Open refraction-ray opened 5 years ago
Random circuit with some conservations
Summary: See Fig3 in PhysRevX.8.031057 for operator spreading in comparison to unconstrained random circuits.
Comments: It is somehow like three steps from random circuit dynamics to fracton circuits. 1 random circuits; 2 random circuits with conserved U(1) charge; 3 random circuits with conserved U(1) charge and dipole of charges. The third step is nothing else but fracton circuits. For the third step, see the reference in https://github.com/quclub/Paper-reading/issues/20#issue-462414652. Accordingly, the system dynamics goes from thermal to somewhat "MBL" or with quantum scars noticed recently in such fracton circuits as in https://github.com/quclub/Paper-reading/issues/8#issue-461424346 and https://github.com/quclub/Paper-reading/issues/2#issue-461350320
Relevant paper
Summary: The two papers both talked about the diffusive of the front of operators in random circuits (Heisenberg picture). The front of OTOC shows diffusive behavior beyond light cone which could described by hydrodynamics. eg. Fig 2 in PhysRevX.8.021013. Random circuit setup is two in two out gates with spin half chain.
Important tools: Operator expansion on operator string basis, and $$\rho_r$$ characterizing the front of operator. Understanding and picture, see page 5&6 eq 12&13 in PhysRevX.8.031057.