Abstract:Aiming at evading the notorious sign problem in classical Monte-Carlo approaches to lattice quantum chromodynamics, we present an approach for quantum computing finite-temperature lattice gauge theories at non-zero density. Based on the thermal pure-quantum-state formalism of statistical mechanics when extended to gauge-theory systems, our approach [1] allows for signproblem-free quantum computations of thermal expectation values and non-equal time correlation functions. By taking a simple lattice gauge theory… Show more
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