def _estimate(self, iterable, **kw):
covar = LaggedCovariance(c00=True,
c0t=True,
ctt=False,
remove_data_mean=True,
reversible=self.reversible,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=self.weights,
ncov_max=self.ncov_max)
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._logger_is_active(self._loglevel_DEBUG):
self.logger.debug(
"Running TICA with tau=%i; Estimating two covariance matrices"
" with dimension (%i, %i)", self._lag, indim, indim)
covar.estimate(iterable, chunksize=self.chunksize, **kw)
self.model.update_model_params(mean=covar.mean,
cov=covar.C00_,
cov_tau=covar.C0t_)
self._diagonalize()
return self.model
def _init_covar(self, partial=False):
# in case of partial, we need to store the state of running covar in this estimator.
args = dict(c00=True,
c0t=True,
ctt=True,
remove_data_mean=True,
reversible=False,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=None,
ncov_max=self.ncov_max)
if partial:
if not hasattr(self, '_covar') or self._covar is None:
self._covar = LaggedCovariance(**args)
# remember running covar for serialization
assert '_covar' not in self.__serialize_fields
self.__serialize_fields.append('_covar')
return self._covar
elif not partial:
# if the previous estimation was a partial_fit, we might have a running covar object,
# which we can safely omit now.
if '_covar' in self.__serialize_fields:
self.__serialize_fields.remove('_covar')
return LaggedCovariance(**args)
def __init__(self,
lag,
epsilon=1e-6,
stride=1,
skip=0,
chunksize=None,
ncov_max=float('inf')):
super(_KoopmanEstimator, self).__init__(chunksize=chunksize)
self._covar = LaggedCovariance(c00=True,
c0t=True,
remove_data_mean=True,
reversible=False,
lag=lag,
bessel=False,
stride=stride,
skip=skip,
ncov_max=ncov_max)
self.set_params(lag=lag,
epsilon=epsilon,
stride=stride,
skip=skip,
ncov_max=ncov_max)
self._estimation_finished = False
def koopman_est(x, y, t):
'''
Description:
Function that calculates the Koopman estimators that satisfy the functions:
chi(x_{t+1}) = (K_xx.T)(chi(x_t))
chi(y_{t+1}) = (K_xy.T)(chi(y_t))
Parameters:
x,y: the matrices we want estimate the operator for
t: timelag
Returns:
Two Koopman matrices that solve the above equation
'''
chi_data, gamma_data = whitening(x, y)
chi_data = chi(x)
n = len(x)
chi_0 = chi_data[:n-t]
chi_t = chi_data[t:]
gamma_t = gamma(y)[t:]
# K_xx = np.linalg.lstsq(chi_0, chi_t)[0]
K_xy = np.linalg.lstsq(chi_0, gamma_t)[0]
obj_x = LC(c0t = True, lag = t)
obj_x.fit(chi(x))
C_00, C_01 = (obj_x.C00_, obj_x.C0t_)
K_xx = np.linalg.inv(C_00).dot(C_01)
# K_xy = 0
return (K_xx, K_xy)
def partial_fit(self, X):
""" incrementally update the covariances and mean.
Parameters
----------
X: array, list of arrays, PyEMMA reader
input data.
Notes
-----
The projection matrix is first being calculated upon its first access.
"""
from pyemma.coordinates import source
iterable = source(X)
if isinstance(self.dim, int):
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._covar is None:
self._covar = LaggedCovariance(c00=True,
c0t=True,
ctt=True,
remove_data_mean=True,
reversible=False,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=None,
ncov_max=self.ncov_max)
self._covar.partial_fit(iterable)
self._model.update_model_params(
mean_0=self._covar.mean, # TODO: inefficient, fixme
mean_t=self._covar.mean_tau,
C00=self._covar.C00_,
C0t=self._covar.C0t_,
Ctt=self._covar.Ctt_)
self._estimated = False
if '_covar' not in self.__serialize_fields:
self.__serialize_fields.append('_covar')
return self
def _estimate(self, iterable, **kw):
self._covar = LaggedCovariance(c00=True,
c0t=True,
ctt=True,
remove_data_mean=True,
reversible=False,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=None,
ncov_max=self.ncov_max)
indim = iterable.dimension()
if isinstance(self.dim, int) and not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._logger_is_active(self._loglevel_DEBUG):
self.logger.debug(
"Running VAMP with tau=%i; Estimating two covariance matrices"
" with dimension (%i, %i)" % (self._lag, indim, indim))
self._covar.estimate(iterable, **kw)
self._model.update_model_params(mean_0=self._covar.mean,
mean_t=self._covar.mean_tau,
C00=self._covar.C00_,
C0t=self._covar.C0t_,
Ctt=self._covar.Ctt_)
self.model._diagonalize()
# if the previous estimation was a partial_fit, we might have a running covar object, which we can safely omit now.
if '_covar' in self.__serialize_fields:
self.__serialize_fields.remove('_covar')
return self._model
class VAMP(StreamingEstimationTransformer, SerializableMixIn):
r"""Variational approach for Markov processes (VAMP)"""
__serialize_version = 0
__serialize_fields = []
def describe(self):
return "[VAMP, lag = %i; max. output dim. = %s]" % (self._lag,
str(self.dim))
def __init__(self,
lag,
dim=None,
scaling=None,
right=True,
epsilon=1e-6,
stride=1,
skip=0,
ncov_max=float('inf')):
r""" Variational approach for Markov processes (VAMP) [1]_.
Parameters
----------
lag : int
lag time
dim : float or int, default=None
Number of dimensions to keep:
* if dim is not set (None) all available ranks are kept:
`n_components == min(n_samples, n_uncorrelated_features)`
* if dim is an integer >= 1, this number specifies the number
of dimensions to keep.
* if dim is a float with ``0 < dim < 1``, select the number
of dimensions such that the amount of kinetic variance
that needs to be explained is greater than the percentage
specified by dim.
scaling : None or string
Scaling to be applied to the VAMP order parameters upon transformation
* None: no scaling will be applied, variance of the order parameters is 1
* 'kinetic map' or 'km': order parameters are scaled by singular value.
Only the left singular functions induce a kinetic map.
Therefore scaling='km' is only effective if `right` is False.
right : boolean
Whether to compute the right singular functions.
If `right==True`, `get_output()` will return the right singular
functions. Otherwise, `get_output()` will return the left singular
functions.
Beware that only `frames[tau:, :]` of each trajectory returned
by `get_output()` contain valid values of the right singular
functions. Conversely, only `frames[0:-tau, :]` of each
trajectory returned by `get_output()` contain valid values of
the left singular functions. The remaining frames might
possibly be interpreted as some extrapolation.
epsilon : float
eigenvalue cutoff. Eigenvalues of :math:`C_{00}` and :math:`C_{11}`
with norms <= epsilon will be cut off. The remaining number of
eigenvalues together with the value of `dim` define the size of the output.
stride: int, optional, default = 1
Use only every stride-th time step. By default, every time step is used.
skip : int, default=0
skip the first initial n frames per trajectory.
ncov_max : int, default=infinity
limit the memory usage of the algorithm from [3]_ to an amount that corresponds
to ncov_max additional copies of each correlation matrix
Notes
-----
VAMP is a method for dimensionality reduction of Markov processes.
The Koopman operator :math:`\mathcal{K}` is an integral operator
that describes conditional future expectation values. Let
:math:`p(\mathbf{x},\,\mathbf{y})` be the conditional probability
density of visiting an infinitesimal phase space volume around
point :math:`\mathbf{y}` at time :math:`t+\tau` given that the phase
space point :math:`\mathbf{x}` was visited at the earlier time
:math:`t`. Then the action of the Koopman operator on a function
:math:`f` can be written as follows:
.. math::
\mathcal{K}f=\int p(\mathbf{x},\,\mathbf{y})f(\mathbf{y})\,\mathrm{dy}=\mathbb{E}\left[f(\mathbf{x}_{t+\tau}\mid\mathbf{x}_{t}=\mathbf{x})\right]
The Koopman operator is defined without any reference to an
equilibrium distribution. Therefore it is well-defined in
situations where the dynamics is irreversible or/and non-stationary
such that no equilibrium distribution exists.
If we approximate :math:`f` by a linear superposition of ansatz
functions :math:`\boldsymbol{\chi}` of the conformational
degrees of freedom (features), the operator :math:`\mathcal{K}`
can be approximated by a (finite-dimensional) matrix :math:`\mathbf{K}`.
