2013
DOI: 10.1063/1.4824279
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Extended X-ray absorption fine structure spectroscopy of selenium-hyperdoped silicon

Abstract: Silicon doped with an atomic percent of chalcogens exhibits strong, uniform sub-bandgap optical absorptance and is of interest for photovoltaic and infrared detector applications. This sub-bandgap absorptance is reduced with subsequent thermal annealing indicative of a diffusion mediated chemical change. However, the precise atomistic origin of absorptance and its deactivation is unclear. Herein, we apply Se K-edge extended X-ray absorption fine structure (EXAFS) spectroscopy to probe the chemical states of se… Show more

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Cited by 29 publications
(27 citation statements)
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“…Some groups have thoroughly investigated Si supersaturated with S or Se prepared by laser irradiation in SF 6 atmosphere or by ion implantation and subsequently pulsed laser melted (PLM). [8][9][10][11][12] An extended infrared photoresponse with high gain levels has been shown. 13,14 In previous works, we have deeply investigated Si supersaturated with Ti 15 or V, 16 and we reported the first solar cell device based on Ti supersaturated Si.…”
Section: 2mentioning
confidence: 99%
“…Some groups have thoroughly investigated Si supersaturated with S or Se prepared by laser irradiation in SF 6 atmosphere or by ion implantation and subsequently pulsed laser melted (PLM). [8][9][10][11][12] An extended infrared photoresponse with high gain levels has been shown. 13,14 In previous works, we have deeply investigated Si supersaturated with Ti 15 or V, 16 and we reported the first solar cell device based on Ti supersaturated Si.…”
Section: 2mentioning
confidence: 99%
“…For each doping concentration, we substituted one silicon atom with a Se impurity and relaxed the atomic positions (so that atomic forces are <0.01 eV/Å) and supercell lattice vectors (so that all stress tensor components are <2 kbar). We chose the substitutional Se configuration, as our electronic structure calculations 23 as well as others 24 indicate the substitutional site to be the minimum energy defect configuration. The QMC results presented here are computed via fixed node diffusion Monte Carlo conducted with the QWalk code 25 , with trial wave functions constructed with a Slater-Jastrow form using SIESTA's DFT orbitals, variance-minimized Jastrow coefficients, and a time step of 0.01 au.…”
mentioning
confidence: 99%
“…The QMC energies are computed by averaging over twisted boundary conditions for all supercells. Defect formation energies for both DFT and QMC were computed using ∆E f = (E Se1:Sin + µ Si ) − (E Sin+1 + µ Se ), wherein each atom's chemical potential µ is determined by the quasiequilibrium of the doped silicon with SiSe 2 chains, which may be present as early stage precipitates 23 .…”
mentioning
confidence: 99%
“…The first large peak in the spectrum is indicative of the scattering signal from the first nearest neighbor (1NN) shell of atoms. 22 It can also be noted that the amplitudes of |v(R)| from higher-order shells (R > 2 Å ) for all other spectra are strongly attenuated, except for the spectrum collected at Zn K-edge for sample Z1T0 (pure ZnO). This suggests that the higher-order shells around the Zn atoms are well-ordered in the pure ZnO sample, verifying its crystalline nature.…”
mentioning
confidence: 99%
“…The energy scale is calibrated by using the absorption edge of reference metallic Zn or Sn thin films measured simultaneously and the XANES and EXAFS are isolated by normalizing the absorption spectrum and subtracting the smooth atomic background absorption signal from the measured absorption signal using the AUTOBK algorithm in Athena with R bkg ¼ 1.0 Å . 21,22 After the background removal, the processed data are transformed from energy space to k-space using the relationship,…”
mentioning
confidence: 99%