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Explore techniques to improve light capture for silicon solar cells, including thermodynamics, nanoscale structures, and photonics. Learn about light trapping and energy balance to increase efficiency and maximize solar energy utilization.
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Křemík a svĕtlo: termodynamika, sluneční články a nanotechnologie Solar Energy Laboratory, Engineering Sciences, University of Southampton, UK Tom Markvart
Outline • Introduction: how to enhance light capture by crystalline silicon solar cells • The thermodynamics of light trapping: from Planck to the photonic bandgap solar cell • Sub-wavelength and nanoscale structures: about molecules, waveguides and photosynthetic light-harvesting.
Energy flux Electromagnetic energy density refractive index . c Electromagnetic energy density refractive index . d Light trapping: a statistical energy balance (Yablonovitch et al, 1982) (Planck, c. 1900)
I- 3 Light trapping in practice Dye sensitised (Grätzel) cell PERL cell - UNSW Light Electron injection Dye Electrolyte (Iodide / Tri-iodide) TiO2 nanocrystals (diameter 20 nm) Iodide I- Tri-iodide Figure courtesy of Martin Green, University of New South Wales. Source: Grätzel lab, EPFL
PV cell Managing light in the frequency space: fluorescent collectors W.H. Weber and J. Lambe, Appl. Opt. 1976 J.S. Batchelder, A.H. Zewail et al, Appl. Opt. 1979
PV cell PV cell Managing light in the frequency space: fluorescent collectors U. Rau et al, Appl. Phys. Lett. 2005; J.C. Goldschmidt et al, SOLMAT 2009. W.H. Weber and J. Lambe, Appl. Opt. 1976 J.S. Batchelder, A.H. Zewail et al, Appl. Opt. 1979 T. Markvart and L. Danos, 25th PVSEC, 2010.
1 DE reflectance Photonic band stop photon energy semiconductor bandgap photonic bandgap Frequency management: with photonics luminescence incident solar spectral flux density Absorption channel Photon transport channel
1mm c-Si with geometric light trapping 1mm c-Si with BSR 1mm c-Si with photonic light trapping Ultrathin c-Si photonic bandgap solar cell 500mm c-Si with BSR Efficiency 500mm cell 30.3% 1 mm cell (BSR only) 15.6% 1mm cell (geometric light trap.) 26.0% 1mm cell (photonic light trap.) 30.7% T. Markvart et al, RSC Adv. 2012
Time-resolved fluorescence DiO / porphyrin LB film (+ SiOx) or directly attached spacer Energy transfer to silicon Dyes c- silicon Kuhn, 1970, Danos et al, 2008, 2010
Dye – silicon energy transfer Near field (optical & dipole-dipole) Far-field effects (reflection) Sommerfeld, 1909; Chance, Prock and Silbey, 1978
Interaction Evanescent field (wave optics) Trapped electro-magnetic field Classical (geometrical optics) Classical (geometrical optics) The evanescent field silicon
to a nanowire solar cell e- membrane Photosynthesis: from a nanochemical factory … D.L. Dexter, J. Luminescence 1979; L. Danos et al, Thin Solid Films 2008; T. Markvart, Prog. Quant. Electron. 2000
Conclusion • We have reviewed the techniques currently available for enhancing the light capture by poorly absorbing materials such as silicon. Aside from geometric concentration these include: • Light trapping, closely linked with the directional equilibrium of the photon gas. Extension to the full thermodynamic equilibrium leads to the concepts of fluorescent concentrators / collectors and the photonic bandgap solar cell. • Sub-wavelength and nanoscale techniques, including photon tunnelling directly into the trapped (waveguiding) modes via the evanescent field, and the excitation of electron-hole pairs mediated by the dipole near field, similar to the light harvesting energy collection in photosynthesis.
Thanks to: Current and previous staff and students at Solar Energy Laboratory, University of Southampton Funding sources: PV21 Supergen, Engineering and Physical Sciences Research Council, UK; The Carbon Trust, UK … and to you for your attention !