The far-infrared spectra of arsenic chalcogenides

1971 ◽  
Vol 24 (4) ◽  
pp. 697 ◽  
Author(s):  
HJ Whitfield

The far-infrared spectra of AsS, As2S3, As4Se3, and As2Se3 are reported for the range 15-400 cm-1. For As4S3 molecules, of symmetry C3v, strong bands at 370 cm-1 and 340 cm-1 arise from symmetric As-S stretching frequencies of symmetry class A1 and a strong band at 176 cm-1 arises from a S-4s-S bending mode of degenerate class E. For As2Se3, bands in the region 90-130 cm-1 are identified as Se-As-Se bending modes and bands between 200 and 280 cm-1 are due to As-Se stretching modes.

1964 ◽  
Vol 42 (10) ◽  
pp. 2201-2208 ◽  
Author(s):  
J. E. Bloor ◽  
J. Schlabitz ◽  
C. C. Walden ◽  
A. Demerdache

The preparation of uranyl phthalocyanine from uranyl chloride and dilithium phthalo-cyanine is described. The infrared and electronic spectra of the complex are quite different from that previously reported for uranyl phthalocyanine and it is suggested that previous workers obtained mainly a mixture of phthalocyanine (PcH2) and inorganic uranyl compounds. The infrared spectra of α- and β-PcH2, β-PcCu, PcLi2, and PcUO2 from 4000 to 300 cm−1; the far infrared spectra of β-PcH2, β-PcCu, and PcUO2 from 300 to 100 cm−1; and the electronic spectrum from 3500 to 10 000 Å of PcUO2 in 1-chloronaphthalene are recorded. A tentative assignment of a band at 278 cm−1 to the O—U—O bending frequency is made. The electronic spectrum of PcUO2 differs from previous spectra of metal phthalocyanines in that it possesses no strong absorption in the 6000–7000 Å region. It does, however, have a strong band at 9145 Å, ε = 4.15 × 104.


1997 ◽  
Vol 50 (6) ◽  
pp. 567 ◽  
Author(s):  
Robert D. Hart ◽  
Graham A. Bowmaker ◽  
Allan H. White

The syntheses of adducts, [(Ph3Sb)3CuX], X = Br, I, NO3, obtained by crystallization of 1 : 3 CuX/SbPh3 mixtures from appropriate solvents are described, together with their room-temperature single-crystal X-ray structure determinations. The bromide, obtained as a chloroform monosolvate from that solvent, is triclinic, P-1, a 13·861(4), b 14·306(4), c 14·347(4) Å, α 84·40(2), β 86·93(2), γ 75·56(2)°, Z = 2 f.u., conventional R on F being 0·053 for No = 4136 independent ‘observed’ (I > 3σ(I)) reflections; this solvate is isomorphous with its previously recorded chloride counterpart. The iodide is triclinic, P-1, a 14·55(1), b 14·385(2), c 23·626(6) Å, α 91·78(1), β 90·77(4), γ 92·54(5)°; Z= 4, R 0·050 for No 6917, and isomorphous with its phosphorus counterpart. The nitrate, although a methanol sesquisolvate, is also isomorphous with the chloride and bromide, a 13·369(9), b 14·398(3), c 14· 504(12) Å, α 82·29(5), β 84·39(6), γ 75·11(4)°, R 0·052 for No 5672. Cu-X are (2·235(5) (Cl)), 2·366(3) (Br), 2· 556(2) ( 2 ) (I), 1·98(1) Å (ONO2), appreciably shorter than in their previously recorded EPh3, E = P, As counterparts. The far-infrared spectra of [(Ph3Sb)3CuX] showed no clear v(CuX) bands, in contrast to the situation reported previously for the corresponding Ph3P and Ph3As compounds. It is likely that v(CuCl) is masked by a strong band at 270 cm-1 due to the Ph3Sb ligand. However, the region below 250 cm-1 in which the v(CuX) bands are expected for the X = Br, I complexes contains no strong ligand bands. Possible reasons for the absence of v(CuX) bands in these complexes are considered.


1987 ◽  
Vol 36 (1) ◽  
pp. 846-849 ◽  
Author(s):  
G. A. Thomas ◽  
H. K. Ng ◽  
A. J. Millis ◽  
R. N. Bhatt ◽  
R. J. Cava ◽  
...  

1973 ◽  
Vol 27 (1) ◽  
pp. 22-26 ◽  
Author(s):  
S. M. Craven ◽  
F. F. Bentley ◽  
D. F. Pensenstadler

The low frequency infrared spectra from 450 to 75 cm−1 of seven oximes and five aldoximes have been recorded for pure samples and for dilute solutions in cyclohexane. An intense characteristic band is present in the solution spectra at 367 ± 10 cm−1. This characteristic band shifts to 275 ± 10 cm−1 in the spectra of the OD compounds. The 367 ± 10 cm−1 and 275 ± 10 cm−1 bands are assigned to OH and OD torsional vibrations. A comparison of the solution spectra with spectra of the solid samples indicated that the OH … N hydrogen bond stretch of oximes and aldoximes occurs in 300 to 200 cm−1 region. Strong bands also are present in 140 to 100 cm−1 region which are due to OH … N bending modes or perhaps lattice vibrations.


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