2015
DOI: 10.1103/physreva.92.062318
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Solving strongly correlated electron models on a quantum computer

Abstract: One of the main applications of future quantum computers will be the simulation of quantum models. While the evolution of a quantum state under a Hamiltonian is straightforward (if sometimes expensive), using quantum computers to determine the ground state phase diagram of a quantum model and the properties of its phases is more involved. Using the Hubbard model as a prototypical example, we here show all the steps necessary to determine its phase diagram and ground state properties on a quantum computer. In p… Show more

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Cited by 290 publications
(335 citation statements)
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“…Transition from Mott insulator state to superfluidity of atoms [78] in an optical lattice coupled to a vibrating mirror has been analyzed, as an example of a strongly interacting quantum system subject to the optomechanical interaction [79]. Recently, a comprehensive strategy for using quantum computers to solve models of strongly correlated electrons, using the Hubbard model as a prototypical example has been reported [80]. More recently, interferometric phase detection controlled by Fano resonances and manipulation of slow light propagation have been reported in the x-ray regime [25,81].…”
Section: Introductionmentioning
confidence: 99%
“…Transition from Mott insulator state to superfluidity of atoms [78] in an optical lattice coupled to a vibrating mirror has been analyzed, as an example of a strongly interacting quantum system subject to the optomechanical interaction [79]. Recently, a comprehensive strategy for using quantum computers to solve models of strongly correlated electrons, using the Hubbard model as a prototypical example has been reported [80]. More recently, interferometric phase detection controlled by Fano resonances and manipulation of slow light propagation have been reported in the x-ray regime [25,81].…”
Section: Introductionmentioning
confidence: 99%
“…Because of the constraint of unitary evolution on a quantum computer, we can measure the Green's function only in real time (or real frequencies [18]). For t ≥ 0, the particle and hole Green's functions in real time are defined as…”
Section: Quantum Algorithm For the Impurity Solvermentioning
confidence: 99%
“…Possible choices for the initial Hamiltonian could be either the atomic limit of turning off all hopping terms, such that the ground state becomes a simple product state of occupied and unoccupied spin orbitals, or turning off interactions, such that the initial state is a Slater determinant that can be efficiently prepared using techniques discussed in Ref. [18]. At the end of the adiabatic process, QPE can be used to measure the energy of the state and collapse the wave function into an eigenstate jΨi of the Hamiltonian.…”
Section: Quantum Algorithm For the Impurity Solvermentioning
confidence: 99%
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