Vibrations moléculaires du nitrate de di-μ-hydroxo-bis(diammine) platine (II) [(NH3)2Pt(OH)2Pt(NH3)2](NO3)2. Partie 2: analyse en coordonnées normales

1982 ◽  
Vol 60 (17) ◽  
pp. 2222-2228 ◽  
Author(s):  
Alain J. P. Alix ◽  
Michel Manfait ◽  
Odile Krug ◽  
Théophile Theophanides

A full normal coordinate analysis of the skeleton [N2′ Pt O2′ Pt N2′] of the di-μ-hydroxo-bis(diammine) platinum(II) nitrate has been performed according to the Point Mass Model approximation and assuming a D2h molecular symmetry.The method of construction of a set of 18 independent symmetry valence coordinates was based on the theory of molecular vibrations in dependent rectilinear coordinates. A refined general valence force field which reproduces satisfactorily the frequencies of the molecule and its deuterated analog has been obtained. Calculations of all distributions of vibrational energy allow us to descry ibe all normal modes of vibration and especially the ones related to the square planar ring modes (Pt2O2) showing evidence of strong couplings.In addition we have calculated independently some fragments of the whole dimeric complex, which may be used for comparison with related compounds.

1992 ◽  
Vol 291 ◽  
Author(s):  
Charles C. Kim ◽  
M. I. Bell ◽  
D. A. McKeown

ABSTRACTThe normal modes of vibration and their frequencies are calculated for benitoite, a mineral whose crystal structure (space group D23h) consists of three-membered silicate rings (Si3O9) linked by Ba+2 and Ti+4 ions. The calculation unambiguously assigns the normal modes to the lines in the Raman and infrared spectra and determines the atomic interactions. On the assumption that mode mixings and splittings due to inter-ring interactions are small, the normal frequencies of the isolated ring of C3h, symmetry are determined. The identification of normal modes characteristic of three-membered silicate rings may prove to be a valuable guide in the interpretation of the infrared and Raman spectra of amorphous silicates, potentially leading to new information on the ring statistics of these materials.


1996 ◽  
Vol 51 (10) ◽  
pp. 1400-1406 ◽  
Author(s):  
D. Rickert ◽  
W. Preetz

The crystal structures of trans-[PtCl2(acac)2](monoclinic, space group P21/c, a - 7.616(5), b = 12.759(5), c = 7.892(5) Å, β = 118.459(5)°, Z = 2), trans-[PtBr2(acac)2] (triclinic, space group P1̅, a = 7.502(5), b = 7.665(5), c = 8.155(5) Å, α = 114~508(5), β = 94.537(5), γ = 117.669(5)°. Z = 1) and trans-[Pt(SCN)2(acac)2] (triclinic, space group P1̅ , a = 7.9095(10), b = 7.9393( 10), c = 7.9631 Å, a = 114.051 (10), β = 100.955(10), γ = 100.573(10)°, Z = 1) have been determined by single crystal X-ray diffraction analysis. The crystal structure of trans- [Ptl2(acac)2] is known from the literature. To enhance the spectroscopic resolution, the IR and Raman spectra of the four complexes have been measured at low temperature (10 K). Using the X-ray data, normal coordinate analyses based on a modified valence force field have been performed and the normal modes of vibration for the octahedral skeleton [PtX2O4] have been assigned. With a set of 19 or 23 force constants taking into account the inner-ligand vibrations a good agreement between observed and calculated frequencies has been achieved. The valence force constants are e.g.fd (PtCl) = 2.16, fd (PtBr) = 1.45, fd (PtI) = 1.01, fd (PtS) = 1.80 mdyn/Å, and fd (PtO) ranges from 1.89 to 1.91 mdyn/Å.


1997 ◽  
Vol 52 (3) ◽  
pp. 315-322 ◽  
Author(s):  
W. Preetz ◽  
A. Krull

Abstract The crystal structures of [(C5H5N)2CH2][OsCl4(ox)] (monoclinic, space group I2/m, a = 10.260(5), b = 13.841(5), c = 12.273(5) Å, β = 92.050(5)°, Z = 4), [(C5H5N)2CH2][OsBr4(ox)]·H2O(monoclinic, space group P21/n, a = 11.666(3),b = 11.591(5), c = 14.926(2) Å, β = 102.45(2)°, Z = 4) and [P(C6H5)4]2 [OsI4(ox)]·2CH2Cl2 (triclinic, space group P1̄, a = 14.597(2), b = 11.9185(9), c = 22.5624(14) Å, α = 80.284(8), β = 78.903(8), γ = 69.432(8)°, Z = 2) have been determined by single crystal X-ray diffraction analysis. The IR and Raman spectra of the three complexes were measured at room temperature. Using the molecular parameters of the X-ray determinations normal coordinate analyses based on a modified valence force field have been performed and the normal modes of vibration are assigned. With a set of 25 force constants and taking into account the innerligand vibrations a good agreement between observed and calculated frequencies has been achieved. The valence force constants of the X-Os-X axis are fd(OsCl) = 1.77, fd(OsBr) = 1.48, fd(OsI) = 1.0 mdyn/Å, of the X′-Os-O• axes are fd(OsCl′) = 1.88, fd(OsBr′) = 1.6, fd(OsI′) =1.1 mdyn/Å and fd(OsO•) ranges from 2.7 to 2.8 mdyn/Å.


