| dc.description.abstract | Designing a material for a particular application requires an atomistic understanding of its
properties. Recent development in first principles methods and supercomputing speeds has
enabled researchers to compute materials properties accurately. This has opened up a window
for computational designing of materials for various applications such as optoelectronics,
thermoelectrics, magnetic shape memory alloys etc. In this thesis, first principles methods
have been utilized to understand the properties of various materials such as TiS2, TiS3, GeO2,
Co3(MoTaAl) alloys, Ni2MnGa and graphene. This thesis has been organized as follows:
• Chapter 1 introduces various functional materials and their application in the thermoelectric,
optoelectronic, high temperature and magnetic shape memory. The microscopic
understanding of materials properties such as structure, energetics, electronic structure,
electronic transport, and lattice dynamics etc. can lead to novel ways of designing materials
properties for various applications.
• Chapter 2 describes the theoretical methodology adopted in this work. It gives a brief
understanding of first principles based density functional theory (DFT) and various approximations
to obtain accurate electronic properties. Methods employed for calculation
of electronic and thermal transport are also discussed briefly.
• In Chapter 3 we explore the tuning of the electronic structure of the transition metal
dichalogenide TiS2. We show that by engineering its electronic structure, it transforms
from a semimetal to a semiconductor under biaxial strain. The thermoelectrics study
shows that a 3 fold enhancement in thermopower can be achieved by application of 5%
biaxial strain. This enhancement is driven by a small bandgap opening of ∼0.15 eV, which
increases its thermopower at the same time decreasing its lattice thermal conductivity
indicating improvement in ZT.
• In Chapter 4 we study the possibility of inherent stacking fault in bulk TiS3 and its effect
on the electronic properties. We find that TiS3 can exist in AB′ and AB′′ geometries. The
energy difference between two structures is about 0.011 eV/f.u. The electronic structure
is independent of the stacking fault due to the weak vdW interaction between the layers.
The calculated thermopower is 200 μV/K in the carrier concentration range of 1×1020
cm−3 - 5×1020 cm−3, which is comparable with other state of the art thermoelectric
materials. The high thermopower and electrical conductivity in the carrier concentration
range of 1×1020 cm−3 - 5×1020 cm−3 leads to a high power factor for both p- and n-type.
Moreover, the power factor for p-type is three times higher than that of n-type carriers
indicating that the thermoelectric performance for p-type will be much better than that
of n-type.
• Chapter 5 reveals the origin behind the large variation in the band gap (∼ 2 eV) of
GeO2 calculated by standard DFT within LDA/GGA, which had remained unresolved.
Using the many-body perturbation theory (GW approximation), we find that this large
variation observed in literature is independent of the method used and depends strongly
on the lattice parameter (volume strain). This strong dependence originates from a change
in hybridization among O-p and Ge-(s and p) orbitals.
• Chapter 6 deals with the structural stability of order intermetallic Co-based superalloys.
We have shown that W free Co3Al order structure can be stabilized in L12 structure by
addition of Mo and Ta atoms. The enthalpy of formation of L12 structure significantly
becomes more negative compared to the DO19 structure by the addition of ≥ 4% of Ta
atoms. This implies that the L12 structure of Co3(Al,Mo,Ta) structure is more stable
compared to DO19. The lowering in the enthalpy of formation is found due to the formation
of the pseudo gap and the decrease in the states at the pseudo gap with increasing Ta
concentration. The stability of the L12 structure can be further improved by the addition
of Ni and Ti atoms.
• In Chapter 7, the lattice dynamics and electronic structure of X2YZ [where X = Ni,
Fe, Co; Y = Mn; Z = Al, Ga, Ge, In, Sn, Sb] stoichiometry compounds are investigated.
The lattice instability of X2MnZ depends on the position of the Fermi energy (EF ) with
respect to the pseudo gap. The phonon mode softening along the Γ-K symmetry direction
is observed for Ni2MnZ in the austenite phase since EF is located above the pseudo gap.
This mode softening is mainly responsible for the MSM effect. On the other hand, Fe2MnZ
and Co2MnZ [Z = Al, Ga, Ge, In, Sn, Sb] in the cubic phase do not show any phonon
mode softening because EF lies in the vicinity of the pseudo gap or at the pseudo gap.
Thus, alloying Fe or Co at the Ni site in Ni2Mn (Z = groups-IV and V) can tune the lattice
modulation. In addition, the magnetic moments of Fe2Mn (Z = groups-IV and V) and
Co2Mn (Z = groups-IV and V) are much higher than those of Ni2Mn (Z = groups-IV and
V), indicating that the magnetic moments of Ni2MnZ can be enhanced. The calculated
phonon dispersion with magnetic moment indicates that the phonon mode softening is
sensitive to the change in the local magnetic moment of the atoms, thereby enabling
tunability in the MSM effect.
• In chapter 8, we show that the mono vacancy defects in graphene can be used as precursors
to form novel clipped structures without explicit use of functional groups. These
clipped structures can be transformed into one-dimensional (1D) double wall nanotubes
(DWCNT) or multi-layered three dimensional (3D) structures. The clipped structures
show good mechanical strength due to covalent bonding between multi-layers. Clipping
also provides a unique way to simultaneously harness the conductivity of both walls of
a double wall nanotube through covalently bonded scattering junctions. With additional
conducting channels and improved mechanical stability, these clipped structures can lead
to a myriad of applications in novel devices.
• Chapter 9 summarizes and concludes the work presented in this thesis. | en_US |
