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. Author manuscript; available in PMC: 2022 Dec 13.
Published in final edited form as: Nature. 2021 Nov 17;599(7885):393–398. doi: 10.1038/s41586-021-03988-0

Extended Data Figure 7.

Extended Data Figure 7.

DEER Difference signal for R = {1,2,3} (light to dark), compared with the imbalance 𝓘(t) for the same parameters. Data are offset for clarity but otherwise share the same axes. 𝓘 is taken from the same dataset as the R = 1 spin-echo data, with the probe spin excluded from the imbalance calculation. After tJ0 ≈ 2, the imbalance is essentially constant at the low but finite steady-state value corresponding to this gradient strength. However, correlation dynamics are still progressing- in particular, correlations as measured by the difference signal only begin to develop for R = 2 after this point. This is similar to the disordered MBL state, in which slow entanglement dynamics continue after the locally conserved populations have reached a steady state [10, 11, 30].