2021
DOI: 10.1016/j.jcrysgro.2021.126218
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Epitaxial growth of rhombohedral β- and cubic γ-CuI

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Cited by 6 publications
(9 citation statements)
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“…The near‐band‐edge optical emission properties of differently prepared Ag x Cu 1 x I layers were investigated by means of PL spectroscopy at 2 K. The corresponding PL spectra are shown for alloy compositions 0 x 1 in Figure 4b. For binary CuI, the observed emission profile is comparable with our previous results [ 18 ] on thin films, which were grown at similar conditions. The emission lines at 3.065 eV and 3.055 eV can be assigned to free exciton–polariton emission from upper (UPB) and lower (LPB) polariton branches, respectively.…”
Section: Resultssupporting
confidence: 90%
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“…The near‐band‐edge optical emission properties of differently prepared Ag x Cu 1 x I layers were investigated by means of PL spectroscopy at 2 K. The corresponding PL spectra are shown for alloy compositions 0 x 1 in Figure 4b. For binary CuI, the observed emission profile is comparable with our previous results [ 18 ] on thin films, which were grown at similar conditions. The emission lines at 3.065 eV and 3.055 eV can be assigned to free exciton–polariton emission from upper (UPB) and lower (LPB) polariton branches, respectively.…”
Section: Resultssupporting
confidence: 90%
“…The values for the mobility are in the range from 12 to 15 cm 2 V −1 s −1 , which is characteristic for γ ‐CuI. [ 18,22 ] With increasing Ag content we observe a strong increase in resistivity of around three orders of magnitude from CuI to AgI. However, due to the surface morphology of especially Ag‐rich Ag x Cu 1 x I layers, no clear statement can be made about the charge carrier density and mobility as a function of the alloy composition.…”
Section: Resultsmentioning
confidence: 98%
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“…Additionally, the halide semiconductor copper iodide (CuI) also attracted research interest, since it features a large and direct band gap ( E g = 3.1 eV) combined with high charge carrier densities up to p ≈ 10 20 cm –3 and hole mobilities up to μ = 44 cm 2 /(V s), resulting in highly conductive films while retaining a high transparency. Further, the high excitonic binding energy ( E x b = 58 meV) renders it promising for various optoelectronic applications. At standard conditions, CuI usually crystallizes solely in the zinc-blende γ-phase with a complex phase diagram at high temperatures and pressures. , However, recently, an orthorhombic β-phase of CuI, previously attributed to be a high-temperature structure, stabilized at room temperature in conjunction with the γ-phase utilizing a close distance sublimation technique …”
Section: Introductionmentioning
confidence: 99%