Gauge group topology of 8D Chaudhuri-Hockney-Lykken vacua
Abstract
Compactifications of the Chaudhuri-Hockney-Lykken (CHL) string to eight dimensions can be characterized by embeddings of root lattices into the rank 12 momentum lattice ΛM, the so-called Mikhailov lattice. Based on these data, we devise a method to determine the global gauge group structure including all U(1) factors. The key observation is that, while the physical states correspond to vectors in the momentum lattice, the gauge group topology is encoded in its dual. Interpreting a nontrivial π1(G) ≡ $$\mathscr{L}$$ for the non-Abelian gauge group G as having gauged a $$\mathscr{L}$$ 1-form symmetry, we also prove that all CHL gauge groups are free of a certain anomaly [1] that would obstruct this gauging. We verify this by explicitly computing $$\mathscr{L}$$ for all 8D CHL vacua with rank(G) = 10. Since our method applies also to T2 compactifications of heterotic strings, we further establish a map that determines any CHL gauge group topology from that of a “parent” heterotic model.
- Authors:
- Publication Date:
- Research Org.:
- Univ. of Pennsylvania, Philadelphia, PA (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC); Simons Foundation Collaboration; Slovenian Research Agency; Fay R. and Eugene L. Langberg Endowed Chair
- OSTI Identifier:
- 1825347
- Alternate Identifier(s):
- OSTI ID: 1979928
- Grant/Contract Number:
- SC013528Y; SC0013528; 724069; P1-0306
- Resource Type:
- Published Article
- Journal Name:
- Physical Review D
- Additional Journal Information:
- Journal Name: Physical Review D Journal Volume: 104 Journal Issue: 8; Journal ID: ISSN 2470-0010
- Publisher:
- American Physical Society
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 79 ASTRONOMY AND ASTROPHYSICS; 71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; compactification; string dualities; strings and branes; discrete symmetries; symmetries; gauge symmetries
Citation Formats
Cvetič, Mirjam, Dierigl, Markus, Lin, Ling, and Zhang, Hao Y. Gauge group topology of 8D Chaudhuri-Hockney-Lykken vacua. United States: N. p., 2021.
Web. doi:10.1103/PhysRevD.104.086018.
Cvetič, Mirjam, Dierigl, Markus, Lin, Ling, & Zhang, Hao Y. Gauge group topology of 8D Chaudhuri-Hockney-Lykken vacua. United States. https://doi.org/10.1103/PhysRevD.104.086018
Cvetič, Mirjam, Dierigl, Markus, Lin, Ling, and Zhang, Hao Y. Tue .
"Gauge group topology of 8D Chaudhuri-Hockney-Lykken vacua". United States. https://doi.org/10.1103/PhysRevD.104.086018.
@article{osti_1825347,
title = {Gauge group topology of 8D Chaudhuri-Hockney-Lykken vacua},
author = {Cvetič, Mirjam and Dierigl, Markus and Lin, Ling and Zhang, Hao Y.},
abstractNote = {Compactifications of the Chaudhuri-Hockney-Lykken (CHL) string to eight dimensions can be characterized by embeddings of root lattices into the rank 12 momentum lattice ΛM, the so-called Mikhailov lattice. Based on these data, we devise a method to determine the global gauge group structure including all U(1) factors. The key observation is that, while the physical states correspond to vectors in the momentum lattice, the gauge group topology is encoded in its dual. Interpreting a nontrivial π1(G) ≡ $\mathscr{L}$ for the non-Abelian gauge group G as having gauged a $\mathscr{L}$ 1-form symmetry, we also prove that all CHL gauge groups are free of a certain anomaly [1] that would obstruct this gauging. We verify this by explicitly computing $\mathscr{L}$ for all 8D CHL vacua with rank(G) = 10. Since our method applies also to T2 compactifications of heterotic strings, we further establish a map that determines any CHL gauge group topology from that of a “parent” heterotic model.},
doi = {10.1103/PhysRevD.104.086018},
journal = {Physical Review D},
number = 8,
volume = 104,
place = {United States},
year = {2021},
month = {10}
}
https://doi.org/10.1103/PhysRevD.104.086018
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