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Exact results for transport properties of one- dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University
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Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

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Page 1: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Exact results for transport properties of one-dimensional hamiltonian systems

Henk van Beijeren

Institute for Theoretical PhysicsUtrecht University

Page 2: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

1) Problems with hydrodynamics in 1 and 2 dimensions.

2) The fluctuating Burgers equation a) Mode coupling results b) Exact results by Prähofer and Spohn

3) Hydrodynamics in one dimension. a) Mode coupling expansions b) Dominance of Prähofer-Spohn terms for long times c) Explicit results

4) Concluding remarks

Page 3: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Hydrodynamics in 1 and 2 dimensions is known since the 1960’s to beplagued by divergence problems. Transport coefficients in linearized hydrodynamic equations are given by Green-Kubo expressions, such as

D

Assuming regular diffusion of mass and of momentum one finds thatthe average velocity of the tagged particle at time t, given it started out with velocity v0 is proportional to v0 t -d/2.

Page 4: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 5: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 6: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Hydrodynamics in 1 and 2 dimensions is known since the 1960’s to beplagued by divergence problems. Transport coefficients in linearized hydrodynamic equations are given by Green-Kubo expressions, such as

D

Assuming regular diffusion of mass and of momentum one finds thatthe average velocity of the tagged particle at time t, given it started out with velocity v (0) is proportional to v (0) t -d/2. The time integral of this diverges for d = 1 or 2.

Page 7: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

One can improve on this by using self-consistent theories. Thesepredict:

2/3

1(0) ( ) ( 2)

ln1

(0) ( ) ( 1)

t dt t

j j t dt

v v

Page 8: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 9: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 10: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

One can improve on this by using self-consistent theories. Thesepredict:

Correspondingly they predict size dependent transport coefficients.In 1d:

2/3

1(0) ( ) ( 2)

ln1

(0) ( ) ( 1)

t dt t

j j t dt

v v

1/3( ) ( 1)L L d

Page 11: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 12: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Fluctuating Burgers equation

Can be used for describing driven, collective single file diffusion, traffic flows and ASEP’s among other things.

Page 13: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Fluctuating Burgers equation

For Fourier components:

Page 14: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Fluctuating Burgers equation

For Fourier components:

May be rewritten into the integral equation

Page 15: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

● → * → ∫ dτ [ ]

Diagrammatic elements:

Page 16: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

0ˆ( , )S k t t

Page 17: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Next iteration:

Page 18: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 19: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

with right vertex weight:

Page 20: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Diagrammatic mode coupling expansion leads to Dyson structure:

Page 21: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 22: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Assume: ( , ) ( ), with (0) 1 h h

Page 23: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

2/3

2/3

1/2

0

Assume: ( , ) ( ), with (0) 1

( , ) ( )

(0) ( ) ~

( ) ( , ) ~

h h

h

J J t t

D k dt M k t k

Page 24: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The Kardar-Parisi-Zhang equations

By integrating the 1d fluctuating Burgers equation over x one obtains the 1d KPZ equation:

Page 25: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The Kardar-Parisi-Zhang equations

By integrating the 1d fluctuating Burgers equation over x one obtains the 1d KPZ equation:

Page 26: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The Kardar-Parisi-Zhang equations

By integrating the 1d fluctuating Burgers equation over x one obtains the 1d KPZ equation:

Prähofer and Spohn found an exact solution for the polynuclear growth model, which belongs to the KPZ universality class.

Page 27: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Main results of PS, translated to the fluctuating Burgers equation:

Exact scaling functions were obtained for the density-densitycorrelation function Ŝ(k,t) (or S(x,t)).

Page 28: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Fluctuating hydrodynamics in one dimension

with

( , ) ( , ) ( , )

n e

p x t p e x t p n x t

x e x n x

and derivatives of s(x, t) and T(x,t) defined in similar way

Page 29: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Linearization plus Fourier transform gives

Page 30: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Linearization plus Fourier transform gives

Diagonalizing gives three hydrodynamic modes,

210 21; ic k k

2 20 p

Tk Dnc

k

Page 31: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The time correlation functions of the hydrodynamic modes satisfy linear equations involving memory kernels, of similar form as thedensity-density time correlation function for the Burgers equation.

Page 32: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The time correlation functions of the hydrodynamic modes satisfy linear equations involving memory kernels, of similar form as thedensity-density time correlation function for the Burgers equation.

Page 33: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

The time correlation functions of the hydrodynamic modes satisfy linear equations involving memory kernels, of similar form as thedensity-density time correlation function for the Burgers equation.

Like for the fluctuating Burgers equation the memory kernels may be expressed through a diagrammatic mode coupling expansion, but now there are three types of lines, corresponding to the three types of hydrodynamic modes and 27 vertices, corresponding to all combinations of lines coming in and running out.

Page 34: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Crucial observation: Due to different propagation speeds of different types of modes internally only couplings of a mode σ to two modes with the same value of σ contribute to the dominant long time behavior.

Page 35: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Crucial observation: Due to different propagation speeds of different types of modes internally only couplings of a mode σ to two modes with the same value of σ contribute to the dominant long time behavior.

Therefore, in a comoving frame the sound-sound time correlation functions to leading order are of the same form as the Burgers density-density time correlation function.

