Abstract:Glassy dynamics of rigid molecules is still a matter of controversy: the physics behind the relaxation process at time scales faster than that ruled by the viscosity, the so called Johari-Goldstein process, is not known. In this work we unravel the mechanism of such a process by using a simple molecular model in which the centers of mass of the molecules are forming an ordered lattice, and molecular reorientation is performed by jumps between equilibrium orientations. We have studied the dynamics of simple qua… Show more
“…The analysis of the isostructural CCl 4 shows that nonequivalent molecules in the unit cell perform reorientational jumps at different time scales due to their different crystalline environments. These results support the conclusion that the dynamic heterogeneity is intimately related to the secondary relaxation observed in these compounds 27,28,31 .…”
Section: Introductionsupporting
confidence: 88%
“…The dynamics of the monoclinic phases of CBr n Cl 4−n , n=0,1,2 compounds has been studied by means of dielectric spectroscopy and nuclear quadrupole resonance (NQR) spectroscopy 27,28 in the temperature range 100 -250 K and 80 -210 K, respectively. The former technique allows the measurement of the dynamic response within a broad time scale but it is insensitive to fine details of molecular motions, whereas the latter has a restricted time window but monitors the movement of individual chlorine atoms.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the NQR experiments are limited to a temperature range between 77 K and 140 K, with the upper end determined by the broadening of the signal 28 . The picture that emerges from the combined analysis is that the three compounds have a very similar dynamic evolution in the monoclinic phase as a function of temperature 27,28 . The analysis of the isostructural CCl 4 shows that nonequivalent molecules in the unit cell perform reorientational jumps at different time scales due to their different crystalline environments.…”
Family of compounds CBr n Cl 4−n has been proven helpful in unraveling microscopic mechanisms responsible of glassy behavior. Some of the family members show translational ordered phases with minimal disorder which appears to reveal glassy features, thus deserving special attention in the search for universal glass anomalies. In this work, we studied CBrCl 3 dynamics by performing extensive molecular dynamics simulations. Molecules of this compound perform reorientational discrete jumps, where the atoms exchange equivalent positions among each other revealing a cage-orientational jump motion fully comparable to the cage-rototranslational jump motion in supercooled liquids. Correlation times were calculated from rotational autocorrelation functions showing good agreement with previous reported dielectric results. From mean waiting and persistence times calculated directly from trajectory results, we are able to explain which microscopic mechanisms lead to characteristic times associated with α and β-relaxation times measured experimentally. We found that two nonequivalent groups of molecules have a longer characteristic time than the other two nonequivalent groups, both of them belonging to the asymmetric unit of the monoclinic (C2/c) lattice.
“…The analysis of the isostructural CCl 4 shows that nonequivalent molecules in the unit cell perform reorientational jumps at different time scales due to their different crystalline environments. These results support the conclusion that the dynamic heterogeneity is intimately related to the secondary relaxation observed in these compounds 27,28,31 .…”
Section: Introductionsupporting
confidence: 88%
“…The dynamics of the monoclinic phases of CBr n Cl 4−n , n=0,1,2 compounds has been studied by means of dielectric spectroscopy and nuclear quadrupole resonance (NQR) spectroscopy 27,28 in the temperature range 100 -250 K and 80 -210 K, respectively. The former technique allows the measurement of the dynamic response within a broad time scale but it is insensitive to fine details of molecular motions, whereas the latter has a restricted time window but monitors the movement of individual chlorine atoms.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the NQR experiments are limited to a temperature range between 77 K and 140 K, with the upper end determined by the broadening of the signal 28 . The picture that emerges from the combined analysis is that the three compounds have a very similar dynamic evolution in the monoclinic phase as a function of temperature 27,28 . The analysis of the isostructural CCl 4 shows that nonequivalent molecules in the unit cell perform reorientational jumps at different time scales due to their different crystalline environments.…”
Family of compounds CBr n Cl 4−n has been proven helpful in unraveling microscopic mechanisms responsible of glassy behavior. Some of the family members show translational ordered phases with minimal disorder which appears to reveal glassy features, thus deserving special attention in the search for universal glass anomalies. In this work, we studied CBrCl 3 dynamics by performing extensive molecular dynamics simulations. Molecules of this compound perform reorientational discrete jumps, where the atoms exchange equivalent positions among each other revealing a cage-orientational jump motion fully comparable to the cage-rototranslational jump motion in supercooled liquids. Correlation times were calculated from rotational autocorrelation functions showing good agreement with previous reported dielectric results. From mean waiting and persistence times calculated directly from trajectory results, we are able to explain which microscopic mechanisms lead to characteristic times associated with α and β-relaxation times measured experimentally. We found that two nonequivalent groups of molecules have a longer characteristic time than the other two nonequivalent groups, both of them belonging to the asymmetric unit of the monoclinic (C2/c) lattice.
“…In some of these cases, it has been demonstrated that the main glass features show up, pointing out the relevance of the orientational degrees of freedom as far as the glass properties are considered. [20][21][22] Also, it should be stressed that for all those disordered systems the collective dynamics of the entities cannot be decoupled from the molecular or localized excitations, and thus the use of pertinent techniques, which encompass the different origins of disorder, should provide important highlights to the glass transition problem.…”
“…The presentation will describe the stable and metastable phases of those compounds revealed by the uncommon inclusion of the pressure variable as well as by the analyses of the two-component systems sharing them. Moreover, the emergence of unstable phases (glasses) [2] within the low-temperature domain will be analyzed and the similarities with the canonical glassformers will be discussed. …”
Many molecular materials composed of globular or pseudoglobular molecules are capable of forming hightemperature orientationally disordered (OD) phases in which long-range positional order exists and orientational order has been lost. Halogen methane derivatives, as tetrahalogenomethane compounds (CX n Y m , where n and m = 0, ..., 4; n + m = 4, and X,Y=F, Cl, Br and I) have been investigated by the Group of Characterization of Materials at the Universitat Politècnica de Catalunya during the last years [1]. In spite of the similarity of the molecules, fine tuning interactions give rise to a polymorphic behavior at normal pressure, i.e. in equilibrium with its vapor, quite different. The rational of the thermodynamics can be achieved when the polymorphism is analyzed in the whole temperature-pressure space. The presentation will describe the stable and metastable phases of those compounds revealed by the uncommon inclusion of the pressure variable as well as by the analyses of the two-component systems sharing them. Moreover, the emergence of unstable phases (glasses) [2] within the low-temperature domain will be analyzed and the similarities with the canonical glassformers will be discussed.
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