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Time sequence prediction with FNN-LSTM

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Right now, we decide up on the plan alluded to within the conclusion of the current Deep attractors: The place deep studying meets chaos: make use of that very same method to generate forecasts for empirical time sequence knowledge.

“That very same method,” which for conciseness, I’ll take the freedom of referring to as FNN-LSTM, is because of William Gilpin’s 2020 paper “Deep reconstruction of unusual attractors from time sequence” (Gilpin 2020).

In a nutshell, the issue addressed is as follows: A system, identified or assumed to be nonlinear and extremely depending on preliminary situations, is noticed, leading to a scalar sequence of measurements. The measurements will not be simply – inevitably – noisy, however as well as, they’re – at finest – a projection of a multidimensional state house onto a line.

Classically in nonlinear time sequence evaluation, such scalar sequence of observations are augmented by supplementing, at each cut-off date, delayed measurements of that very same sequence – a way known as delay coordinate embedding (Sauer, Yorke, and Casdagli 1991). For instance, as a substitute of only a single vector X1, we may have a matrix of vectors X1, X2, and X3, with X2 containing the identical values as X1, however ranging from the third statement, and X3, from the fifth. On this case, the delay can be 2, and the embedding dimension, 3. Numerous theorems state that if these parameters are chosen adequately, it’s attainable to reconstruct the whole state house. There’s a downside although: The theorems assume that the dimensionality of the true state house is understood, which in lots of real-world purposes, received’t be the case.

That is the place Gilpin’s thought is available in: Prepare an autoencoder, whose intermediate illustration encapsulates the system’s attractor. Not simply any MSE-optimized autoencoder although. The latent illustration is regularized by false nearest neighbors (FNN) loss, a way generally used with delay coordinate embedding to find out an ample embedding dimension. False neighbors are those that are shut in n-dimensional house, however considerably farther aside in n+1-dimensional house. Within the aforementioned introductory submit, we confirmed how this method allowed to reconstruct the attractor of the (artificial) Lorenz system. Now, we wish to transfer on to prediction.

We first describe the setup, together with mannequin definitions, coaching procedures, and knowledge preparation. Then, we inform you the way it went.

Setup

From reconstruction to forecasting, and branching out into the actual world

Within the earlier submit, we educated an LSTM autoencoder to generate a compressed code, representing the attractor of the system. As typical with autoencoders, the goal when coaching is similar because the enter, that means that general loss consisted of two parts: The FNN loss, computed on the latent illustration solely, and the mean-squared-error loss between enter and output. Now for prediction, the goal consists of future values, as many as we want to predict. Put otherwise: The structure stays the identical, however as a substitute of reconstruction we carry out prediction, in the usual RNN manner. The place the standard RNN setup would simply immediately chain the specified variety of LSTMs, we have now an LSTM encoder that outputs a (timestep-less) latent code, and an LSTM decoder that ranging from that code, repeated as many instances as required, forecasts the required variety of future values.

This after all implies that to guage forecast efficiency, we have to examine towards an LSTM-only setup. That is precisely what we’ll do, and comparability will develop into fascinating not simply quantitatively, however qualitatively as properly.

We carry out these comparisons on the 4 datasets Gilpin selected to reveal attractor reconstruction on observational knowledge. Whereas all of those, as is clear from the photographs in that pocket book, exhibit good attractors, we’ll see that not all of them are equally suited to forecasting utilizing easy RNN-based architectures – with or with out FNN regularization. However even people who clearly demand a distinct strategy permit for fascinating observations as to the affect of FNN loss.

Mannequin definitions and coaching setup

In all 4 experiments, we use the identical mannequin definitions and coaching procedures, the one differing parameter being the variety of timesteps used within the LSTMs (for causes that can develop into evident once we introduce the person datasets).

Each architectures had been chosen to be easy, and about comparable in variety of parameters – each mainly encompass two LSTMs with 32 models (n_recurrent will likely be set to 32 for all experiments).

FNN-LSTM

FNN-LSTM appears to be like almost like within the earlier submit, other than the truth that we break up up the encoder LSTM into two, to uncouple capability (n_recurrent) from maximal latent state dimensionality (n_latent, stored at 10 similar to earlier than).

