Contents
Crystal Structures
Space group: Pna21 (NOTE: For crystal modeling purposes, select the spacegroup as Pbn21 )
Point group: C2v
Lattice constants:
Wyckoff positions:
Reference [4]
Synthesis and growth methods
Crystalline MgGeN2 thin solid films growth: J.E. Van Nostrand at al; using the technique of molecular beam epitaxy (MBE) in a nitrogen plasma source.[3]
Electronic band structure
Band Gap:
Effective masses:
Conduction band minimum splittings and effective masses:
mcx=0.31 mcy=0.30 mcz=0.28 [4]
Valence band maximum splittings and effective masses:
These data from reference [4]
Parameters of effective Hamiltonian: inverse-mass parameters Ai,Bi,Ci (.2h/2me), energy splitting (meV). [4]
Figures:
Figure 1: Electronic band structure of MgGeN2 [4]
Figure 2: Band structure near valence band maximum [4]
Figure 3: Density of states and partial density of states [4]
Vibrational Properties
The phonons of the orthorhombic ternary nitrides at the gamma point can be classified by the irreducible representation of the point group C2v.
There are 12 modes of each a1, a2, b1, and b2 symmetry.
All modes are Raman active. The a1, b1, b2 are IR active as well. Longitudinal modes a1L, b1L, b2L are affected by LO-TO splitting.
Computed frequencies of zone-center phonons: from reference [2]
Full set of zone-center phonon frequencies (in cm-1): from reference [6]
Predicted Raman and IR spectra can be found in ref. [6] as well as phonon band structure and density of states.
Phonon calculations were also reported in [7] but do not provide a table of numerical results, only a figure.
Born effective charge tensor components:
Reference: [6]
Reference: [7]
Elastic Properties
Bulk moduli and pressure derivative:
Dielectric Properties
Second order non linearity
MgGeN2 follows the relation χ(2)zzz=-2 χ(2)xxz where χ: Susceptibility.(pm V−1)) [2]
χ(2)zzz = −14.49
χ(2)xzx = χ(2)zxx = 8.80
χ(2)yzy = χ(2)zyy = 7.58
References:
[1]. Yu. M. Basalaev and P. V. Demushin, J. Struct. Chem. Vol. 51, No. 6, pp. 1191-1194, 2010
[2]. J Huang, L Tang and M H Lee, J. Phys.: Cond. Matter Vol. 13, No 46.
[3]. J Van nostrand,J Albrecht,R. Cortez, K. leedy,B. Johnson and M. o’keefe, Phys.: Condens. Matter (2001) 10417–10431.
[4]. A. P. Jaroenjittichai and Walter R. L. Lambrecht,Phys. Rev. B,94, 125201
[5]. T. Misaki, X. Wu, A. Wakahara, and A. Yoshida, Proc. Int. Workshop on Nitride Semiconductors IPAP Conf., Series 1, (2001), pp. 685-688.
[6]. S. Pramchu, A. P. Jaroenjittichai, and Y. Laosiritaworn, Ceramics Intl. (2017) [pending print]
[7] M. Råsander, J. B. Quirk, T. Wang, R. Davies, and M. A. Moram, arXive:1705.01515
[8] Sai Lyu and Walter R. L. Lambrecht, Solid State Communications 299, 113664 (2019).
εxx = 4.80 εyy = 4.71 εzz = 4.86 [2]