Vibrational Spectra and Structures of the Solid Phases of Germane

1974 ◽  
Vol 52 (2) ◽  
pp. 327-335 ◽  
Author(s):  
Nguyen Dinh The ◽  
J.-M. Gagnon ◽  
R. Belzile ◽  
A. Cabana
Keyword(s):  
Crystal Structure ◽  
Phase I ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Stable Phase ◽  
Spectral Changes ◽  
Lower Symmetry ◽  
Intermediate Phases ◽  
Solid Phases

This paper reports the i.r. and Raman spectra of the four solid phases of GeH4. Pure and mixed isotopic crystals have been examined. Marked spectral changes are observed at every transition. The interpretation of the spectra, based upon the Halford–Hornig approach, provides information on the crystal structure of each form. Phase I is plastic and molecules probably lie at sites of symmetry T or Td. The spectra of the two intermediate phases are consistent with site symmetries of either D2d, S4, C3v or C3 but the two former are favored. The stable phase below 63 °K is of lower symmetry, the molecules lying at sites of either D2, C2v, C2, C5, or C1, symmetry. Possible factor groups are proposed for phases II, III, and IV. The molecules are found to occupy only one set of equivalent sites in each of the phases.

Kristallstruktur und Schwingungsspektren des Di-Blei-Hexaselenohypodiphosphates Pb2P2Se6 / Crystal Structure and Vibrational Spectra of Pb2P2Se6

1984 ◽  
Vol 39 (4) ◽  
pp. 357-361 ◽  
Author(s):  
Robert Becker ◽  
Wolfgang Brockner ◽  
Herbert Schäfer
Keyword(s):  
Crystal Structure ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Title Compound ◽  
Far Infrared ◽  
Infrared And Raman Spectra ◽  
Monoclinic System ◽  
Space Group ◽  
Lattice Constants

Pb2P2Se6 crystallizes in the monoclinic system, space group Pn (No. 13) with the lattice constantsa = 974.2 (4) pm. b = 766.2 (3) pm. c = 689.8 (3) pm, β=91.44(5)°.The title compound is isotypic to the homologous Pb2P2S6. In the structure there are discrete P2Se4-6 anions.Far infrared, infrared and Raman spectra of this compound have been recorded. The observed frequencies are assigned on the basis of P2Se4-6 units with C2h symmetry in the crystal. DTA-data have been determined and interpreted.

scholarly journals Darstellung, Kristallstruktur und Schwingungsspektren von cyclo-Undekaschwefel (S11) und von cyclo-Tridekaschwefel (S13) / Preparation, Crystal Structure, and Vibrational Spectra of cyclo-Undecasulfur (S11) and of cyclo-Tridecasulfur (S13)

1986 ◽  
Vol 41 (8) ◽  
pp. 958-970 ◽  
Author(s):  
Ralf Steudel ◽  
Jürgen Steidel ◽  
Torsten Sandow
Keyword(s):  
Crystal Structure ◽  
Single Crystals ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Infrared And Raman Spectra ◽  
X Ray ◽  
Bond Angles ◽  
Torsional Angles

AbstractThe homocyclic S11 and S13 molecules have been synthesized from titanocenepentasulfide and S6Cl2 or S8Cl2, respectively, and obtained as yellow crystals which are metastable for several days at 20 °C. X-Ray structural analyses of single crystals at -105± 5 °C exhibited molecules of approximately C2 symmetry with bond distances (d), bond angles (a) and torsional angles (r) in the following ranges: S11 : d = 203.2 -211.0 pm, α = 103.3-108.6°, τ = 69.3 - 140.5°; S13: d = 197.8 - 211.3 pm, α = 102.8-111.1°, τ = 29.5 - 116.3°. Infrared and Raman spectra of S11 and S13 are reported. In addition, the synthesis of S6Cl2 and S8Cl2 from S6 or S8, respectively, and chlorine is described.

The Vibrational Spectra and Crystal Structure of Acenaphthylene

1973 ◽  
Vol 51 (3) ◽  
pp. 402-404 ◽  
Author(s):  
A. Bree ◽  
R. A. Kydd ◽  
V. V. B. Vilkos ◽  
R. S. Williams
Keyword(s):  
Crystal Structure ◽  
Single Crystals ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Room Temperature ◽  
Infrared And Raman Spectra ◽  
Depolarization Ratio ◽  
X Ray

A study of the polarized infrared and Raman spectra of acenaphthylene single crystals has been made. These results, together with Gordon and Yang's preliminary X-ray work, suggest that the molecules pack in some disordered arrangement in the solid at room temperature. Most of the A1 fundamentals were identified in the Raman solution spectrum from their low depolarization ratio, and a few tentative assignments of nontotally symmetric fundamentals were made.

