Fortuity in the D1-D5 system
6 affiliations
- 1Beijing Institute of Mathematical Sciences and Applications
- 2Tsinghua University
- 3Yau Mathematical Sciences Center
- 4Harvard University
- 5Texas A&M University
- 6University of Southern California
Abstract
We reformulate the lifting problem in the D1-D5 CFT as a supercharge cohomology problem, and enumerate BPS states according to the fortuitous/monotone classification. Working in the deformed T^4 T 4 symmetric orbifold theory, we give precise definitions of monotone and fortuitous cohomology classes generalizing the definitions in [C.-M. Chang and Y.-H. Lin, arXiv: 2402.10129] and illustrate them in the N=1 N = 1 theory. For N=2 N = 2 , we construct the cohomology explicitly and match it to the exact BPS partition function. We further describe how to assemble BPS states at smaller N N into BPS states at larger N N , and interpret their holographic duals as black hole bound states and massive stringy excitations on smooth horizonless (e.g. Lunin-Mathur) geometries.
Related
BibTeX
@article{chang2026fortuity,
title = {{Fortuity in the D1-D5 system}},
author = {Chi-Ming Chang and Ying‐Hsuan Lin and Haoyu Zhang},
journal = {SciPost Physics},
year = {2026},
month = oct,
doi = {10.21468/scipostphys.21.4.096},
url = {https://scipost.org/10.21468/SciPostPhys.21.4.096},
note = {CC BY 4.0},
}
RIS
TY - JOUR
TI - Fortuity in the D1-D5 system
AU - Chi-Ming Chang
AU - Ying‐Hsuan Lin
AU - Haoyu Zhang
PY - 2026
DA - 2026/10/19
JO - SciPost Physics
DO - 10.21468/scipostphys.21.4.096
UR - https://scipost.org/10.21468/SciPostPhys.21.4.096
AB - We reformulate the lifting problem in the D1-D5 CFT as a supercharge cohomology problem, and enumerate BPS states according to the fortuitous/monotone classification. Working in the deformed T^4 T 4 symmetric orbifold theory, we give precise definitions of monotone and fortuitous cohomology classes generalizing the definitions in [C.-M. Chang and Y.-H. Lin, arXiv: 2402.10129] and illustrate them in the N=1 N = 1 theory. For N=2 N = 2 , we construct the cohomology explicitly and match it to the exact BPS partition function. We further describe how to assemble BPS states at smaller N N into BPS states at larger N N , and interpret their holographic duals as black hole bound states and massive stringy excitations on smooth horizonless (e.g. Lunin-Mathur) geometries.
SN - 2542-4653
ER -