ETS-10 crystals with the average size (Lave) of 35, 14, 6, and 2 μm were synthesized hydrothermally at 473 K [2, 3]. Raman spectra of these crystals showed all the bands characteristic for ETS-10 [4, 5]. However, the full width at half maximum (FWHM) and the position of the most intense Raman band that was assigned to the symmetric Ti – O stretching vibrations in the …Ti–O–Ti–O–Ti… chains varied from sample to sample. The FWHM of this band increased from 19-21 cm-1 for the larger (Lave≥14 µm) crystals to 38-39 cm-1 for the smaller (Lave≤6 µm) crystals. In addition, the band position shifted to higher frequency, i.e., from 725 cm-1 for the crystals with Lave≥14 µm to 733 cm-1 for the crystals with Lave≤6 µm. The band broadening and shift to higher frequency observed for the smaller crystals suggest more stacking defects in these crystals (i.e., wider length distribution of the …Ti–O–Ti–O–Ti… chains). Diffuse reflectance UV-vis spectroscopic analysis showed that the absorption edge of the spectra for the larger ETS-10 crystals appeared progressively more red-shifted from the spectra of the smallest ETS-10 crystals. This red shift may be attributed to the fewer defects present along the …Ti–O–Ti–O–Ti… chains in the larger ETS-10 crystals. Consistent with Raman spectroscopic analysis, this result suggests increased average length of the …Ti–O–Ti–O–Ti… chains embedded in increasingly larger ETS-10 crystals.
[1] C. Lamberti, Micropor. Mesopor. Mater., 30 (1999) 155.
[2] Z. Ji, J. Warzywoda, A. Sacco Jr., Micropor. Mesopor. Mater., 81 (2005) 1.
[3] Z. Ji, J. Warzywoda, A. Sacco Jr., Micropor. Mesopor. Mater., 109 (2008) 1.
[4] N. C. Jeong, M. H. Lee and K. B. Yoon, Angew. Chem., Int. Ed., 46 (2007) 5868.
[5] P.D. Southon and R.F. Howe, Chem. Mater., 14 (2002) 4209.