Tony Pantev
University of Pennsylvania
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Featured researches published by Tony Pantev.
Journal of High Energy Physics | 2006
Volker Braun; Yang-Hui He; Burt A. Ovrut; Tony Pantev
We show the existence of realistic vacua in string theory whose observable sector has exactly the matter content of the MSSM. This is achieved by compactifying the E_8 x E_8 heterotic superstring on a smooth Calabi-Yau threefold with an SU(4) gauge instanton and a Z_3 x Z_3 Wilson line. Specifically, the observable sector is N=1 supersymmetric with gauge group SU(3)_C x SU(2)_L x U(1)_Y x U(1)_{B-L}, three families of quarks and leptons, each family with a right-handed neutrino, and one Higgs-Higgs conjugate pair. Importantly, there are no extra vector-like pairs and no exotic matter in the zero mode spectrum. There are, in addition, 6 geometric moduli and 13 gauge instanton moduli in the observable sector. The holomorphic SU(4) vector bundle of the observable sector is slope-stable.
Journal of High Energy Physics | 2001
Ron Donagi; Burt A. Ovrut; Tony Pantev; Daniel Waldram
We give a proof of the existence of G = SU(5), stable holomorphic vector bundles on elliptically bered Calabi-Yau threefolds with fundamental group Z2. ThebundlesweconstructhaveEulercharacteristic3andananomalythatcanbe absorbed by M-theory ve-branes. Such bundles provide the basis for constructing the standard model in heterotic M-theory. They are also applicable to vacua of the weakly coupled heterotic string. We explicitly present a class of three family models with gauge group SU(3)CSU(2)LU(1)Y.
Communications in Mathematical Physics | 2010
Andrei Căldăraru; Jacques Distler; Simeon Hellerman; Tony Pantev; Eric Sharpe
In this paper we discuss some examples of abelian gauged linear sigma models realizing twisted derived equivalences between non-birational spaces, and realizing geometries in novel fashions. Examples of gauged linear sigma models with non-birational Kähler phases are a relatively new phenomenon. Most of our examples involve gauged linear sigma models for complete intersections of quadric hypersurfaces, though we also discuss some more general cases and their interpretation. We also propose a more general understanding of the relationship between Kähler phases of gauged linear sigma models, namely that they are related by (and realize) Kuznetsov’s ‘homological projective duality.’ Along the way, we shall see how ‘noncommutative spaces’ (in Kontsevich’s sense) are realized physically in gauged linear sigma models, providing examples of new types of conformal field theories. Throughout, the physical realization of stacks plays a key role in interpreting physical structures appearing in GLSMs, and we find that stacks are implicitly much more common in GLSMs than previously realized.
Journal of High Energy Physics | 2004
Ron Donagi; Burt A. Ovrut; Rene Reinbacher; Tony Pantev
Structure group SU(4) gauge vacua of both weakly and strongly coupled heterotic superstring theory compactified on torus-fibered Calabi-Yau threefolds Z with 2 × 2 fundamental group are presented. This is accomplished by constructing invariant, stable, holomorphic rank four vector bundles on the simply connected cover of Z. Such bundles can descend either to Hermite-Yang-Mills instantons on Z or to twisted gauge fields satisfying the Hermite-Yang-Mills equation corrected by a non-trivial flat B-field. It is shown that large families of such instantons satisfy the constraints imposed by particle physics phenomenology. The discrete parameter spaces of those families are presented, as well as a lower bound on the dimension of the continuous moduli of any such vacuum. In conjunction with 2 × 2 Wilson lines, these SU(4) gauge vacua can lead to standard-like models at low energy with an additional U(1)B−L symmetry. This U(1)B−L symmetry is very helpful in naturally suppressing nucleon decay.
Advances in Theoretical and Mathematical Physics | 2007
Simeon Hellerman; Andre Henriques; Tony Pantev; Eric Sharpe; Matthew Ando
In this paper we study CFT’s associated to gerbes. These theories suffer from a lack of cluster decomposition, but this problem can be resolved: the CFT’s are the same as CFT’s for disconnected targets. Such theories also lack cluster decomposition, but in that form, the lack is manifestly not very problematic. In particular, we shall see that this matching of CFT’s, this duality between noneffective-gaugings and sigma models on disconnected targets, is a worldsheet duality related to T-duality. We perform a wide variety of tests of this claim, ranging from checking partition functions at arbitrary genus to D-branes to mirror symmetry. We also discuss a number of applications of these results, including predictions for quantum cohomology and Gromov-Witten theory and additional physical understanding of the geometric Langlands program.
Memoirs of the American Mathematical Society | 2008
Ron Donagi; Tony Pantev
Introduction The Brauer group and the Tate-Shafarevich group Smooth genus one fibrations Surfaces Modified
arXiv: High Energy Physics - Theory | 2004
Volker Braun; Burt A. Ovrut; Tony Pantev; Rene Reinbacher
T
Advances in Theoretical and Mathematical Physics | 2006
Tony Pantev; Eric Sharpe
-duality and the SYZ conjecture Appendix A. Duality for representations of
Journal of High Energy Physics | 2003
Burt A. Ovrut; Rene Reinbacher; Tony Pantev
1
Journal of Topology | 2017
Damien Calaque; Tony Pantev; Bertrand Toën; Michel Vaquié; Gabriele Vezzosi
-motives, by Dmitry Arinkin Bibliography.