scholarly journals Lieb–Robinson bounds and growth of correlations in Bose mixtures

2021 ◽  
pp. 1-27
Author(s):  
Alessandro Michelangeli ◽  
Nicola Santamaria

For a mixture of interacting Bose gases initially prepared in a regime of condensation (uncorrelation), it is proved that in the course of the time evolution observables of disjoint sets of particles of each species have correlation functions that remain asymptotically small in the total number of particles and display a controlled growth in time. This is obtained by means of ad hoc estimates of Lieb–Robinson type on the propagation of the interaction, established here for the multi-component Bose mixture.

We consider simulations of dipolar systems under periodic boundary conditions in which a large sphere consisting of periodic replications of a central simulation cell is surrounded by a continuum of dielectric constant ε'. We develop a perturbation theory expressing correlation functions with ε" in terms of correlation functions with ε' exactly to order N* 1 , N being the number of particles in the sample. In the thermodynamic limit, the correlation functions and internal energy density are independent of e The Kirkwood g -factor is strongly dependent on ε ' but in such a way as to make the dielectric constant independent of ε'. The dependence upon ε' of h A {r) at large r, described in paper I, is explained in terms of the perturbation series.


2020 ◽  
Vol 124 (11) ◽  
Author(s):  
Álvaro M. Alhambra ◽  
Jonathon Riddell ◽  
Luis Pedro García-Pintos

2020 ◽  
Vol 8 (2) ◽  
Author(s):  
Claudius Hubig ◽  
Annabelle Bohrdt ◽  
Michael Knap ◽  
Fabian Grusdt ◽  
Ignacio Cirac

Infinite projected entangled pair states (iPEPS) provide a convenient variational description of infinite, translationally-invariant two-dimensional quantum states. However, the simulation of local excitations is not directly possible due to the translationally-invariant ansatz. Furthermore, as iPEPS are either identical or orthogonal, expectation values between different states as required during the evaluation of non-equal-time correlators are ill-defined. Here, we show that by introducing auxiliary states on each site, it becomes possible to simulate both local excitations and evaluate non-equal-time correlators in an iPEPS setting under real-time evolution. We showcase the method by simulating the t-Jt−J model after a single hole has been placed in the half-filled antiferromagnetic background and evaluating both return probabilities and spin correlation functions, as accessible in quantum gas microscopes.


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