2018
DOI: 10.1103/physrevd.97.036004
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Quantum computation of scattering amplitudes in scalar quantum electrodynamics

Abstract: We present a quantum algorithm for the calculation of scattering amplitudes of massive charged scalar particles in scalar quantum electrodynamics. Our algorithm is based on continuous-variable quantum computing architecture resulting in exponential speedup over classical methods. We derive a simple form of the Hamiltonian including interactions, and a straightforward implementation of the constraint due to gauge invariance.

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Cited by 16 publications
(14 citation statements)
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“…1. The scalar field digitization techniques of Jordan-Preskill-Lee [6-9, 34, 36, 50], a momentum-space mode expansion [42] and a harmonic oscillator basis are relevant for NISQ-era hardware implementations. The number of qubits per site needed to reduce the digitization and discretization systematic errors below near-term hardware noise levels are n Q ∼ 4 for potentials with m 2 > 0 and n Q > ∼ 6 for potentials with m 2 < 0.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…1. The scalar field digitization techniques of Jordan-Preskill-Lee [6-9, 34, 36, 50], a momentum-space mode expansion [42] and a harmonic oscillator basis are relevant for NISQ-era hardware implementations. The number of qubits per site needed to reduce the digitization and discretization systematic errors below near-term hardware noise levels are n Q ∼ 4 for potentials with m 2 > 0 and n Q > ∼ 6 for potentials with m 2 < 0.…”
Section: Discussionmentioning
confidence: 99%
“…In numerical computations of non-perturbative field theories, such as LQCD, the system is typically defined with regard to fields in position space, while components of calculations involve determining eigenvectors of the Dirac operator in the presence of a particular configuration of gauge fields. In the study of systems with few sites in each spatial direction, it is likely the case that calculating with the momentum-space modes is efficient [42]. First implementation of this quantization procedure on quantum devices has been completed by an ORNL team [87].…”
Section: +1 Dimensional λφ 4 Scalar Field Theorymentioning
confidence: 99%
“…The choice of scalar field is inspired by its simplicity, ubiquity, unique status of having a thoroughly examined qubit digitization [32][33][34][35][36], and having been proven to be BQP (bounded-error quantum polynomial time) complete [37]. The latter of these motivating factors indicates that any efficient quantum calculation, of fields or otherwise, can be transformed with polynomial resources to a scattering process of the interacting scalar field through the manipulation of classical external sources.…”
Section: Introductionmentioning
confidence: 99%
“…We first evolve the wavepacket with the free Hamiltonian H 0 , which is diagonal in the momentum representation. This is followed by a squeezing operation (analogous to that performed in quantum optics [90,91]), a quantum Fourier transformation [92] from momentum space to position space, and lastly, an implementation of the interaction term in position space, where it is local.…”
Section: Quantum Algorithmmentioning
confidence: 99%