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Following the previous article, this article aims to complete the analysis of the regime change optimization. Here we add the regime_landmark
parameter to the optimization.
As we have seen previously, the FLOSS algorithm is built on top of the Matrix Profile (MP). Thus, we have proposed several parameters that may or not impact the FLOSS prediction performance.
The variables for building the MP are:
mp_threshold
: the minimum similarity value to be considered for 1-NN.time_constraint
: the maximum distance to look for the nearest neighbor.window_size
: the default parameter always used to build an MP.Later, the FLOSS algorithm also has a parameter that needs tuning to optimize the prediction:
regime_threshold
: the threshold below which a regime change is considered.regime_landmark
: the point in time where the regime threshold is applied.Using the tidymodels
framework, we performed a basic grid search on all these parameters, now limiting the exploration
on the MP and focusing on the FLOSS parameters.
The workflow is as follows:
mp_threshold
: 0.0, 0.4, 0.6 and 0.8;time_constraint
: 0, 800 and 1500;window_size
: 25, 50, 75, 100, 125 and 150;regime_threshold
: 0.05 to 0.90, by 0.05 steps;regime_landmark
: 1 to 10, by 0.5 steps.The results were then combined with the previous optimization and deduplicated.
As before, we started by computing the importance of each parameter1. We used the same approach using the Bayesian Additive Regression Trees (BART) model to fit the tuning parameters as predictors of the FLOSS score.
Before starting the parameter importance analysis, we need to consider the parameter interactions since this is usually the weak spot of the analysis techniques.
The first BART model was fitted using the following parameters:
\[\begin{equation} \begin{aligned} E( score ) &= \alpha + time\_constraint\\ &\quad + mp\_threshold + window\_size\\ &\quad + regime\_threshold + regime\_landmark \end{aligned} \tag{1.1} \end{equation}\]
After checking the interactions, this is the refitted model:
\[\begin{equation} \begin{aligned} E( score ) &= \alpha + time\_constraint\\ &\quad + mp\_threshold + window\_size\\ &\quad + regime\_threshold + regime\_landmark\\ &\quad + \left(regime\_threshold \times regime\_landmark\right)\\ &\quad + \left(mp\_threshold \times regime\_landmark\right)\\ &\quad + \left(mp\_threshold \times window\_size\right) \end{aligned} \tag{1.2} \end{equation}\]
Fig. 1.2 shows the variable interaction strength between pairs of variables. That allows us to
verify if there are any significant interactions between the variables. Using the information from the first model fit,
equation (1.1), we see that regime_threshold
interacts strongly with regime_landmark
. This interaction
was already expected, and we see that even after refitting the model, equation (1.2), this interaction is
still strong.
This is not a problem per se but a signal we must be aware of when exploring the parameters.
After evaluating the interactions, we can then perform the analysis of the variable importance. The goal is to understand how the FLOSS score behaves when we change the parameters.
The techniques for evaluating the variable importances were described in the previous article.
Using the three techniques simultaneously allows a broad comparison of the model behavior3. All three methods are model-agnostic (separates interpretation from the model), but as we have seen, each method has its advantages and disadvantages4.
Fig. 1.3 then shows the variable importance using three methods: Feature Importance Ranking Measure
(FIRM) using Individual Conditional Expectation (ICE), Permutation-based, and Shapley Additive explanations (SHAP). The
first line of this figure shows an interesting result that probably comes from the main disadvantage of the FIRM method:
the method does not take into account interactions. We see that FIRM is the only one that disagrees with the other
two methods, giving much importance to window_size
.
In the second line, taking into account the interactions, we see that all methods somewhat agree with each other,
accentuating the importance of regime_threshold
, which makes sense as it is the most evident parameter we need to set
to determine if the Arc Counts are low enough to indicate a regime change.
Fig. 1.4 and 1.5 show the effect of each feature on the FLOSS score. The
more evident difference is the shape of the effect of time_constraint
that initially suggested better results with
larger values. However, removing the interactions seems to be a flat line.
Based on Figures 1.3 and 1.5 we can infer that:
regime_threshold
: is the most important feature, has an optimal value to be set, and since the high interaction with the regime_landmark
, both must be tuned simultaneously.
