Abstract:We present a molecular dynamics study of the liquid and plastic crystalline phases of CCl 3 Br. We investigated the short-range orientational order using a recently developed classification method and we found that both phases behave in a very similar way. The only differences occur at very short molecular separations, which are shown to be very rare. The rotational dynamics was explored using time correlation functions of the molecular bonds. We found that the relaxation dynamics corresponds to an isotropic d… Show more
“…4 for plastic and liquid CBr 2 Cl 2 ; only a slight difference can be noticed between the two phases. This statement was also true in the case of CBrCl 3 [6], supporting the strong resemblance between the two halomethane compounds. The pattern, in general, follows the one shown for CBrCl 3 : the 2:2 orientations are the most populous beyond 8 Å, as was observed for the whole family of CBr n Cl 4-n (n=0, 1, 2, 4).…”
Section: Orientational Correlationssupporting
confidence: 62%
“…This way, corner-to-corner (1:1); corner-to-edge (1:2); corner-to-face (1:3); edge-to-edge (2:2); edge-face (2:3); face-to-face (3:3) orientations may be distinguished. The clarity of this scheme permits its application to other systems consisting of tetrahedral molecules such as CCl 4 [3], CBrCl 3 [6] and CBr 4 [13]; it is also our intention here to compare our present results with these earlier works [3,6,13].…”
Section: Orientational Correlationsmentioning
confidence: 72%
“…A common feature that makes these systems attractive is that an orientationally disordered crystalline phase -also called 'plastic crystal' -appears between the low-temperature ordered phase and the liquid phase [5,6,10]. In this special phase the molecular centres are located in a highsymmetry lattice (face centered cubic, body centered cubic or rhombohedral), but the molecules can rotate around their equilibrium position.…”
Abstract. Neutron diffraction results obtained for plastic crystalline dichlorodibromomethane (CBr 2 Cl 2 ) have been modelled by means of the Reverse Monte Carlo method. Comparison with its liquid phase is provided at several levels of the atomic structure (total scattering structure factors, partial radial distribution functions, orientational and dipole-dipole correlations). Results reveal that the relative orientation of neighbouring molecules largely depends on the steric effect. The small dipole moment has not as strong influence as the steric effect on the short range order. Our observations fit well with earlier findings presented for the series CBr n Cl 4-n (n=0, 1, 2, 4).
“…4 for plastic and liquid CBr 2 Cl 2 ; only a slight difference can be noticed between the two phases. This statement was also true in the case of CBrCl 3 [6], supporting the strong resemblance between the two halomethane compounds. The pattern, in general, follows the one shown for CBrCl 3 : the 2:2 orientations are the most populous beyond 8 Å, as was observed for the whole family of CBr n Cl 4-n (n=0, 1, 2, 4).…”
Section: Orientational Correlationssupporting
confidence: 62%
“…This way, corner-to-corner (1:1); corner-to-edge (1:2); corner-to-face (1:3); edge-to-edge (2:2); edge-face (2:3); face-to-face (3:3) orientations may be distinguished. The clarity of this scheme permits its application to other systems consisting of tetrahedral molecules such as CCl 4 [3], CBrCl 3 [6] and CBr 4 [13]; it is also our intention here to compare our present results with these earlier works [3,6,13].…”
Section: Orientational Correlationsmentioning
confidence: 72%
“…A common feature that makes these systems attractive is that an orientationally disordered crystalline phase -also called 'plastic crystal' -appears between the low-temperature ordered phase and the liquid phase [5,6,10]. In this special phase the molecular centres are located in a highsymmetry lattice (face centered cubic, body centered cubic or rhombohedral), but the molecules can rotate around their equilibrium position.…”
Abstract. Neutron diffraction results obtained for plastic crystalline dichlorodibromomethane (CBr 2 Cl 2 ) have been modelled by means of the Reverse Monte Carlo method. Comparison with its liquid phase is provided at several levels of the atomic structure (total scattering structure factors, partial radial distribution functions, orientational and dipole-dipole correlations). Results reveal that the relative orientation of neighbouring molecules largely depends on the steric effect. The small dipole moment has not as strong influence as the steric effect on the short range order. Our observations fit well with earlier findings presented for the series CBr n Cl 4-n (n=0, 1, 2, 4).
