Wavefunction-related Quantum Transport in Graphene
The state of a microscopic particle in quantum mechanics can be represented by a wavefunction, and the square of its amplitude represents the probability of finding a particle at that location.
For open quantum systems, the probability density of particles present in a small region can be calculated by the wave function to obtain the local density of states (LDOS) of particles.
As an important physical quantity describing the behavior of electrons in graphene, the wavefunction has significant implications for understanding the differences between relativistic
Dirac fermions in graphene and the behavior of two-dimensional electron gases described by the Schrödinger equation in traditional systems.
The focus of this research project is primarily twofold: firstly, the detection of LDOS in graphene, and secondly, the impact of LDOS on the magnetic transport of graphene quantum dots.
Related papers: Phys. Rev. B 107, 085420 (2023); Phys. Rev. B 101, 085404 (2020)
Many-body spectral statistics of graphene billiards
Most studies in the field of quantum chaos are focused on single-particle non-relativistic systems, making the investigation of the relationship between many-body interactions,
relativistic quantum mechanics, and classical dynamics highly valuable. Therefore, we will study the behavior of wavefunctions and the corresponding energy spectra in graphene
billiards considering many-body interactions in the mean-field approximation.
Related papers: Phys. Rev. Research 5, 013050 (2023)