The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’...

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The Glass Transition Giulio Biroli IPhT CEA Saclay

Transcript of The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’...

Page 1: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

The Glass TransitionGiulio BiroliIPhT CEA Saclay

Page 2: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

The glass ‘transition’

Amorphous rigid material

! ! 10!2Pa · s

! ! 1012Pa · sA tiny molecule moves of few

Angstroms in a second!

At Tg by definition ! = 1012Pa · s

! ! " ! exp!

DT0

T " T0

"

from experiments

Page 3: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

Questions

• Is it a order-disorder transition?

• What kind of order? Amorphous order? How to define it? How to measure it?

• How to build a theory? New techniques?

• What are the real space signatures of the collective-critical phenomenon?

May be yes, but the order that is growing is ‘disordered’

Huge number of amorphous ground states; how to handle this?

Page 4: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

Ubiquity of glass transitionsNot only molecular liquids but also...

colloids and soft matter systems and...

Amorphous rigid material

granular materials and...

...error correcting codes and computer science

Page 5: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

Dynamical correlations

A lot!

• Dynamical field or overlap function as order parameter:

o(r, t, 0) = !"(r, t)!"(r, 0) Mean field theory, Field theory, simulations, effective models.

Page 6: The Glass Transition - Accueil - IHESvanhove/IHESIPHT2010/talks/biroli.pdfThe glass ‘transition’ Amorphous rigid material η ∝ 10−2Pa· s η ∝ 1012Pa· s A tiny molecule

Ideal thermodynamic glass transitionHow to unveil the existence of amorphous order and do quantitative

computations?

equilibrium configuration in state !

Thermodynamics inside the cavity with the quenched

boundary condition provided by . !

Order Parameter: overlap with Replica, Mean Field Theory (1 RSB), Simulations, Kac Models,

Renormalization Group.

!