Simulating scalar field theories on quantum computers with limited resources

TL;DR

This paper introduces a quantum algorithm for simulating $$^4$ scalar field theories on qubit computers, enabling efficient state preparation in both symmetric and broken phases with resource scaling proportional to lattice size.

Contribution

It presents a novel quantum algorithm combining variational and adiabatic methods for efficient $$^4$ state preparation, including techniques to handle phase transition degeneracies.

Findings

Efficient $$^4$ state preparation over a range of parameters.

Optimization of adiabatic evolution reduces time complexity.

Method to address broken-symmetry degeneracy using external fields.

Abstract

We present a quantum algorithm for implementing $\phi^4$ lattice scalar field theory on qubit computers. The field is represented in the discretized field amplitude basis. The number of qubits and elementary gates required by the implementation of the evolution operator is proportional to the lattice size. The algorithm allows efficient $\phi^4$ state preparation for a large range of input parameters in both the normal and broken-symmetry phases. The states are prepared using a combination of variational and adiabatic evolution methods. First, the ground state of a local Hamiltonian, which includes the $\phi^4$ self-interaction, is prepared using short variational circuits. Next, this state is evolved by switching on the coupling between the lattice sites adiabatically. The parameters defining the local Hamiltonian are adjustable and constitute the input of our algorithm. We present a method to optimize these parameters in order to reduce the adiabatic time required for state preparation. For preparing broken-symmetry states, the adiabatic evolution problems caused by crossing the phase transition critical line and by the degeneracy of the broken-symmetry ground state can be addressed using an auxiliary external field which gradually turns off during the adiabatic process. We show that the time dependence of the external field during the adiabatic evolution is important for addressing the broken-symmetry ground state degeneracy. The adiabatic time dependence on the inverse error tolerance can be reduced from quadratic to linear by using a field strength that decreases exponentially in time relative to one that decreases linearly.