Skip to content

Commit 9864ea2

Browse files
committed
use proper siunitx [ci skip]
1 parent 1be95cd commit 9864ea2

File tree

1 file changed

+13
-13
lines changed

1 file changed

+13
-13
lines changed

manuscript/manuscript.tex

Lines changed: 13 additions & 13 deletions
Original file line numberDiff line numberDiff line change
@@ -248,7 +248,7 @@ \subsection{Variational approach and TICA}
248248
\begin{equation}
249249
\mathbf{y}(t) = \mathbf{U}_d^\top \tilde{\mathbf{x}}(t),
250250
\end{equation}
251-
where, in practice, $d$ is chosen such that a specific fraction of kinetic variance $c_d$ is retained (e.g., $95\%$).
251+
where, in practice, $d$ is chosen such that a specific fraction of kinetic variance $c_d$ is retained (e.g., \SI{95}{\percent}).
252252

253253
\subsection{Hidden Markov state models}
254254

@@ -356,7 +356,7 @@ \subsection{The PyEMMA workflow}
356356

357357
For the remainder of this manuscript we will walk through the first notebook~00.
358358
In notebook~00 we analyze a dataset of the Trp-Leu-Ala-Leu-Leu pentapeptide (Fig.~\ref{fig:io-to-tica}a),
359-
consisting of~$25$ independent MD trajectories conducted in implicit solvent with frames saved at an interval of~$0.1$~ns.
359+
consisting of~$25$ independent MD trajectories conducted in implicit solvent with frames saved at an interval of~\SI{0.1}{\nano\second}.
360360
We present the results obtained in this notebook,
361361
thereby providing an example of how results generated using PyEMMA can be integrated into research publications.
362362
The figures that will be displayed in the following are created in the showcase notebook~00 and can be easily reproduced.
@@ -375,7 +375,7 @@ \subsection{Feature selection}
375375
\caption{Example analysis of the conformational dynamics of a pentapeptide backbone:
376376
(a)~The Trp-Leu-Ala-Leu-Leu pentapeptide in licorice representation~\cite{vmd}.
377377
(b)~The VAMP-2 score indicates which of the tested featurizations contains the highest kinetic variance.
378-
(c)~The sample free energy projected onto the first two time-lagged independent components (ICs) at lag time $\tau=0.5$~ns shows multiple minima and
378+
(c)~The sample free energy projected onto the first two time-lagged independent components (ICs) at lag time $\tau=\SI{0.5}{\nano\second}$ shows multiple minima and
379379
(d)~the time series of the first two ICs of the first trajectory show rare jumps.}
380380
\label{fig:io-to-tica}
381381
\end{figure}
@@ -398,7 +398,7 @@ \subsection{Feature selection}
398398
it is important to ensure that properties that we optimize are robust as a function of lag time.
399399
Consequently, we compute the VAMP-2 score at several lag times (notebook~00).
400400
We find that the relative rankings of the different molecular features are highly robust as a function of lag time.
401-
We show one example of this ranking and the absolute VAMP-2 scores for lag time~$0.5$~ns in Fig.~\ref{fig:io-to-tica}b.
401+
We show one example of this ranking and the absolute VAMP-2 scores for lag time~\SI{0.5}{\nano\second} in Fig.~\ref{fig:io-to-tica}b.
402402
We find that backbone torsions contain more kinetic variance than the backbone heavy atom positions or the distances between them (Fig.~\ref{fig:io-to-tica}b).
403403
This suggests that backbone torsions are the best of the options evaluated for MSM construction.
404404

@@ -410,7 +410,7 @@ \subsection{Dimensionality reduction}
410410
which typically contains many degrees of freedom,
411411
to a lower dimensional space that can be discretized with higher resolution and better statistical efficiency.
412412
TICA is a special case of the variational principle~\cite{noe-vac,nueske-vamk} and is designed to find a projection preserving the long-timescale dynamics in the dataset.
413-
Here, performing TICA on the backbone torsions at lag time~$0.5$~ns yields a four dimensional subspace using a~$95\%$ kinetic variance cutoff
413+
Here, performing TICA on the backbone torsions at lag time~\SI{0.5}{\nano\second} yields a four dimensional subspace using a~\SI{95}{\percent} kinetic variance cutoff
414414
(note that we perform a $\cos/\sin$-transformation of the torsions before TICA in order to preserve their periodicity).
415415
The sample free energy projected onto the first two independent components (ICs) exhibits several minima (Fig.~\ref{fig:io-to-tica}c).
416416
Discrete jumps between the minima can be observed by visualizing the transformation of the first trajectory into these ICs (Fig.~\ref{fig:io-to-tica}d).
@@ -435,19 +435,19 @@ \subsection{MSM estimation and validation}
435435
(a)~The convergence behavior of the implied timescales associated with the four slowest processes.
436436
The solid lines refer to the maximum likelihood result while the dashed lines show the ensemble mean computed with a Bayesian sampling procedure~\cite{ben-rev-msm}.
437437
The black line (marking equality of timescale and lag time) with grey area indicates the timescale horizon below which the MSM cannot resolve processes.
438-
As implied timescales are well-converged at $\tau=0.5$~ns, this lag time is chosen for subsequent MSM estimation.
439-
(b)~Chapman-Kolmogorov test computed using an MSM estimated with lag time $\tau=0.5$~ns assuming~5 metastable states.
438+
As implied timescales are well-converged at $\tau=\SI{0.5}{\nano\second}$, this lag time is chosen for subsequent MSM estimation.
439+
(b)~Chapman-Kolmogorov test computed using an MSM estimated with lag time $\tau=\SI{0.5}{\nano\second}$ assuming~5 metastable states.
440440
Predictions from this model agree with higher lag time estimates within confidence intervals.
441441
Implied timescales convergence as well as a passing Chapman-Kolmogorov test are a necessary condition in MSM validation.
442-
In both panels, the (non-grey) shaded areas indicate~$95\%$ confidence intervals computed with the aforementioned Bayesian sampling procedure.}
442+
In both panels, the (non-grey) shaded areas indicate~\SI{95}{\percent} confidence intervals computed with the aforementioned Bayesian sampling procedure.}
443443
\label{fig:its-and-ck}
444444
\end{figure}
445445

