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dc.contributor.authorNguyen, N. V.pt_BR
dc.contributor.authorSayan, S.pt_BR
dc.contributor.authorLevin, Igorpt_BR
dc.contributor.authorEhrstein, James R.pt_BR
dc.contributor.authorBaumvol, Israel Jacob Rabinpt_BR
dc.contributor.authorDriemeier, Carlos Eduardopt_BR
dc.contributor.authorKrug, Cristianopt_BR
dc.contributor.authorWielunski, Leszek S.pt_BR
dc.contributor.authorHung, Puiyee Y.pt_BR
dc.contributor.authorDiebold, Alainpt_BR
dc.date.accessioned2020-01-22T04:10:23Zpt_BR
dc.date.issued2005pt_BR
dc.identifier.issn0734-2101pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/204762pt_BR
dc.description.abstractWe report the optical properties of unannealed hafnium–aluminate HfAlO films grown by atomic layer chemical vapor deposition ALCVD and correlate them with the aluminum contents in the films. Vacuum ultraviolet spectroscopic ellipsometry VUV-SE , high-resolution transmission electron microscopy HRTEM , channeling Rutherford backscattering spectrometry RBS , and resonant nuclear reaction analysis NRA were employed to characterize these films. In the analyses of ellipsometry data, a double Tauc–Lorentz dispersion produces a best fit to the experimental VUV-SE data. As a result, the determined complex pseudodielectric functions of the films clearly exhibit a dependency on the aluminum densities measured by RBS and NRA. We show that the optical fundamental band gap Eg shifts from 5.56±0.05 eV for HfO2 to 5.92±0.05 eV for HfAlO. The latter was grown by using an equal number of pulses of H2O/HfCl4 and H2O/TMA trimethylaluminum precursors in each deposition cycle for HfO2 and Al2O3, respectively. The shift of Eg to higher photon energies with increasing aluminum content indicates that intermixing of HfO2 and Al2O3 occurred during the ALCVD growth process. We found that Eg varies linearly with the mole fraction x of Al2O3 in the alloy HfO2 x Al2O3 1−x, but has a parabolic dependency with the aluminum density. We also observed a consistent decrease in the magnitudes of the real 1 and imaginary 2 part of of HfAlO films with respect to those of HfO2 as the Al density increased. The absence of the 5.7 eV peak in the spectrum, which was previously reported for polycrystalline HfO2 films, indicates that these films are amorphous as confirmed by their HRTEM images.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofJournal of Vacuum Science & Technology a : Vacuum, Surfaces and Films. New York. Vol. 23, no. 6 (Nov./Dec. 2005), p. 1706-1713pt_BR
dc.rightsOpen Accessen
dc.subjectFísica da matéria condensadapt_BR
dc.subjectEstado amorfopt_BR
dc.subjectFilmes finos dieletricospt_BR
dc.subjectIntervalo proibido de energiapt_BR
dc.subjectConstantes óticaspt_BR
dc.subjectRetroespalhamento rutherfordpt_BR
dc.subjectMicroscopia eletrônica de transmissãopt_BR
dc.subjectEspectros ultravioletapt_BR
dc.titleOptical band gaps and composition dependence of hafnium–aluminate thin films grown by atomic layer chemical vapor depositionpt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000530106pt_BR
dc.type.originEstrangeiropt_BR


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