate conformal embeddings and the corresponding graphs have self-fusion. From these embeddings, or from their associated modular…

Quantum Algebra · Mathematics 2009-04-14 Robert Coquereaux , Gil Schieber

The $E_8$ root lattice can be constructed from the modular curve $X(13)$ by the invariant theory for the simple group $\text{PSL}(2, 13)$. This gives a different construction of the $E_8$ root lattice. It also gives an explicit construction…

Number Theory · Mathematics 2017-06-09 Lei Yang

We give an overview of the issue of anomalies in field theories with extra dimensions. We start by reviewing in a pedagogical way the computation of the standard perturbative gauge and gravitational anomalies on non-compact spaces, using…

High Energy Physics - Theory · Physics 2009-11-10 C. A. Scrucca , M. Serone

The structure of the commutator algebra for conformal quantum mechanics is considered. Specifically, it is shown that the emergence of a dimensional scale by renormalization implies the existence of an anomaly or quantum-mechanical symmetry…

High Energy Physics - Theory · Physics 2007-05-23 Gino N. J. Ananos , Horacio E. Camblong , Carlos Gorrichategui , Ernesto Hernadez , Carlos R. Ordonez

We give a new construction of the minimal unitary representation of the exceptional group E_8(8) on a Hilbert space of complex functions in 29 variables. Due to their manifest covariance with respect to the E_7(7) subgroup of E_8(8) our…

High Energy Physics - Theory · Physics 2011-02-09 M. Gunaydin , K. Koepsell , H. Nicolai
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