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Density large-deviations of nonconserving driven models Density large-deviations of nonconserving driven models

Density large-deviations of nonconserving driven models - PowerPoint Presentation

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Density large-deviations of nonconserving driven models - PPT Presentation

5 th KIAS Conference on Statistical Physics Seoul Korea July 2012 Or Cohen and David Mukamel Ensemble theory out of equilibrium T µ Equilibrium Ensemble theory out of equilibrium ID: 264866

model nonconserving conserving slow nonconserving model slow conserving order equilibrium abc amp phys ensemble dynamics driven rev limit sum

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Slide1

Density large-deviations of nonconserving driven models

5th KIAS Conference on Statistical Physics, Seoul, Korea, July 2012

Or Cohen and David

MukamelSlide2

Ensemble theory out of equilibrium ?

T , µ

EquilibriumSlide3

Ensemble theory out of equilibrium ?

T , µ

Equilibrium

Driven diffusive systems

p

q

w

-

w

+

conserving steady stateSlide4

Ensemble theory out of equilibrium ?

T , µ

Equilibrium

Driven diffusive systems

p

q

w

-

w

+

Can we infer about the

nonconserving

system from the steady state properties of the conserving system ?

conserving steady stateSlide5

Ensemble theory out of equilibrium ?

T , µ

Equilibrium

Driven diffusive systems

p

q

w

-

w

+Slide6

Generic driven diffusive model

conserving

(sum over

η’ with same N)

nonconserving(sum over η

’ with N’≠N)

w

R

C

w

L

C

w

-

NC

w

+

NC

L sitesSlide7

Generic driven diffusive model

conserving(sum over η

’ with same N)

nonconserving(sum over

η’ with N’≠N)

w

R

C

w

L

C

w

-

NC

w

+

NC

Guess a steady

state of the form :

L sitesSlide8

Generic driven diffusive model

conserving(sum over η

’ with same N)

nonconserving(sum over

η’ with N’≠N)

It is consistent if :

w

R

C

w

L

C

w

-

NC

w

+

NC

In many cases :

Guess a steady

state of the form :

L sitesSlide9

Slow nonconserving dynamics

To leading order in

ε

we obtainSlide10

Slow nonconserving dynamics

= 1D - Random walk in a potential

To leading order in

ε

we obtainSlide11

Slow nonconserving dynamics

= 1D - Random walk in a potential

Steady state solution :

To leading order in

ε

we obtainSlide12

Outline

Limit of slow nonconserving

Example of the ABC model

Nonequilibrium chemical potential (dynamics dependent !)

ConclusionsSlide13

ABC model

A

B

C

AB BA

BC CB

CA AC

Dynamics :

q

1

q

1

q

1

Ring of size L

Evans,

Kafri

,

Koduvely

&

Mukamel

- Phys. Rev.

Lett

. 1998 Slide14

ABC model

A

B

C

AB BA

BC CB

CA AC

Dynamics :

q

1

q

1

q

1

Ring of size L

q=1

q<1

Evans,

Kafri

,

Koduvely

&

Mukamel

- Phys. Rev.

Lett

. 1998

A

BB

C

A

CC

B

A

C

A

B

A

C

B

AAAAA

BBBBB

CCCCCSlide15

ABC model

t

x

A

B

CSlide16

Nonconserving ABC model

0X X0 X=A

,B,

C

1

1

A

B

C

0

Lederhendler

&

Mukamel

-

Phys. Rev.

Lett

.

2010

A

B

B

A

B

C

C

B

C

A

A

C

q

1

q

1

q

1

1

2

1

2

Conserving model

(canonical ensemble)

+

fixedSlide17

Conserving model

Clincy

, Derrida & Evans -

Phys. Rev. E 2003

Weakly asymmetric

thermodynamic limitSlide18

Conserving model

Clincy

, Derrida & Evans -

Phys. Rev. E 2003

Weakly asymmetric

thermodynamic limit

known

For low

β

’s

Density profile

2

nd orderSlide19

Conserving model

Clincy

, Derrida & Evans -

Phys. Rev. E 2003

Weakly asymmetric

thermodynamic limit

Density profile

known

2

nd

order

For low

β’sSlide20

Nonconserving ABC model

0X X0 X=A

,B,

C

1

1

A

B

C

0

Lederhendler

&

Mukamel

-

Phys. Rev.

Lett

.

2010

A

B

B

A

B

C

C

B

C

A

A

C

q

1

q

1

q

1

A

B

C

000

pe

-3

βμ

p

1

2

3

1

2

1

2

3

Conserving model

(canonical ensemble)

Nonconserving

model

(grand canonical ensemble)

+

+

+Slide21

Slow nonconserving model

Slow nonconserving

limit

A

B

C

000

pe

-3

βμ

pSlide22

Slow nonconserving model

Slow nonconserving

limit

A

B

C

000

pe

-3

βμ

p

saddle point approx.Slide23

Slow nonconserving model

A

BC 000

pe

-3

βμ

pSlide24

Slow

nonconserving model

A

BC 000

pe

-3

βμ

p

This is similar to equilibrium : Slide25

Large deviation function of r

High µ

Low µ

First order phase transition (only in the

nonconserving

model)Slide26

Inequivalence of ensembles

Conserving = Canonical

Nonconserving =

Grand canonical

2

nd order transition

ordered

1

st order transition

tricritical point

disordered

ordered

disordered

For

N

A

=

N

B

N

C

:Slide27

Why is µS(N) the chemical potential ?

N

1

N

2

SLOWSlide28

Why is µ

S

(N) the chemical potential ?

N

1

N

2

Gauge measures

SLOW

SLOWSlide29

Conclusions

Nonequlibrium ‘grand canonical ensemble’ - Slow

nonconserving

dynamicsExample to ABC model

1st order phase transition for

nonmonotoneous µs(r) and inequivalence

of ensembles.Nonequilibrium chemical potential

( dynamics dependent ! )

Thank you !

Any

questions ?

Cohen & Mukamel - PRL

108, 060602 (2012)