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How Mysterious is the Mysterious Glass Transition?

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Title: How Mysterious is the Mysterious Glass Transition?


1
How Mysterious is the Mysterious Glass Transition?
Itamar Procaccia The Weizmann
Institute of Science
Weizmann Institute Einat Aharonov, Eran
Bouchbinder, Valery Ilyin, Edan Lerner,
Ting-Shek Lo, Natalya Makedonska, Ido Regev and
Nurith Schupper. Emory University George
Hentschel
Leiden, August 25 2008
2
Glass phenomenology
The three common conceptes jamming,
Vogel-Fulcher, Kauzmann
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A very popular model a 50-50 binary mixture of
particles interacting via soft repulsion potential
With ratio of diameters 1.4
Simulations both Monte Carlo and Molecular
Dynamics with 4096 particles enclosed in an area
L x L with periodic boundary conditions. We ran
simulations at a chosen temperature, fixed volume
and fixed N. The units of mass, length, time and
temperature are
Previous work (lots) Deng, Argon and Yip, P.
Harrowell et al, etc for Tgt0.5 the system is a
fluid for T smaller - dynamical relaxation
slows down considerably.
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The conclusion was that defects do not show any
singular behaviour , so they were discarded as
a diagnostic tool.
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The liquid like defects disappear at the glass
transition!
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For temperature gt 0.8
For 0.3 lt T lt 0.8
Associated with the disappearance of liquid like
defects there is an increase of typical scale
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Rigorous Results(J.P. Eckmann and I.P.,
arXiv0802.3404)
The system is ergodic at all temperatures
10
Consequences there is no Vogel-Fulcher
temperature! There is no Kauzman
tempearture! There is no jamming!
(the three nos of Khartoum)
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Statistical Mechanics
We define the energy of a cell of type i
Similarly we can measure the areas of cells of
type i
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Denote the number of boxes available for largest
cells
Then the number of boxes available for the second
largest cells is
The number of possible configurations W is then
Denote
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A low temperature phase
Note that here the hexagons have disappeared
entirely!
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First result
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Specific heat anomalies
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The anomalies are due to micro-melting
(micro-freezing of crystalline clusters)
We have an equation of state !!!
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Summary
The glass transition is not an abrupt
transition, rather a very smeared out phenomenon
in which relaxation times increase at the T
decreases. There is no singularity on the way,
no jamming, no Vogel-Fulcher, no Kauzman
Since nothing gets singular, statistical
mechanics is useful
We showed how to relate the statistical mechanics
and structural information in a quantitative way
to the slowing down and to the relaxation
functions . We could also explain in some detail
the anomalies of the specific heat
Remaining task How to use the increased
understanding to write a proper theory of the
mechanical properties of amorphous solid
materials. (work in progress).
24
Some references
E. Aharonov, E. Bouchbinder, V. Ilyin, N.
Makedonska, I. Procaccia and N. Schupper, Direct
Identification of the Glass Transition Growing
Length Scale and the Onset of Plasticity,
Europhys. Lett. 77, 56002 (2007) . Also
cond-mat/0608305 .Valery Ilyin, Edan Lerner,
Ting-Shek Lo, Itamar Procaccia, Statistical
Mechanics of the Glass Transition in
One-Component Liquids with Anisotropic
Potential, Phys. Rev. Lett.,99, 135702 (2007) .
Also arXiv0705.1043v1Valery Ilyin, Nataliya
Makedonska, Itamar Procaccia, Nurith Schupper,
Mechanical Properties of Glass Forming Systems,
Phys. Rev. E 76, 052401 (2007). Also
arXiv0705.1834v1 H. G. E. Hentschel, V. Ilyin,
N. Makedonska, I. Procaccia and N. Schupper,
Statistical mechanics of the glass transition as
revealed by a Voronoi tesselation, Phys. Rev. E
75, 050404 (2007) Also cond-mat/0608443
.H.G.E.Hentschel and Itamar Procaccia, Theory
of Relaxation Dynamics in Glass-Forming
Hydrogen-Bonded Liquids, Phys.Rev. E.77,031507
(2008). Also arXiv0709.4404
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  • Valery Ilyin, Itamar Procaccia, Ido Regev, Nurith
    Schupper,
  • Ageing and Relaxation in Glass Forming Systems,
    Phys. Rev. E 77, 061509 (2008) Also
    arXiv0803.2602Jean-Pierre Eckmann and Itamar
    Procaccia, Ergodicity and Slowing Down in
    Glass-Forming Systems with Soft Potentials No
    Finite-Temperature Singularities, Phys. Rev. E,
    78, 011503 (2008)., Also arXiv0802.4346Edan
    Lerner and Itamar Procaccia, Quantitative Theory
    of a Relaxation Function in a Glass-Forming
    System, Phys. Rev. Lett., submitted. Movie
    Avi(9M), Mpeg ( 4M). Also arXiv0804.1205 Edan
    Lerner, Itamar Procaccia and Ido Regev,
    Quantitative Theory of a Time-Correlation
    Function in a One-Component Glass-Forming Liquid
    with Anisotropic Potential, PRE., submitted.
    Also arXiv0806.3685
  • H. G. E. Hentschel, Valery Ilyin and Itamar
    Procaccia, Non-Universality of the Specific Heat
    in Glass Forming Systems, Phys. Rev. Lett.,
    submitted. AlsoarXiv0808.2736H. G. E.
    Hentschel, Valery Ilyin, Itamar Procaccia and
    Nurith Schupper, Theory of Specific Heat in Glass
    Forming Systems. Phys. Rev. E, submitted.
    AlsoarXiv0808.2138

26
Strains, stresses etc.
We are interested in the shear modulus
Dynamics of the stress
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Zwanzig-Mountain (1965)
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