Hot carrier cells: an example of third generation photovoltaics

Third generation photovoltaic approaches aim to use multiple energy level approaches to circumvent the Schockley- Queisser limit but to still allow use of thin film approaches. Hence they offer significant potential to reduce cost per Watt and move solar cell technologies towards the levels necessary to achieve LCOE values that give grid parity. The Hot Carrier solar cell is a Third Generation device that aims to tackle the carrier thermalisation loss after absorption of above band-gap photons. It is theoretically capable of extremely high efficiencies, 65% under one sun, very close to the maximum thermodynamic limit. However, it relies on slowing the rate of carrier cooling in the absorber from ps to ns. This very tough challenge can perhaps be addressed through nanostructures and modulation of phonon dispersions. The mechanisms of carrier cooling are discussed and methods to interrupt this process investigated to give a list of properties required of an absorber material. Quantum well or nano-well structures and large mass difference compounds with phonon band gaps are discussed in the context of enhancing phonon bottleneck and hence slowing carrier cooling. Materials for these structures are discussed and potential combined structures to maximize phonon bottleneck and slow carrier cooling are suggested.

[1]  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 .

[2]  Gavin Conibeer,et al.  Phonon lifetimes in model quantum dot superlattice systems with applications to the hot carrier solar cell , 2010 .

[3]  S. Shrestha,et al.  Progress on Hot Carrier solar cells at UNSW , 2006 .

[4]  Kwiseon Kim,et al.  Structure and phonons ofZnGeN2 , 2005 .

[5]  G. P. Srivastava,et al.  Long-wavelength nonequilibrium optical phonon dynamics in cubic and hexagonal semiconductors , 2004 .

[6]  H. Bilz,et al.  Phonon Dispersion Relations in Insulators , 1979 .

[7]  M. Zebarjadi,et al.  Thermoelectric Transport in a ZrN/ScN Superlattice , 2009 .

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

[9]  Gavin Conibeer,et al.  Hot carrier solar cells: Principles, materials and design , 2010 .

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

[11]  Weili Liu,et al.  Thermal conductivity of Si/Ge superlattices , 1999, Eighteenth International Conference on Thermoelectrics. Proceedings, ICT'99 (Cat. No.99TH8407).

[12]  S. Dalui,et al.  Synthesis of B-Sb by rapid thermal annealing of B/Sb multilayer films , 2006 .

[13]  Klein,et al.  Folded acoustic and quantized optic phonons in (GaAl)As superlattices. , 1985, Physical review. B, Condensed matter.

[14]  Martin A. Green,et al.  Third generation photovoltaics , 2002, 2002 Conference on Optoelectronic and Microelectronic Materials and Devices. COMMAD 2002. Proceedings (Cat. No.02EX601).

[15]  Gavin Conibeer,et al.  Investigation of theoretical efficiency limit of hot carriers solar cells with a bulk indium nitride absorber , 2010 .

[16]  A. Debernardi PHONON LINEWIDTH IN III-V SEMICONDUCTORS FROM DENSITY-FUNCTIONAL PERTURBATION THEORY , 1998 .

[17]  W. Schaff,et al.  Time-resolved spectroscopy of recombination and relaxation dynamics in InN , 2003 .

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

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

[20]  Arun Kumar Pal,et al.  BSb films: Synthesis and characterization , 2007 .

[21]  P. A. Cox The Elements: Their Origin, Abundance, and Distribution , 1989 .