# DL-related packages
library(tensorflow)
library(keras)
library(tfdatasets)
library(tfautograph)
library(reticulate)

# going to wish these later
library(tidyverse)
library(cowplot)

encoder_model <- operate(n_timesteps,
                          n_features,
                          n_recurrent,
                          n_latent,
                          identify = NULL) {
  
  keras_model_custom(identify = identify, operate(self) {
    
    self$noise <- layer_gaussian_noise(stddev = 0.5)
    self$lstm1 <-  layer_lstm(
      models = n_recurrent,
      input_shape = c(n_timesteps, n_features),
      return_sequences = TRUE
    ) 
    self$batchnorm1 <- layer_batch_normalization()
    self$lstm2 <-  layer_lstm(
      models = n_latent,
      return_sequences = FALSE
    ) 
    self$batchnorm2 <- layer_batch_normalization()
    
    operate (x, masks = NULL) {
      x %>%
        self$noise() %>%
        self$lstm1() %>%
        self$batchnorm1() %>%
        self$lstm2() %>%
        self$batchnorm2() 
    }
  })
}

decoder_model <- operate(n_timesteps,
                          n_features,
                          n_recurrent,
                          n_latent,
                          identify = NULL) {
  
  keras_model_custom(identify = identify, operate(self) {
    
    self$repeat_vector <- layer_repeat_vector(n = n_timesteps)
    self$noise <- layer_gaussian_noise(stddev = 0.5)
    self$lstm <- layer_lstm(
      models = n_recurrent,
      return_sequences = TRUE,
      go_backwards = TRUE
    ) 
    self$batchnorm <- layer_batch_normalization()
    self$elu <- layer_activation_elu() 
    self$time_distributed <- time_distributed(layer = layer_dense(models = n_features))
    
    operate (x, masks = NULL) {
      x %>%
        self$repeat_vector() %>%
        self$noise() %>%
        self$lstm() %>%
        self$batchnorm() %>%
        self$elu() %>%
        self$time_distributed()
    }
  })
}

n_latent <- 10L
n_features <- 1
n_hidden <- 32

encoder <- encoder_model(n_timesteps,
                         n_features,
                         n_hidden,
                         n_latent)

decoder <- decoder_model(n_timesteps,
                         n_features,
                         n_hidden,
                         n_latent)

The regularizer, FNN loss, is unchanged:

loss_false_nn <- operate(x) {
  
  # altering these parameters is equal to
  # altering the energy of the regularizer, so we hold these mounted (these values
  # correspond to the unique values utilized in Kennel et al 1992).
  rtol <- 10 
  atol <- 2
  k_frac <- 0.01
  
  okay <- max(1, flooring(k_frac * batch_size))
  
  ## Vectorized model of distance matrix calculation
  tri_mask <-
    tf$linalg$band_part(
      tf$ones(
        form = c(tf$solid(n_latent, tf$int32), tf$solid(n_latent, tf$int32)),
        dtype = tf$float32
      ),
      num_lower = -1L,
      num_upper = 0L
    )
  
  # latent x batch_size x latent
  batch_masked <-
    tf$multiply(tri_mask[, tf$newaxis,], x[tf$newaxis, reticulate::py_ellipsis()])
  
  # latent x batch_size x 1
  x_squared <-
    tf$reduce_sum(batch_masked * batch_masked,
                  axis = 2L,
                  keepdims = TRUE)
  
  # latent x batch_size x batch_size
  pdist_vector <- x_squared + tf$transpose(x_squared, perm = c(0L, 2L, 1L)) -
    2 * tf$matmul(batch_masked, tf$transpose(batch_masked, perm = c(0L, 2L, 1L)))
  
  #(latent, batch_size, batch_size)
  all_dists <- pdist_vector
  # latent
  all_ra <-
    tf$sqrt((1 / (
      batch_size * tf$vary(1, 1 + n_latent, dtype = tf$float32)
    )) *
      tf$reduce_sum(tf$sq.(
        batch_masked - tf$reduce_mean(batch_masked, axis = 1L, keepdims = TRUE)
      ), axis = c(1L, 2L)))
  
  # Keep away from singularity within the case of zeros
  #(latent, batch_size, batch_size)
  all_dists <-
    tf$clip_by_value(all_dists, 1e-14, tf$reduce_max(all_dists))
  
  #inds = tf.argsort(all_dists, axis=-1)
  top_k <- tf$math$top_k(-all_dists, tf$solid(okay + 1, tf$int32))
  # (#(latent, batch_size, batch_size)
  top_indices <- top_k[[1]]
  
  #(latent, batch_size, batch_size)
  neighbor_dists_d <-
    tf$collect(all_dists, top_indices, batch_dims = -1L)
  #(latent - 1, batch_size, batch_size)
  neighbor_new_dists <-
    tf$collect(all_dists[2:-1, , ],
              top_indices[1:-2, , ],
              batch_dims = -1L)
  
