A digital quantum simulation of the Agassi model from nuclear physics is proposed and analyzed. The proposal is worked out for the case with four different sites. Numerical simulations and analytical estimations are presented to illustrate the feasibility of this proposal with current technology. The proposed approach is fully scalable to a larger number of sites. The use of a quantum correlation function as a probe to explore the quantum phases by quantum simulating the time dynamics, with no need of computing the ground state, is also studied. Evidence is given showing that the amplitude of the time dynamics of a correlation function in this quantum simulation is linked to the different quantum phases of the system. This approach establishes an avenue for the digital quantum simulation of useful models in nuclear physics.
A digital quantum simulation of the Agassi model from nuclear physics is proposed and analyzed. The proposal is worked out for the case with four different sites. Numerical simulations and analytical estimations are presented to illustrate the feasibility of this proposal with current technology. The proposed approach is fully scalable to a larger number of sites. The use of a quantum correlation function as a probe to explore the quantum phases by quantum simulating the time dynamics, with no need of computing the ground state, is also studied. Evidence is given showing that the amplitude of the time dynamics of a correlation function in this quantum simulation is linked to the different quantum phases of the system. This approach establishes an avenue for the digital quantum simulation of useful models in nuclear physics.
A digital quantum simulation for the extended Agassi model is proposed using a quantum platform with eight trapped ions. The extended Agassi model is an analytically solvable model including both short range pairing and long range monopole-monopole interactions with applications in nuclear physics and in other many-body systems. In addition, it owns a rich phase diagram with different phases and the corresponding phase transition surfaces. The aim of this work is twofold: on one hand, to propose a quantum simulation of the model at the present limits of the trapped ions facilities and, on the other hand, to show how to use a machine learning algorithm on top of the quantum simulation to accurately determine the phase of the system. Concerning the quantum simulation, this proposal is scalable with polynomial resources to larger Agassi systems. Digital quantum simulations of nuclear physics models assisted by machine learning may enable one to outperform the fastest classical computers in determining fundamental aspects of nuclear matter.
A central challenge in nuclear physics is understanding quantum many-body systems governed by the strong nuclear force. The inherent complexity of these systems, combined with the limitations of classical computational methods, underscores the need for new approaches to study nuclear structure and dynamics. Here, we demonstrate that a spin-based digital quantum simulator using nuclear magnetic resonance, where nuclear spins simulate interacting fermions, offers a powerful tool to address this challenge. As a first step, we experimentally simulate the Agassi model, which encapsulates the interplay between collective and single-particle behaviors in finite nuclei. By representing nucleons as both bosons (nucleon pairs) and fermions (individual unpaired nucleons), the Agassi model captures highly non-linear interactions and is particularly suited for studying nuclear phase transitions, such as those between spherical and deformed shapes. We experimentally measure the correlation function as an order parameter during the evolution of the many-body system, successfully detecting a quantum phase transition. Specifically, we observe a sharp transition between the symmetric phase and the broken symmetry phase. This work underscores the potential of quantum simulation as a transformative tool in nuclear physics, particularly for exploring complex quantum many-body systems with applications in nuclear structure and reaction dynamics.
Quantum simulation is one of the most relevant applications of quantum computation for the near future, due to its scientific impact and also because quantum simulation algorithms are typically less demanding than generalized quantum computations. Ultimately, the success of a quantum simulation depends on the amount and reliability of information one is able to extract from the results. In such a context, this work reviews the theory behind quantum simulation, with a focus on digital quantum simulation. The concepts of efficiency and reliability in quantum simulations are discussed, particularly for implementations of digital simulation algorithms in state-of-the-art quantum computers. A review of approaches for quantum characterization, verification and validation techniques (QCVV) is also presented. A digital quantum simulation of the Schrödinger equation for a single particle in 1 spatial dimension was experimentally implemented and analyzed, along with a quantum state tomography procedure for characterization of the final quantum state and evaluation of simulation reliability. From the literature, it is shown that digital quantum simulation is theoretically sound and experimentally feasible, with several applications in a wide range of physics-related fields. Nonetheless, a number of conditions arise that must be observed for a truly efficient implementation of a digital quantum simulation, from theoretical conception to experimental circuit design. The review of QCVV techniques highlights the need for characterization and validation techniques that could be efficiently implemented for current models of quantum computation, particularly in instances where classical verification is not tractable. However, there are proposals for efficient verification procedures when a set of parameters defining the final result of the simulation is known. The experimental simulation demonstrated partial success in comparison with an ideal quantum simulation. From the results it is apparent that better coherence times, better reliability and finer control are as decisive for the advancement of quantum computing power as the more-publicized number of qubits of a given device.
The calculation of dynamic response functions is expected to be an early application benefiting from rapidly developing quantum hardware resources. The ability to calculate real-time quantities of strongly correlated quantum systems is one of the most exciting applications that can easily reach beyond the capabilities of traditional classical hardware. Response functions of fermionic systems at moderate momenta and energies corresponding roughly to the Fermi energy of the system are a potential early application because the relevant operators are nearly local, and the energies can be resolved in moderately short real time, reducing the spatial resolution and gate depth required. This is particularly the case in quasielastic electron and neutrino scattering from nuclei, a topic of great interest in the nuclear and particle physics communities and directly related to experiments designed to probe neutrino properties. In this work we use current quantum hardware and error mitigation protocols to calculate response functions for a highly simplified nuclear model through calculations of a 2-point real time correlation function for a modified Fermi-Hubbard model in two dimensions with three distinguishable nucleons on four lattice sites.
Resolving quantum many-body problems represents one of the greatest challenges in physics and physical chemistry, due to the prohibitively large computational resources that would be required by using classical computers. A solution has been foreseen by directly simulating the time evolution through sequences of quantum gates applied to arrays of qubits, i.e. by implementing a digital quantum simulator. Superconducting circuits and resonators are emerging as an extremely promising platform for quantum computation architectures, but a digital quantum simulator proposal that is straightforwardly scalable, universal, and realizable with state-of-the-art technology is presently lacking. Here we propose a viable scheme to implement a universal quantum simulator with hybrid spin-photon qubits in an array of superconducting resonators, which is intrinsically scalable and allows for local control. As representative examples we consider the transverse-field Ising model, a spin-1 Hamiltonian, and the two-dimensional Hubbard model and we numerically simulate the scheme by including the main sources of decoherence.
Here we present a superadiabatic scheme on a quantum computer to quickly prepare the ground state of the Agassi model, a typical quadrupole plus pairing model with broad applications in nuclear physics as well as many-body systems. By virtue of the Floquet-engineering counterdiabatic driving, this method can accelerate the conventional quantum adiabatic driving without extra control fields. Compared to the adiabatic protocol, the resulting scheme allows for a drastic increase in the final fidelity within a short evolution time, which can effectively inhibit the decoherence effects in quantum simulators. Numerical simulations demonstrate the feasibility of this proposal for fast generating the ground state of Agassi model with different sites. This research opens an avenue for future quantum simulations, and provides a useful method to address currently unanswered questions in nuclear physics using intermediate-scale quantum coprocessors.