The approximation is computed as follows: From the time-dependent
input features :math:`\boldsymbol{\chi}(t)`, we compute the mean
:math:`\boldsymbol{\mu}_{0}` (:math:`\boldsymbol{\mu}_{1}`) from
all data excluding the last (first) :math:`\tau` steps of every
trajectory as follows:
.. math::
\boldsymbol{\mu}_{0} :=\frac{1}{T-\tau}\sum_{t=0}^{T-\tau}\boldsymbol{\chi}(t)
\boldsymbol{\mu}_{1} :=\frac{1}{T-\tau}\sum_{t=\tau}^{T}\boldsymbol{\chi}(t)
Next, we compute the instantaneous covariance matrices
:math:`\mathbf{C}_{00}` and :math:`\mathbf{C}_{11}` and the
time-lagged covariance matrix :math:`\mathbf{C}_{01}` as follows:
.. math::
\mathbf{C}_{00} :=\frac{1}{T-\tau}\sum_{t=0}^{T-\tau}\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{0}\right]\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{0}\right]
\mathbf{C}_{11} :=\frac{1}{T-\tau}\sum_{t=\tau}^{T}\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{1}\right]\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{1}\right]
\mathbf{C}_{01} :=\frac{1}{T-\tau}\sum_{t=0}^{T-\tau}\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{0}\right]\left[\boldsymbol{\chi}(t+\tau)-\boldsymbol{\mu}_{1}\right]
The Koopman matrix is then computed as follows:
.. math::
\mathbf{K}=\mathbf{C}_{00}^{-1}\mathbf{C}_{01}
It can be shown [1]_ that the leading singular functions of the
half-weighted Koopman matrix
.. math::
\bar{\mathbf{K}}:=\mathbf{C}_{00}^{-\frac{1}{2}}\mathbf{C}_{01}\mathbf{C}_{11}^{-\frac{1}{2}}
encode the best reduced dynamical model for the time series.
The singular functions can be computed by first performing the
singular value decomposition
.. math::
\bar{\mathbf{K}}=\mathbf{U}^{\prime}\mathbf{S}\mathbf{V}^{\prime}
and then mapping the input conformation to the left singular
functions :math:`\boldsymbol{\psi}` and right singular
functions :math:`\boldsymbol{\phi}` as follows:
.. math::
\boldsymbol{\psi}(t):=\mathbf{U}^{\prime\top}\mathbf{C}_{00}^{-\frac{1}{2}}\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{0}\right]
\boldsymbol{\phi}(t):=\mathbf{V}^{\prime\top}\mathbf{C}_{11}^{-\frac{1}{2}}\left[\boldsymbol{\chi}(t)-\boldsymbol{\mu}_{1}\right]
References
----------
.. [1] Wu, H. and Noe, F. 2017. Variational approach for learning Markov processes from time series data.
arXiv:1707.04659v1
.. [2] Noe, F. and Clementi, C. 2015. Kinetic distance and kinetic maps from molecular dynamics simulation.
J. Chem. Theory. Comput. doi:10.1021/acs.jctc.5b00553
.. [3] Chan, T. F., Golub G. H., LeVeque R. J. 1979. Updating formulae and pairwiese algorithms for
computing sample variances. Technical Report STAN-CS-79-773, Department of Computer Science, Stanford University.
"""
StreamingEstimationTransformer.__init__(self)
self.set_params(lag=lag,
dim=dim,
scaling=scaling,
right=right,
epsilon=epsilon,
stride=stride,
skip=skip,
ncov_max=ncov_max)
@property
def dim(self):
""" Number of dimensions to keep
* if dim is not set (None) all available ranks are kept:
`n_components == min(n_samples, n_features)`
* if dim is an integer >= 1, this number specifies the number
of dimensions to keep.
* if dim is a float with ``0 < dim < 1``, select the number
of dimensions such that the amount of kinetic variance
that needs to be explained is greater than the percentage
specified by dim.
"""
return self.model.dim
@dim.setter
def dim(self, value):
self.model.dim = value
@property
def epsilon(self):
"""singular value cutoff.
Singular values of :math:`C0` with norms <= epsilon will be cut off. The remaining number of
singular values define the size of the output.
"""
return self.model.epsilon
@epsilon.setter
def epsilon(self, value):
self.model.epsilon = value
@property
def scaling(self):
"""Scaling to be applied to the VAMP order parameters upon transformation
* None: no scaling will be applied, variance of the order parameters is 1
* 'kinetic map' or 'km': order parameters are scaled by singular value
Only the left singular functions induce a kinetic map.
Therefore scaling='km' is only effective if `right` is False.
"""
return self.model.scaling
@scaling.setter
def scaling(self, value):
self.model.scaling = value
def _init_covar(self, partial=False):
# in case of partial, we need to store the state of running covar in this estimator.
args = dict(c00=True,
c0t=True,
ctt=True,
remove_data_mean=True,
reversible=False,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=None,
ncov_max=self.ncov_max)
if partial:
if not hasattr(self, '_covar') or self._covar is None:
self._covar = LaggedCovariance(**args)
# remember running covar for serialization
assert '_covar' not in self.__serialize_fields
self.__serialize_fields.append('_covar')
return self._covar
elif not partial:
# if the previous estimation was a partial_fit, we might have a running covar object,
# which we can safely omit now.
if '_covar' in self.__serialize_fields:
self.__serialize_fields.remove('_covar')
return LaggedCovariance(**args)
@property
def model(self):
# this should ensure we always have a model, in case this estimator is used in sklearn-like fashion.
if not hasattr(self, '_model'):
self._model = VAMPModel()
return self._model
def _estimate(self, iterable, **kw):
covar = self._init_covar()
indim = iterable.dimension()
if isinstance(self.dim, int) and not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._logger_is_active(self._loglevel_DEBUG):
self.logger.debug(
"Running VAMP with tau=%i; Estimating two covariance matrices"
" with dimension (%i, %i)" % (self._lag, indim, indim))
covar.estimate(iterable, **kw)
self.model.update_model_params(mean_0=covar.mean,
mean_t=covar.mean_tau,
C00=covar.C00_,
C0t=covar.C0t_,
Ctt=covar.Ctt_)
self.model._diagonalize()
return self.model
def partial_fit(self, X):
""" incrementally update the covariances and mean.
Parameters
----------
X: array, list of arrays, PyEMMA reader
input data.
Notes
-----
The projection matrix is first being calculated upon its first access.
"""
from pyemma.coordinates import source
iterable = source(X)
if isinstance(self.dim, int):
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
self._covar = self._init_covar(partial=True)
self._covar.partial_fit(iterable)
self.model.update_model_params(
mean_0=self._covar.mean, # TODO: inefficient, fixme
mean_t=self._covar.mean_tau,
C00=self._covar.C00_,
C0t=self._covar.C0t_,
Ctt=self._covar.Ctt_)
self._estimated = False
return self.model
def dimension(self):
"""real output dimension after low-rank approximation."""
return self.model.dimension()
def _transform_array(self, X):
r"""Projects the data onto the dominant singular functions.
Parameters
----------
X : ndarray(n, m)
the input data
Returns
-------
Y : ndarray(n,)
the projected data
If `self.right` is True, projection will be on the right singular
functions. Otherwise, projection will be on the left singular
functions.
"""
# TODO: in principle get_output should not return data for *all* frames!
# TODO: implement our own iterators? This would also include random access to be complete...
if self.right:
X_meanfree = X - self._model.mean_t
Y = np.dot(X_meanfree, self._model.V[:, 0:self.dimension()])
else:
X_meanfree = X - self._model.mean_0
Y = np.dot(X_meanfree, self._model.U[:, 0:self.dimension()])
return Y.astype(self.output_type())
@property
def singular_values(self):
r"""Singular values of the half-weighted Koopman matrix (usually denoted :math:`\sigma`)
Returns
-------
singular values: 1-D np.array
"""
return self.model.singular_values
@property
def singular_vectors_right(self):
r"""Transformation matrix that represents the linear map from feature space to the space of right singular functions.
Notes
-----
Right "singular vectors" V of the VAMP problem (equation 13 in [1]_), columnwise
Returns
-------
vectors: 2-D ndarray
Coefficients that express the right singular functions in the
basis of mean-free input features.
References
----------
.. [1] Wu, H. and Noe, F. 2017. Variational approach for learning Markov processes from time series data.
arXiv:1707.04659v1
"""
return self.model.V
@property
def singular_vectors_left(self):
r"""Transformation matrix that represents the linear map from feature space to the space of left singular functions.
Notes
-----
Left "singular vectors" U of the VAMP problem (equation 13 in [1]_), columnwise
Returns
-------
vectors: 2-D ndarray
Coefficients that express the left singular functions in the
basis of mean-free input features.
References
----------
.. [1] Wu, H. and Noe, F. 2017. Variational approach for learning Markov processes from time series data.
arXiv:1707.04659v1
"""
return self.model.U
@property
def cumvar(self):
r"""Cumulative sum of the squared and normalized singular values
Returns
-------
cumvar: 1D np.array
"""
return self.model.cumvar
@property
def show_progress(self):
if self._covar is None:
return False
else:
return self._covar.show_progress
@show_progress.setter
def show_progress(self, value):
if self._covar is not None:
self._covar.show_progress = value
def expectation(self,
observables,
statistics,
lag_multiple=1,
observables_mean_free=False,
statistics_mean_free=False):
r"""Compute future expectation of observable or covariance using the approximated Koopman operator.
