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corfun.f90
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corfun.f90
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! corfun.f90
! Time correlation function, directly and by FFT
PROGRAM corfun
!------------------------------------------------------------------------------------------------!
! This software was written in 2016/17 !
! by Michael P. Allen <[email protected]>/<[email protected]> !
! and Dominic J. Tildesley <[email protected]> ("the authors"), !
! to accompany the book "Computer Simulation of Liquids", second edition, 2017 ("the text"), !
! published by Oxford University Press ("the publishers"). !
! !
! LICENCE !
! Creative Commons CC0 Public Domain Dedication. !
! To the extent possible under law, the authors have dedicated all copyright and related !
! and neighboring rights to this software to the PUBLIC domain worldwide. !
! This software is distributed without any warranty. !
! You should have received a copy of the CC0 Public Domain Dedication along with this software. !
! If not, see <http://creativecommons.org/publicdomain/zero/1.0/>. !
! !
! DISCLAIMER !
! The authors and publishers make no warranties about the software, and disclaim liability !
! for all uses of the software, to the fullest extent permitted by applicable law. !
! The authors and publishers do not recommend use of this software for any purpose. !
! It is made freely available, solely to clarify points made in the text. When using or citing !
! the software, you should not imply endorsement by the authors or publishers. !
!------------------------------------------------------------------------------------------------!
! Define underlying process by generalized Langevin equation
! with memory function expressed as a decaying exponential function
! See G Ciccotti and JP Ryckaert Mol Phys 40 141 (1980)
! and AD Baczewski and SD Bond J Chem Phys 139 044107 (2013)
! We assume that the program is linked with the FFTW library (version 3)
! but it could easily be adapted to use a different library
! With older FFT routines it was necessary to transform a number of points = exact power of 2
! which, for us, would mean nstep = 2**j (for integer j) and fft_len=2*nstep
! This is no longer true, so we do not restrict nstep in this way,
! but the transform should be more efficient if nstep happens to take such values
! Advantage can be taken of the fact that the data is real, but for clarity
! we just use the complex FFT with imaginary parts of the data set to zero
USE, INTRINSIC :: iso_fortran_env, ONLY : input_unit, output_unit, error_unit, iostat_end, iostat_eor, &
& COMPILER_VERSION, COMPILER_OPTIONS
USE, INTRINSIC :: iso_c_binding
USE maths_module, ONLY : random_normal, expm1
IMPLICIT NONE
INCLUDE 'fftw3.f03'
REAL :: m ! Memory function coefficients
REAL :: kappa ! Memory function decay rates
REAL :: s ! GLE auxiliary variables
REAL :: delta ! Time step
REAL :: vt ! Velocity at time t
REAL, DIMENSION(:), ALLOCATABLE :: v ! Stored velocities (nstep)
REAL, DIMENSION(:), ALLOCATABLE :: v0 ! Stored velocity origins (n0)
INTEGER, DIMENSION(:), ALLOCATABLE :: t0 ! Times of origins (n0)
REAL, DIMENSION(:), ALLOCATABLE :: c ! Velocity correlation function (direct method) (0:nt)
REAL, DIMENSION(:), ALLOCATABLE :: c_fft ! Velocity correlation function (FFT method) (0:nt)
REAL, DIMENSION(:), ALLOCATABLE :: n ! Normalizing function (0:nt)
INTEGER :: nt ! Number of timesteps to correlate
INTEGER :: nstep ! Number of timesteps in run
INTEGER :: nequil ! Number of equilibration timesteps
INTEGER :: n0 ! Number of time origins to store
INTEGER :: origin_interval ! Interval for time origins
INTEGER :: dt ! Time difference
INTEGER :: t ! Time (equivalent to step number in file)
LOGICAL :: full
INTEGER :: k, mk, nk
INTEGER :: unit, ioerr
REAL :: temperature, stddev, x, e, b, d
REAL :: cpu_1, cpu_2, cpu_3, cpu_4
