2007
DOI: 10.1063/1.2775813
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Effects of alloying and localized electronic states on the resonant Raman spectra of Zn1−xMgxO nanocrystals

Abstract: Using resonant Raman spectroscopy, the authors report on the alloying effect and localization of electronic states in Zn1−xMgxO (x<0.15) nanostructures with average sizes in the range of 20–150nm. Anomalous intensity enhancement of the second-order longitudinal optical phonon has been observed, which is due to Fröhlich interaction via the localized exciton as the resonant intermediate electronic states. The alloying-induced disorder due to Mg incorporation led to the enhancement of exciton localization … Show more

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Cited by 42 publications
(38 citation statements)
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“…1(b). This phonon blueshifts with increasing x, in agreement with previous studies, 14,15 Terahertz time-domain spectroscopy 17,18 was utilized to determine the complex magnetoconductivity in the frequency range 100 GHz < ω/2π <2 THz. Samples were placed in the variable-temperature insert of a split-coil superconducting magnet, which applied a magnetic field B along the c-axis.…”
supporting
confidence: 61%
“…1(b). This phonon blueshifts with increasing x, in agreement with previous studies, 14,15 Terahertz time-domain spectroscopy 17,18 was utilized to determine the complex magnetoconductivity in the frequency range 100 GHz < ω/2π <2 THz. Samples were placed in the variable-temperature insert of a split-coil superconducting magnet, which applied a magnetic field B along the c-axis.…”
supporting
confidence: 61%
“…The figure includes also data previously reported in the literature 28, 30 , together with those derived from the analysis of the spectra shown in Fig. 3.…”
Section: Resultsmentioning
confidence: 89%
“…Starts: experimental data from layers series (i). Circles: data reported from references 28, 30 . Full line shows the fitting of the data according to Equation 1. …”
Section: Resultsmentioning
confidence: 99%
“…It is, while, noticeable that these phonon peaks are at higher frequencies than those in the un-doped ZnO as well as weak and broad. These features are often observed in polar alloy semiconductors and have been generally believed to be due to the reduced mass change of oscillating pairs [29]. The ZnO non-polar E 2 modes are mainly excited by the vibration of oxygen atoms (E 2 -high) and Zn atoms (E 2 -low) and in general, as the crystal is alloyed, the phonons can be confined in space, owing to the potential fluctuation by the alloy disorder, which result in the relaxation of the selection rule in Raman scattering [30].…”
Section: Resultsmentioning
confidence: 98%