# Source code for MDAnalysis.lib.correlations

```
# -*- Mode: python; tab-width: 4; indent-tabs-mode:nil; coding:utf-8 -*-
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# MDAnalysis --- https://www.mdanalysis.org
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# (see the file AUTHORS for the full list of names)
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#
# Please cite your use of MDAnalysis in published work:
#
# R. J. Gowers, M. Linke, J. Barnoud, T. J. E. Reddy, M. N. Melo, S. L. Seyler,
# D. L. Dotson, J. Domanski, S. Buchoux, I. M. Kenney, and O. Beckstein.
# MDAnalysis: A Python package for the rapid analysis of molecular dynamics
# simulations. In S. Benthall and S. Rostrup editors, Proceedings of the 15th
# Python in Science Conference, pages 102-109, Austin, TX, 2016. SciPy.
# doi: 10.25080/majora-629e541a-00e
#
# N. Michaud-Agrawal, E. J. Denning, T. B. Woolf, and O. Beckstein.
# MDAnalysis: A Toolkit for the Analysis of Molecular Dynamics Simulations.
# J. Comput. Chem. 32 (2011), 2319--2327, doi:10.1002/jcc.21787
#
"""Correlations utilities --- :mod:`MDAnalysis.lib.correlations`
=================================================================================
:Authors: Paul Smith & Mateusz Bieniek
:Year: 2020
:Copyright: GNU Public License v2
.. versionadded:: 1.0.0
This module is primarily for internal use by other analysis modules. It
provides functionality for calculating the time autocorrelation function
of a binary variable (i.e one that is either true or false at each
frame for a given atom/molecule/set of molecules). This module includes
functions for calculating both the time continuous autocorrelation and
the intermittent autocorrelation. The function :func:`autocorrelation`
calculates the continuous autocorrelation only. The data may be
pre-processed using the function :func:`intermittency` in order to
acount for intermittency before passing the results to
:func:`autocorrelation`.
This module is inspired by seemingly disparate analyses that rely on the same
underlying calculation, including the survival probability of water around
proteins [Araya-Secchi2014]_, hydrogen bond lifetimes [Gowers2015]_, [Araya-Secchi2014]_,
and the rate of cholesterol flip-flop in lipid bilayers [Gu2019]_.
.. seeAlso::
Analysis tools that make use of modules:
* :class:`MDAnalysis.analysis.waterdynamics.SurvivalProbability`
Calculates the continuous or intermittent survival probability
of an atom group in a region of interest.
* :class:`MDAnalysis.analysis.hbonds.hbond_analysis`
Calculates the continuous or intermittent hydrogen bond
lifetime.
.. rubric:: References
.. [Gu2019] Gu, R.-X.; Baoukina, S.; Tieleman, D. P. (2019)
Cholesterol Flip-Flop in Heterogeneous Membranes.
J. Chem. Theory Comput. 15 (3), 2064–2070.
https://doi.org/10.1021/acs.jctc.8b00933.
"""
from __future__ import absolute_import, division
import numpy as np
from copy import deepcopy
[docs]def autocorrelation(list_of_sets, tau_max, window_step=1):
r"""Implementation of a discrete autocorrelation function.
The autocorrelation of a property :math:`x` from a time :math:`t=t_0` to :math:`t=t_0 + \tau`
is given by:
.. math::
C(\tau) = \langle \frac{ x(t_0)x(t_0 +\tau) }{ x(t_0)x(t_0) } \rangle
where :math:`x` may represent any property of a particle, such as velocity or
potential energy.
This function is an implementation of a special case of the time
autocorrelation function in which the property under consideration can
be encoded with indicator variables, :math:`0` and :math:`1`, to represent the binary
state of said property. This special case is often referred to as the
survival probability (:math:`S(\tau)`). As an example, in calculating the survival
probability of water molecules within 5 Å of a protein, each water
molecule will either be within this cutoff range (:math:`1`) or not (:math:`0`). The
total number of water molecules within the cutoff at time :math:`t_0` will be
given by :math:`N(t_0)`. Other cases include the Hydrogen Bond Lifetime as
well as the translocation rate of cholesterol across a bilayer.
The survival probability of a property of a set of particles is
given by:
.. math::
S(\tau) = \langle \frac{ N(t_0, t_0 + \tau )} { N(t_0) }\rangle
where :math:`N(t0)` is the number of particles at time :math:`t_0` for which the feature
is observed, and :math:`N(t0, t_0 + \tau)` is the number of particles for which
this feature is present at every frame from :math:`t_0` to :math:`N(t0, t_0 + \tau)`.
The angular brackets represent an average over all time origins, :math:`t_0`.
See [Araya-Secchi2014]_ for a description survival probability.
Parameters
----------
list_of_sets : list
List of sets. Each set corresponds to data from a single frame. Each element in a set
may be, for example, an atom id or a tuple of atoms ids. In the case of calculating the
survival probability of water around a protein, these atom ids in a given set will be
those of the atoms which are within a cutoff distance of the protein at a given frame.
tau_max : int
The last tau (lag time, inclusive) for which to calculate the autocorrelation. e.g if tau_max = 20,
the survival probability will be calculated over 20 frames.
window_step : int, optional
The step size for t0 to perform autocorrelation. Ideally, window_step will be larger than
tau_max to ensure independence of each window for which the calculation is performed.
