Defects in graphene give rise to zero modes that are often related to the sharp peak in the local density of states near the defect site. Here we solved all zero modes induced by a single defect in the finite-size graphene and show that their contributions to the local density of states vanish in the thermodynamic limit. Instead, lots of resonant states emerge at low energies and eventually lead to a power-law singularity in the local density of states. Our findings show that the impurity problem in graphene should be treated as a collective phenomenon rather than a single impurity state
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
We analyze the nature of the single-particle states, away from the Dirac point in the presence of lo...
[[abstract]]Defects in graphene give rise to zero modes that are often related to the sharp peak in ...
Intrinsic defects give rise to scattering processes governing the transport properties of mesoscopic...
Graphene consists of an atom-thick layer of carbon atoms arranged in a honeycomb lattice, and its lo...
We present exact analytical calculations of scanning tunneling currents in locally disordered graphe...
We study the effects of impurities on the electronic properties of graphene. The tight-binding Hamil...
We study the interplay between the edge states and a single impurity in a zigzag graphene nanoribbon...
The density of states rho(E) of graphene is investigated within the tight-binding (Huckel) approxima...
In this paper, the average density of states (ADOS) in graphene with binary alloy disorders is calcu...
We introduce a model for amorphous grain boundaries in graphene and find that stable structures can ...
It is pointed out that due to direct couplings of electronic states, point defects on graphene are s...
We address local inelastic scattering from the vibrational impurity adsorbed onto graphene and the e...
We study the behavior of the local density of states in an armchair graphene nanoribbon with a poten...
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
We analyze the nature of the single-particle states, away from the Dirac point in the presence of lo...
[[abstract]]Defects in graphene give rise to zero modes that are often related to the sharp peak in ...
Intrinsic defects give rise to scattering processes governing the transport properties of mesoscopic...
Graphene consists of an atom-thick layer of carbon atoms arranged in a honeycomb lattice, and its lo...
We present exact analytical calculations of scanning tunneling currents in locally disordered graphe...
We study the effects of impurities on the electronic properties of graphene. The tight-binding Hamil...
We study the interplay between the edge states and a single impurity in a zigzag graphene nanoribbon...
The density of states rho(E) of graphene is investigated within the tight-binding (Huckel) approxima...
In this paper, the average density of states (ADOS) in graphene with binary alloy disorders is calcu...
We introduce a model for amorphous grain boundaries in graphene and find that stable structures can ...
It is pointed out that due to direct couplings of electronic states, point defects on graphene are s...
We address local inelastic scattering from the vibrational impurity adsorbed onto graphene and the e...
We study the behavior of the local density of states in an armchair graphene nanoribbon with a poten...
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
The interaction between the Fermi sea of conduction electrons and a nonadiabatic attractive impurity...
We analyze the nature of the single-particle states, away from the Dirac point in the presence of lo...