Abstract

Obtaining accurate properties of many-body interacting quantum matter is a long-standing challenge in theoretical physics and chemistry, rooting into the complexity of the many-body wave-function. Classical representations of many-body states constitute a key tool for both analytical and numerical approaches to interacting quantum problems. Here, we introduce a technique to construct classical representations of many-body quantum systems based on artificial neural networks. Our constructions are based on the deep Boltzmann machine architecture, in which two layers of hidden neurons mediate quantum correlations. The approach reproduces the exact imaginary-time evolution for many-body lattice Hamiltonians, is completely deterministic, and yields networks with a polynomially-scaling number of neurons. We provide examples where physical properties of spin Hamiltonians can be efficiently obtained. Also, we show how systematic improvements upon existing restricted Boltzmann machines ansatze can be obtained. Our method is an alternative to the standard path integral and opens new routes in representing quantum many-body states.

Highlights

  • Obtaining accurate properties of many-body interacting quantum matter is a long-standing challenge in theoretical physics and chemistry, rooting into the complexity of the many-body wave-function

  • A tremendous amount of successful developments in quantum physics builds upon the mapping between many-body quantum systems and effective classical theories

  • Perturbative approaches based on the graphical resummation of classes of diagrams are at the heart of many-body analytical approaches in various fields of research, ranging from particle to condensedmatter physics[5]

Read more

Summary

Introduction

Obtaining accurate properties of many-body interacting quantum matter is a long-standing challenge in theoretical physics and chemistry, rooting into the complexity of the many-body wave-function. In one dimensHJiÀoσ1nxl1⁄4,σwxmPeþohdld;σemdylciσoHymmblþpmoondσsezl σtazmhnÁed, HwahHmer2iel1⁄4toσnPdiaennehlv;oemintnietHoPblamooundldid, manwatdirtihceevse.nHBblbemoconandud=sse: the bond Hamiltonian Hblmond is a building block in higher dimensional models, construction of an exact DBM representation the of the ground states bond-propagator hσz cjeaÀnδτbHeblmoandchΨieWved=bCy fiσnzdjΨinWg solutions , where for the parameters W are such that the previous equation is satisfied for all the possible hσzj, and for an arbitrary finite normalization constant C.

Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.