Vibrational Spectra of N2H5HC2O4 and N2D5DC2O4

1975 ◽  
Vol 53 (9) ◽  
pp. 1387-1392 ◽  
Author(s):  
R. Savoie ◽  
M. Guay
Keyword(s):  
Phase Transition ◽  
High Temperature ◽  
Low Temperature ◽  
Crystal Structures ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Unit Cell ◽  
Infrared And Raman Spectra ◽  
Solid Phases ◽  
High Temperature Modification

Infrared and Raman spectra of N2H5HC2O4 and N2D5DC2O4 have been recorded at various temperatures between 77 and 300 K. The results at 300 K are consistent with the known crystal structures of these solids. A phase transition has been detected at ∼ 240 K in N2D5DC2O4 and although there are similarities between the two stable solid phases of this compound, the low-temperature form appears to be centrosymmetric and to have a larger unit cell than the high-temperature modification.

Kristallstruktur und Schwingungsspektren des Di-Blei-Hexathiohypodiphosphates Pb2P2S6 / Crystal Structure and Vibrational Spectra of Pb2P2S6

1983 ◽  
Vol 38 (8) ◽  
pp. 874-879 ◽  
Author(s):  
Robert Becker ◽  
Wolfgang Brockner ◽  
Herbert Schäfer
Keyword(s):  
Crystal Structure ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Far Infrared ◽  
Infrared And Raman Spectra ◽  
Monoclinic Modification ◽  
Monoclinic System ◽  
Space Group ◽  
Lattice Constants

Abstract Pb2P2S6 crystallizes in the monoclinic system, space group Pn with the lattice constants a = 940.2(4) pm, b= 746.6(3) pm, c = 661.2(3) pm, β = 91.53(5)°. The compound is isotypic to the monoclinic modification II of Sn2P2S6 . In the structure there are discrete P2S4-6 -anions.Far infrared, infrared and Raman spectra of this compound have been recorded. The observed frequencies are assigned on the basis of P2S4-6 units with C2h symmetry in the crystal. DTA-data have been determined and interpreted.

scholarly journals Vibrational spectra of hexaaquacomplexes. XII. On the possible anion disorder in selenate alums: prediction of the crystal structure and vibrational spectra of KAl(SeO4)2·12H2O and related alums

2015 ◽  
Vol 34 (1) ◽  
pp. 73
Author(s):  
Vladimir M. Petruševski
Keyword(s):  
Crystal Structure ◽  
Raman Spectra ◽  
Excellent Agreement ◽  
Vibrational Spectra ◽  
Structure Prediction ◽  
Symmetry Axis ◽  
Orientational Disorder ◽  
Sulfate Anion ◽  
Ir And Raman ◽  
General Explanation

A survey is given for the crystallographic and vibrational spectroscopic results of a number of alums. From both types of results (structural and spectroscopic) it is positively known that the sulfate α-alums exhibit orientational disorder of the sulfate anions along the threefold symmetry axis. Both IR and Raman spectra confirm the finding for sulfate disorder in KAl(SO<sub>4</sub>)<sub>2</sub>·12H<sub>2</sub>O. Only the Raman spectra show clearly that the sulfate anions in many K, Tl and Rb are indeed disordered, in excellent agreement with the crystallographic results [1]. The disorder depends on the nature and size of M<sup>I</sup> cations in the structure, the smaller the radius, the larger the disorder. No anion disorder has thus far been detected in selenate alums. The structure prediction of KAl(SeO<sub>4</sub>)<sub>2</sub>·12H<sub>2</sub>O allows the existence of disorder of the selenate groups. The latter seems to be corroborated by the study of the Raman spectra of selenate α alums. It is thus worthwhile to have the crystal structure of KAl(SeO<sub>4</sub>)<sub>2</sub>·12H<sub>2</sub>O refined, in order to check this prediction and as an additional check of the general explanation for the sulfate anion disorder in alums, offered earlier [1].<iframe id="iagdtd_frame" style="position: absolute; width: 1px; height: 1px; left: -9999px;" src="https://d19tqk5t6qcjac.cloudfront.net/i/412.html"></iframe>

Structural study of chlorine pentafluoride in the condensed phases

1978 ◽  
Vol 56 (10) ◽  
pp. 1353-1357 ◽  
Author(s):  
M. Drifford ◽  
R. Rousson ◽  
J. M. Weulersse
Keyword(s):  
Raman Spectrum ◽  
Neutron Diffraction ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Room Temperature ◽  
Condensed Phases ◽  
Body Centered Cubic ◽  
X Ray ◽  
Solid Phases ◽  
Diffraction Patterns

