4.6 Article

Substrate-controlled band positions in CH3NH3Pbl3 perovskite films

Journal

PHYSICAL CHEMISTRY CHEMICAL PHYSICS
Volume 16, Issue 40, Pages 22122-22130

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/C4CP03533J

Keywords

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Funding

  1. National Renewable Energy Laboratory Director's Fellowship
  2. U.S. Department of Energy/National Renewable Energy Laboratory's Laboratory Directed Research and Development (LDRD) program
  3. Division of Chemical Sciences, Geosciences, and Biosciences
  4. Office of Basic Energy Sciences of the US Department of Energy
  5. US Department of Energy
  6. Office of Basic Energy Sciences, Energy Frontier Research Centers [DE-AC36-08GO28308]
  7. US-India Partnership to Advance Clean Energy Research (PACE-R)
  8. Solar Energy Research Institute for India and the United States (SERIIUS)
  9. Government of India, through the Department of Science and Technology [IUSSI4JCERDC-SERIIUS/2012]

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Using X-ray and ultraviolet photoelectron spectroscopy, the surface band positions of solution-processed CH(3)NH(3)Pbl(3) perovskite thin films deposited on an insulating substrate (Al2O3), various n-type (TiO2, ZrO2, ZnO, and F:SnO2 (FTO)) substrates, and various p-type (PEDOT:PSS, NiO, and Cu2O) substrates are studied. Many-body GW calculations of the valence band density of states, with spin orbit interactions included, show a clear correspondence with our experimental spectra and are used to confirm our assignment of the valence band maximum. These surface-sensitive photoelectron spectroscopy measurements result in shifting of the CH(3)NH(3)Pbl(3) valence band position relative to the Fermi energy as a function of substrate type, where the valence band to Fermi energy difference reflects the substrate type (insulating-, n-, or p-type). Specifically, the insulating- and n-type substrates increase the CH(3)NH(3)Pbl(3) valence band to Fermi energy difference to the extent of pinning the conduction band to the Fermi level; whereas, the p-type substrates decrease the valence band to Fermi energy difference. This observation implies that the substrate's properties enable control over the band alignment of CH(3)NH(3)Pbl(3) perovskite thin-film devices, potentially allowing for new device architectures as well as more efficient devices.

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