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Springer eBooks

Time-Dependent Hamiltonians

Ladislav Šamaj

Published Mar 31, 2006• 1 citation
Publisher
DOI
10.1007/0-387-22741-5_8

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Derivative of Unitary is not always -iHU

A S Muddu

$i\dot{U} = HU$ (or $\dot{U} = -iHU$) is the equation that is said to govern the evolution of a unitary matrix $U$ given the Hamiltonian $H$ of the system. This equation is said to hold true even if the Hamiltonian is time dependent. We show iU = HU (or $\dot{U} = -iHU$) is the equation that is said to govern the evolution of a unitary matrix $U$ given the Hamiltonian $H$ of the system. This equation is said to hold true even if the Hamiltonian is time dependent. We show in this paper that $i\dot{U} = HU$ may not always hold for time dependent Hamiltonians.this paper that $i\dot{U} = HU$ may not always hold for time dependent Hamiltonians.

•Dec 23, 2020•0 citations
Simulating Hamiltonian dynamics is one of the most fundamental and significant tasks for characterising quantum materials. Recently, a series of quantum algorithms employing block-encoding of Hamiltonians have succeeded in providing efficient simulation of time-evolution operators on quantum computers. While time-independent Hamiltonians can be simulated by the quantum eigenvalue transformation (QET) or quantum singularvalue transformation with the optimal query complexity in time ttt and desirable accuracy ε\varepsilonε, generic time-dependent Hamiltonians face at larger query complexity and more complicated oracles due to the difficulty of handling time-dependency. In this paper, we establish a QET-based approach for simulating time-dependent Hamiltonians with multiple time-periodicity. Such time-dependent Hamiltonians involve a variety of nonequilibrium systems such as time-periodic systems (Floquet systems) and time-quasiperiodic systems. Overcoming the difficulty of time-dependency, our protocol can simulate the dynamics under multi-periodic time-dependent Hamiltonians with optimal/nearly-optimal query complexity both in time ttt and desirable accuracy ε\varepsilonε, and simple oracles as well as the optimal algorithm for time-independent cases.
Simulating Hamiltonian dynamics is one of the most fundamental and significant tasks for characterizing quantum materials. Recently, a series of quantum algorithms employing block encoding of Hamiltonians have succeeded in providing efficient simulation of time-evolution operators on quantum computers. While time-independent Hamiltonians can be simulated by the quantum eigenvalue transformation (QET) or quantum singular value transformation with the optimal query complexity in time ttt and desirable accuracy $\ensuremath{\varepsilon}$, generic time-dependent Hamiltonians face at larger query complexity and more complicated oracles due to the difficulty of handling time-dependency. In this paper, we establish a QET-based approach for simulating time-dependent Hamiltonians with multiple time periodicity. Such time-dependent Hamiltonians involve a variety of nonequilibrium systems such as time-periodic systems (Floquet systems) and time-quasiperiodic systems. Overcoming the difficulty of time dependency, our protocol can simulate the dynamics under multiperiodic time-dependent Hamiltonians with optimal and nearly optimal query complexity both in time ttt and desirable accuracy $\ensuremath{\varepsilon}$, and simple oracles as well as the optimal algorithm for time-independent cases.
iU˙=HUi\dot{U} = HUiU˙=HU (or U˙=−iHU\dot{U} = -iHUU˙=−iHU) is the equation that is said to govern the evolution of a unitary matrix UUU given the Hamiltonian HHH of the system. This equation is said to hold true even if the Hamiltonian is time dependent. We show iU = HU (or U˙=−iHU\dot{U} = -iHUU˙=−iHU) is the equation that is said to govern the evolution of a unitary matrix UUU given the Hamiltonian HHH of the system. This equation is said to hold true even if the Hamiltonian is time dependent. We show in this paper that iU˙=HUi\dot{U} = HUiU˙=HU may not always hold for time dependent Hamiltonians.this paper that iU˙=HUi\dot{U} = HUiU˙=HU may not always hold for time dependent Hamiltonians.