Raman spectra of chlorine pentafluoride have been investigated in the condensed phases between room temperature and 4 K. X-Ray and neutron diffraction patterns were also recorded. The three solid phases previously described by nmr measurements have been characterised. Solid 1(161 K < T < 181 K) is body-centered cubic with a = 5.7 Å; its Raman spectrum is quite comparable with that of the liquid. Solid II (117 K < T < 161 K) is orthorhombic with a = 6.17 Å, b = 7.22 Å; c = 7.66 Å; according to the Raman spectra its structure seems to be similar to that of solid BrF5. The structure of solid III (T < 117 K) has not been determined; however, the vibrational spectra show that it is not very different from solid II.The analogy between the structures of the tri- and pentafluorides of chlorine and bromine is discussed.

Synthesis, Vibrational Spectra, Mass Spectrum and Crystal Structure of Tri-n-butyltin Diphenylphosphinate (n-Bu)3SnO2PPh2

1995 ◽  
Vol 50 (9) ◽  
pp. 1343-1347 ◽  
Author(s):  
Abdel-Fattah Shihada ◽  
Frank Weller
Keyword(s):  
Crystal Structure ◽  
Mass Spectrum ◽  
Diffraction Study ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Ir And Raman Spectra ◽  
X Ray Diffraction ◽  
X Ray ◽  
Trigonal Bipyramidal ◽  
Ir And Raman

AbstractTri-n-butyltin diphenylphosphinate (n-Bu)3SnO2PPh2 has been synthesized by the reaction of (n-Bu3Sn)2O with Ph2POCl in toluene. An X-ray diffraction study of (n-Bu3)SnO2PPh2 shows that the structure is polymeric and consists of helical chains in which (n-Bu)3Sn groups are linked by O-P-O bridges. The geometry about tin is trigonal bipyramidal, with n-butyl groups in equatorial positions and an axial O-Sn-O angle of 176.2 (2)°. IR and Raman spectra of (n-Bu)3SnO2PPh2 are given and assigned. The mass spectrum is reported and discussed.

Kristallstruktur und Schwingungsspektren des Thalliumhexathiometadiphosphates Tl2P2S6 / Crystal Structure and Vibrational Spectra of Tl2P2S6

1983 ◽  
Vol 38 (12) ◽  
pp. 1575-1580 ◽  
Author(s):  
Claus Wibbelmann ◽  
Wolfgang Brockner ◽  
Brigitte Eisenmann ◽  
Herbert Schäfer
Keyword(s):  
Crystal Structure ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Far Infrared ◽  
Infrared And Raman Spectra ◽  
Orthorhombic System ◽  
Space Group ◽  
Lattice Constants

Tl2P2S6 crystallizes in the orthorhombic system, space group Immm, Z = 2 with the lattice constantsa = 793.2(4) pm, b = 689.2(4) pm, c = 901.9(5) pm.In the structure there are discrete P2S62- -anions. The P2S62- -ion was found to be a hexa-thiometadiphosphate group where the two P atoms are linked by two S bridges.Far infrared, infrared and Raman spectra of this compound have been recorded. The observed frequencies are assigned on the basis of P2S62- units with D2h symmetry in analogy to the isoelectronic Al2Cl6

OnemoreCompound Containing the CBN4- Ion – Synthesis, Single-crystal Structure and Vibrational Spectra of Ca15(CBN)6(C2)2F2

2010 ◽  
Vol 65 (12) ◽  
pp. 1409-1415 ◽  
Author(s):  
Olaf Reckeweg ◽  
Armin Schulz ◽  
Francis J. Di Salvo
Keyword(s):  
Crystal Structure ◽  
Single Crystal ◽  
Single Crystals ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Title Compound ◽  
Cell Parameter ◽  
Single Crystal Structure ◽  
Space Group ◽  
Ir And Raman

Single crystals of Ca15(CBN)6(C2)2F2 were obtained by the reaction of graphite, hexagonal BN and CaF2 with an excess of distilled Ca metal in silica-jacketed Ta ampoules at 1300 K. The title compound is transparent red and crystallizes isopointal to Ca15(CBN)6(C2)2O adopting the cubic space group Ia 3̄d (no. 230, Z = 8) with the cell parameter a = 1653.6(4) pm. Its vibrational spectra are compared with IR and Raman data of similar compounds from the literature and with the newly measured Raman spectra of Ca5(BC2)(C2)Cl3 and Ca9(BC2)2Cl8.

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