Page 36: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Crucial observation: Due to different propagation speeds of different types of modes internally only couplings of a mode σ to two modes with the same value of σ contribute to the dominant long time behavior.

Therefore, in a comoving frame the sound-sound time correlation functions to leading order are of the same form as the Burgers density-density time correlation function.

Leading long-time and small wave number results:

2/3

1/2

1/52 23/5

( , ) exp( ) [( 2 ) ]

8 2 ( )

19.444

( ) 2 ( )1 3 3(0) ( )

5 5 1.0528

PS

HH

EH H

S k t i ckt f V k

Vk

k

V c VJ J t t

L V V

01/2

02( ) s

c nV

c n

Page 37: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 38: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Heat mode to leading order does not couple to a pair of heat modes,but only to couple of equal type sound modes. Therefore heat conduction coeffient behaves differently from sound damping constant, because pair of sound modes in resting frame oscillates as exp(σic0kt).

Page 39: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Heat mode to leading order does not couple to a pair of heat modes,but only to couple of equal type sound modes. Therefore heat conduction coeffient behaves differently from sound damping constant, because pair of sound modes in resting frame oscillates as exp(σic0kt).

Main results:

2

2

1/3 2/3 1/30

2

1/3 2/3 2/3

( , ) exp( ( ) | |)

2.1056 ( )( ) ( )

2 ( ) ( )

2.1056 ( )1(0) ( )

2 3 (1/ 3) ( )

H T

Hp T p

HH H p

E

S k t D k k t

Vk nC D k nC

V c k

VJ J t nC

L V t

Page 40: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 41: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Mean square displacement pf a tagged paricle may be obtained from the collective dynamics through the identity

Explicitly:

2

2 2

2 3/5 3/5

2

2/31/3

ˆ ˆ1 ( ,0) ( , )( ) (0)

ˆ( , ) ( ,0) ( , )

2( ) (0) (3 / 5)

with =1.05282

with

BE

p

H

S k S k tx t x dk

n k

S k t n k n k t

ktx t x t

mnc nc

V

c V

Page 42: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 43: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.
Page 44: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Concluding remarks:

1. For typical hamiltonian systems in 1d the dominant transport properties can be expressed in terms of thermodynamic properties alone. The long time and small wave number behavior is known exactly in terms of the Prähofer-Spohn scaling functions.

Page 45: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Concluding remarks:

1. For typical hamiltonian systems in 1d the dominant transport properties can be expressed in terms of thermodynamic properties alone. The long time and small wave number behavior is known exactly in terms of the Prähofer-Spohn scaling functions.

2. The corrections to the leading terms are appreciable.This is becausecouplings of e.g. a sound mode to two opposite type sound modes or two heat modes decay only slightly faster with time than couplings to two equal type sound modes. The exponents of these correction terms can be obtained exactly, but the amplitudes only approximately.

Page 46: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

Concluding remarks:

1. For typical hamiltonian systems in 1d the dominant transport properties can be expressed in terms of thermodynamic properties alone. The long time and small wave number behavior is known exactly in terms of the Prähofer-Spohn scaling functions.

2. The corrections to the leading terms are appreciable.This is becausecouplings of e.g. a sound mode to two opposite type sound modes or two heat modes decay only slightly faster with time than couplings to two equal type sound modes. The exponents of these correction terms can be obtained exactly, but the amplitudes only approximately.

3. Previous mode-coupling theories by Delfini et al. give a very good approximation for weakly anharmonic potentials. They require corrections otherwise, as energy density contributes to the sound modes .

Page 47: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

4. Sound damping becomes almost normal if This happens for

In fact sound attenuation is still, logarithmically,

superdiffusive. Heat conduction becomes more strongly superdiffusive.No more KPZ.

0.V

0

0.

s

c n

n

Page 48: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

4. Sound damping becomes almost normal if This happens for

In fact sound attenuation is still, logarithmically,

superdiffusive. Heat conduction becomes more strongly superdiffusive.No more KPZ.

5. In spite of the diverging Green-Kubo integrals the transport coefficients in the nonlinear hydrodynamic equations need not be infinite.The long time tails in the current-current correlation functions aredue to the nonlinearities in the hydrodynamic equations. Whether or not the transport coefficients in the nonlinear hydrodynamic equationsare in fact divergent to my opinion is an open question.

0.V

0

0.

s

c n

n

Page 49: Exact results for transport properties of one-dimensional hamiltonian systems Henk van Beijeren Institute for Theoretical Physics Utrecht University.

4. Sound damping becomes almost normal if This happens for

In fact sound attenuation is still, logarithmically,

superdiffusive. Heat conduction becomes more strongly superdiffusive.No more KPZ.

5. In spite of the diverging Green-Kubo integrals the transport coefficients in the nonlinear hydrodynamic equations need not be infinite.The long time tails in the current-current correlation functions aredue to the nonlinearities in the hydrodynamic equations. Whether or not the transport coefficients in the nonlinear hydrodynamic equationsare in fact divergent to my opinion is an open question.

Ref.: HvB arXiv:1106.3298v3 [cond-mat.stat-mech], PRL 108.180601 (2012)

0.V

0

0.

s

c n

n