Wilson GF

Quinn AD, O Hare NJ, Wallis FJ, Wilson GF (1994) Gd-DTPA An alternative contrast medium for CT. J Comput Assist Tomogr 18 634... 

The established method for calculating the vibrational frequencies of molecules is the Wilson GF method.27 In this method, the potential energy of a molecule is defined in terms of the force constants by a matrix F, and the kinetic energy, which depends on the geometry of the molecule, is defined by a matrix G. Using the methods of classical mechanics, the following equation may be derived. 

To model quantitatively an IINS spectrum, it is only necessary to obtain the amplitudes of motion of the atoms in the vibrational modes. These can be calculated by a variety of methods, such as the balls-and-springs approach of the Wilson GF matrix method, ab-initio calculations, and molecular dynamics this point expresses what is undoubtedly the greatest strength of IINS spectroscopy. Examples are presented below. 

Fig. 9. Comparison of the IINS spectrum (TFXA, ISIS) of the deactivated palladium catalyst (solid line) and the results from the Wilson GF matrix method analysis of the spectrum (dashed line). The model is shown in the top right-hand corner.

Kane D, Murphy JM, Keating S, Wilson GF, Mulcahy FM. Renal ultrasonic findings in sulphadiazine-induced renal failure. The British journal of radiology. 1996 Oct 69(826) 925-8. 

In the early 1950s Morino and his co-workers in Japan established a systematic treatment for the calculated of amplitudes of vibration from harmonic force fields, based on the widely used Wilson GF matrix method... 

Thus modes at 360 and 585 involve the wag, those at 386, 425 and 485 involve the rock and that at 457 cm" the torsion. A Wilson GF matrix method study of the cyclohexyl complex [42] came to similar conclusions, but considered that the modes were coupled to to the W-C stretches, which occur in the same region as the linear bends ( 11.2.6). This was done by introducing an interaction force constant between the... 

This analysis highlights the need for information from all three t3T)es of vibrational spectroscopy and the crucial role that the INS intensities play in the assignments. The assignments can be substantiated by generating the INS spectrum by the Wilson GF method and the result is compared to the experimental spectrum in Fig. 6.25. The agreement for the internal modes is good but the analysis has omitted the strongest feature in the spectrum, the librational mode at 460 cm. ... 

Fig. 6.25 INS spectra of Mg2[FeH6] (a) experimental, (b) calculated from the Wilson GF method and (c) calculated by periodic DFT.

The substrate (or adsorbent) was modelled in one dimension by a linear chain of five carbon atoms, (We could have chosen any other atom.) A terminal carbon atom represents a surface atom and the remaining atoms the bulk. There is only one force constant, the C-C stretching force constant (C—C of C2 12.16 mdyn A" ). The dynamics were treated by the Wilson GF method. The substrate then had four vibrations similar to longitudinal acoustic modes (LAM) ( 10.1.2) LAM1,170 cm LAM2, 330 cm LAM3, 455 cm LAM4, 535 cm. The calculated INS spectrum comprised four bands of equal, weak intensity. 

Fig. 7.12 INS spectra (BT4, NIST) of (a) ethyne on platinum black annealed at 300 K with 500 mbar of dihydrogen (b) ethyne on platinum black adsorbed at 120 K, no dihydrogen. Reproduced from [64] with permission from the American Institute of Physics. [Os3(n2-CO)(CO)9( i3-Ti -C2H2)] (c) experimental, (d) modelled with the Wilson GF method. Reproduced from [67] with permission from the PCCP Owner Societies, (e) [Co2(CO)6(li2-ri -C2H2)], experimental (INBeF, ILL). Reproduced from [66] with permission from the American Chemical Society. Note that the peak pattern of adsorbed ethyne (b) is similar to that of ethyne in the osmium complex (c). Note also the additional peaks near 500 and 1400 cm when adsorbed ethyne was treated with hydrogen (a).

The experimental INS spectra of the Os and Co complexes and the spectrum of the Os complex modelled with the Wilson GF matrix method are shown in Fig. 7.12. Assignments for C symmetry are shown in Table 7.7. The vibrational modes of the osmium complex are illustrated in Fig. 7.14 (p. 311). 

For the cobalt complex INS peaks with significant intensity and assignments from the Wilson GF method are given in Table 7.7. The spectrum of the cobalt complex is remarkably different from that of the osmium complex (cf Table 7.7 and Fig. 7.12) the wavenumbers of the C-H deformations are ca 300 cm" lower for the Co complex compared with the Os complex. 

Zeise s salt, K[Pt(C2H4)Cl3]H20, is the best known and most-studied ethene-metal complex. The structure is related to the structure of the square planar [PtCU] ion, ethene replacing one Cl with its C=C axis perpendicular to the PtC plane. It is regarded as a model of ethene binding to a transition metal centre. The INS spectrum of the anhydrous complex is shown in Fig. 7.18 [77].The spectrum was assigned with the aid of a Wilson GF method calculation, see Table 7.11. However, a more recent spectrum. Fig. 1.1, shows that the factor group splitting of the... 

