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J. Chem. Phys. 136, 064701 (2012); http://dx.doi.org/10.1063/1.3682559 (10 pages)

The role of surface defects in multi-exciton generation of lead selenide and silicon semiconductor quantum dots

Heather M. Jaeger1, Sean Fischer2, and Oleg V. Prezhdo1

1University of Rochester, Department of Chemistry, Rochester, New York 14627-0216, USA
2University of Washington, Department of Chemistry, Seattle, Washington 98195-1700, USA

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(Received 3 October 2011; accepted 19 January 2012; published online 8 February 2012)

Multi-exciton generation (MEG), the creation of more than one electron-hole pair per photon absorbed, occurs for excitation energies greater than twice the bandgap (Eg). Imperfections on the surface of quantum dots, in the form of atomic vacancies or incomplete surface passivation, lead to less than ideal efficiencies for MEG in semiconductor quantum dots. The energetic onset for MEG is computed with and without surface defects for nanocrystals, Pb4Se4, Si7, and Si7H2. Modeling the correlated motion of two electrons across the bandgap requires a theoretical approach that incorporates many-body effects, such as post-Hartree-Fock quantum chemical methods. We use symmetry-adapted cluster with configuration interaction to study the excited states of nanocrystals and to determine the energetic threshold of MEG. Under laboratory conditions, lead selenide nanocrystals produce multi-excitons at excitation energies of 3 Eg, which is attributed to the large dielectric constant, small Coulomb interaction, and surface defects. In the absence of surface defects the MEG threshold is computed to be 2.6 Eg. For lead selenide nanocrystals with non-bonding selenium valence electrons, Pb3Se4, the MEG threshold increases to 2.9 Eg. Experimental evidence of MEG in passivated silicon quantum dots places the onset of MEG at 2.4 Eg. Our calculations show that the lowest multi-exciton state has an excitation energy of 2.5 Eg, and surface passivation enhances the optical activity of MEG. However, incomplete surface passivation resulting in a neutral radical on the surface drives the MEG threshold to 4.4 Eg. Investigating the mechanism of MEG at the atomistic level provides explanations for experimental discrepancies and suggests ideal materials for photovoltaic conversion.

© 2012 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. THEORETICAL METHODS
  3. RESULTS AND DISCUSSION
    1. Atomic vacancies in lead selenide quantum dots
    2. Surface-passivated silicon quantum dots
  4. CONCLUSIONS

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KEYWORDS, PACS, and IPC

PACS

  • 71.55.Cn

    Elemental semiconductors

  • 71.55.Ht

    Other nonmetals

  • 73.20.Mf

    Collective excitations (including excitons, polarons, plasmons and other charge-density excitations)

  • 73.21.La

    Quantum dots

  • 71.35.Gg

    Exciton-mediated interactions

  • 71.35.Lk

    Collective effects (Bose effects, phase space filling, and excitonic phase transitions)

International Patent Classification (IPC)

  • B82B1/00

    Nano-structures

  • B82B3/00

    Manufacture or treatment of nano-structures

  • H01L21/02

    Manufacture or treatment of semiconductor devices or of parts thereof

  • H01L21/70

    Manufacture or treatment of devices consisting of a plurality of solid state components or integrated circuits formed in or on a common substrate or of specific parts thereof; Manufacture of integrated circuit devices or of specific parts thereof

ARTICLE DATA

PUBLICATION DATA

ISSN

0021-9606 (print)  
1089-7690 (online)

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