1997 ◽  
Vol 52 (8) ◽  
pp. 965-974 ◽  
Author(s):  
K Dallmann ◽  
W Preetz

The crystal structures of trans-[OsCl2(acac)2] (triclinic, space group P1̄, a = 7.4114(5), b = 7.6419(9), c = 7.9944(6) Å, α = 62.692(7), β = 87.687(6), γ = 60.667(6)°, Z = 1), trans-[OsBr2(acac)2] (triclinic, space group P1̄, a = 7.467(3), b = 7.621(3), c = 8.260(3) Å, α = 115.03(3), β = 92.78(3), γ = 117.91(3)°, Z = 1), cis-[OsCl2(acac)2] (monoclinic, space group C2/c, a = 13.8532(13), b = 7.7990(8), c = 13.6202(12) Å, β = 108.375(10)°, Z = 4) and cis-[OsBr2(acac)2] (monoclinic, space group C2/c, a = 13.944(2), b = 8.0347(13), c = 13.743(2) Å, β = 106.757(12)°, Z = 4) have been determined by single crystal X-ray diffraction analysis. To enhance the spectroscopic resolution, the IR and Raman spectra of the six complexes have been measured at low temperature (10 K). Using the molecular parameters of the X-ray determinations normal coordinate analyses based on a modified valence force field have been performed for trans-[OsCl2(acac)2], trans-[OsBr2(acac)2] and cis-[OsCl2(acac)2], and the normal modes of vibration assigned. With sets of 31 or 32 force constants, taking into account the innerligand vibrations, a good agreement between observed and calculated frequencies has been achieved. The valence force constants for the X-Os-X axes are fd(OsCl) = 1.81, fd(OsBr) =1.61 mdyn/Å, and for the Cl′-Os-O* axis are fd(OsCl’) = 1.94, fd(OsO*) = 2.81 mdyn/Å and fd(OsO) ranges from 3.27 to 3.31 mdyn/Å.


1998 ◽  
Vol 53 (2) ◽  
pp. 232-238 ◽  
Author(s):  
K. Dallmann ◽  
W. Preetz

Abstract In the reaction of K2[OsCl6] with boiling water/acetylacetone (1:1) a mixture of different chloro-acetylacetonato complexes is formed, from which [Os(acac)3] can be isolated by column chromatography with dichloromethane on silica gel. The crystal structure of [Os(acac)3] (mo­noclinic, space group P21/c,a = 13.968(5), b = 7.517(5), c = 16.455(5) Å ,β = 98.939(5)°, Z = 4) has been determined by single crystal X-ray diffraction analysis. High resolution IR and Raman spectra were measured at low temperature (10K). Based on the molecular parameters of the X-ray structure determination a normal coordinate analysis has been performed and the normal modes of vibration have been assigned. With a set of 32 force constants, taking into account the intraligand vibrations, a good agreement between observed and calculated frequencies has been achieved. The valence force constants are fd(OsO) = 3.19 and fd(OC) = 6.74 mdyn/Å.


1972 ◽  
Vol 50 (16) ◽  
pp. 2691-2696 ◽  
Author(s):  
H. F. Shurvell ◽  
M. R. Gold ◽  
A. R. Norris

The infrared and laser–Raman spectra of liquid dimethyliodoarsine, (CH3)2AsI, have been recorded. Assignments of the observed frequencies have been made to the 24 normal modes of vibration of the molecule. A normal coordinate calculation has been carried out in support of the assignment.


1998 ◽  
Vol 53 (1) ◽  
pp. 93-100 ◽  
Author(s):  
W. Preetz ◽  
J.-G. Uttecht

By reaction of (n-Bu4N)2[Pt(ox)2] with elemental halogens in dichloromethane the complexes trans-[PtX2(ox)2]2- (X = Cl, Br, I) are formed. The crystal structures of trans-(py2CH2)[PtCl2(ox)2] · C4H6O3 (1) (monoclinic, space group P21/n, a = 12.119(3), b = 14.926(2), c = 12.666(4) Å, β = 91.26(3)°, Z = 4), trans-(py2CH2)[PtBr2(ox)2] (2) (monoclinic, space group P21/n, a = 7.402(8), b = 16.997(3), c = 14.898(3) Å, β = 98.15(3)°, Z = 4) and trans-(py2CH2)[PtI2(ox)2] ·C3H7NO (3) (orthorhombic, space group Pnma, a = 10.380(9), b = 13.973(2), c = 17.440(4) Å, Z = 4) have been determined by single crystal X-ray diffraction analysis. Highly resolution IR and Raman spectra were measured at low temperature (10 K). Using the molecular parameters of the X-ray determinations normal coordinate analyses based on a modified valence force field have been performed and the normal modes of vibration are assigned. The valence force constants are fd(PtCl) = 2.19, fd(PtBr) = 1.68, fd(PtI) = 1.28 mdyn/Å and fd(PtO) ranges from 2.71 to 2.82 mdyn/Å. The observed 195Pt NMR shifts are δ(195Pt) = 6472.4 (X = Cl), 6027.1 (Br) and 5142.7 ppm (I).


1979 ◽  
Vol 34 (11) ◽  
pp. 1269-1274 ◽  
Author(s):  
Erik Bjarnov

Vinyl ketene (1,3-butadiene-1-one) has been synthesized by vacuum pyrolysis of 3-butenoic 2-butenoic anhydride. The microwave and infrared spectra of vinyl ketene in the gas phase at room temperature have been studied. The trans-rotamer has been identified, and the spectroscopic constants were found to be Ã= 39571(48) MHz, B̃ = 2392.9252(28) MHz, C̃ = 2256.0089(28) MHz, ⊿j = 0.414(31) kHz, and ⊿JK = - 34.694(92) kHz. The electrical dipole moment was found to be 0.987(23) D with μa = 0.865(14) D and μb = 0.475(41) D. A tentative assignment has been made for 17 of the 21 normal modes of vibration


2009 ◽  
Vol 24 (6) ◽  
pp. 543-552 ◽  
Author(s):  
P. LAGANT ◽  
G. VERGOTEN ◽  
G. FLEURY ◽  
M.H. LOUCHEUX-LEFEBVRE

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