INTEGER(C_INT) :: fft_len ! the number of points for FFT
COMPLEX(C_DOUBLE_COMPLEX), DIMENSION(:), ALLOCATABLE :: fft_inp ! data to be transformed (0:fft_len-1)
COMPLEX(C_DOUBLE_COMPLEX), DIMENSION(:), ALLOCATABLE :: fft_out ! data to be transformed (0:fft_len-1)
TYPE(C_PTR) :: fft_plan ! plan needed for FFTW
NAMELIST /nml/ nt, origin_interval, nstep, nequil, delta, temperature
WRITE ( unit=output_unit, fmt='(a)' ) 'corfun'
WRITE ( unit=output_unit, fmt='(2a)' ) 'Compiler: ', COMPILER_VERSION()
WRITE ( unit=output_unit, fmt='(2a/)' ) 'Options: ', COMPILER_OPTIONS()
WRITE( unit=output_unit, fmt='(a)' ) 'Illustrates methods for calculating time correlation functions'
WRITE( unit=output_unit, fmt='(a)' ) 'using synthetic data from a generalized Langevin equation'
CALL RANDOM_INIT ( .FALSE., .TRUE. ) ! Initialize random number generator
! Example default values
! Agreement (to numerical precision) of direct and FFT methods is expected if origin_interval=1
nt = 1000 ! Max time for correlation function
origin_interval = 1 ! This could reasonably be increased to 10 or 20 to improve efficiency
nstep = 2**20 ! Number of steps, about a million for example
nequil = 10000 ! Number of equilibration timesteps
delta = 0.01 ! Timestep for simulation
temperature = 1.0 ! Temperature for simulation
! Namelist from standard input
READ ( unit=input_unit, nml=nml, iostat=ioerr )
IF ( ioerr /= 0 ) THEN
WRITE ( unit=error_unit, fmt='(a,i15)') 'Error reading namelist nml from standard input', ioerr
IF ( ioerr == iostat_eor ) WRITE ( unit=error_unit, fmt='(a)') 'End of record'
IF ( ioerr == iostat_end ) WRITE ( unit=error_unit, fmt='(a)') 'End of file'
STOP 'Error in corfun'
END IF
n0 = nt / origin_interval + 1
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Number of steps in run = ', nstep
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Equilibration steps = ', nequil
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Max correlation time nt = ', nt
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Origin interval = ', origin_interval
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Number of time origins n0 = ', n0
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Time step delta = ', delta
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Temperature = ', temperature
ALLOCATE ( v(nstep), v0(n0), t0(n0) )
ALLOCATE ( c(0:nt), c_fft(0:nt), n(0:nt) )
fft_len = 2*nstep ! Actual length of FFT data
ALLOCATE ( fft_inp(0:fft_len-1), fft_out(0:fft_len-1) )
! The memory function model is defined here
! Values used by Baczewski and Bond in their example are
! (m,kappa)
! (1.0,1.0) (underdamped)
! (0.5,2.0) (critically damped)
! (0.25,4.0) (overdamped)
m = 1.0
kappa = 1.0
WRITE ( unit=output_unit, fmt='(a,t40,*(f15.6))' ) 'm = ', m
WRITE ( unit=output_unit, fmt='(a,t40,*(f15.6))' ) 'kappa = ', kappa
! Coefficients used in algorithm
x = delta*kappa
e = EXP(-x) ! theta in B&B paper
b = -expm1(-2*x) ! 1-exp(-2*x), preserving accuracy for small x
d = -expm1(-x) ! 1-exp(-x), preserving accuracy for small x
b = SQRT ( b )
b = b * SQRT ( kappa/2.0 ) ! alpha in B&B paper
stddev = SQRT(2.0*temperature)
! Data generation
CALL CPU_TIME ( cpu_1 )
! Initial values
vt = 0.0
s = 0.0
DO t = -nequil, nstep ! Loop over steps including an equilibration period
! Velocity Verlet type algorithm for vt and auxiliary variable s
vt = vt + 0.5 * delta * s
s = e * s - d * m * vt + b * SQRT(m) * random_normal ( 0.0, stddev )
vt = vt + 0.5*delta*s
IF ( t > 0 ) v(t) = vt ! Store velocities, after equilibration
END DO ! End loop over steps including an equilibration period
CALL CPU_TIME ( cpu_2 )
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'CPU time to generate data = ', cpu_2-cpu_1
! Data analysis (direct method)
c(:) = 0.0
n(:) = 0.0
mk = 0 ! Storage location of time origin
full = .FALSE.
DO t = 1, nstep ! Main loop correlating data
IF ( MOD(t-1,origin_interval) == 0 ) THEN
mk = mk + 1
IF ( mk > n0 ) THEN
full = .TRUE.