Parameters
----------
observables : np.ndarray((input_dimension, n_observables))
Coefficients that express one or multiple observables in
the basis of the input features.
statistics : np.ndarray((input_dimension, n_statistics)), optional
Coefficients that express one or multiple statistics in
the basis of the input features.
This parameter can be None. In that case, this method
returns the future expectation value of the observable(s).
lag_multiple : int
If > 1, extrapolate to a multiple of the estimator's lag
time by assuming Markovianity of the approximated Koopman
operator.
observables_mean_free : bool, default=False
If true, coefficients in `observables` refer to the input
features with feature means removed.
If false, coefficients in `observables` refer to the
unmodified input features.
statistics_mean_free : bool, default=False
If true, coefficients in `statistics` refer to the input
features with feature means removed.
If false, coefficients in `statistics` refer to the
unmodified input features.
Notes
-----
A "future expectation" of a observable g is the average of g computed
over a time window that has the same total length as the input data
from which the Koopman operator was estimated but is shifted
by lag_multiple*tau time steps into the future (where tau is the lag
time).
It is computed with the equation:
.. math::
\mathbb{E}[g]_{\rho_{n}}=\mathbf{q}^{T}\mathbf{P}^{n-1}\mathbf{e}_{1}
where
.. math::
P_{ij}=\sigma_{i}\langle\psi_{i},\phi_{j}\rangle_{\rho_{1}}
and
.. math::
q_{i}=\langle g,\phi_{i}\rangle_{\rho_{1}}
and :math:`\mathbf{e}_{1}` is the first canonical unit vector.
A model prediction of time-lagged covariances between the
observable f and the statistic g at a lag-time of lag_multiple*tau
is computed with the equation:
.. math::
\mathrm{cov}[g,\,f;n\tau]=\mathbf{q}^{T}\mathbf{P}^{n-1}\boldsymbol{\Sigma}\mathbf{r}
where :math:`r_{i}=\langle\psi_{i},f\rangle_{\rho_{0}}` and
:math:`\boldsymbol{\Sigma}=\mathrm{diag(\boldsymbol{\sigma})}` .
"""
return self.model.expectation(
observables,
statistics,
lag_multiple=lag_multiple,
statistics_mean_free=statistics_mean_free,
observables_mean_free=observables_mean_free)
def cktest(self,
n_observables=None,
observables='phi',
statistics='psi',
mlags=10,
n_jobs=1,
show_progress=True,
iterable=None):
r"""Do the Chapman-Kolmogorov test by computing predictions for higher lag times and by performing estimations at higher lag times.
Notes
-----
This method computes two sets of time-lagged covariance matrices
* estimates at higher lag times :
.. math::
\left\langle \mathbf{K}(n\tau)g_{i},f_{j}\right\rangle_{\rho_{0}}
where :math:`\rho_{0}` is the empirical distribution implicitly defined
by all data points from time steps 0 to T-tau in all trajectories,
:math:`\mathbf{K}(n\tau)` is a rank-reduced Koopman matrix estimated
at the lag-time n*tau and g and f are some functions of the data.
Rank-reduction of the Koopman matrix is controlled by the `dim`
parameter of :func:`vamp <pyemma.coordinates.vamp>`.
* predictions at higher lag times :
.. math::
\left\langle \mathbf{K}^{n}(\tau)g_{i},f_{j}\right\rangle_{\rho_{0}}
where :math:`\mathbf{K}^{n}` is the n'th power of the rank-reduced
Koopman matrix contained in self.
The Champan-Kolmogorov test is to compare the predictions to the
estimates.
Parameters
----------
n_observables : int, optional, default=None
Limit the number of default observables (and of default statistics)
to this number.
Only used if `observables` are None or `statistics` are None.
observables : np.ndarray((input_dimension, n_observables)) or 'phi'
Coefficients that express one or multiple observables :math:`g`
in the basis of the input features.
This parameter can be 'phi'. In that case, the dominant
right singular functions of the Koopman operator estimated
at the smallest lag time are used as default observables.
statistics : np.ndarray((input_dimension, n_statistics)) or 'psi'
Coefficients that express one or multiple statistics :math:`f`
in the basis of the input features.
This parameter can be 'psi'. In that case, the dominant
left singular functions of the Koopman operator estimated
at the smallest lag time are used as default statistics.
mlags : int or int-array, default=10
multiples of lag times for testing the Model, e.g. range(10).
A single int will trigger a range, i.e. mlags=10 maps to
mlags=range(10).
Note that you need to be able to do a model prediction for each
of these lag time multiples, e.g. the value 0 only make sense
if model.expectation(lag_multiple=0) will work.
n_jobs : int, default=1
how many jobs to use during calculation
show_progress : bool, default=True
Show progressbars for calculation?
iterable : any data format that `pyemma.coordinates.vamp()` accepts as input, optional
It `iterable` is None, the same data source with which VAMP
was initialized will be used for all estimation.
Otherwise, all estimates (not predictions) from data will be computed
from the data contained in `iterable`.
Returns
-------
vckv : :class:`VAMPChapmanKolmogorovValidator <pyemma.coordinates.transform.VAMPChapmanKolmogorovValidator>`
Contains the estimated and the predicted covarince matrices.
The object can be plotted with :func:`plot_cktest <pyemma.plots.plot_cktest>` with the option `y01=False`.
"""
if n_observables is not None:
if n_observables > self.dimension():
warnings.warn(
'Selected singular functions as observables but dimension '
'is lower than requested number of observables.')
n_observables = self.dimension()
else:
n_observables = self.dimension()
if isinstance(observables, str) and observables == 'phi':
observables = self.singular_vectors_right[:, 0:n_observables]
observables_mean_free = True
else:
ensure_ndarray(observables, ndim=2)
observables_mean_free = False
if isinstance(statistics, str) and statistics == 'psi':
statistics = self.singular_vectors_left[:, 0:n_observables]
statistics_mean_free = True
else:
ensure_ndarray_or_None(statistics, ndim=2)
statistics_mean_free = False
ck = VAMPChapmanKolmogorovValidator(self.model,
self,
observables,
statistics,
observables_mean_free,
statistics_mean_free,
mlags=mlags,
n_jobs=n_jobs,
show_progress=show_progress)
if iterable is None:
iterable = self.data_producer
ck.estimate(iterable)
return ck
def score(self, test_data=None, score_method='VAMP2'):
"""Compute the VAMP score for this model or the cross-validation score between self and a second model estimated form different data.
Parameters
----------
test_data : any data format that `pyemma.coordinates.vamp()` accepts as input
If `test_data` is not None, this method computes the cross-validation score
between self and a VAMP model estimated from `test_data`. It is assumed that
self was estimated from the "training" data and `test_data` is the test data.
The score is computed for one realization of self and `test_data`. Estimation
of the average cross-validation score and partitioning of data into test and
training part is not performed by this method.
If `test_data` is None, this method computes the VAMP score for the model
contained in self.
The model that is estimated from `test_data` will inherit all hyperparameters
from self.
score_method : str, optional, default='VAMP2'
Available scores are based on the variational approach for Markov processes [1]_:
* 'VAMP1' Sum of singular values of the half-weighted Koopman matrix [1]_ .
If the model is reversible, this is equal to the sum of
Koopman matrix eigenvalues, also called Rayleigh quotient [1]_.
* 'VAMP2' Sum of squared singular values of the half-weighted Koopman matrix [1]_ .
If the model is reversible, this is equal to the kinetic variance [2]_ .
* 'VAMPE' Approximation error of the estimated Koopman operator with respect to
the true Koopman operator up to an additive constant [1]_ .
Returns
-------
score : float
If `test_data` is not None, returns the cross-validation VAMP score between
self and the model estimated from `test_data`. Otherwise return the selected
VAMP-score of self.
References
----------
.. [1] Wu, H. and Noe, F. 2017. Variational approach for learning Markov processes from time series data.
arXiv:1707.04659v1
.. [2] Noe, F. and Clementi, C. 2015. Kinetic distance and kinetic maps from molecular dynamics simulation.
J. Chem. Theory. Comput. doi:10.1021/acs.jctc.5b00553
"""
from pyemma._ext.sklearn.base import clone as clone_estimator
est = clone_estimator(self)
# clone does not invoke our constructor, so we have explicitly create a new model instance.
est._model = VAMPModel()
if test_data is None:
return self.model.score(None, score_method=score_method)
else:
est.estimate(test_data)
return self.model.score(est.model, score_method=score_method)
def __init__(self,
lag,
dim=-1,
var_cutoff=0.95,
kinetic_map=True,
commute_map=False,
epsilon=1e-6,
stride=1,
skip=0,
reversible=True,
weights=None,
ncov_max=float('inf')):
r""" Time-lagged independent component analysis (TICA) [1]_, [2]_, [3]_.