“…For the present study, we have adapted the construction that was developed for CXY 3 liquids 10 (for more examples, see Refs. [26][27][28]). The PX 3 trigonal pyramid (or, in other words, distorted tetrahedron) can be supplemented by a virtual atom, positioned where the lone electron pair of the P atom would be, to form a more regular tetrahedron; the resulting geometrical body is therefore very similar to a CXY 3 molecule.…”
Section: Calculation Of the Orientational Correlation Functionsmentioning
Synchrotron X-ray diffraction measurements have been conducted on liquid phosphorus trichloride, tribromide and triiodide. Molecular Dynamics simulations for these molecular liquids were performed with a dual purpose: (1) to establish whether existing intermolecular potential functions can provide a picture that is consistent with diffraction data; (2) to generate reliable starting configurations for subsequent Reverse Monte Carlo modelling. Structural models (i.e., sets of coordinates of thousands of atoms) that were fully consistent with experimental diffraction information, within errors, have been prepared by means of the Reverse Monte Carlo method.Comparison with reference systems, generated by hard sphere-like Monte Carlo simulations, was also carried out to demonstrate the extent to which simple space filling effects determine the structure of the liquids (and thus, also estimating the information content of measured data). Total scattering structure factors, partial radial distribution functions and orientational correlations as a function of distances between the molecular centres have been calculated from the models. In general, more or less antiparallel arrangements of the primary molecular axes that are found to be the most favourable orientation of two neighbouring molecules. In liquid PBr 3 electrostatic interactions seem to play a more important role in determining intermolecular correlations than in the other two liquids; molecular arrangements in both PCl 3 and PI 3 are largely driven by steric effects.
“…While the case of alcali silicates is probably an extreme one, in the sense that the network of tetrahedra is extremely disordered due to the effect of alcali atoms on the network, the present approach can probably lead to interesting insights on the interplay between dynamics and order in other families of network forming systems which show different degrees of ordering, e.g. plastic glasses [25,31]. By monitoring the type and relative abundance of selected atoms at the vertices of tetrahedra the connection between dynamics and structure can be studied in detail and may allow to gain important insights in the nature of glassy behavior of complex systems.…”
We report on the dynamic and structural characterization of lithium metasilicate Li2SiO3, a network forming ionic glass, by means of molecular dynamics simulations. The system is characterized by a network of SiO4 tetrahedra disrupted by Li ions which diffuse through the network. Measures of mean square displacement of Si and O atoms allow us to identify a temperature at which tetrahedra stop moving relative to each other. This temperature Tc ≈ 1500 K can be characterized within the framework of mode coupling theory. At a much lower temperature Tg ≈ 1000 K, a change in the slope of the volume versus temperature data allows to single out the glass transition. We find signatures of both transitions in structural order parameters, related to the orientation of tetrahedra. Going down in temperature we find that, around the mode coupling transition temperature, a set of order parameters which measure the relative orientation of tetrahedra cease to increase and stay constant below Tc. Another well known measure of orientational order, the bond orientational order parameter, which in the studied system measures local order within single tetrahedrons, is found to continue growing below Tc until Tg, below which it remains constant. Our results allow to relate two characteristic dynamic transitions with corresponding structural transitions, as observed in two different orientational order parameters. Furthermore, the results indicate that the network of thetrahedra continue to relax well below the point where neighboring tetrahedra cannot rearrange relative to each other, and the glass is reached only upon a process of relaxation of atoms which form the thetrahedron, as quantified by the change in the bond orientational order parameters.
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