446446
A necessary condition for Markovian dynamics in our reduced space is that the ITS are approximately constant as a function of $\tau$;
447447
accordingly, we chose the smallest possible $\tau$ which fulfills this condition within the model uncertainty.
448448
The uncertainty bounds are computed using a Bayesian scheme~\cite{ben-rev-msm,noe-tmat-sampling} with~$100$ samples.
449-
In our example, we find that the four slowest ITS converge quickly and are constant within a $95\%$ confidence interval for lag times above~$0.5$~ns (Fig.~\ref{fig:its-and-ck}a).
450-
Using this lag time we can now estimate a (Bayesian) MSM with $\tau=0.5$~ns.
449+
In our example, we find that the four slowest ITS converge quickly and are constant within a \SI{95}{\percent} confidence interval for lag times above~\SI{0.5}{\nano\second} (Fig.~\ref{fig:its-and-ck}a).
450+
Using this lag time we can now estimate a (Bayesian) MSM with $\tau=\SI{0.5}{\nano\second}$.
451451

452452
To test the validity of our MSM, we perform a Chapman-Kolmogorov (CK) test.
453453
Visualizing the full transition probability matrix $T$ is difficult;
@@ -457,7 +457,7 @@ \subsection{MSM estimation and validation}
457457
The CK test (Fig.~\ref{fig:its-and-ck}b) shows that predictions from our MSM (blue-dashed lines)
458458
agrees well with MSMs estimated with longer lag times (black-solid lines)
459459
Thus, the CK test confirms that five metastable states is an appropriate choice
460-
and shows that the MSM we have estimated at lag time $\tau=0.5$~ns indeed predicts the
460+
and shows that the MSM we have estimated at lag time $\tau=\SI{0.5}{\nano\second}$ indeed predicts the
461461
long-timescale behavior of our system within error (blue/shaded area).
462462

463463
In notebook~03, we demonstrate in detail how to estimate and validate MSMs with PyEMMA.
@@ -525,7 +525,7 @@ \subsection{Analyzing the MSM}
525525

526526
The mean first passage times (MFPTs) out of and into the macrostate $\mathcal{S}_1$ compute to
527527
\[ \begin{array}{crcr}
528-
\textrm{direction} & \textrm{mean / ns} && \textrm{std / ns} \\
528+
\textrm{direction} & \textrm{mean / \si{\nano\second}} && \textrm{std / \si{\nano\second}} \\
529529
\hline
530530
\mathcal{S}_1 \to \mathcal{S}_{(2,3,4,5)} & 9.0 & \pm & 1.9 \\
531531
\mathcal{S}_{(2,3,4,5)} \to \mathcal{S}_1 & 2496.4 & \pm & 470.0
@@ -551,7 +551,7 @@ \subsection{Connecting the MSM with experimental data}
551551
(a)~the Trp-1 SASA autocorrelation function yields a weak signal which, however,
552552
(b)~can be enhanced if the system is prepared in the nonequilibrium condition $\mathcal{S}_1$.
553553
The solid/orange lines denote the maximum likelihood MSM result;
554-
the dashed/blue lines and the the shaded areas indicate sample means and~$95\%$ confidence intervals computed with a Bayesian sampling procedure~\cite{ben-rev-msm}.}
554+
the dashed/blue lines and the the shaded areas indicate sample means and~\SI{95}{\percent} confidence intervals computed with a Bayesian sampling procedure~\cite{ben-rev-msm}.}
555555
\label{fig:msm-exp-obs}
556556
\end{figure}
557557

0 commit comments

Comments
 (0)