4.8 Article

The Effects of Doping Density and Temperature on the Optoelectronic Properties of Formamidinium Tin Triiodide Thin Films

期刊

ADVANCED MATERIALS
卷 30, 期 44, 页码 -

出版社

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adma.201804506

关键词

charge-carrier mobility; charge-carrier recombination; hybrid perovskite photovoltaics; SnF2; THz spectroscopy

资金

  1. Engineering and Physical Sciences Research Council (EPSRC), UK
  2. EPSRC [EP/M015254/1, EP/M024881/1, EP/L024667/1] Funding Source: UKRI
  3. Engineering and Physical Sciences Research Council [EP/M015254/1, EP/M024881/1] Funding Source: researchfish

向作者/读者索取更多资源

Optoelectronic properties are unraveled for formamidinium tin triiodide (FASnI(3)) thin films, whose background hole doping density is varied through SnF2 addition during film fabrication. Monomolecular charge-carrier recombination exhibits both a dopant-mediated part that grows linearly with hole doping density and remnant contributions that remain under tin-enriched processing conditions. At hole densities near 10(20) cm(-3), a strong Burstein-Moss effect increases absorption onset energies by approximate to 300 meV beyond the bandgap energy of undoped FASnI(3) (shown to be 1.2 eV at 5 K and 1.35 eV at room temperature). At very high doping densities (10(20) cm(-3)), temperature-dependent measurements indicate that the effective charge-carrier mobility is suppressed through scattering with ionized dopants. Once the background hole concentration is nearer 10(19) cm(-3) and below, the charge-carrier mobility increases with decreasing temperature according to approximate to T-1.2, suggesting that it is limited mostly by intrinsic interactions with lattice vibrations. For the lowest doping concentration of 7.2 x 10(18) cm(-3), charge-carrier mobilities reach a value of 67 cm(2) V-1 s(-1) at room temperature and 470 cm(2) V-1 s(-1) at 50 K. Intraexcitonic transitions observed in the THz-frequency photoconductivity spectra at 5 K reveal an exciton binding energy of only 3.1 meV for FASnI(3), in agreement with the low bandgap energy exhibited by this perovskite.

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