4.6 Article

Femtosecond two-photon absorption spectroscopy of copper indium sulfide quantum dots: A structure-optical properties relationship

Journal

OPTICAL MATERIALS
Volume 86, Issue -, Pages 455-459

Publisher

ELSEVIER SCIENCE BV
DOI: 10.1016/j.optmat.2018.10.023

Keywords

CuInS2 quantum dots; Two-photon absorption; Parabolic effective-mass approximation model; Femtosecond laser; Nanomaterials; Wavelength-tunable femtosecond Z-scan technique

Funding

  1. FAPEMIG (Fundacao de Amparo a Pesquisa do Estado de Minas Gerais) [APQ-01203-16]
  2. FAPESP (Fundacao de Amparo a Pesquisa do Estado de Sao Paulo) [2011/12399-0, 2015/20032-0, 2016/20886-1]
  3. CNPq (Conselho Nacional de Desenvolvimento Cientifico e Tecnologico)
  4. LNNano (Laboratorio Nacional de Nanotecnologia)
  5. CAPES (Coordenacao de Aperfeicoamento de Pessoal de Nivel Superior)
  6. Air Force Office of Scientific Research [FA9550-12-1-0028, FA9550-15-1-0521]

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We have interpreted the two-photon absorption spectrum of water-soluble copper indium sulfide (CIS) QDs with stoichiometry 0.18 (Cu), 0.42 (In), and 2 (S) and an average diameter of approximately 2.6 nm. For that, we employed the wavelength-tunable femtosecond Z-scan technique and the parabolic effective-mass approximation model, in which the excitonic transition energies were phenomenologically corrected due to the stoichiometry of the nanocrystal. This model considers a conduction band and three valence sub-bands allowing excitonic transitions via centrosymmetric (Delta l = +/- 1, where l is the angular momentum of the absorbing state) and non-centrosymmetric (Delta l= 0) channels. In such case, this became relevant because the CIS QDs with chalco- pyrite crystalline structure is a non-centrosymmetric semiconductor. Thus, our experimental results pointed out two 2 PA allowed bands located at 715 nm (2hv = 3.47 eV) and 625 run (2hv = 3.97 eV) with cross sections of (6.3 +/- 1.0) x 10(2) GM and (4.5 +/- 0.7) x 10(2) GM, respectively. According to the theoretical model, these 2 PA bands can be ascribed to the 1P(1/2) (h(3))-> 1S(3/2) (e) (lower energy band) and 1P(1/2) (h(heavy)) -> 1S(3)(/2) (e) (90%)/(10%) 1P(1/2)(h(split-off)) -> 1P(3/2) (e) (higher energy band) excitonic transitions. A good agreement (magnitude and spectral position) between the experimental and theoretical data were obtained. However, our experimental data suggest that the higher-energy 2 PA band may have other contributions due to the mixing between the heavy-and the light-hole bands, which the effective mass model does not take into consideration.

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