2011
DOI: 10.1103/physrevb.83.201201
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Compositional evolution of Bi-induced acceptor states in GaAs1xBixalloy

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Cited by 33 publications
(31 citation statements)
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“…7, Bi-induced perturbations in the physical constants of the semiconductor must be con-sidered. Though the optical constants of GaAsBi are not well known, there are good estimates for changes in complex dielectric function and absorption coefficient [29,30]; the band bending may be estimated assuming Fermi pinning at the Bi-induced acceptor states [11]. However, including these factors increases the spectroscopic estimation of p by only a factor of 2 to 4, rather than orders of magnitude.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…7, Bi-induced perturbations in the physical constants of the semiconductor must be con-sidered. Though the optical constants of GaAsBi are not well known, there are good estimates for changes in complex dielectric function and absorption coefficient [29,30]; the band bending may be estimated assuming Fermi pinning at the Bi-induced acceptor states [11]. However, including these factors increases the spectroscopic estimation of p by only a factor of 2 to 4, rather than orders of magnitude.…”
Section: Resultsmentioning
confidence: 99%
“…These attractive properties are mainly related to the large disparity in atomic size and electronegativity between Bi and As, and to the relativistic corrections induced by the bismuth. Recently, Nargelas et al [10] showed alloying nominally undoped GaAs with group V Bi counterintuitively introduces p-type carriers: holes thermally excited from Bi-induced acceptor levels lying 26.8 meV above the valence band edge [11]. Pettinari et al [12] revealed -through electrical transport measurements -that the hole concentration rises with x up to p = 2.4 × 10 17 cm −3 at x = 10.6%.…”
Section: Introductionmentioning
confidence: 99%
“…The lifetime broadened line width is 0.008 meV (refs 30,31). The signal dependence on magnetic flux density B was determined with a 33 T (0.33 MG) water-cooled Bitter magnet, with the field axis, the light propagation direction and the normal to the sample plane all parallel, that is, the Faraday geometry 23 . For polarized experiments, a wire grid polarizer and an x-cut quartz quarter wave plate were mounted with optical axes at 45°to each other directly on top of the sample.…”
Section: Methodsmentioning
confidence: 99%
“…Given the above questions, and the renewed interest in the high-field regime, it is crucial to validate experimentally the theory for the absorption spectra on which the inferred fields are based. Doing so directly for hydrogen is impractical because the required fields are two to three orders of magnitude beyond what is currently available in any laboratory 22,23 . Such tests become even more essential where atomic species beyond hydrogen are being considered, for example, helium [10][11][12] or molecular hydrogen [24][25][26][27] as for these cases the multiple particle calculations required are complex and involve approximations (for example, basis-state choices and sizes) that are not a priori guaranteed.…”
mentioning
confidence: 99%
“…[3][4][5] In general, incorporating Bi is very challenging due to the large differences in the Group V atomic radii (Bi is 31% larger than As) and electronegativities (Bi is 9% smaller than As). 3,6 Recent studies indicate that Bi forms acceptor levels 7 introducing holes in nominally undoped GaAs 1−y Bi y . 8 Herein we report on two GaAs 1−y Bi y Raman signatures which can be used to determine the Bi composition (y) and predict 300K photoluminescence intensity.…”
mentioning
confidence: 99%