Parameters
----------
lag : int
lag time
dim : int, optional, default -1
Maximum number of significant independent components to use to reduce dimension of input data. -1 means
all numerically available dimensions (see epsilon) will be used unless reduced by var_cutoff.
Setting dim to a positive value is exclusive with var_cutoff.
var_cutoff : float in the range [0,1], optional, default 0.95
Determines the number of output dimensions by including dimensions until their cumulative kinetic variance
exceeds the fraction subspace_variance. var_cutoff=1.0 means all numerically available dimensions
(see epsilon) will be used, unless set by dim. Setting var_cutoff smaller than 1.0 is exclusive with dim
kinetic_map : bool, optional, default True
Eigenvectors will be scaled by eigenvalues. As a result, Euclidean distances in the transformed data
approximate kinetic distances [4]_. This is a good choice when the data is further processed by clustering.
commute_map : bool, optional, default False
Eigenvector_i will be scaled by sqrt(timescale_i / 2). As a result, Euclidean distances in the transformed
data will approximate commute distances [5]_.
epsilon : float
eigenvalue norm cutoff. Eigenvalues of C0 with norms <= epsilon will be
cut off. The remaining number of eigenvalues define the size
of the output.
stride: int, optional, default = 1
Use only every stride-th time step. By default, every time step is used.
skip : int, default=0
skip the first initial n frames per trajectory.
reversible: bool, default=True
symmetrize correlation matrices C_0, C_{\tau}. At the moment, setting reversible=False is not implemented.
weights: object, optional, default = None
An object that allows to compute re-weighting factors to estimate equilibrium means and correlations from
off-equilibrium data. The only requirement is that weights possesses a method weights(X), that accepts a
trajectory X (np.ndarray(T, n)) and returns a vector of re-weighting factors (np.ndarray(T,)).
Notes
-----
Given a sequence of multivariate data :math:`X_t`, computes the mean-free
covariance and time-lagged covariance matrix:
.. math::
C_0 &= (X_t - \mu)^T (X_t - \mu) \\
C_{\tau} &= (X_t - \mu)^T (X_{t + \tau} - \mu)
and solves the eigenvalue problem
.. math:: C_{\tau} r_i = C_0 \lambda_i(tau) r_i,
where :math:`r_i` are the independent components and :math:`\lambda_i(tau)` are
their respective normalized time-autocorrelations. The eigenvalues are
related to the relaxation timescale by
.. math:: t_i(tau) = -\tau / \ln |\lambda_i|.
When used as a dimension reduction method, the input data is projected
onto the dominant independent components.
References
----------
.. [1] Perez-Hernandez G, F Paul, T Giorgino, G De Fabritiis and F Noe. 2013.
Identification of slow molecular order parameters for Markov model construction
J. Chem. Phys. 139, 015102. doi:10.1063/1.4811489
.. [2] Schwantes C, V S Pande. 2013.
Improvements in Markov State Model Construction Reveal Many Non-Native Interactions in the Folding of NTL9
J. Chem. Theory. Comput. 9, 2000-2009. doi:10.1021/ct300878a
.. [3] L. Molgedey and H. G. Schuster. 1994.
Separation of a mixture of independent signals using time delayed correlations
Phys. Rev. Lett. 72, 3634.
.. [4] Noe, F. and Clementi, C. 2015. Kinetic distance and kinetic maps from molecular dynamics simulation.
J. Chem. Theory. Comput. doi:10.1021/acs.jctc.5b00553
.. [5] Noe, F., Banisch, R., Clementi, C. 2016. Commute maps: separating slowly-mixing molecular configurations
for kinetic modeling. J. Chem. Theory. Comput. doi:10.1021/acs.jctc.6b00762
"""
default_var_cutoff = get_default_args(self.__init__)['var_cutoff']
if dim != -1 and var_cutoff != default_var_cutoff:
raise ValueError(
'Trying to set both the number of dimension and the subspace variance. Use either or.'
)
if kinetic_map and commute_map:
raise ValueError(
'Trying to use both kinetic_map and commute_map. Use either or.'
)
if not reversible:
raise NotImplementedError(
"Reversible=False is currently not implemented.")
# if (kinetic_map or commute_map) and not reversible:
# raise NotImplementedError('kinetic_map and commute_map are not yet implemented for irreversible processes.')
super(TICA, self).__init__()
if dim > -1:
var_cutoff = 1.0
self._covar = LaggedCovariance(c00=True,
c0t=True,
ctt=False,
remove_data_mean=True,
reversible=reversible,
lag=lag,
bessel=False,
stride=stride,
skip=skip,
weights=weights,
ncov_max=ncov_max)
# empty dummy model instance
self._model = TICAModel()
self.set_params(lag=lag,
dim=dim,
var_cutoff=var_cutoff,
kinetic_map=kinetic_map,
commute_map=commute_map,
epsilon=epsilon,
reversible=reversible,
stride=stride,
skip=skip,
weights=weights,
ncov_max=ncov_max)
class TICA(StreamingEstimationTransformer):
r""" Time-lagged independent component analysis (TICA)"""
def __init__(self,
lag,
dim=-1,
var_cutoff=0.95,
kinetic_map=True,
commute_map=False,
epsilon=1e-6,
stride=1,
skip=0,
reversible=True,
weights=None,
ncov_max=float('inf')):
r""" Time-lagged independent component analysis (TICA) [1]_, [2]_, [3]_.
Parameters
----------
lag : int
lag time
dim : int, optional, default -1
Maximum number of significant independent components to use to reduce dimension of input data. -1 means
all numerically available dimensions (see epsilon) will be used unless reduced by var_cutoff.
Setting dim to a positive value is exclusive with var_cutoff.
var_cutoff : float in the range [0,1], optional, default 0.95
Determines the number of output dimensions by including dimensions until their cumulative kinetic variance
exceeds the fraction subspace_variance. var_cutoff=1.0 means all numerically available dimensions
(see epsilon) will be used, unless set by dim. Setting var_cutoff smaller than 1.0 is exclusive with dim
kinetic_map : bool, optional, default True
Eigenvectors will be scaled by eigenvalues. As a result, Euclidean distances in the transformed data
approximate kinetic distances [4]_. This is a good choice when the data is further processed by clustering.
commute_map : bool, optional, default False
Eigenvector_i will be scaled by sqrt(timescale_i / 2). As a result, Euclidean distances in the transformed
data will approximate commute distances [5]_.
epsilon : float
eigenvalue norm cutoff. Eigenvalues of C0 with norms <= epsilon will be
cut off. The remaining number of eigenvalues define the size
of the output.
stride: int, optional, default = 1
Use only every stride-th time step. By default, every time step is used.
skip : int, default=0
skip the first initial n frames per trajectory.
reversible: bool, default=True
symmetrize correlation matrices C_0, C_{\tau}. At the moment, setting reversible=False is not implemented.
weights: object, optional, default = None
An object that allows to compute re-weighting factors to estimate equilibrium means and correlations from
off-equilibrium data. The only requirement is that weights possesses a method weights(X), that accepts a
trajectory X (np.ndarray(T, n)) and returns a vector of re-weighting factors (np.ndarray(T,)).
Notes
-----
Given a sequence of multivariate data :math:`X_t`, computes the mean-free
covariance and time-lagged covariance matrix:
.. math::
C_0 &= (X_t - \mu)^T (X_t - \mu) \\
C_{\tau} &= (X_t - \mu)^T (X_{t + \tau} - \mu)
and solves the eigenvalue problem
.. math:: C_{\tau} r_i = C_0 \lambda_i(tau) r_i,
where :math:`r_i` are the independent components and :math:`\lambda_i(tau)` are
their respective normalized time-autocorrelations. The eigenvalues are
related to the relaxation timescale by
.. math:: t_i(tau) = -\tau / \ln |\lambda_i|.
When used as a dimension reduction method, the input data is projected
onto the dominant independent components.
References
----------
.. [1] Perez-Hernandez G, F Paul, T Giorgino, G De Fabritiis and F Noe. 2013.
Identification of slow molecular order parameters for Markov model construction
J. Chem. Phys. 139, 015102. doi:10.1063/1.4811489
.. [2] Schwantes C, V S Pande. 2013.
Improvements in Markov State Model Construction Reveal Many Non-Native Interactions in the Folding of NTL9
J. Chem. Theory. Comput. 9, 2000-2009. doi:10.1021/ct300878a
.. [3] L. Molgedey and H. G. Schuster. 1994.
Separation of a mixture of independent signals using time delayed correlations
Phys. Rev. Lett. 72, 3634.
.. [4] Noe, F. and Clementi, C. 2015. Kinetic distance and kinetic maps from molecular dynamics simulation.
