Matter in transition

We explore a novel type of transition in certain 6D and 4D quantum field theories, in which the matter content of the theory changes while the gauge group and other parts of the spectrum remain invariant. Such transitions can occur, for example, for SU(6) and SU(7) gauge groups, where matter fields...

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Bibliographic Details
Main Authors: Anderson, Lara B. (Author), Gray, James (Author), Raghuram, Nikhil (Contributor), Taylor, Washington (Contributor)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: Springer Berlin Heidelberg, 2016-06-23T19:12:32Z.
Subjects:
Online Access:Get fulltext
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100 1 0 |a Anderson, Lara B.  |e author 
100 1 0 |a Massachusetts Institute of Technology. Center for Theoretical Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Raghuram, Nikhil  |e contributor 
100 1 0 |a Taylor, Washington  |e contributor 
700 1 0 |a Gray, James  |e author 
700 1 0 |a Raghuram, Nikhil  |e author 
700 1 0 |a Taylor, Washington  |e author 
245 0 0 |a Matter in transition 
260 |b Springer Berlin Heidelberg,   |c 2016-06-23T19:12:32Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/103299 
520 |a We explore a novel type of transition in certain 6D and 4D quantum field theories, in which the matter content of the theory changes while the gauge group and other parts of the spectrum remain invariant. Such transitions can occur, for example, for SU(6) and SU(7) gauge groups, where matter fields in a three-index antisymmetric representation and the fundamental representation are exchanged in the transition for matter in the two-index antisymmetric representation. These matter transitions are realized by passing through superconformal theories at the transition point. We explore these transitions in dual F-theory and heterotic descriptions, where a number of novel features arise. For example, in the heterotic description the relevant 6D SU(7) theories are described by bundles on K3 surfaces where the geometry of the K3 is constrained in addition to the bundle structure. On the F-theory side, non-standard representations such as the three-index antisymmetric representation of SU(N) require Weierstrass models that cannot be realized from the standard SU(N) Tate form. We also briefly describe some other situations, with groups such as Sp(3), SO(12), and SU(3), where analogous matter transitions can occur between different representations. For SU(3), in particular, we find a matter transition between adjoint matter and matter in the symmetric representation, giving an explicit Weierstrass model for the F-theory description of the symmetric representation that complements another recent analogous construction. 
520 |a United States. Department of Energy (contract #DE-SC00012567) 
520 |a National Science Foundation (U.S.) (Grant No. PHY-1066293) 
546 |a en 
655 7 |a Article 
773 |t Journal of High Energy Physics