0000000000615890

AUTHOR

Th. Theenhaus

showing 3 related works from this author

Dynamical precursor of nematic order in a dense fluid of hard ellipsoids of revolution

2004

We investigate hard ellipsoids of revolution in a parameter regime where no long range nematic order is present but already finite size domains are formed which show orientational order. Domain formation leads to a substantial slowing down of a collective rotational mode which separates well from the usual microscopic frequency regime. A dynamic coupling of this particular mode into all other modes provides a general mechanism which explains an excess peak in spectra of molecular fluids. Using molecular dynamics simulation on up to 4096 particles and on solving the molecular mode coupling equation we investigate dynamic properties of the peak and prove its orientational origin.

PhysicsRange (particle radiation)Condensed matter physicsRelaxation (NMR)BiophysicsComplex systemFOS: Physical sciencesSurfaces and InterfacesGeneral ChemistryDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksCondensed Matter - Soft Condensed MatterSpectral lineMolecular dynamicsLiquid crystalMode couplingSoft Condensed Matter (cond-mat.soft)General Materials ScienceSoft matterBiotechnology
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Microscopic Dynamics of Hard Ellipsoids in their Liquid and Glassy Phase

2001

To investigate the influence of orientational degrees of freedom onto the dynamics of molecular systems in its supercooled and glassy regime we have solved numerically the mode-coupling equations for hard ellipsoids of revolution. For a wide range of volume fractions $\phi$ and aspect ratios $x_{0}$ we find an orientational peak in the center of mass spectra $\chi_{000}^{''}(q,\omega)$ and $\phi_{000}^{''} (q,\omega)$ about one decade below a high frequency peak. This orientational peak is the counterpart of a peak appearing in the quadrupolar spectra $\chi_{22m}^{''}(q,\omega)$ and $\phi_{22m}^{''}(q,\omega)$. The latter peak is almost insensitive on $\phi$ for $x_{0}$ close to one, i.e. f…

PhysicsRange (particle radiation)Condensed matter physicsDegrees of freedom (physics and chemistry)FOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksCondensed Matter - Soft Condensed MatterCondensed Matter PhysicsCoupling (probability)OmegaSpectral lineElectronic Optical and Magnetic MaterialsPhase (matter)Materials ChemistryCeramics and CompositesSoft Condensed Matter (cond-mat.soft)Center of massSupercooling
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Microscopic dynamics of molecular liquids and glasses: Role of orientations and translation-rotation coupling

2001

We investigate the dynamics of a fluid of dipolar hard spheres in its liquid and glassy phase, with emphasis on the microscopic time or frequency regime. This system shows rather different glass transition scenarios related to its rich equilibrium behavior which ranges from a simple hard sphere fluid to a long range ferroelectric orientational order. In the liquid phase close to the ideal glass transition line and in the glassy regime a medium range orientational order occurs leading to a softening of an orientational mode. To investigate the role of this mode we use the molecular mode-coupling equations to calculate the spectra $\phi_{lm}^{\prime \prime}(q,\omega)$ and $\chi _{lm}''(q,\ome…

PhysicsCondensed matter physicsOrder (ring theory)FOS: Physical sciencesCenter of massIdeal (ring theory)Hard spheresDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksMoment of inertiaCoupling (probability)OmegaSpectral line
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