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1.
J Chem Theory Comput ; 2024 Jul 01.
Article in English | MEDLINE | ID: mdl-38950444

ABSTRACT

We consider the question of how correlated the system hardness is between classical algorithms of electronic structure theory in ground state estimation and quantum algorithms. To define the system hardness for classical algorithms, we employ empirical criterion based on the deviation of electronic energies produced by coupled cluster and configuration interaction methods from the exact ones along multiple bonds dissociation in a set of molecular systems. For quantum algorithms, we have selected the Variational Quantum Eigensolver (VQE) and Quantum Phase Estimation (QPE) methods. As characteristics of the system hardness for quantum methods, we analyzed circuit depths for the state preparation, the number of quantum measurements needed for the energy expectation value, and various cost characteristics for the Hamiltonian encodings via Trotter approximation and linear combination of unitaries (LCU). Our results show that the quantum resource requirements are mostly unaffected by classical hardness, with the only exception being the state preparation part, which contributes to both VQE and QPE algorithm costs. However, there are clear indications that constructing the initial state with a significant overlap with the true ground state is easier than obtaining the state with an energy expectation value within chemical precision. These results support optimism regarding the identification of a molecular system where a quantum algorithm excels over its classical counterpart, as quantum methods can maintain efficiency in classically challenging systems.

2.
J Chem Theory Comput ; 19(22): 8201-8209, 2023 Nov 28.
Article in English | MEDLINE | ID: mdl-37939198

ABSTRACT

Computational cost of energy estimation for molecular electronic Hamiltonians via quantum phase estimation (QPE) grows with the difference between the largest and smallest eigenvalues of the Hamiltonian. In this work, we propose a preprocessing procedure that reduces the norm of the Hamiltonian without changing its eigenspectrum for the target states of a particular symmetry. The new procedure, block-invariant symmetry shift (BLISS), builds an operator T̂ such that the cost of implementing H^-T^ is reduced compared to that of H, yet H^-T^ acts on the subspaces of interest the same way as H does. BLISS performance is demonstrated for a linear combination of unitaries (LCU)-based QPE approaches on a set of small molecules. Using the number of electrons as the symmetry specifying the target set of states, BLISS provided a factor of 2 reduction of 1-norm for several LCU decompositions compared to their unshifted versions.

3.
J Chem Phys ; 154(12): 124126, 2021 Mar 28.
Article in English | MEDLINE | ID: mdl-33810687

ABSTRACT

Light harvesting processes are often computationally studied from a time-dependent viewpoint, in line with ultrafast coherent spectroscopy experiments. Yet, natural processes take place in the presence of incoherent light, which induces a stationary state. Such stationary states can be described using the eigenbasis of the molecular Hamiltonian, but for realistic systems, a full diagonalization is prohibitively expensive. We propose three efficient computational approaches to obtain the stationary state that circumvents system Hamiltonian diagonalization. The connection between the incoherent perturbations, decoherence, and Kraus operators is established.

4.
J Chem Phys ; 149(21): 214101, 2018 Dec 07.
Article in English | MEDLINE | ID: mdl-30525721

ABSTRACT

Due to a continuum of electronic states present in periodic systems, the description of molecular dynamics on surfaces poses a serious computational challenge. One of the most used families of approaches in these settings are friction theories, which up to a random fluctuating force term are based on the Ehrenfest approach. Yet, a mean-field treatment of electronic degrees of freedom in the Ehrenfest method makes this approach inaccurate in some cases. Our aim is to clarify when Ehrenfest breaks down for molecular dynamics on surfaces. Answering this question provides limits of applicability for more approximate friction theories derived from Ehrenfest. We assess the Ehrenfest method on one-dimensional, numerically exactly solvable models with a large but finite number of electronic states. Using the Landau-Zener formula and the Massey parameter, an expression that determines when Ehrenfest breaks down is deduced.

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