J. Chem. Theory. Comput. doi:10.1021/acs.jctc.5b00553
.. [5] Noe, F., Banisch, R., Clementi, C. 2016. Commute maps: separating slowly-mixing molecular configurations
for kinetic modeling. J. Chem. Theory. Comput. doi:10.1021/acs.jctc.6b00762
"""
default_var_cutoff = get_default_args(self.__init__)['var_cutoff']
if dim != -1 and var_cutoff != default_var_cutoff:
raise ValueError(
'Trying to set both the number of dimension and the subspace variance. Use either or.'
)
if kinetic_map and commute_map:
raise ValueError(
'Trying to use both kinetic_map and commute_map. Use either or.'
)
if not reversible:
raise NotImplementedError(
"Reversible=False is currently not implemented.")
# if (kinetic_map or commute_map) and not reversible:
# raise NotImplementedError('kinetic_map and commute_map are not yet implemented for irreversible processes.')
super(TICA, self).__init__()
if dim > -1:
var_cutoff = 1.0
self._covar = LaggedCovariance(c00=True,
c0t=True,
ctt=False,
remove_data_mean=True,
reversible=reversible,
lag=lag,
bessel=False,
stride=stride,
skip=skip,
weights=weights,
ncov_max=ncov_max)
# empty dummy model instance
self._model = TICAModel()
self.set_params(lag=lag,
dim=dim,
var_cutoff=var_cutoff,
kinetic_map=kinetic_map,
commute_map=commute_map,
epsilon=epsilon,
reversible=reversible,
stride=stride,
skip=skip,
weights=weights,
ncov_max=ncov_max)
@property
def lag(self):
""" lag time of correlation matrix :math:`C_{\tau}` """
return self._lag
@lag.setter
def lag(self, new_tau):
self._lag = new_tau
def describe(self):
try:
dim = self.dimension()
except AttributeError:
dim = self.dim
return "[TICA, lag = %i; max. output dim. = %i]" % (self._lag, dim)
def dimension(self):
""" output dimension """
if self.dim > -1:
return self.dim
d = None
if self.dim != -1 and not self._estimated: # fixed parametrization
d = self.dim
elif self._estimated: # parametrization finished. Dimension is known
dim = len(self.eigenvalues)
if self.var_cutoff < 1.0: # if subspace_variance, reduce the output dimension if needed
dim = min(dim,
np.searchsorted(self.cumvar, self.var_cutoff) + 1)
d = dim
elif self.var_cutoff == 1.0: # We only know that all dimensions are wanted, so return input dim
d = self.data_producer.dimension()
else: # We know nothing. Give up
raise RuntimeError(
'Requested dimension, but the dimension depends on the cumulative variance and the '
'transformer has not yet been estimated. Call estimate() before.'
)
return d
@property
def mean(self):
""" mean of input features """
return self._model.mean
@property
@deprecated('please use the "mean" property')
def mu(self):
"""DEPRECATED: please use the "mean" property"""
return self.mean
@mean.setter
def mean(self, value):
self._model.mean = value
def estimate(self, X, **kwargs):
r"""
Chunk-based parameterization of TICA. Iterates over all data and estimates
the mean, covariance and time lagged covariance. Finally, the
generalized eigenvalue problem is solved to determine
the independent components.
"""
return super(TICA, self).estimate(X, **kwargs)
def partial_fit(self, X):
""" incrementally update the covariances and mean.
Parameters
----------
X: array, list of arrays, PyEMMA reader
input data.
Notes
-----
The projection matrix is first being calculated upon its first access.
"""
from pyemma.coordinates import source
iterable = source(X)
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
self._covar.partial_fit(iterable)
self._model.update_model_params(
mean=self._covar.mean, # TODO: inefficient, fixme
cov=self._covar.cov,
cov_tau=self._covar.cov_tau)
self._used_data = self._covar._used_data
self._estimated = False
return self
def _estimate(self, iterable, **kw):
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._logger_is_active(self._loglevel_DEBUG):
self._logger.debug(
"Running TICA with tau=%i; Estimating two covariance matrices"
" with dimension (%i, %i)" % (self._lag, indim, indim))
self._covar.estimate(iterable, **kw)
self._model.update_model_params(mean=self._covar.mean,
cov=self._covar.cov,
cov_tau=self._covar.cov_tau)
self._diagonalize()
return self._model
def _transform_array(self, X):
r"""Projects the data onto the dominant independent components.
Parameters
----------
X : ndarray(n, m)
the input data
Returns
-------
Y : ndarray(n,)
the projected data
"""
X_meanfree = X - self.mean
Y = np.dot(X_meanfree, self.eigenvectors[:, 0:self.dimension()])
return Y.astype(self.output_type())
def _diagonalize(self):
# diagonalize with low rank approximation
self._logger.debug("diagonalize Cov and Cov_tau.")
try:
eigenvalues, eigenvectors = eig_corr(self._covar.cov,
self._covar.cov_tau,
self.epsilon,
sign_maxelement=True)
except ZeroRankError:
raise ZeroRankError(
'All input features are constant in all time steps. No dimension would be left after dimension reduction.'
)
if self.kinetic_map and self.commute_map:
raise ValueError(
'Trying to use both kinetic_map and commute_map. Use either or.'
)
if self.kinetic_map: # scale by eigenvalues
eigenvectors *= eigenvalues[None, :]
if self.commute_map: # scale by (regularized) timescales
timescales = 1 - self.lag / np.log(np.abs(eigenvalues))
# dampen timescales smaller than the lag time, as in section 2.5 of ref. [5]
regularized_timescales = 0.5 * timescales * np.maximum(
np.tanh(np.pi * ((timescales - self.lag) / self.lag) + 1), 0)
eigenvectors *= np.sqrt(regularized_timescales / 2)
self._logger.debug("finished diagonalisation.")
# compute cumulative variance
cumvar = np.cumsum(np.abs(eigenvalues)**2)
cumvar /= cumvar[-1]
self._model.update_model_params(cumvar=cumvar,
eigenvalues=eigenvalues,
eigenvectors=eigenvectors)
self._estimated = True
@property
@_lazy_estimation
def timescales(self):
r"""Implied timescales of the TICA transformation
For each :math:`i`-th eigenvalue, this returns
.. math::
t_i = -\frac{\tau}{\log(|\lambda_i|)}
where :math:`\tau` is the :py:obj:`lag` of the TICA object and :math:`\lambda_i` is the `i`-th
:py:obj:`eigenvalue <eigenvalues>` of the TICA object.
Returns
-------
timescales: 1D np.array
numpy array with the implied timescales. In principle, one should expect as many timescales as
input coordinates were available. However, less eigenvalues will be returned if the TICA matrices
were not full rank or :py:obj:`var_cutoff` was parsed
"""
return -self.lag / np.log(np.abs(self.eigenvalues))
@property
@_lazy_estimation
def feature_TIC_correlation(self):
r"""Instantaneous correlation matrix between mean-free input features and TICs
Denoting the input features as :math:`X_i` and the TICs as :math:`\theta_j`, the instantaneous, linear correlation
between them can be written as
.. math::
\mathbf{Corr}(X_i - \mu_i, \mathbf{\theta}_j) = \frac{1}{\sigma_{X_i - \mu_i}}\sum_l \sigma_{(X_i - \mu_i)(X_l - \mu_l} \mathbf{U}_{li}
The matrix :math:`\mathbf{U}` is the matrix containing, as column vectors, the eigenvectors of the TICA
generalized eigenvalue problem .
Returns
-------
feature_TIC_correlation : ndarray(n,m)
correlation matrix between input features and TICs. There is a row for each feature and a column
for each TIC.
