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Intermediate Band Solar Cell

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Single gab solar cell makes poor use of solar spectrum ... Each band is described by its own quasi Fermi level. Band to band transitions must be radiative ... – PowerPoint PPT presentation

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Title: Intermediate Band Solar Cell


1
Intermediate Band Solar Cell
  • Device physics
  • University of Utrecht
  • 24 January 2004
  • Rob Harmsen

2
Overview
  • Introduction
  • Main principles of IBSC
  • Conditions
  • Efficiency
  • Shockley Read Hall recombination
  • IBSC Materials
  • Conclusion

3
Single gab solar cell makes poor use of solar
spectrum
  • Multi Junction cell
  • Solar thermo-photovoltaic
  • Molecular based cells
  • Intermediate band solar cell (IBSC)

4
Intermediate band (IB)
  • Extra current without voltage degradation

5
Conditions
  • Each band is described by its own quasi Fermi
    level
  • Band to band transitions must be radiative
  • Infinite carrier mobility, Ideal contacts etc

6
Efficiency
  • Single gab 40.7
  • Tandem cell 55.4
  • IBSC 64.1
  • Better quantum efficiency then tandem.

7
Shockley Read Hall recombinationTrap v.s. IB
  • Traps between CB and VB are normally considered
    as a source of non-radiative recombination
    (SRH).
  • How can the IB be only a radiative recombination
    source?
  • TrapLocalized v.s. IBDelocalized

8
Shockley Read Hall recombinationEnergy
  • Phonon energy tenths of meV
  • Bandgap hundreds of meV
  • IB, simultaneous interaction with tenths of
    phonons (unlikely).
  • Trap, impurity is excited, then emission of
    phonons (not simultaneous).

9
Shockley Read Hall recombination Not likely if
  • Impurities are in periodical pattern.
    Vibrational modes tenths meV
  • Quantum dots. thousands of atoms, not a single
    impurity

10
IB Materials
  • Ga4X3M XAs or P, Mmetal

11
Quantum Dot
  • InyGa1-yAs Dot in AlxGa1-xAs material
  • Materials have been made
  • No increase of efficiency observed
  • Quantum efficiency/photon energy indicate
    principles of IBSC

12
Nanoporous Materials
  • Nanoporous material TiO2
  • Cavities filled with PbS as Quantum dot
  • Electrolyte CH3OH as P contact forms HCOOH. Even
    if illuminated with low energy photons.
  • solid state P-type contact photovoltaic behavior
    is lost.
  • Evidence of IBSC principles has not been found yet

13
Conclusions
  • IBSC, theoretically efficiency of 63
  • Each band must have a separate quasi Fermi
    level.
  • Band to band transitions must be radiative.
  • If IB is de-localized SRH recombination plays no
    role (i.e. QDs).
  • New materials have been found, indicating these
    work according to IBSC principles
  • No improvement of efficiency has been found yet.
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