Contents
Crystal Structures
Spacegroup: Pna21 (or Pbn21 with current axes choice)
(NOTE: For the crystal modeling purposes, select the spacegroup as Pbn21 )
Point group: C2v
Lattice constants:
Wyckoff positions:
Electronic band structure.
The lowest band gap is indirect: the VBM is near Y, the CBM at Gamma.
The lowest direct gap is at Gamma-Gamma.
Indirect and gap:
5.44 eV QSGW+0.8Sigma+exciton binding energy + zero-point motion correction [3]
3.60 eV LDA [3]
Direct band gap:
5.66 eV QSGW+0.8Sigma+exciton binding energy + zero-point motion correction [3]
3.84 eV LDA [3]
4.46 eV Expt. absorption [4]
Effective masses[2]:
conduction band minimum:
mcx=0.30, mcy=0.47, mcz=0.21
valence band maximum near Y:
mvx=0.55, mvy=0.33, mvz=1.09
valence band maximum at Gamma splittings and effective masses
Figure 1: Band structure of ZnSiN2 using QSGW method. . From data of ref. [3]
Figure 2: Band structure of ZnSiN2 near the VBM. [3]
Figure 3: Partial densities of states in ZnSiN2. [3]
Vibrational properties
There are 12 modes of a2, 11 of a1, b1 and b2 symmetry.
All modes are Raman active. The a1, b1, b2, are IR active and exhibit LO-TO splitting.
The Raman tensors for a1 have xx, yy, zz components, for a2, xy, for b1 xz and for b2 yz components
with x||a, y||b, z||c.
a1 is IR active for z polarization E||c
b1 is IR active for x polarization E||a
b2 is IR active for y polarization E||b
Reference: [5]
Expt. [1] Infrared reflectivity.
Predicted Raman intensities and Raman tensor values and Infrared spectra can be found in [2]
Comparison of IR spectrum of b1 modes between theory and experiment can be found in [5].
Born effective charge tensors.
Ref. [2]
Elastic Properties
Bulk moduli and pressure derivative
Elastic stiffness constants Cij (Mbar=100GPa)
Elastic compliances Sij (Mbar-1)
Reference: [6]
Piezo-electric constants and spontaneous polarization (cm-2)
Reference: [6]
Dielectric Properties.
High-frequency ε∞and static dielectric constants ε0
Reference: [2]
Index of refraction
Reference: [2]
Non-linear optical coefficients
Second order non-linear optics coefficients (pm/V)
Reference:[6]
Linear electro-optical coefficients (pm/V)
d15=d31
-2.19
nx
2.200
d34=d32
-2.09
ny
2.206
nz
2.300
d33
5.60
Reference:[6]
References
[1]. A. Mintairov, J. Merz, A. Osinsky, V. Fuflyigin, and L. Zhu, Appl. Phys. Lett. 76, 2517 (2000).
[2]. T. R. Paudel and W. R. L. Lambrecht, Phys. Rev. B 78,115204 (2008).
[3]. A. Punya, W. R. L. Lambrecht, and M. van Schilfgaarde, Phys. Rev. B 84,165204 (2011)
[5]. T. R. Paudel, W. R. L. Lambrecht, Phys. Rev. B 76, 115205 (2007)
[6]. T. R. Paudel, W. R. L. Lambrecht, Phys. Rev. B 79, 245205 (2009).