Heat capacity of α-GaN : Isotope effects

Until recently, the heat capacity of GaN had only been measured for polycrystalline powder samples. Semiempirical as well as \textit{first-principles} calculations have appeared within the past few years. We present in this article measurements of the heat capacity of hexagonal single crystals of GaN in the 20-1400K temperature range. We find that our data deviate significantly from the literature values for polycrystalline materials. The dependence of the heat capacity on the isotopic mass has also been investigated recently for monatomic crystals such as diamond, silicon, and germanium. Multi-atomic crystals are expected to exhibit a different dependence of these heat capacities on the masses of each of the isotopes present. These effects have not been investigated in the past. We also present \textit{first-principles} calculations of the dependence of the heat capacities of GaN, as a canonical binary material, on each of the Ga and N masses. We show that they are indeed different, as expected from the fact that the Ga mass affects mainly the acoustic, that of N the optic phonons. It is hoped that these calculations will encourage experimental measurements of the dependence of the heat capacity on isotopic masses in binary and more complex semiconductors.

[1]  Disorder-induced phonon self-energy of semiconductors with binary isotopic composition , 2001, cond-mat/0107102.

[2]  Heat capacity of isotopically enriched 28Si, 29Si and 30Si in the temperature range 4 K , 2004, cond-mat/0412264.

[3]  R. Tolman,et al.  The Principles of Statistical Mechanics. By R. C. Tolman. Pp. xix, 661. 40s. 1938. International series of monographs on physics. (Oxford) , 1939, The Mathematical Gazette.

[4]  T. Xu,et al.  Structure and Heat Capacity of Wurtzite GaN from 113 to 1073 K , 1999 .

[5]  A. Brukl,et al.  Die Oxyde des Galliums , 1931 .

[6]  A. Zunger,et al.  Self-interaction correction to density-functional approximations for many-electron systems , 1981 .

[7]  A. Yazawa,et al.  High temperature heat content measurements of the III-V (III: Al, Ga, In V: N, P, As, Sb) compounds , 1989 .

[8]  M. Cardona,et al.  Isotopic dependence of the heat capacity of c-C, Si, and Ge: an ab initio calculation , 2004 .

[9]  R. W. Henn,et al.  Thermal conductivity of isotopically enriched silicon , 2000 .

[10]  S. Baroni,et al.  Dependence of the crystal lattice constant on isotopic composition: Theory and ab initio calculations for C, Si, and Ge , 1994 .

[11]  J. Junquera,et al.  Ab initio local vibrational modes of light impurities in silicon , 2001, cond-mat/0109306.

[12]  R. Davis,et al.  Phonon density of states of bulk gallium nitride , 1998 .

[13]  B. Marí,et al.  Effect of N isotopic mass on the photoluminescence and cathodoluminescence spectra of gallium nitride , 2004 .

[14]  William F. Banholzer,et al.  Thermal conductivity of isotopically modified single crystal diamond. , 1993 .

[15]  Xavier Gonze,et al.  Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional perturbation theory , 1997 .

[16]  F. Ruymgaart,et al.  Thermodynamics of impurities in semiconductors , 2004 .

[17]  Manuel Cardona Electron-phonon interaction in tetrahedral semiconductors , 2005 .

[18]  Testa,et al.  Green's-function approach to linear response in solids. , 1987, Physical review letters.

[19]  A. V. Gusev,et al.  Thermal conductivity of isotopically enriched 28Si: revisited , 2004 .

[20]  D. Sedmidubský,et al.  High temperature enthalpy and heat capacity of GaN , 2003 .

[21]  T. R. Anthony,et al.  Measurements of the heat capacity of diamond with different isotopic compositions , 2005 .

[22]  Izabella Grzegory,et al.  High pressure growth of bulk GaN from solutions in gallium , 2001 .

[23]  M. Cardona,et al.  Raman Study of the Anomalous TO Phonon Structure in GaP with Controlled Isotopic Composition , 1999 .

[24]  W. Klemm,et al.  Messungen an Gallium- und Indium-Verbindungen. X. Über die Chalkogenide von Gallium und Indium , 1934 .

[25]  A. A. Maradudin,et al.  Theory of lattice dynamics in the harmonic approximation , 1971 .

[26]  J. Karpinski,et al.  Equilibrium pressure of N2 over GaN and high pressure solution growth of GaN , 1984 .

[27]  A. Einstein Die Plancksche Theorie der Strahlung und die Theorie der spezifischen Wärme [AdP 22, 180 (1907)] , 2005, Annalen der Physik.

[28]  Leonard Kleinman,et al.  Efficacious Form for Model Pseudopotentials , 1982 .

[29]  Emilio Artacho,et al.  LINEAR-SCALING AB-INITIO CALCULATIONS FOR LARGE AND COMPLEX SYSTEMS , 1999 .

[30]  M. Cardona,et al.  Phonon dispersion curves in wurtzite-structure GaN determined by inelastic x-ray scattering. , 2001, Physical review letters.

[31]  K. Itagaki,et al.  High temperature heat contents of III-V semiconductor systems , 1990 .

[32]  E. Haller,et al.  High purity isotopically enriched ^70Ge and ^74Ge single crystals: Isotope separation, growth, and properties , 1993 .

[33]  P. Debye Zur Theorie der spezifischen Wärmen , 1912 .

[34]  Eugene E. Haller,et al.  Thermal conductivity of germanium crystals with different isotopic compositions , 1997 .

[35]  B. Alder,et al.  THE GROUND STATE OF THE ELECTRON GAS BY A STOCHASTIC METHOD , 2010 .

[36]  Daniel Sánchez-Portal,et al.  Density‐functional method for very large systems with LCAO basis sets , 1997 .

[37]  T. Kikegawa,et al.  Precise measurement of equation-of-state and elastic properties for GaN up to 16 GPa , 2002 .

[38]  S. Estreicher,et al.  Specific heat and entropy of GaN , 2004 .