Default is 1.
Returns
--------
tau_timeseries : list of int
the values of tau for which the autocorrelation was calculated
timeseries : list of int
the autocorelation values for each of the tau values
timeseries_data : list of list of int
the raw data from which the autocorrelation is computed, i.e :math:`S(\tau)` at each window.
This allows the time dependant evolution of :math:`S(\tau)` to be investigated.
.. versionadded:: 0.19.2
"""
# check types
if (type(list_of_sets) != list and len(list_of_sets) != 0) or type(list_of_sets[0]) != set:
raise TypeError("list_of_sets must be a one-dimensional list of sets") # pragma: no cover
# Check dimensions of parameters
if len(list_of_sets) < tau_max:
raise ValueError("tau_max cannot be greater than the length of list_of_sets") # pragma: no cover
tau_timeseries = list(range(1, tau_max + 1))
timeseries_data = [[] for _ in range(tau_max)]
# calculate autocorrelation
for t in range(0, len(list_of_sets), window_step):
Nt = len(list_of_sets[t])
if Nt == 0:
continue
for tau in tau_timeseries:
if t + tau >= len(list_of_sets):
break
# continuous: IDs that survive from t to t + tau and at every frame in between
Ntau = len(set.intersection(*list_of_sets[t:t + tau + 1]))
timeseries_data[tau - 1].append(Ntau / float(Nt))
timeseries = [np.mean(x) for x in timeseries_data]
# at time 0 the value has to be one
tau_timeseries.insert(0, 0)
timeseries.insert(0, 1)
return tau_timeseries, timeseries, timeseries_data
[docs]def correct_intermittency(list_of_sets, intermittency):
r"""Preprocess data to allow intermittent behaviour prior to calling :func:`autocorrelation`.
Survival probabilty may be calculated either with a strict continuous requirement or
a less strict intermittency. If calculating the survival probability water around a
protein for example, in the former case the water must be within a cutoff distance
of the protein at every frame from :math:`t_0` to :math:`t_0 + \tau` in order for it to be considered
present at :math:`t_0 + \tau`. In the intermittent case, the water molecule is allowed to
leave the region of interest for up to a specified consecutive number of frames whilst still
being considered present at :math:`t_0 + \tau`.
This function pre-processes data, such as the atom ids of water molecules within a cutoff
distance of a protein at each frame, in order to allow for intermittent behaviour, with a
single pass over the data.
For example, if an atom is absent for a number of frames equal or smaller than the parameter
:attr:`intermittency`, then this absence will be removed and thus the atom is considered to have
not left.
e.g 7,A,A,7 with `intermittency=2` will be replaced by 7,7,7,7, where A=absence.
The returned data can be used as input to the function :func:`autocorrelation` in order
to calculate the survival probability with a given intermittency.
See [Gowers2015]_ for a description of
intermittency in the calculation of hydrogen bond lifetimes.
# TODO - is intermittency consitent with list of sets of sets? (hydrogen bonds)
Parameters
----------
list_of_sets: list
In the simple case of e.g survival probability, a list of sets of atom ids present at each frame, where a
single set contains atom ids at a given frame, e.g [{0, 1}, {0}, {0}, {0, 1}]
intermittency : int
The maximum gap allowed. The default `intermittency=0` means that if the datapoint is missing at any frame, no
changes are made to the data. With the value of `intermittency=2`, all datapoints missing for up to two
consecutive frames will be instead be considered present.
Returns
-------
list_of_sets: list
returns a new list with the IDs with added IDs which disappeared for <= :attr:`intermittency`.
e.g If [{0, 1}, {0}, {0}, {0, 1}] is a list of sets of atom ids present at each frame and `intermittency=2`,
both atoms will be considered present throughout and thus the returned list of sets will be
[{0, 1}, {0, 1}, {0, 1}, {0, 1}].
"""
if intermittency == 0:
return list_of_sets
list_of_sets = deepcopy(list_of_sets)
for i, ids in enumerate(list_of_sets):
# initially update each frame as seen 0 ago (now)
seen_frames_ago = {i: 0 for i in ids}
for j in range(1, intermittency + 2):
for atomid in seen_frames_ago.keys():
# no more frames
if i + j >= len(list_of_sets):
continue
# if the atom is absent now
if not atomid in list_of_sets[i + j]:
# increase its absence counter
seen_frames_ago[atomid] += 1
continue
# the atom is found
if seen_frames_ago[atomid] == 0:
# the atom was present in the last frame
continue
# it was absent more times than allowed
if seen_frames_ago[atomid] > intermittency:
continue
# the atom was absent but returned (within <= intermittency_value)
# add it to the frames where it was absent.
# Introduce the corrections.
for k in range(seen_frames_ago[atomid], 0, -1):
list_of_sets[i + j - k].add(atomid)
seen_frames_ago[atomid] = 0
return list_of_sets
```