def tpt(T, A, B, mu=None, qminus=None, qplus=None, rate_matrix=False):
r""" Computes the A->B reactive flux using transition path theory (TPT)
Parameters
----------
T : (M, M) ndarray or scipy.sparse matrix
Transition matrix (default) or Rate matrix (if rate_matrix=True)
A : array_like
List of integer state labels for set A
B : array_like
List of integer state labels for set B
mu : (M,) ndarray (optional)
Stationary vector
qminus : (M,) ndarray (optional)
Backward committor for A->B reaction
qplus : (M,) ndarray (optional)
Forward committor for A-> B reaction
rate_matrix = False : boolean
By default (False), T is a transition matrix.
If set to True, T is a rate matrix.
Returns
-------
tpt: pyemma.msm.flux.ReactiveFlux object
A python object containing the reactive A->B flux network
and several additional quantities, such as stationary probability,
committors and set definitions.
Notes
-----
The central object used in transition path theory is
the forward and backward comittor function.
TPT (originally introduced in [1]) for continous systems has a
discrete version outlined in [2]. Here, we use the transition
matrix formulation described in [3].
See also
--------
pyemma.msm.analysis.committor, ReactiveFlux
References
----------
.. [1] W. E and E. Vanden-Eijnden.
Towards a theory of transition paths.
J. Stat. Phys. 123: 503-523 (2006)
.. [2] P. Metzner, C. Schuette and E. Vanden-Eijnden.
Transition Path Theory for Markov Jump Processes.
Multiscale Model Simul 7: 1192-1219 (2009)
.. [3] F. Noe, Ch. Schuette, E. Vanden-Eijnden, L. Reich and
T. Weikl: Constructing the Full Ensemble of Folding Pathways
from Short Off-Equilibrium Simulations.
Proc. Natl. Acad. Sci. USA, 106, 19011-19016 (2009)
"""
import pyemma.msm.analysis as msmana
if len(A) == 0 or len(B) == 0:
raise ValueError('set A or B is empty')
n = T.shape[0]
if len(A) > n or len(B) > n or max(A) > n or max(B) > n:
raise ValueError('set A or B defines more states, than given transition matrix.')
if (rate_matrix is False) and (not msmana.is_transition_matrix(T)):
raise ValueError('given matrix T is not a transition matrix')
if (rate_matrix is True):
raise NotImplementedError('TPT with rate matrix is not yet implemented - But it is very simple, so feel free to do it.')
# we can compute the following properties from either dense or sparse T
# stationary dist
if mu is None:
mu = msmana.stationary_distribution(T)
# forward committor
if qplus is None:
qplus = msmana.committor(T, A, B, forward=True)
# backward committor
if qminus is None:
if msmana.is_reversible(T, mu=mu):
qminus = 1.0-qplus
else:
qminus = msmana.committor(T, A, B, forward=False, mu=mu)
# gross flux
grossflux = flux_matrix(T, mu, qminus, qplus, netflux = False)
# net flux
netflux = to_netflux(grossflux)
# construct flux object
from reactive_flux import ReactiveFlux
F = ReactiveFlux(A, B, netflux, mu=mu, qminus=qminus, qplus=qplus, gross_flux=grossflux)
# done
return F
def test_backward_comittor(self):
P = self.bdc.transition_matrix()
un = committor(P, [0, 1], [8, 9], forward=False)
u = self.bdc.committor_backward(1, 8)
assert_allclose(un, u)
def test_backward_comittor(self):
P = self.bdc.transition_matrix_sparse()
un = committor(P, range(10), range(90, 100), forward=False)
u = self.bdc.committor_backward(9, 90)
assert_allclose(un, u)
def test_backward_comittor(self):
P = self.bdc.transition_matrix_sparse()
un = committor(P, range(10), range(90, 100), forward=False)
u = self.bdc.committor_backward(9, 90)
assert_allclose(un, u)
def test_backward_comittor(self):
P = self.bdc.transition_matrix()
un = committor(P, [0, 1], [8, 9], forward=False)
u = self.bdc.committor_backward(1, 8)
assert_allclose(un, u)
def tpt(T, A, B, mu=None, qminus=None, qplus=None, rate_matrix=False):
r""" Computes the A->B reactive flux using transition path theory (TPT)
Parameters
----------
T : (M, M) ndarray or scipy.sparse matrix
Transition matrix (default) or Rate matrix (if rate_matrix=True)
A : array_like
List of integer state labels for set A
B : array_like
List of integer state labels for set B
mu : (M,) ndarray (optional)
Stationary vector
qminus : (M,) ndarray (optional)
Backward committor for A->B reaction
qplus : (M,) ndarray (optional)
Forward committor for A-> B reaction
rate_matrix = False : boolean
By default (False), T is a transition matrix.