The hydrogenation is catalysed by nickel and other transition metals. Vibrational spectroscopy (infrared, HREELS, INS) has been applied to determining the orientation and binding of benzene on the catalyst surface. We suimnarise INS studies of benzene, adsorbed benzene and model complexes. The intensities and frequencies of the vibrational modes are computed by the Wilson GF method. The benzene molecule... 

Fig. 7.35 INS spectra of pure thiophene (top, solid line), the spectrum calculated with the Wilson GF method (middle, broken line) and thiophene on a reduced and sulfided Mo(14%)/Al203 catalyst (bottom, histograms). The peaks are labelled according to the scheme of Fig. 7.36, A to J in increasing energy. Reproduced from [140] with permission from the PCCP Owner Societies.

The method adopted to obtain the foree constants from the vibrational frequencies treated the molecule as a system of point masses connected by springs that obeyed Hooke s law, so the system was purely harmonic. The approach was codified in a classic book [3] and is known as the Wilson GF matrix method. The basis of the method is described in 4.2.2 and in more detail in [4,5]. The key equation is ... 

Fig. 8.2 INS spectra of maleic anhydride [2] (a) experimental, (b) calculated using the Wilson GF matrix method, (c) from a DFT calculation (using the B3LYP functional with the 6-31G(d,p) basis set) of the isolated molecule and (d) from a periodic DFT calculation of the complete unit cell.

It is possible, albeit complex, to extract the force constants from an ab initio calculation and so is not usually done. Table 8.1 compares the force constants for maleic anhydride obtained from the Wilson GF matrix method with those obtained from the ab initio calculation. 

A branched alkane which has been studied by INS is neopentane (2,2-dimethylpropane, C(CH3)4) [14]. Fig. 8.4 shows a comparison of the INS spectrum and that calculated using a classic Wilson GF force field... 

Fig. 8.4 INS spectrum of neopentane recorded at (a) 30K (IN4, ILL) and (b) at 80K (INlBeF, ILL), (c) and (d) are spectra of the same regions calculated with the classic Wilson GF force field [15]. Reproduced from [14] with permission from Academic Press.

More polycyclic alkanes have been treated by INS spectroscopy. The spectrum of of adamantane (tricyclo[3.3.1.1 ]decane, CioHie) is shown in Fig. 4.6. Norbomane and some of its mono- and dimethyl derivatives (see Fig. 8.5 for the structures) were extensively studied and force fields developed using the Wilson GF matrix method [17—19]. Given the low symmetry and relatively large number of atoms present, this was a tour de force of spectroscopy. 

There have been several Wilson GF calculations of the isolated chain for both syndiotactic [20] and isotactic polypropylene [21,22]. There is also a lattice dynamics calculation for the full unit cell of isotactic polypropylene [23]. All of these are at Ar = 0 where the infrared and Raman active modes occur and as a result, these modes are well assigned [4]. There are two calculations of the dispersion curves [24,25] for a... 

In this section we will consider polydimethylsiloxane (PDMS) as an example of the type of work that is possible with amorphous polymers. The structure and INS spectrum of PDMS are shown in Fig. 10.21a [40]. The repeat unit shown in Fig. 10.21b was used to model the spectrum using the Wilson GF matrix method [41]. The major features are reproduced skeletal bending modes below 100 cm", the methyl torsion and its overtone at 180 and 360 cm respectively, the coupled methyl rocking modes and Si-0 and Si-C stretches at 700-1000 cm and the unresolved methyl deformation modes 1250-1500 cm. The last are not clearly seen because the intensity of the methyl torsion results in a large Debye-Waller factor, so above 1000 em or so, most of the intensity occurs in the phonon wings. 

Fig. 10.21 (a) The structure and INS spectrum of polydimethylsiloxane. (b) Wilson GF fit to PDMS using just the model fragment shown. 

Fig. 11.3 INS spectrum of (a) K2[PtCl6] and (b) K2[PdCl4]. The dashed lines are a fit to the internal modes using the Wilson GF matrix method.

Wilson GF, Courtman DW, Klement P, Lee JM, Yeger H. Acellular matrix a biomaterials approach for coronary artery bypass and heart valve replacement. Ann Thorac Surg 1995 60(2) S353-8. 

Morino and his co-workers established a systematic treatment for the calculation of mean amplitudes of vibration from harmonic force fields, based on the widely used Wilson GF matrix method, which is still the foundation for the majority of such calculations. The theory of such calculations has been developed considerably since, notably by Cyvin and coworkers. With the advent of modern computers, the calculation of mean amplitudes using these methods has become a routine procedure. The resultant extensive literature has been reviewed by Cyvin. ... 

The harmonic force constants thus obtained have been used in a Wilson GF procedure modified by periodic boundary conditions to compute phonon dispersion curves. These curves enabled the phonon density of states to be evaluated in a manner similar to that employed in obtaining the electronic density of states from the electronic band structure. 

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