"""
feature_sigma = np.sqrt(np.diag(self.cov))
return np.dot(self.cov, self.eigenvectors[:, :self.dimension()]
) / feature_sigma[:, np.newaxis]
@property
def cov(self):
""" covariance matrix of input data. """
return self._model.cov
@cov.setter
def cov(self, value):
self._model.cov = value
@property
def cov_tau(self):
""" covariance matrix of time-lagged input data. """
return self._model.cov_tau
@cov_tau.setter
def cov_tau(self, value):
self._model.cov_tau = value
@property
@_lazy_estimation
def eigenvalues(self):
r"""Eigenvalues of the TICA problem (usually denoted :math:`\lambda`
Returns
-------
eigenvalues: 1D np.array
"""
return self._model.eigenvalues
@property
@_lazy_estimation
def eigenvectors(self):
r"""Eigenvectors of the TICA problem, columnwise
Returns
-------
eigenvectors: (N,M) ndarray
"""
return self._model.eigenvectors
@property
@_lazy_estimation
def cumvar(self):
r"""Cumulative sum of the the TICA eigenvalues
Returns
-------
cumvar: 1D np.array
"""
return self._model.cumvar
def output_type(self):
# TODO: handle the case of conjugate pairs
if np.all(np.isreal(self.eigenvectors[:, 0:self.dimension()])) or \
np.allclose(np.imag(self.eigenvectors[:, 0:self.dimension()]), 0):
return super(TICA, self).output_type()
else:
return np.complex64
class _KoopmanEstimator(StreamingEstimator):
'''only for computing u
The user-accessible way for computing K is TICA()
'''
def __init__(self,
lag,
epsilon=1e-6,
stride=1,
skip=0,
chunksize=None,
ncov_max=float('inf')):
super(_KoopmanEstimator, self).__init__(chunksize=chunksize)
self._covar = LaggedCovariance(c00=True,
c0t=True,
remove_data_mean=True,
reversible=False,
lag=lag,
bessel=False,
stride=stride,
skip=skip,
ncov_max=ncov_max)
self.set_params(lag=lag,
epsilon=epsilon,
stride=stride,
skip=skip,
ncov_max=ncov_max)
self._estimation_finished = False
def partial_fit(self, X):
from pyemma.coordinates import source
self._covar.partial_fit(source(X))
self._estimation_finished = False
self._estimated = True
return self
def _finish_estimation(self):
R = spd_inv_split(self._covar.cov,
epsilon=self.epsilon,
canonical_signs=True)
# Set the new correlation matrix:
M = R.shape[1]
K = np.dot(R.T, np.dot((self._covar.cov_tau), R))
K = np.vstack((K, np.dot((self._covar.mean_tau - self._covar.mean),
R)))
ex1 = np.zeros((M + 1, 1))
ex1[M, 0] = 1.0
self._K = np.hstack((K, ex1))
self._R = R
self._estimation_finished = True
self._estimated = True
def _estimate(self, iterable, **kwargs):
self._covar.estimate(iterable, **kwargs)
self._finish_estimation()
return self
@property
def K_pc_1(self):
'Koopman operator on the modified basis (PC|1)'
self._check_estimated()
if not self._estimation_finished:
self._finish_estimation()
return self._K
@property
def u_pc_1(self):
'weights in the modified basis'
self._check_estimated()
return _compute_u(self.K_pc_1)
@property
def u(self):
'weights in the input basis'
self._check_estimated()
u_mod = self.u_pc_1
N = self._R.shape[0]
u_input = np.zeros(N + 1)
u_input[0:N] = self._R.dot(u_mod[0:-1]) # in input basis
u_input[N] = u_mod[-1] - self.mean.dot(self._R.dot(u_mod[0:-1]))
return u_input
@property
def weights(self):
'weights in the input basis (encapsulated in an object)'
self._check_estimated()
u_input = self.u
return _KoopmanWeights(u_input[0:-1], u_input[-1])
@property
def R(self):
'weightening transformation'
self._check_estimated()
if not self._estimation_finished:
self._finish_estimation()
return self._R
@property
def mean(self):
self._check_estimated()
return self._covar.mean
class TICA(TICABase, SerializableMixIn):
r""" Time-lagged independent component analysis (TICA)"""
__serialize_version = 0
def __init__(self,
lag,
dim=-1,
var_cutoff=0.95,
kinetic_map=True,
commute_map=False,
epsilon=1e-6,
stride=1,
skip=0,
reversible=True,
weights=None,
ncov_max=float('inf')):
r""" Time-lagged independent component analysis (TICA) [1]_, [2]_, [3]_.
Parameters
----------
lag : int
lag time
dim : int, optional, default -1
Maximum number of significant independent components to use to reduce dimension of input data. -1 means
all numerically available dimensions (see epsilon) will be used unless reduced by var_cutoff.
Setting dim to a positive value is exclusive with var_cutoff.
var_cutoff : float in the range [0,1], optional, default 0.95
Determines the number of output dimensions by including dimensions until their cumulative kinetic variance
exceeds the fraction subspace_variance. var_cutoff=1.0 means all numerically available dimensions
(see epsilon) will be used, unless set by dim. Setting var_cutoff smaller than 1.0 is exclusive with dim
kinetic_map : bool, optional, default True
Eigenvectors will be scaled by eigenvalues. As a result, Euclidean distances in the transformed data
approximate kinetic distances [4]_. This is a good choice when the data is further processed by clustering.
commute_map : bool, optional, default False
Eigenvector_i will be scaled by sqrt(timescale_i / 2). As a result, Euclidean distances in the transformed
data will approximate commute distances [5]_.
epsilon : float
eigenvalue norm cutoff. Eigenvalues of C0 with norms <= epsilon will be
cut off. The remaining number of eigenvalues define the size
of the output.
stride: int, optional, default = 1
Use only every stride-th time step. By default, every time step is used.
skip : int, default=0
skip the first initial n frames per trajectory.
reversible: bool, default=True
symmetrize correlation matrices C_0, C_{\tau}.
weights: object or list of ndarrays, optional, default = None
* An object that allows to compute re-weighting factors to estimate equilibrium means and correlations from
off-equilibrium data. The only requirement is that weights possesses a method weights(X), that accepts a
trajectory X (np.ndarray(T, n)) and returns a vector of re-weighting factors (np.ndarray(T,)).
* A list of ndarrays (ndim=1) specifies the weights for each frame of each trajectory.
Notes
-----
Given a sequence of multivariate data :math:`X_t`, computes the mean-free
covariance and time-lagged covariance matrix:
.. math::
C_0 &= (X_t - \mu)^T (X_t - \mu) \\
C_{\tau} &= (X_t - \mu)^T (X_{t + \tau} - \mu)
and solves the eigenvalue problem
.. math:: C_{\tau} r_i = C_0 \lambda_i(tau) r_i,
where :math:`r_i` are the independent components and :math:`\lambda_i(tau)` are
their respective normalized time-autocorrelations. The eigenvalues are
related to the relaxation timescale by
.. math:: t_i(tau) = -\tau / \ln |\lambda_i|.
When used as a dimension reduction method, the input data is projected
onto the dominant independent components.
References
----------
.. [1] Perez-Hernandez G, F Paul, T Giorgino, G De Fabritiis and F Noe. 2013.
Identification of slow molecular order parameters for Markov model construction
J. Chem. Phys. 139, 015102. doi:10.1063/1.4811489
.. [2] Schwantes C, V S Pande. 2013.
Improvements in Markov State Model Construction Reveal Many Non-Native Interactions in the Folding of NTL9
J. Chem. Theory. Comput. 9, 2000-2009. doi:10.1021/ct300878a
.. [3] L. Molgedey and H. G. Schuster. 1994.
Separation of a mixture of independent signals using time delayed correlations
Phys. Rev. Lett. 72, 3634.
.. [4] Noe, F. and Clementi, C. 2015. Kinetic distance and kinetic maps from molecular dynamics simulation.
J. Chem. Theory. Comput. doi:10.1021/acs.jctc.5b00553
.. [5] Noe, F., Banisch, R., Clementi, C. 2016. Commute maps: separating slowly-mixing molecular configurations
for kinetic modeling. J. Chem. Theory. Comput. doi:10.1021/acs.jctc.6b00762
"""
super(TICA, self).__init__()
if kinetic_map and commute_map:
raise ValueError(
'Trying to use both kinetic_map and commute_map. Use either or.'
)
if (kinetic_map or commute_map) and not reversible:
kinetic_map = False
commute_map = False
warnings.warn(
"Cannot use kinetic_map or commute_map for non-reversible processes, both will be set to"
"False.")
# this instance will be set by partial fit.
self._covar = None
self.dim = dim
self.var_cutoff = var_cutoff
self.set_params(lag=lag,
dim=dim,
var_cutoff=var_cutoff,
kinetic_map=kinetic_map,
commute_map=commute_map,
epsilon=epsilon,
reversible=reversible,
stride=stride,
skip=skip,
weights=weights,
ncov_max=ncov_max)
@property
def model(self):
if not hasattr(self, '_model') or self._model is None:
self._model = TICAModelBase()
return self._model
def describe(self):
try:
dim = self.dimension()
except RuntimeError:
dim = self.dim
return "[TICA, lag = %i; max. output dim. = %i]" % (self._lag, dim)
def estimate(self, X, **kwargs):
r"""
Chunk-based parameterization of TICA. Iterates over all data and estimates
the mean, covariance and time lagged covariance. Finally, the
generalized eigenvalue problem is solved to determine
the independent components.
"""
return super(TICA, self).estimate(X, **kwargs)
def partial_fit(self, X):
""" incrementally update the covariances and mean.
Parameters
----------
X: array, list of arrays, PyEMMA reader
input data.
Notes
-----
The projection matrix is first being calculated upon its first access.
