Fortuity and fragility in supersymmetric SYK
hep-th, cond-mat.str-el
Submitted: 2026-08-12
Updated: 2026-10-16
Comments: 44 pages, 15 figures, 2 tables. v2: minor changes
License: http://creativecommons.org/licenses/by/4.0/
The gist: In the N=2 supersymmetric SYK model with N fermions, every BPS state is fortuitous: at fixed charge, it exists only over a finite range of N.
Terminology
Abstract
In the N=2 supersymmetric SYK model with N fermions, every BPS state is fortuitous: at fixed charge, it exists only over a finite range of N. Allowing the charge to increase, we show that BPS classes may instead be uplifted along lattice walks inside the fortuity window, potentially to arbitrarily large N. However, there is no canonical uplift. We therefore introduce a decoder D whose spectrum quantifies exact uplift and its metric cost. We call the failure or increasing cost of uplifting harmonic representatives metric fragility. Chen's single-matrix model and the protected tower of the two-flavor SYK model realize bare and genuinely dressed mechanisms of perfect uplift, respectively. In the generic one-flavor model, exact uplift eventually fails. The Lin-Maldacena-Rozenberg-Shan-type operator D D exhibits level statistics consistent with the Gaussian unitary ensemble. Its eigenvalues quantify the metric continuity of BPS states across system size, while their correlations probe chaos within the BPS sector. Metric fragility and BPS chaos are thus encoded in complementary observables of the same operator, distinguishing chaotic BPS sectors from exactly solvable towers.
Related papers
- One generation of the Standard Model as a quantum error-correcting code
- S-duality, boundary states, and higher-form symmetries on ALE spaces
- Quantum simulation of traversable-wormhole-inspired quantum teleportation in a chaotic binary sparse SYK model
- Perfect Particle Transmission through Duality Defects
- Entanglement Wedge Reconstruction Beyond the Large N Limit via the Twirled Petz Map
- Horizons and Soft Quantum Information