2006
DOI: 10.1063/1.2360910
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Locating hexagonal and cubic phases in boron nitride using wavelength-selective optically detected x-ray absorption spectroscopy

Abstract: Locating hexagonal and cubic phases in boron nitride using wavelength-selective optically detected x-ray absorption spectroscopy, D.A. Evans, A.R. Vearey-Roberts, N.R.J. Poolton Appl Phys Lett 89, (2006) 161107Cubic and hexagonal phases of boron nitride (c-BN and h-BN) have been identified and located using optically detected x-ray absorption spectroscopy (ODXAS). Each phase was identified by distinct resonance features in the B K-edge absorption spectra. In a mixed-phase sample of predominantly c-BN, combined… Show more

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Cited by 4 publications
(4 citation statements)
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“…The reverse jumps have been observed in the PLY spectra due to the competition between different de-excitation channels and luminescence yields. [9][10][11][12][13] In contrast, the S K-edge PLY is similar to those obtained for TEY and FLY, which is observed in other OLED materials and semiconductor nanostructures. 5,13,14 This observation indicates that the luminescence chromophore is related to sulfur excitation and subsequent energy transfer.…”
Section: Resultssupporting
confidence: 80%
“…The reverse jumps have been observed in the PLY spectra due to the competition between different de-excitation channels and luminescence yields. [9][10][11][12][13] In contrast, the S K-edge PLY is similar to those obtained for TEY and FLY, which is observed in other OLED materials and semiconductor nanostructures. 5,13,14 This observation indicates that the luminescence chromophore is related to sulfur excitation and subsequent energy transfer.…”
Section: Resultssupporting
confidence: 80%
“…The zero order PLY at both edges is inverted with respect to the TEY specifically showing a decrease in luminescence upon reaching the 1s → π* transition, but clearly reflects many of the same spectral features in both instances. This anticorrelation between the PLY and TEY is a well-known phenomenon in optical luminescence yield spectra and has been thoroughly analyzed by Emura et al , Essentially, the negative edge jump seen in the PLY spectrum arises due to competition between different excitation-luminescence channels, each having different luminescence yields. In X-ray absorption below both the C and N K shell thresholds, all the shallow core levels of C, N, and Mg are excited and will participate in producing e−h pairs.…”
Section: Resultsmentioning
confidence: 93%
“…This feature is entirely absent in pure σ -bonded c-BN, and confirms the structural integrity of each material in this study. (Its wider application to BN using wavelength-selectivity is described elsewhere [15].) The crucial point about the technique, however, is that the sample's structural identity is confirmed via the same luminescence yield in which the definitive bandgap measurements are to be extracted, as discussed in the following section.…”
Section: X-ray Excited Luminescence Emission and Excitation (Odxas)mentioning
confidence: 99%
“…(iii) The radiation can be extended into the XUV energy range where the technique of x-ray absorption spectroscopy provides a probe of the local bonding environment (the K -edges of both B and N lie within the energy range 190-450 eV). This is particularly sensitive to sp 2 and sp 3 bonding in BN and the spectra can be recorded using bulk-sensitive luminescence yield [15,16] as well as more conventional surface-sensitive electron yield methods. The advantage of using luminescence excitation, therefore, is that a self-consistent measurement method is available for determining both the sample's chemistry and structure and its band-gap energy.…”
Section: Introductionmentioning
confidence: 99%