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Time-Correlation Functions. Charusita Chakravarty Indian Institute of Technology Delhi. Organization. Time Correlation Function: Definitions and Properties Linear Response Theory : Fluctuation-Dissipation Theorem Onsager’s Regression Hypothesis Response Functions Chemical Kinetics

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time correlation functions
Time-Correlation Functions

Charusita Chakravarty

Indian Institute of Technology Delhi

organization
Organization
  • Time Correlation Function: Definitions and Properties
  • Linear Response Theory :
    • Fluctuation-Dissipation Theorem
    • Onsager’s Regression Hypothesis
    • Response Functions
  • Chemical Kinetics
  • Transport Properties
    • Self-diffusivity
    • Ionic Conductivity
    • Viscosity
  • Absorption of Electromagnetic Radiation
  • Space-time Correlation Functions
time correlation functions1
Time Correlation Functions
  • Time-dependent trajectory of a classical system:
  • Since the classical system is deterministic, a time-dependent

quantity can be written as :

  • Correlation function as atime average over a trajectory:
slide4

Time-correlation functions can be written as ensemble averages by summing over all possible initial conditions:

Probability of observing a microstate

  • Limiting behaviour
  • Alternative definition of time-correlation function in terms of deviations of time-dependent properties from mean values.
slide5

Stationarity for systems with continuous interparticle forces, TCFs must be even functions of the time delay:

  • Time-derivative with respect to time origins must be zero
  • Short-time expansion of autocorrelation functions
typical velocity autocorrelation function
Typical velocity autocorrelation function

Zero slope at origin

Rebound from

Solvent cage

D. Chandler

small deviations from equilibrium classical linear response theory
Small Deviations from Equilibrium:Classical Linear Response Theory
  • Apply a weak perturbing field f to the system that couples to some physical property of the system
    • Electric field/ionic motion
    • Electromagnetic radiation/charges or molecular dipoles

System allowed to relax freely

Equilibrium

established

System prepared

in non-equilibrium

state by applying

perturbing field f

B(t)

D. Chandler

time=0

linear response theory contd
Linear Response Theory (contd.)

Let the time-dependent perturbation be such that

At t=0, the probability of observing a configuration:

How will the observed value of a quantity B(t) change with time when the perturbation is turned off at time t=0?

Time-dependent value of

B for a given set of initial

conditions

Integrate over initial

conditions of perturbed

system at t=0

linear response theory contd1
Linear Response Theory (contd.)

Consider the effect of perturbations only upto first-order:

D. Chandler, Introduction to Modern Statistical Mechanics

slide10

For t>0, the observed value of B will be given by

Multiply the numerator and denominator by (1/Q) where Q is the partition function of the unperturbed system

Denominator

slide11

Numerator:

Time-dependent behaviour of B:

onsager s regression hypothesis
Onsager’s regression hypothesis

The relaxation of macroscopic non-equilibrium disturbances is governed by the same dynamics as the regression of spontaneous microscopic fluctuations in the equilibrium system

Macroscopic

relaxation

Equilibrium

Time-correlation

function

response functions
Response Functions

For a weak perturbation , we can define a response function:

The response of the system to an impulsive perturbation:

To correspond to the linear response situation studied earlier:

slide14

Provides an alternative route to evaluate the time-dependent response as an integral over a time-correlation function

transport properties
Transport Properties
  • Flux=-transport coefficient X gradient
  • Non-equilibrium MD: create a perturbation and watch the time-dependent response
  • Equilibrium MD: measure the time-correlation function
self diffusivity
Self-diffusivity

Consider an external field that couples to the position of a tagged particle such that

The steady state velocity of the tagged particle will then be:

slide17

Can one identify the mobility, as defined below, with the macroscopic velocity:

Fick’s Law:

Flux of diffusing species= Diffusivity X Concentration gradient

Combining with the equation of continuity derived by imposing conservation of mass of tagged particles, gives :

Diffusion Equation

slide18

If the original concentration profile is a delta-function, then the concentration profile at a later time (t) will be a d-dimensional Gaussian:

Consider the second-moment of one-dimensional distribution:

Einstein relation

By writing the displacement as

one can show that

This definition of self-diffusivity will be the same as that of the mobility derived from linear reponse theory

ionic conductivity
Ionic Conductivity

Consider an external electric field Ex applied to an ionic melt. Under steady state conditions, the system will develop a net current:

The ionic conductivity per unit volume, s, will be defined by:

Effect of the external field on the Hamiltonian:

When the field is switched off at t=0, the current will decay towards the zero value characteristic of the unperturbed system.

Rate of change of net

dipole moment

Charge on

particle i

velocity

particle i

slide20

To apply the relation:

to compute the time-dependent decay of the current, we set:

to obtain:

Conductivity per unit volume will then be given by:

linear response theory and spectroscopy
Linear Response Theory and Spectroscopy
  • Let f(t) be a periodic, monochromatic disturbance:
  • Time-dependent energy:
  • Rate of absorption of energy:
linear response theory and spectroscopy contd
Linear Response Theory and Spectroscopy (contd.)
  • Time-dependent value of A reflects response to applied field:
  • The average rate of absorption or energy dissipation is given by:
  • For a periodic field:
linear response theory and spectroscopy contd1
Linear Response Theory and Spectroscopy (contd.)
  • Fourier transform of response function is defined as:
  • Compute average rate of absorption of energy over one time period T=2p/w
linear response theory and spectroscopy contd2
Linear Response Theory and Spectroscopy (contd.)
  • Using linear response theory
  • Absorption spectrum
simple harmonic oscillator
Simple Harmonic Oscillator
  • Let the quantity A coupled to the periodic perturbation obey SHO dynamics:
  • Time-dependence of A:
  • Absorption spectrum
infrared absorption by a dilute gas of polar molecules
Infrared Absorption by a Dilute Gas of Polar Molecules
  • X-component of total dipole moment will couple to oscillating electric field .
  • Independent dipole approximation:
  • Perturbed Hamiltonian:
  • Change in dipole moment with time:
  • Thermal distribution of angular velocities, P(w), will be reflected in absorption profile
space time correlation functions neutron scattering experiments
Space-Time Correlation Functions:Neutron Scattering Experiments

Number density at a point r at a time t:

Conservation of particle number:

Van Hove Correlation Function for a homogeneous fluid:

space time correlation functions contd
Space-Time Correlation Functions (contd)

Can divide the double summation into two parts:

Self contribution

Distinct contribution

Fourier transform of the number density

space time correlation functions contd1
Space-Time Correlation Functions (contd.)

Intermediate scattering function

Static structure factor

Dynamic structure factor

Sum rule

references
References
  • D. Frenkel and B. Smit, Understanding Molecular Simulations: From Algorithms to Applications
  • D. C. Rapaport, The Art of Molecular Dynamics Simulation (Details of how to implement algorithms for molecular systems)
  • M. P. Allen and D. J. Tildesley, Computer Simulation of Liquids (SHAKE, RATTLE, Ewald subroutines)
  • Haile, Molecular Dynamics Simulation: Elementary Methods
  • D. Chandler, Introduction to Modern Statistical Mechanics (Linear Response Theory)
  • D. A. McQuarrie, Statistical Mechanics (Spectroscopic Properties)
  • J.-P. Hansen and I. R. McDonald, The Theory of Simple Liquids (Almost everything)