📝 SummarXiv

Abstract

The accurate computation of low-energy spectra of strongly correlated quantum many-body systems, typically accessed via Greens-functions, is a long-standing problem posing enormous challenges to numerical methods. When the spectral decomposition is obtained from Fourier transforming a time series, the Nyquist-Shannon theorem limits the frequency resolution $\Delta\omega$ according to the numerically accessible time domain size $T$ via $\Delta\omega = 2/T$. In tensor network methods, increasing the domain size is exponentially hard due to the ubiquitous spread of correlations, limiting the frequency resolution and thereby restricting this ansatz class mostly to one-dimensional systems with small quasi-particle velocities. Here, we show how this fundamental limitation can be overcome using complex-time Krylov spaces. At the example of the critical $S-1/2$ Heisenberg model and light bipolarons in the two-dimensional Su-Schrieffer-Heeger model, we demonstrate the enormous improvements in accuracy, which can be achieved using this method.