4.7 Article

Transport in ITO Nanocrystals with Short- to Long-Wave Infrared Absorption for Heavy-Metal-Free Infrared Photodetection

Journal

ACS APPLIED NANO MATERIALS
Volume 2, Issue 3, Pages 1621-1630

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsanm.9b00067

Keywords

oxide nanocrystals; transport; photoconduction; plasmon; intraband absorption; infrared; heavy metal-free; photodetection

Funding

  1. ERC starting grant blackQD [756225]
  2. Region Ile-de-France
  3. French state funds within the Investissements d'Avenir programme [ANR-11-IDEX-0004-02]
  4. grant Nanodose
  5. IPER-Nano2
  6. Chinese Scholar council
  7. Nexdot

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Nanocrystals are often described as interesting materials for the design of low-cost optoelectronic devices, especially in the infrared range. However, the driving materials reaching infrared absorption generally contain heavy metals (Pb and Hg) with a high toxicity. An alternative strategy to achieve infrared transition is the use of doped semiconductors presenting intraband or plasmonic transition in the short-, mid-, and long-wave infrared. This strategy may offer more flexibility regarding the range of possible candidate materials. In particular, significant progress has been achieved for the synthesis of doped oxides and for the control of their doping magnitude. Among them, tin doped indium oxide (ITO) is the one providing the broadest spectral tunability. Here we test the potential of such ITO nanoparticles for photoconduction in the infrared. We demonstrate that 1%03 nanoparticles present an intraband absorption in the mid-infrared range which is transformed into a plasmonic feature as doping is introduced. We have determined the cross section associated with the plasmonic transition to be in the 1-3 X 10(-13) cm(2) range. We have observed that the nanocrystals can be made conductive and photoconductive thanks to a ligand exchange using a short carboxylic acid, leading to a dark conduction with n-type character. We present evidence that the observed photoresponse in the infrared is the result of a bolometric effect.

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