Minimum Trotterization Formulas for a Time-Dependent Hamiltonian

When a time propagator e δ t A for duration δ t consists of two noncommuting parts A = X + Y , Trotterization approximately decomposes the propagator into a product of exponentials of X and Y . Various Trotterization formulas have been utilized in quantum and classical computers, but much less is kn...

Full description

Saved in:
Bibliographic Details
Published inQuantum (Vienna, Austria) Vol. 7; p. 1168
Main Authors Ikeda, Tatsuhiko N., Abrar, Asir, Chuang, Isaac L., Sugiura, Sho
Format Journal Article
LanguageEnglish
Published Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften 06.11.2023
Online AccessGet full text

Cover

Loading…
More Information
Summary:When a time propagator e δ t A for duration δ t consists of two noncommuting parts A = X + Y , Trotterization approximately decomposes the propagator into a product of exponentials of X and Y . Various Trotterization formulas have been utilized in quantum and classical computers, but much less is known for the Trotterization with the time-dependent generator A ( t ) . Here, for A ( t ) given by the sum of two operators X and Y with time-dependent coefficients A ( t ) = x ( t ) X + y ( t ) Y , we develop a systematic approach to derive high-order Trotterization formulas with minimum possible exponentials. In particular, we obtain fourth-order and sixth-order Trotterization formulas involving seven and fifteen exponentials, respectively, which are no more than those for time-independent generators. We also construct another fourth-order formula consisting of nine exponentials having a smaller error coefficient. Finally, we numerically benchmark the fourth-order formulas in a Hamiltonian simulation for a quantum Ising chain, showing that the 9-exponential formula accompanies smaller errors per local quantum gate than the well-known Suzuki formula.
ISSN:2521-327X
2521-327X
DOI:10.22331/q-2023-11-06-1168