If set to True, T is a rate matrix.
Returns
-------
tpt: pyemma.msm.flux.ReactiveFlux object
A python object containing the reactive A->B flux network
and several additional quantities, such as stationary probability,
committors and set definitions.
Notes
-----
The central object used in transition path theory is
the forward and backward comittor function.
TPT (originally introduced in [1]) for continous systems has a
discrete version outlined in [2]. Here, we use the transition
matrix formulation described in [3].
See also
--------
pyemma.msm.analysis.committor, ReactiveFlux
References
----------
.. [1] W. E and E. Vanden-Eijnden.
Towards a theory of transition paths.
J. Stat. Phys. 123: 503-523 (2006)
.. [2] P. Metzner, C. Schuette and E. Vanden-Eijnden.
Transition Path Theory for Markov Jump Processes.
Multiscale Model Simul 7: 1192-1219 (2009)
.. [3] F. Noe, Ch. Schuette, E. Vanden-Eijnden, L. Reich and
T. Weikl: Constructing the Full Ensemble of Folding Pathways
from Short Off-Equilibrium Simulations.
Proc. Natl. Acad. Sci. USA, 106, 19011-19016 (2009)
"""
import pyemma.msm.analysis as msmana
if len(A) == 0 or len(B) == 0:
raise ValueError('set A or B is empty')
n = T.shape[0]
if len(A) > n or len(B) > n or max(A) > n or max(B) > n:
raise ValueError('set A or B defines more states, than given transition matrix.')
if (rate_matrix is False) and (not msmana.is_transition_matrix(T)):
raise ValueError('given matrix T is not a transition matrix')
if (rate_matrix is True):
raise NotImplementedError(
'TPT with rate matrix is not yet implemented - But it is very simple, so feel free to do it.')
# we can compute the following properties from either dense or sparse T
# stationary dist
if mu is None:
mu = msmana.stationary_distribution(T)
# forward committor
if qplus is None:
qplus = msmana.committor(T, A, B, forward=True)
# backward committor
if qminus is None:
if msmana.is_reversible(T, mu=mu):
qminus = 1.0 - qplus
else:
qminus = msmana.committor(T, A, B, forward=False, mu=mu)
# gross flux
grossflux = flux_matrix(T, mu, qminus, qplus, netflux=False)
# net flux
netflux = to_netflux(grossflux)
# construct flux object
from reactive_flux import ReactiveFlux
F = ReactiveFlux(A, B, netflux, mu=mu, qminus=qminus, qplus=qplus, gross_flux=grossflux)
# done
return F
def test_forward_comittor(self):
P=self.bdc.transition_matrix_sparse()
un=committor(P, range(10), range(90,100), forward=True)
u=self.bdc.committor_forward(9, 90)
self.assertTrue(np.allclose(un, u))
def test_forward_comittor(self):
P=self.bdc.transition_matrix()
un=committor(P, [0, 1], [8, 9], forward=True)
u=self.bdc.committor_forward(1, 8)
self.assertTrue(np.allclose(un, u))