Translated Abstract
Aluminium nitride (AlN) belongs to the third generation semiconductor materials, exhibiting
prominent features such as wide bandgap, high electronic saturation mobility and low
permittivity. Thus AlN has potential applications in fabricating deep ultra-violet emitters and
optoelectronic detectors, and attracts much attention. Due to hexagonal wurtzite structure
and strong ionic bonding between the atoms, AlN possesses large spontaneous polarization,
significantly influencing the optoelectronic properties of devices. Thus the spontaneous
polarization is an inevitable issue in the study of wide bandgap semiconductors. In this
dissertation, based on the modern polarization theory and employing the first principles, the
spontaneous polarization of bulk and one dimension nanostructure is systematically
researched. The findings are of guiding significance help for improving the properties of
optoelectronic and piezoelectronic devices.
The spontaneous polarization and piezoelectric constants of wurtzite AlN, ZnO and GaN are
calculated by using the Berry phase method and maximally localized Wannier functions,
respectively. The relations between the spontaneous polarization and the crystal structures
are also investigated. The result indicates that the spontaneous polarization and piezoelectric
constants of AlN are the 1argest one among the three semiconductors. The spontaneous
polarization of AlN is two times more than that of the other two semiconductors. Analyzing
the contribution of electronic part and ionic part, we found that it is the maximum deviation
from the parameter u of ideal wurtzite structure and high ionicity of N-Al bond that lead to
the strong spontaneous polarization.
We point out the deficiencies of the approach used in the literature to calculate the
spontaneous polarization. On the basis of the discussion of local dipole, a correction formula
is given. By using the charge depth of the formula unit, we also proposed a new method to
directly calculate the spontaneous polarization of wurtzite structure without building the
reference structure. The production of the spontaneous polarization can be intuitively
explanation in terms of this method. Comparing with the Berry phase method, owning to the
production of the Wannier centers, the maximally localized Wannier functions has a unique
advantage in analyzing spontaneous polarization, electric structures and atomic bonding,
which will give a more clear physical picture.
The electronic structure of the intrinsic point defects is firstly calculated through the
maximally Wannier functions. Because vacancy is one of the most common point defect in
the crystal growth, which influences many properties of the crystal. By using first-principles
plane-wave ultrasoft Pseudopotential method and based on the density functional theory, the
maximally localized Wannier functions of the vacancy with different charge state are
calculated. With the shape and center of the computed Wannier function, the electronic
structure and the spontaneous polarization change in the [ 0001],[-1010] and [-12-10]
orientation are studied respectively. It is found that the electrons of the dangling bonds
displace to the positions of the vacancies in N vacancy structure, while the electrons keep
away from the vacancy and move to the other side of N atoms in Al vacancy structure. Since
the vacancy breaks the centrosymmetry of the
[-1010 ] and [-12-10] orientation, polarization
will be induced in these two directions, and the polarization increase as the charge increase.
In the [ 0001] orientation of the N vacancy structure, the spontaneous polarization will
reverse as the charge state of vacancy increase because of the dramatic variation of the
electronic structure. Contrary to the N vacancy, although the spontaneous polarization of Al
vacancy increases as the charge state increases, the polarization reversion does not occur in
the Al vacancy structure. For Comparison, the spontaneous polarization variation of ZnO
caused by O vacancy and Zn interstitial is also computed. It is found that the polarization
properties induced by the vacancy is similar to that of AlN. The polarization change induced
by the vacancy interaction in ZnO is further researched. It is found that the system energy is
more stable when the two vacancies get close to each other, and the strong interaction causes
will decrease the spontaneous polarization, which can be used to regulate the polarization.
The prominent properties of the nano-structure of AlN are attracted much attention in recent
years. By building the nanowires with different sizes, the spontaneous polarization and
piezoelectric properties of AlN nanowires (NWs) are investigated in terms of local dipole
obtained by maximally localized Wannier functions. It is found that the value of spontaneous
polarization is larger in NWs than in the bulk, and will increase by decreasing the NWs size.
A further analysis is performed from the point of view of lattice and surface relaxation
occurring in the NWs. We show that surface relaxation enhances the spontaneous
polarization, while the change of lattice parameter plays a negative role. For the piezoelectric
property, we find that it is slightly improved compared with bulk and is similar in a certain
range of NW diameters. These findings are of guiding significance help for the fabrication of
piezoelectric devices based on AlN NWs.
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