4.7 Article

pn-Junction nanorods in a polymer matrix: A paradigm shift from conventional hybrid bulk-heterojunction solar cells

Journal

SOLAR ENERGY MATERIALS AND SOLAR CELLS
Volume 143, Issue -, Pages 319-325

Publisher

ELSEVIER SCIENCE BV
DOI: 10.1016/j.solmat.2015.07.020

Keywords

Hybrid bulk-heterojunction (BHJ) solar cells; pn-Junction in a nanorod; Cu2SICdS pn-junction; Charge separation in pn-junctions; Polymer:nanorod hybrid BHJ

Funding

  1. DeitY project [12(1)/2012-EMCD]
  2. SERIIUS project [IUSSTF/JCERDC-SERIIUS/2012]
  3. CSIR [09/080(0843)/2012-EMR-I, 519699, 09/080(0779)/2011-EMR-I, 510847]

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We report introduction of pn-junction nanorods in a polymer matrix to form hybrid bulk-heterojunction (BHJ) solar cells. This is a paradigm shift from conventional hybrid solar cells, where quantum dots or nanorods of an inorganic semiconductor and a conjugated polymer form a BHJ. The pn-junctions were formed in n-type CdS nanorods through a controlled cationic exchange process; here p-type Cu2S formed from one end of CdS due to selective reactivity of crystalline planes of the nanorods. Due to an epitaxial attachment between Cu2S and CdS semiconductors in the nanorod, a depletion region hence formed in the pn-junction, which is a classical example of type-II band-alignment at the interface. The junction separated charge carriers under illumination through a drift of minority carriers across the depletion region. Hybrid BHJs based on Cu2SICdS pn-junction nanorods in a conventional polymer matrix therefore acted as efficient solar cells as compared to similar BHJ devices with nanorods of individual materials, that is Cu2S or CdS. We varied the relative lengths of p- and n-sections of the pn-junctions that in turn controlled charge separation and carrier transport processes to optimize the solar cell performance. (c) 2015 Elsevier B.V. All rights reserved.

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