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1.
Acta Crystallogr B ; 55(Pt 6): 1014-1029, 1999 Dec 01.
Article in English | MEDLINE | ID: mdl-10927444

ABSTRACT

The compounds tetrakis(trimethylsilyl)methane C[Si(CH(3))(3)](4) (TC) and tetrakis(trimethylsilyl)silane Si[Si(CH(3))(3)](4) (TSi) have crystal structures with the molecules in a cubic closed-packed (c.c.p.) stacking. At room temperature both structures have space group Fm{\bar 3}m (Z = 4) with a = 13.5218 (1) Å, V = 2472.3 (1) Å(3) for TSi, and a = 12.8902 (2) Å, V = 2141.8 (1) Å(3) for TC. X-ray scattering data can be described by a molecule with approximately sixfold orientational disorder, ruling out a structure with free rotating molecules. Upon cooling, TSi exhibits a first-order phase transition at T(c) = 225 K, as is characterized by a jump of the lattice parameter of Deltaa = 0.182 Å and by an exothermal maximum in differential scanning calorimetry (DSC) with DeltaH = 11.7 kJ mol(-1) and DeltaS = 50.0 J mol(-1) K(-1). The structure of the low-temperature phase is refined against X-ray powder data measured at 200 K. It has space group P2(1)3 (Z = 4), a = 13.17158 (6) Å and V = 2285.15 (2) Å(3). The molecules are found to be ordered as a result of steric interactions between neighboring molecules, as is shown by analyzing distances between atoms and by calculations of the lattice energy in dependence on the orientations of the molecules. TC has a phase transition at T(c1) = 268 K, with Deltaa(1) = 0.065 Å, DeltaH(1) = 3.63 kJ mol(-1) and DeltaS(1) = 13.0 J mol(-1) K(-1). A second first-order phase transition occurs at T(c2) = 225 K, characterized by Deltaa(2) = 0.073 Å, DeltaH(2) = 6.9 kJ mol(-1) and DeltaS(2) = 30.0 J mol(-1) K(-1). The phase transition at higher temperature has not been reported previously. New NMR experiments show a small anomaly in the temperature dependence of the peak positions in NMR to occur at T(c2). Rietveld refinements were performed for the low-temperature phase measured at T = 150 K [space group P2(1)3, lattice parameter a = 12.609 (3) Å], and for the intermediate phase measured at T = 260 K [space group Pa{\bar 3}, lattice parameter a = 12.7876 (1) Å]. The low-temperature phase of TC is formed isostructural to the low-temperature phase of TSi. In the intermediate phase the molecules exhibit a twofold orientational disorder.

3.
Phys Rev B Condens Matter ; 54(17): 11849-11852, 1996 Nov 01.
Article in English | MEDLINE | ID: mdl-9985012
9.
Phys Rev B Condens Matter ; 49(13): 9186-9189, 1994 Apr 01.
Article in English | MEDLINE | ID: mdl-10009703
10.
Phys Rev B Condens Matter ; 49(15): 10818-10821, 1994 Apr 15.
Article in English | MEDLINE | ID: mdl-10009925
11.
12.
Phys Rev Lett ; 71(9): 1383-1386, 1993 Aug 30.
Article in English | MEDLINE | ID: mdl-10055526
13.
Phys Rev B Condens Matter ; 46(8): 5024-5027, 1992 Aug 15.
Article in English | MEDLINE | ID: mdl-10004275
14.
Phys Rev B Condens Matter ; 45(1): 543-546, 1992 Jan 01.
Article in English | MEDLINE | ID: mdl-10000225
15.
Phys Rev Lett ; 62(20): 2409-2412, 1989 May 15.
Article in English | MEDLINE | ID: mdl-10039978
16.
Phys Rev Lett ; 61(17): 1962-1965, 1988 Oct 24.
Article in English | MEDLINE | ID: mdl-10038943
17.
Phys Rev B Condens Matter ; 37(14): 8495-8498, 1988 May 15.
Article in English | MEDLINE | ID: mdl-9944202
19.
Phys Rev B Condens Matter ; 37(6): 2826-2828, 1988 Feb 15.
Article in English | MEDLINE | ID: mdl-9944857
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