How a complexity measure reveals long-lived, non‑propagating modes in a heavy BMN matrix model
Researchers studied the BMN matrix model — a quantum mechanical system of matrices often used as a toy laboratory for questions about quantum gravity — using a tool called Krylov complexity. Krylov complexity tracks how a quantum state or operator spreads when you repeatedly apply the system’s Hamiltonian (the energy operator). The team focused on the large mass deformation limit, meaning a parameter µ in the model is taken to be large. This limit simplifies some calculations and highlights how the model behaves when heavy modes dominate.
Concretely, the authors computed several diagnostic quantities for both the spread of states and the growth of operators. These include moments and return amplitudes, the Lanczos coefficients that define the Krylov basis, and orthogonal polynomials that arise from the Gram–Schmidt construction of that basis. They propose a general scaling for the moments at large mass: the n-th moment scales like Mn = α(n) µ^n, with coefficients α(n) fixed by the model’s parameters. For the spread of states, the short-time behaviour of a standard complexity measure C(t) is quadratic, C(t) ≈ ζ µ^2 t^2, where ζ depends on the Lanczos coefficients. The authors also find that, for operator growth up to fourth order, only even moments survive — a sign that they are tracking a Hermitian operator’s time evolution.
To probe the spectrum and excitations, the team built a resolvent (an operator-valued Green’s function) by taking Laplace transforms of Krylov wavefunctions. From the resolvent they obtain a spectral function and, by integrating it, a density of states. They find a clear separation of behaviour: at high frequency (the ultraviolet, or UV), the spectral function vanishes and the system is strongly damped. Near zero frequency (the infrared, or IR) the spectral function shows divergences that signal unusual low-energy physics. Isolating the physical contribution leads to exceptionally stable collective modes with lifetimes that scale like τ ∝ 1/ω^3 (ω is frequency). Because these modes do not propagate like ordinary waves, the authors interpret them as diffusive or relaxation modes rather than ballistic excitations.