Literature DB >> 17359062

Observation of fractional Stokes-Einstein behavior in the simplest hydrogen-bonded liquid.

F Fernandez-Alonso1, F J Bermejo, S E McLain, J F C Turner, J J Molaison, K W Herwig.   

Abstract

Quasielastic neutron scattering has been used to investigate the single-particle dynamics of hydrogen fluoride across its entire liquid range at ambient pressure. For T>230 K, translational diffusion obeys the celebrated Stokes-Einstein relation, in agreement with nuclear magnetic resonance studies. At lower temperatures, we find significant deviations from the above behavior in the form of a power law with exponent xi=-0.71+/-0.05. More striking than the above is a complete breakdown of the Debye-Stokes-Einstein relation for rotational diffusion. Our findings provide the first experimental verification of fractional Stokes-Einstein behavior in a hydrogen-bonded liquid, in agreement with recent computer simulations [S. R. Becker, Phys. Rev. Lett. 97, 055901 (2006)10.1103/PhysRevLett.97.055901].

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Year:  2007        PMID: 17359062     DOI: 10.1103/PhysRevLett.98.077801

Source DB:  PubMed          Journal:  Phys Rev Lett        ISSN: 0031-9007            Impact factor:   9.161


  3 in total

1.  The role of the dynamic crossover temperature and the arrest in glass-forming fluids.

Authors:  F Mallamace; C Corsaro; H E Stanley; S-H Chen
Journal:  Eur Phys J E Soft Matter       Date:  2011-09-23       Impact factor: 1.890

2.  Transport properties of glass-forming liquids suggest that dynamic crossover temperature is as important as the glass transition temperature.

Authors:  Francesco Mallamace; Caterina Branca; Carmelo Corsaro; Nancy Leone; Jeroen Spooren; Sow-Hsin Chen; H Eugene Stanley
Journal:  Proc Natl Acad Sci U S A       Date:  2010-12-08       Impact factor: 11.205

3.  Structural origin of fractional Stokes-Einstein relation in glass-forming liquids.

Authors:  Shaopeng Pan; Z W Wu; W H Wang; M Z Li; Limei Xu
Journal:  Sci Rep       Date:  2017-01-06       Impact factor: 4.379

  3 in total

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