"""
from pyemma.coordinates import source
iterable = source(X, chunksize=self.chunksize)
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._covar is None:
self._covar = LaggedCovariance(c00=True,
c0t=True,
ctt=False,
remove_data_mean=True,
reversible=self.reversible,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=self.weights,
ncov_max=self.ncov_max)
self._covar.partial_fit(iterable)
self.model.update_model_params(
mean=self._covar.mean, # TODO: inefficient, fixme
cov=self._covar.C00_,
cov_tau=self._covar.C0t_)
self._estimated = False
return self
def _estimate(self, iterable, **kw):
covar = LaggedCovariance(c00=True,
c0t=True,
ctt=False,
remove_data_mean=True,
reversible=self.reversible,
lag=self.lag,
bessel=False,
stride=self.stride,
skip=self.skip,
weights=self.weights,
ncov_max=self.ncov_max)
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError(
"requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if self._logger_is_active(self._loglevel_DEBUG):
self.logger.debug(
"Running TICA with tau=%i; Estimating two covariance matrices"
" with dimension (%i, %i)", self._lag, indim, indim)
covar.estimate(iterable, chunksize=self.chunksize, **kw)
self.model.update_model_params(mean=covar.mean,
cov=covar.C00_,
cov_tau=covar.C0t_)
self._diagonalize()
return self.model
def _diagonalize(self):
# diagonalize with low rank approximation
self.logger.debug("diagonalize Cov and Cov_tau.")
try:
eigenvalues, eigenvectors = eig_corr(self.cov,
self.cov_tau,
self.epsilon,
sign_maxelement=True)
except ZeroRankError:
raise ZeroRankError(
'All input features are constant in all time steps. No dimension would be left after dimension reduction.'
)
if self.kinetic_map and self.commute_map:
raise ValueError(
'Trying to use both kinetic_map and commute_map. Use either or.'
)
if self.kinetic_map: # scale by eigenvalues
eigenvectors *= eigenvalues[None, :]
if self.commute_map: # scale by (regularized) timescales
timescales = 1 - self.lag / np.log(np.abs(eigenvalues))
# dampen timescales smaller than the lag time, as in section 2.5 of ref. [5]
regularized_timescales = 0.5 * timescales * np.maximum(
np.tanh(np.pi * ((timescales - self.lag) / self.lag) + 1), 0)
eigenvectors *= np.sqrt(regularized_timescales / 2)
self.logger.debug("finished diagonalisation.")
# compute cumulative variance
cumvar = np.cumsum(np.abs(eigenvalues)**2)
cumvar /= cumvar[-1]
self.model.update_model_params(cumvar=cumvar,
eigenvalues=eigenvalues,
eigenvectors=eigenvectors)
self._estimated = True
def __init__(self, lag, max_columns,
dim=-1, var_cutoff=TICABase._DEFAULT_VARIANCE_CUTOFF, epsilon=1e-6,
stride=1, skip=0, reversible=True, ncov_max=float('inf'),
initial_columns=None, nsel=1, selection_strategy='spectral-oasis', neig=None):
r""" Sparse sampling implementation [1]_ of time-lagged independent component analysis (TICA) [2]_, [3]_, [4]_.
Parameters
----------
lag : int
lag time
max_columns : int
Maximum number of columns (features) to use in the approximation.
dim : int, optional, default -1
Maximum number of significant independent components to use to reduce dimension of input data. -1 means
all numerically available dimensions (see epsilon) will be used unless reduced by var_cutoff.
Setting dim to a positive value is exclusive with var_cutoff.
var_cutoff : float in the range [0,1], optional, default 0.95
Determines the number of output dimensions by including dimensions until their cumulative kinetic variance
exceeds the fraction subspace_variance. var_cutoff=1.0 means all numerically available dimensions
(see epsilon) will be used, unless set by dim. Setting var_cutoff smaller than 1.0 is exclusive with dim.
epsilon : float, optional, default 1e-6
Eigenvalue norm cutoff. Eigenvalues of :math:`C_0` with norms <= epsilon will be
cut off. The remaining number of eigenvalues define the size
of the output.
stride: int, optional, default 1
Use only every stride-th time step. By default, every time step is used.
skip : int, optional, default 0
Skip the first initial n frames per trajectory.
reversible: bool, optional, default True
Symmetrize correlation matrices :math:`C_0`, :math:`C_{\tau}`.
initial_columns : list, ndarray(k, dtype=int), int, or None, optional, default None
Columns used for an initial approximation. If a list or an 1-d ndarray
of integers is given, use these column indices. If an integer is given,
use that number of randomly selected indices. If None is given, use
one randomly selected column.
nsel : int, optional, default 1
Number of columns to select and add per iteration and pass through the data.
Larger values provide for better pass-efficiency.
selection_strategy : str, optional, default 'spectral-oasis'
Strategy to use for selecting new columns for the approximation.
Can be 'random', 'oasis' or 'spectral-oasis'.
neig : int or None, optional, default None
Number of eigenvalues to be optimized by the selection process.
If None, use the whole available eigenspace
Notes
-----
Perform a sparse approximation of time-lagged independent component analysis (TICA)
:class:`TICA <pyemma.coordinates.transform.TICA>`. The starting point is the
generalized eigenvalue problem
.. math:: C_{\tau} r_i = C_0 \lambda_i(\tau) r_i.
Instead of computing the full matrices involved in this problem, we conduct
a Nyström approximation [5]_ of the matrix :math:`C_0` by means of the
accelerated sequential incoherence selection (oASIS) algorithm [6]_ and,
in particular, its extension called spectral oASIS [1]_.
Iteratively, we select a small number of columns such that the resulting
Nyström approximation is sufficiently accurate. This selection represents
in turn a subset of important features, for which we obtain a generalized
eigenvalue problem similar to the one above, but much smaller in size.
Its generalized eigenvalues and eigenvectors provide an approximation
to those of the full TICA solution [1]_.
References
----------
.. [1] F. Litzinger, L. Boninsegna, H. Wu, F. Nüske, R. Patel, R. Baraniuk, F. Noé, and C. Clementi.
Rapid calculation of molecular kinetics using compressed sensing (2018). (submitted)
.. [2] Perez-Hernandez G, F Paul, T Giorgino, G De Fabritiis and F Noe. 2013.
Identification of slow molecular order parameters for Markov model construction
J. Chem. Phys. 139, 015102. doi:10.1063/1.4811489
.. [3] Schwantes C, V S Pande. 2013.
Improvements in Markov State Model Construction Reveal Many Non-Native Interactions in the Folding of NTL9
J. Chem. Theory. Comput. 9, 2000-2009. doi:10.1021/ct300878a
.. [4] L. Molgedey and H. G. Schuster. 1994.
Separation of a mixture of independent signals using time delayed correlations
Phys. Rev. Lett. 72, 3634.
.. [5] P. Drineas and M. W. Mahoney.
On the Nystrom method for approximating a Gram matrix for improved kernel-based learning.
Journal of Machine Learning Research, 6:2153-2175 (2005).
.. [6] Raajen Patel, Thomas A. Goldstein, Eva L. Dyer, Azalia Mirhoseini, Richard G. Baraniuk.
oASIS: Adaptive Column Sampling for Kernel Matrix Approximation.
arXiv: 1505.05208 [stat.ML].
"""
super(NystroemTICA, self).__init__()
self._covar = LaggedCovariance(c00=True, c0t=True, ctt=False, remove_data_mean=True, reversible=reversible,
lag=lag, bessel=False, stride=stride, skip=skip, ncov_max=ncov_max)
self._diag = LaggedCovariance(c00=True, c0t=True, ctt=False, remove_data_mean=True, reversible=reversible,
lag=lag, bessel=False, stride=stride, skip=skip, ncov_max=ncov_max,
diag_only=True)
self._oasis = None
self.dim = dim
self.var_cutoff = var_cutoff
self.set_params(lag=lag, max_columns=max_columns,
epsilon=epsilon, reversible=reversible, stride=stride, skip=skip,
ncov_max=ncov_max,
initial_columns=initial_columns, nsel=nsel, selection_strategy=selection_strategy, neig=neig)
class NystroemTICA(TICABase, SerializableMixIn):
r""" Sparse sampling implementation of time-lagged independent component analysis (TICA)"""
__serialize_version = 0
__serialize_fields = ()
def __init__(self, lag, max_columns,
dim=-1, var_cutoff=TICABase._DEFAULT_VARIANCE_CUTOFF, epsilon=1e-6,
stride=1, skip=0, reversible=True, ncov_max=float('inf'),
initial_columns=None, nsel=1, selection_strategy='spectral-oasis', neig=None):
r""" Sparse sampling implementation [1]_ of time-lagged independent component analysis (TICA) [2]_, [3]_, [4]_.
Parameters
----------
lag : int
lag time
max_columns : int
Maximum number of columns (features) to use in the approximation.
dim : int, optional, default -1
Maximum number of significant independent components to use to reduce dimension of input data. -1 means
all numerically available dimensions (see epsilon) will be used unless reduced by var_cutoff.