In this setting, high thresholds significantly impact the score, probably due to an increase in false positives starting on >0.65 the overall impact is mostly negative.
regime_landmark
: is not as important as the regime_threshold,
but since there is a high interaction, it must
not be underestimated. It is known that the Arc Counts have more uncertainty as we approach the margin of the
streaming, and this becomes evident looking at how the score is negatively affected for values below 3.5s.
window_size
: has a near zero impact on the score when correctly set. Nevertheless, for higher window values,
the score is negatively affected. This high value probably depends on the data domain. In this setting, the model is
being tuned towards the changes from atrial fibrillation/non-fibrillation; thus, the “shape of interest” is small
compared to the whole heartbeat waveform. Window sizes smaller than 150 are more suitable in this case. As Beyer et
al. noted, “as dimensionality increases, the distance to the nearest data point approaches the distance to the
farthest data point”5, which means that the bigger the window size, the smaller will be the contrast
between different regimes.
mp_threshold
: has a fair impact on the score, but primarily by not using it. We start to see a negative
impact on the score with values above 0.60, while a constant positive impact with lower values.
time_constraint
: is a parameter that must be interpreted cautiously. The 0 (zero) value means no
constraint, which is equivalent to the size of the FLOSS history buffer (in our setting, 5000). We can see that
this parameter’s impact throughout the possible values is constantly near zero.
In short, for the MP computation, the parameter that is worth tuning is the window_size
, while for the FLOSS
computation, both regime_threshold
(mainly) and regime_landmark
shall be tuned.
According to the FLOSS paper6, the window_size
is indeed a feature that can be tuned; nevertheless,
the results appear to be similar in a reasonably wide range of window sizes, up to a limit, consistent with our findings.
At this point, the grid search tested a total of 23,389 models with resulting (individual) scores from 0.0002 to 1669.83 (Q25: 0.9838, Q50: 1.8093, Q75: 3.3890).
First, we will visualize how the models (in general) performed throughout the individual recordings.
Fig. 1.6 shows a violin plot of equal areas clipped to the minimum value. The blue color indicates the recordings with a small IQR (interquartile range) of model scores. We see on the left half 10% of the recordings with the worst minimum score, and on the right half, 10% of the recordings with the best minimum score.
Next, we will visualize some of these predictions to understand why some recordings were difficult to segment. For us to have a simple baseline: a recording with just one regime change, and the model predicts exactly one regime change, but far from the truth, the score will be roughly 1.
Fig. 1.7 shows the best effort in predicting the most complex recordings. One information not declared before is that if the model does not predict any change, it will put a mark on the zero position. On the other side, the truth markers positioned at the beginning and the end of the recording were removed, as these locations lack information and do not represent a streaming setting. Compared to the corresponding figure in the previous article, we can see that even the most complex recordings had better predictions.
Fig. 1.8 shows the best performances of the best recordings. Notice that there are recordings with a significant duration and few regime changes, making it hard for a “trivial model” to predict randomly.
An online interactive version of all the datasets and predictions can be accessed at Shiny app.
Fig. 1.9 shows the distribution of the FLOSS score of the 10% worst (left side) and 10% best models across the recordings (right side). The bluish color highlights the models with SD below 3 and IQR below 1.
Here again, we can compare with the previous article and see an improvement in the performance, as the models present lower SD and IQR.
Fig. 1.10 the performance of the six best models. They are ordered from left to right, from the worst record to the best record. The top model is the one with the lowest mean across the scores. The blue line indicates the mean score, and the red line the median score. The scores above 3 are squished in the plot and colored according to the scale in the legend. Notice the improvement on the blue and red lines compared to the previous article.
We can see that some records (namely #19, #41, #93, #100, #107) are contained in the set of “difficult” records shown in Fig. 1.6.
The current status of the project shows that FLOSS is up to the task of signaling possible regime changes.
After introducing the regime_landmark
feature, the performance improves significantly, and we can narrow down the tuning space to a small number of parameters.
In parallel, another score measure is being developed based on the concept of Precision and Recall, but for time-series7. It is expected that such a score measure will help to choose the best final model where most of the significant regime changes are detected, keeping a reasonable amount of false positives that will be ruled out further by the classification algorithm.
Further evaluation will be performed in more datasets; later, the results will be presented here.
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zoo 1.8-12 2023-04-13 [1] CRAN (R 4.3.0)
[1] /workspace/.cache/R/renv/proj_libs/develop-e2b961e1/R-4.3/x86_64-pc-linux-gnu
[2] /usr/lib/R/library
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