mk = mk - n0 ! Overwrite older values
END IF
t0(mk) = t ! Store time origins
v0(mk) = v(t) ! Store velocity at time origins
END IF
IF ( full ) THEN
nk = n0 ! Correlate with all stored time origins
ELSE
nk = mk ! Correlate with those stored so far
END IF
DO k = 1, nk ! Loop over time origins
dt = t - t0(k)
IF ( dt >= 0 .AND. dt <= nt ) THEN ! Check that dt is in range
c(dt) = c(dt) + v(t) * v0(k) ! Increment correlation function
n(dt) = n(dt) + 1.0 ! Increment normalizing factor
END IF ! End check that dt is in range
END DO ! End loop over time origins
END DO ! End main loop correlating data
IF ( ANY ( n(:) < 0.5 ) ) THEN ! should never happen
WRITE ( unit=error_unit, fmt='(a)') 'Normalization array error'
STOP 'Error in corfun'
END IF
c(:) = c(:) / n(:) ! Normalise by number of increments
CALL CPU_TIME ( cpu_3 )
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'CPU time for direct method = ', cpu_3-cpu_2
! Data analysis (FFT method)
! Prepare data for FFT
fft_inp = CMPLX(0.0) ! Fill input array with zeros
fft_inp(0:nstep-1) = CMPLX(v) ! Put data into first part (real only)
! Forward FFT
fft_plan = fftw_plan_dft_1d ( fft_len, fft_inp, fft_out, FFTW_FORWARD, FFTW_ESTIMATE) ! Set up plan
CALL fftw_execute_dft ( fft_plan, fft_inp, fft_out ) ! Execute FFT
CALL fftw_destroy_plan ( fft_plan ) ! Release plan
fft_out = fft_out * CONJG ( fft_out ) ! Square modulus
! Reverse FFT
fft_plan = fftw_plan_dft_1d ( fft_len, fft_out, fft_inp, FFTW_BACKWARD, FFTW_ESTIMATE) ! Set up plan
CALL fftw_execute_dft ( fft_plan, fft_out, fft_inp ) ! Execute FFT
CALL fftw_destroy_plan ( fft_plan ) ! Release plan
fft_inp = fft_inp / REAL ( fft_len ) ! Normalization factor associated with FFT itself
n(:) = [ ( nstep-t, t = 0, nt ) ] ! Normalization factors associated with number of time origins
IF ( ANY ( n(:) < 0.5 ) ) THEN ! should never happen
WRITE ( unit=error_unit, fmt='(a)') 'Normalization array error'
STOP 'Error in corfun'
END IF
c_fft = REAL ( fft_inp(0:nt) ) / n(:) ! Apply normalization associated with number of time origins
CALL CPU_TIME ( cpu_4 )
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'CPU time for FFT method = ', cpu_4-cpu_3
WRITE ( unit=output_unit, fmt='(a)' ) 'Output to corfun.out'
OPEN ( newunit=unit, file='corfun.out', status='replace', iostat=ioerr )
IF ( ioerr /= 0 ) THEN
WRITE ( unit=error_unit, fmt='(a,i15)') 'Error opening file', ioerr
STOP 'Error in corfun'
END IF
DO t = 0, nt
WRITE ( unit=unit, fmt='(i10,3f15.8)' ) t, c(t), c_fft(t), c_exact(t*delta)
END DO
CLOSE(unit=unit)
DEALLOCATE ( v, v0, t0, c, c_fft, n )
DEALLOCATE ( fft_inp, fft_out )
CONTAINS
FUNCTION c_exact ( t ) RESULT ( c )
IMPLICIT NONE
REAL :: c ! Returns analytically known correlation function, for
REAL, INTENT(in) :: t ! given time
! See AD Baczewski and SD Bond J Chem Phys 139 044107 (2013)
! In general the exact correlation function may be obtained from the inverse Laplace transform
! C(s) = (kT/m) * 1 / ( s + M(s) ) where both C(t) and M(t) are sums of exponentials in t
! M(s) = sum_p m_p*kappa_p / (s+kappa_p) p = 1..Np (note amplitude mp*kappa_p)
! C(s) = sum_p c_p / (s+k_p) p = 1..Np+1
! The coefficients c_p and k_p may be determined in terms of the m_p and kappa_p
! by solving an equation of order Np+1 and using partial fractions
! Here we just do this for the simplest case Np=1
! Agreement with the simulated function is only expected to within statistical error
REAL :: del, omega, kp, km, cp, cm
IF ( kappa > 4.0 * m ) THEN ! Real roots
del = SQRT ( 0.25*kappa**2 - m*kappa )
kp = 0.5*kappa + del
km = 0.5*kappa - del
cp = -km/(kp-km)
cm = kp/(kp-km)
c = cp*EXP(-kp*t) + cm*EXP(-km*t)
ELSE ! Complex roots
omega = SQRT ( m*kappa - 0.25*kappa**2 )
c = EXP(-0.5*kappa*t) * ( COS(omega*t) + (0.5*kappa/omega)*SIN(omega*t) )
END IF
END FUNCTION c_exact
END PROGRAM corfun