Potential of hafnium nitride for the hot carrier solar cell

The Hot Carrier solar cell is a third generation photovoltaic concept which has the potential to achieve high efficiencies, exceeding the Shockley-Queisser limit for a conventional p-n junction solar cell. The theoretical efficiencies achievable for the Hot Carrier solar cell is 65% for non-concentrated solar radiation and 85% for maximally concentrated light, very close to the limits of an infinite tandem solar cell. The approach of the Hot Carrier solar cell is to extract carriers generated before thermalisation to the bandgap edge occurs when their excess energy is lost to the environment as heat. To achieve this, the rate of carrier cooling in the absorber must be slowed down sufficiently enough to allow carriers to be collected while they are hot. This work investigates using hafnium nitride as such an absorber to restrict mechanisms of carrier cooling. Hafnium nitride’s phononic properties, where a large ‘phononic band gap’ exist can reduce the carrier cooling rate by means of a phonon bottleneck such that optical phonons cannot decay into acoustic phonons by means of the Klemens’ mechanism. Optical phonon-electron scattering can maintain a hot electron population while acoustic phonons are irrecoverable and lost as heat. The electronic and phononic properties of hafnium nitride are evaluated for their suitability to be used in a Hot Carrier solar cell absorber. Recent work on the fabrication of hafnium nitride at UNSW is presented.

[1]  N. Lehner,et al.  Erratum: Phonon anomalies in transition-metal nitrides: HfN , 1984 .

[2]  H. Seo,et al.  Growth and physical properties of epitaxial HfN layers on MgO(001) , 2004 .

[3]  L. Hirst,et al.  Fundamental losses in solar cells , 2009 .

[4]  P. G. Klemens,et al.  Anharmonic Decay of Optical Phonons , 1966 .

[5]  Börje Johansson,et al.  Cubic Hf3N4 and Zr3N4: A class of hard materials , 2003 .

[6]  Peter Kroll,et al.  Hafnium nitride with thorium phosphide structure: physical properties and an assessment of the Hf-N, Zr-N, and Ti-N phase diagrams at high pressures and temperatures. , 2003, Physical review letters.

[7]  A. Othonos Probing ultrafast carrier and phonon dynamics in semiconductors , 1998 .

[8]  J. I. Davies,et al.  Hot carrier energy loss rates in GaInAs/InP quantum wells , 1988 .

[9]  K. Sasaki,et al.  Influence of Sputtering Parameters on the Formation Process of High-Quality and Low-Resistivity HfN Thin Film , 1999 .

[10]  B. Ridley,et al.  The LO phonon lifetime in GaN , 1996 .

[11]  D. Dunlavy,et al.  Dependence of hot carrier luminescence on barrier thickness in GaAs/AlGaAs superlattices and multiple quantum wells , 1990 .

[12]  P. Würfel,et al.  Solar energy conversion with hot electrons from impact ionisation , 1997 .

[13]  Levi,et al.  Hot-carrier cooling in GaAs: Quantum wells versus bulk. , 1993, Physical review. B, Condensed matter.

[14]  R. T. Ross,et al.  Efficiency of hot-carrier solar energy converters , 1982 .

[15]  M. Green,et al.  Interplay between the hot phonon effect and intervalley scattering on the cooling rate of hot carriers in GaAs and InP , 2012 .

[16]  A. A. Safonov,et al.  Structure and electronic properties of zirconium and hafnium nitrides and oxynitrides , 2005 .

[17]  H. Seo,et al.  Effect of off stoichiometry on Raman scattering from epitaxial and polycrystalline HfNx (0.85≤x≤ 1.50) grown on MgO(001) , 2008 .

[18]  H. Queisser,et al.  Detailed Balance Limit of Efficiency of p‐n Junction Solar Cells , 1961 .

[19]  J. Cuomo,et al.  Higher nitrides of hafnium, zirconium, and titanium synthesized by dual ion beam deposition , 1986 .

[20]  M. Green Third generation photovoltaics : advanced solar energy conversion , 2006 .

[21]  Gavin Conibeer,et al.  Slowing of carrier cooling in hot carrier solar cells , 2008 .

[22]  Umesh V. Waghmare,et al.  Electronic structure, phonons, and thermal properties of ScN, ZrN, and HfN: A first-principles study , 2010 .