Setting dim to a positive value is exclusive with var_cutoff.
var_cutoff : float in the range [0,1], optional, default 0.95
Determines the number of output dimensions by including dimensions until their cumulative kinetic variance
exceeds the fraction subspace_variance. var_cutoff=1.0 means all numerically available dimensions
(see epsilon) will be used, unless set by dim. Setting var_cutoff smaller than 1.0 is exclusive with dim.
epsilon : float, optional, default 1e-6
Eigenvalue norm cutoff. Eigenvalues of :math:`C_0` with norms <= epsilon will be
cut off. The remaining number of eigenvalues define the size
of the output.
stride: int, optional, default 1
Use only every stride-th time step. By default, every time step is used.
skip : int, optional, default 0
Skip the first initial n frames per trajectory.
reversible: bool, optional, default True
Symmetrize correlation matrices :math:`C_0`, :math:`C_{\tau}`.
initial_columns : list, ndarray(k, dtype=int), int, or None, optional, default None
Columns used for an initial approximation. If a list or an 1-d ndarray
of integers is given, use these column indices. If an integer is given,
use that number of randomly selected indices. If None is given, use
one randomly selected column.
nsel : int, optional, default 1
Number of columns to select and add per iteration and pass through the data.
Larger values provide for better pass-efficiency.
selection_strategy : str, optional, default 'spectral-oasis'
Strategy to use for selecting new columns for the approximation.
Can be 'random', 'oasis' or 'spectral-oasis'.
neig : int or None, optional, default None
Number of eigenvalues to be optimized by the selection process.
If None, use the whole available eigenspace
Notes
-----
Perform a sparse approximation of time-lagged independent component analysis (TICA)
:class:`TICA <pyemma.coordinates.transform.TICA>`. The starting point is the
generalized eigenvalue problem
.. math:: C_{\tau} r_i = C_0 \lambda_i(\tau) r_i.
Instead of computing the full matrices involved in this problem, we conduct
a Nyström approximation [5]_ of the matrix :math:`C_0` by means of the
accelerated sequential incoherence selection (oASIS) algorithm [6]_ and,
in particular, its extension called spectral oASIS [1]_.
Iteratively, we select a small number of columns such that the resulting
Nyström approximation is sufficiently accurate. This selection represents
in turn a subset of important features, for which we obtain a generalized
eigenvalue problem similar to the one above, but much smaller in size.
Its generalized eigenvalues and eigenvectors provide an approximation
to those of the full TICA solution [1]_.
References
----------
.. [1] F. Litzinger, L. Boninsegna, H. Wu, F. Nüske, R. Patel, R. Baraniuk, F. Noé, and C. Clementi.
Rapid calculation of molecular kinetics using compressed sensing (2018). (submitted)
.. [2] Perez-Hernandez G, F Paul, T Giorgino, G De Fabritiis and F Noe. 2013.
Identification of slow molecular order parameters for Markov model construction
J. Chem. Phys. 139, 015102. doi:10.1063/1.4811489
.. [3] Schwantes C, V S Pande. 2013.
Improvements in Markov State Model Construction Reveal Many Non-Native Interactions in the Folding of NTL9
J. Chem. Theory. Comput. 9, 2000-2009. doi:10.1021/ct300878a
.. [4] L. Molgedey and H. G. Schuster. 1994.
Separation of a mixture of independent signals using time delayed correlations
Phys. Rev. Lett. 72, 3634.
.. [5] P. Drineas and M. W. Mahoney.
On the Nystrom method for approximating a Gram matrix for improved kernel-based learning.
Journal of Machine Learning Research, 6:2153-2175 (2005).
.. [6] Raajen Patel, Thomas A. Goldstein, Eva L. Dyer, Azalia Mirhoseini, Richard G. Baraniuk.
oASIS: Adaptive Column Sampling for Kernel Matrix Approximation.
arXiv: 1505.05208 [stat.ML].
"""
super(NystroemTICA, self).__init__()
self._covar = LaggedCovariance(c00=True, c0t=True, ctt=False, remove_data_mean=True, reversible=reversible,
lag=lag, bessel=False, stride=stride, skip=skip, ncov_max=ncov_max)
self._diag = LaggedCovariance(c00=True, c0t=True, ctt=False, remove_data_mean=True, reversible=reversible,
lag=lag, bessel=False, stride=stride, skip=skip, ncov_max=ncov_max,
diag_only=True)
self._oasis = None
self.dim = dim
self.var_cutoff = var_cutoff
self.set_params(lag=lag, max_columns=max_columns,
epsilon=epsilon, reversible=reversible, stride=stride, skip=skip,
ncov_max=ncov_max,
initial_columns=initial_columns, nsel=nsel, selection_strategy=selection_strategy, neig=neig)
@property
def model(self):
if not hasattr(self, '_model') or self._model is None:
self._model = NystroemTICAModel()
return self._model
@property
def initial_columns(self):
return self._initial_columns
@initial_columns.setter
def initial_columns(self, initial_columns):
if not (initial_columns is None
or isinstance(initial_columns, (int, FunctionType, np.ndarray))):
raise ValueError('initial_columns has to be one of these types (None, int, function, ndarray),'
'but was {}'.format(type(initial_columns)))
if initial_columns is None:
initial_columns = 1
if isinstance(initial_columns, int):
i = initial_columns
initial_columns = lambda N: np.random.choice(N, i, replace=False)
if isinstance(initial_columns, np.ndarray):
initial_columns = ensure_int_vector(initial_columns)
self._initial_columns = initial_columns
def describe(self):
try:
dim = self.dimension()
except RuntimeError:
dim = self.dim
return "[NystroemTICA, lag = %i; max. columns = %i; max. output dim. = %i]" % (self.lag, self.max_columns, dim)
def estimate(self, X, **kwargs):
r"""
Chunk-based parameterization of NystroemTICA.
Iterates over all data several times to select important columns and
estimate the mean, covariance and time-lagged covariance. Finally, the
small-scale generalized eigenvalue problem is solved to determine
the approximate independent components.
"""
return super(NystroemTICA, self).estimate(X, **kwargs)
def _estimate(self, iterable, **kw):
from pyemma.coordinates.data import DataInMemory
if not isinstance(iterable, DataInMemory):
self.logger.warning('Every iteration of the selection process involves streaming of all data and featurization. '
'Depending on your setup, this might be inefficient.')
indim = iterable.dimension()
if not self.dim <= indim:
raise RuntimeError("requested more output dimensions (%i) than dimension"
" of input data (%i)" % (self.dim, indim))
if callable(self.initial_columns):
self.initial_columns = self.initial_columns(indim)
if not len(np.array(self.initial_columns).shape) == 1:
raise ValueError('initial_columns must be either None, an integer, a list, or a 1-d numpy array.')
self._diag.estimate(iterable, **kw)
self._covar.column_selection = self.initial_columns
self._covar.estimate(iterable, **kw)
self.model.update_model_params(cov_tau=self._covar.C0t_)
self._oasis = oASIS_Nystroem(self._diag.C00_, self._covar.C00_, self.initial_columns)
self._oasis.set_selection_strategy(strategy=self.selection_strategy, nsel=self.nsel, neig=self.neig)
while self._oasis.k < np.min((self.max_columns, self._oasis.n)):
cols = self._oasis.select_columns()
if cols is None or len(cols) == 0 or np.all(np.in1d(cols, self._oasis.column_indices)):
self.logger.warning("Iteration ended prematurely: No more columns to select.")
break
self._covar.column_selection = cols
self._covar.estimate(iterable, **kw)
ix = self._oasis.add_columns(self._covar.C00_, cols)
ix = np.in1d(cols, ix)
if np.any(ix):
added_columns = self._covar.C0t_[:, ix]
self.model.update_model_params(cov_tau=np.concatenate((self._model.cov_tau, added_columns), axis=1))
self.model.update_model_params(mean=self._covar.mean,
diag=self._diag.C00_,
cov=self._oasis.Ck,
column_indices=self._oasis.column_indices)
self._diagonalize()
return self.model
def _diagonalize(self):
# diagonalize with low rank approximation
self.logger.debug("Diagonalize Cov and Cov_tau.")
Wktau = self._model.cov_tau[self._model.column_indices, :]
try:
eigenvalues, eigenvectors = eig_corr(self._oasis.Wk, Wktau, self.epsilon, sign_maxelement=True)
except ZeroRankError:
raise ZeroRankError('All input features are constant in all time steps. '
'No dimension would be left after dimension reduction.')
self.logger.debug("Finished diagonalization.")
# compute cumulative variance
cumvar = np.cumsum(np.abs(eigenvalues) ** 2)
cumvar /= cumvar[-1]
self._model.update_model_params(cumvar=cumvar,
eigenvalues=eigenvalues,
eigenvectors=eigenvectors)
self._estimated = True
@property
def column_indices(self):
""" Indices of columns used in the approximation. """
return self.model.column_indices
