2013
DOI: 10.1016/j.vibspec.2013.05.004
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Vibrational spectra and factor group analysis of rare-earth chromium borates, RCr3(BO3)4, with R=La–Ho

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Cited by 38 publications
(22 citation statements)
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“…According to a factor‐group analysis the vibrations of B‐O bond in the rare earth orthoborates with the general formula RM 3 (BO 3 ) 4 (R ‐ Nd, Ga, Y; M ‐ Al, Ga, Cr, Fe), which crystallize in rhombohedral and in monoclinic structures, main frequencies of the vibrations of this bond located in a region 1400–570 cm −1 . Hence, bands in the region from 1400 to 1100 cm −1 due to asymmetrical stretching vibrations, 1060–960 cm −1 due to symmetrical stretching vibrations of the B‐O boron triangles, and bands in the range 820 – 570 cm −1 due symmetric and asymmetric deformations of vibration of B‐O bond in the boron triangles.…”
Section: Resultsmentioning
confidence: 99%
“…According to a factor‐group analysis the vibrations of B‐O bond in the rare earth orthoborates with the general formula RM 3 (BO 3 ) 4 (R ‐ Nd, Ga, Y; M ‐ Al, Ga, Cr, Fe), which crystallize in rhombohedral and in monoclinic structures, main frequencies of the vibrations of this bond located in a region 1400–570 cm −1 . Hence, bands in the region from 1400 to 1100 cm −1 due to asymmetrical stretching vibrations, 1060–960 cm −1 due to symmetrical stretching vibrations of the B‐O boron triangles, and bands in the range 820 – 570 cm −1 due symmetric and asymmetric deformations of vibration of B‐O bond in the boron triangles.…”
Section: Resultsmentioning
confidence: 99%
“…In the overwhelming number of cases, the crystal structures (first of all, coordinates of atoms) of the samples were refined by the full-profile Rietveld method on polycrystalline samples obtained by the solid-state reaction (LnFe 3 (BO 3 ) 4 with the Ln = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, (Y), Ho; LnGa 3 (BO 3 ) 4 with the Ln = Sm, Gd, Y, Ho, Er) [34,53] or on single crystals synthesized by the flux method and ground to a powder (LnAl 3 (BO 3 ) 4 with the Ln = Nd, Sm, Eu, Gd, Tb, Dy, (Y), Ho, Er, Yb; LnFe 3 (BO 3 ) 4 with the Ln = Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, (Y), Ho; LnGa 3 (BO 3 ) 4 with the Ln = Gd) [1,54,56,59,61,66,68]. Assignment of a series of rare-earth orthoborates (LnAl 3 (BO 3 ) 4 with the Ln = Nd, Eu, Gd, Tb, Dy, (Y), Ho, Er, Tm, Yb; LnFe 3 (BO 3 ) 4 with the Ln = Eu, Gd, Y; LnCr 3 (BO 3 ) 4 with the Ln = Sm, Eu, Gd, Tb, Dy; LnGa 3 (BO 3 ) 4 with the Ln = Nd, Eu, Gd, (Y), Ho) to the space group R32 is performed on powdered single crystals obtained by the flux method using IR spectroscopy coupled with the group-theoretical analysis [26,42,45,51,70,71,73], temperature-dependent high-resolution optical absorption Fourier spectroscopy and Raman spectroscopy (LnFe 3 (BO 3 ) 4 with the Ln = Pr, Nd) [57,58,60].…”
Section: Methodsmentioning
confidence: 99%
“…IR/S, T s = 143 K [65] R32: D/P [1], D/? [27], IR/S (50:50, 900-950 • C; 70:30, 1040-1050 • C) [70], IR/S (1:1; 1.5:1; 2.3:1) [71], IR/S [26,45] R32: D/? [27], D/P [34,54], IR/P [45] R32: ?…”
Section: Space Groups For Thementioning
confidence: 99%
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“…Порядковый номер Согласно результатам фактор-группового анализа колебаний связи В-О в редкоземельных ортоборатах с общей формулой RM 3 (BO 3 ) 4 (R -Nd, Ga, Y; M -Al, Ga, Cr, Fe), кристаллизующихся как в ромбоэдрической, так и в моноклинной структурах, основные частоты колебаний этой связи расположены в области волновых чисел 1400-570 см -1 [15][16][17]. Следуя выводам этих работ, мы можем отнести полосы в области от 1400 до 1100 см -1 к валентным асимметричным колебаниям, полосы в области 1060-960 см -1 -к валентным симметричным колебаниям связи В-О борных треугольников, а полосы в области спектра 820 -570 см -1 -к деформационным симметричным и асимметричным колебаниям связи В-О борных треугольников.…”
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