Spin Dynamics in Open Quantum Systems: A DLvN-TDDFT Approach
Kashinath T Chavan1, Oded Hod2, Juan E Peralta1
1Department of Physics, Central Michigan University, Mount Pleasant, Michigan 48859, United States.
Journal of Chemical Theory and Computation
|May 26, 2026
Summary
We developed a new computational method, driven Liouville-von Neumann (DLvN-TDDFT), to simulate electron spin transport in quantum systems. This approach reveals complex spin dynamics in magnetic nanoribbons, advancing spintronics research.
Area of Science:
- Quantum mechanics
- Condensed matter physics
- Materials science
Background:
- Modeling electron spin transport in open quantum systems is crucial for spintronics.
- Existing methods may not fully capture dynamical spin phenomena.
Purpose of the Study:
- To introduce and validate a novel computational framework for simulating spin-polarized electron transport.
- To explore spin dynamics in low-dimensional magnetic materials.
Main Methods:
- Developed a spin-uncompensated driven Liouville-von Neumann methodology.
- Integrated this into the time-dependent density functional theory (DLvN-TDDFT) framework.
- Validated the approach using benchmark simulations of molecular junctions.
Main Results:
- Applied the DLvN-TDDFT to a magnetic zigzag graphene nanoribbon junction.
- Observed rich spin-resolved current dynamics under external electric fields.
- Demonstrated the framework's capability to model complex spin behavior.
Conclusions:
- The DLvN-TDDFT framework is a powerful tool for studying dynamical spintronic phenomena.
- This methodology shows promise for investigating spin transport in low-dimensional open quantum systems.
Related Concept Videos
Spin–Spin Coupling Constant: Overview
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Fermi Level Dynamics
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Spin–Spin Coupling: One-Bond Coupling
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
The Van der Waals Equation
The ideal gas law is based on two simplifying assumptions: first, that there are no intermolecular attractions between gas molecules, and second, that the volume occupied by the molecules themselves is negligible compared with the volume of the container. However, these assumptions don't hold up under all conditions - specifically, at high pressures and low temperatures, as gas tends to deviate from ideal gas behavior.The van der Waals equation is an enhanced version of the ideal gas law,...
Van der Waals Equation
The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
Molecular Orbital Theory I
Overview of Molecular Orbital Theory