  # Eq. 4 of Kennel et al.
  #(latent - 1, batch_size, batch_size)
  scaled_dist <- tf$sqrt((
    tf$sq.(neighbor_new_dists) -
      # (9, 8, 2)
      tf$sq.(neighbor_dists_d[1:-2, , ])) /
      # (9, 8, 2)
      tf$sq.(neighbor_dists_d[1:-2, , ])
  )
  
  # Kennel situation #1
  #(latent - 1, batch_size, batch_size)
  is_false_change <- (scaled_dist > rtol)
  # Kennel situation 2
  #(latent - 1, batch_size, batch_size)
  is_large_jump <-
    (neighbor_new_dists > atol * all_ra[1:-2, tf$newaxis, tf$newaxis])
  
  is_false_neighbor <-
    tf$math$logical_or(is_false_change, is_large_jump)
  #(latent - 1, batch_size, 1)
  total_false_neighbors <-
    tf$solid(is_false_neighbor, tf$int32)[reticulate::py_ellipsis(), 2:(k + 2)]
  
  # Pad zero to match dimensionality of latent house
  # (latent - 1)
  reg_weights <-
    1 - tf$reduce_mean(tf$solid(total_false_neighbors, tf$float32), axis = c(1L, 2L))
  # (latent,)
  reg_weights <- tf$pad(reg_weights, record(record(1L, 0L)))
  
  # Discover batch common exercise
  
  # L2 Exercise regularization
  activations_batch_averaged <-
    tf$sqrt(tf$reduce_mean(tf$sq.(x), axis = 0L))
  
  loss <- tf$reduce_sum(tf$multiply(reg_weights, activations_batch_averaged))
  loss
  
}

Coaching is unchanged as properly, other than the truth that now, we frequently output latent variable variances along with the losses. It is because with FNN-LSTM, we have now to decide on an ample weight for the FNN loss element. An “ample weight” is one the place the variance drops sharply after the primary n variables, with n thought to correspond to attractor dimensionality. For the Lorenz system mentioned within the earlier submit, that is how these variances appeared:

     V1       V2        V3        V4        V5        V6        V7        V8        V9       V10
 0.0739   0.0582   1.12e-6   3.13e-4   1.43e-5   1.52e-8   1.35e-6   1.86e-4   1.67e-4   4.39e-5

If we take variance as an indicator of significance, the primary two variables are clearly extra essential than the remainder. This discovering properly corresponds to “official” estimates of Lorenz attractor dimensionality. For instance, the correlation dimension is estimated to lie round 2.05 (Grassberger and Procaccia 1983).

Thus, right here we have now the coaching routine:

train_step <- operate(batch) {
  with (tf$GradientTape(persistent = TRUE) %as% tape, {
    code <- encoder(batch[[1]])
    prediction <- decoder(code)
    
    l_mse <- mse_loss(batch[[2]], prediction)
    l_fnn <- loss_false_nn(code)
    loss <- l_mse + fnn_weight * l_fnn
  })
  
  encoder_gradients <-
    tape$gradient(loss, encoder$trainable_variables)
  decoder_gradients <-
    tape$gradient(loss, decoder$trainable_variables)
  
  optimizer$apply_gradients(purrr::transpose(record(
    encoder_gradients, encoder$trainable_variables
  )))
  optimizer$apply_gradients(purrr::transpose(record(
    decoder_gradients, decoder$trainable_variables
  )))
  
  train_loss(loss)
  train_mse(l_mse)
  train_fnn(l_fnn)
  
  
}

training_loop <- tf_function(autograph(operate(ds_train) {
  for (batch in ds_train) {
    train_step(batch)
  }
  
  tf$print("Loss: ", train_loss$end result())
  tf$print("MSE: ", train_mse$end result())
  tf$print("FNN loss: ", train_fnn$end result())
  
  train_loss$reset_states()
  train_mse$reset_states()
  train_fnn$reset_states()
  
}))


mse_loss <-
  tf$keras$losses$MeanSquaredError(discount = tf$keras$losses$Discount$SUM)

train_loss <- tf$keras$metrics$Imply(identify = 'train_loss')
train_fnn <- tf$keras$metrics$Imply(identify = 'train_fnn')
train_mse <-  tf$keras$metrics$Imply(identify = 'train_mse')

# fnn_multiplier ought to be chosen individually per dataset
# that is the worth we used on the geyser dataset
fnn_multiplier <- 0.7
fnn_weight <- fnn_multiplier * nrow(x_train)/batch_size

# studying price can also want adjustment
optimizer <- optimizer_adam(lr = 1e-3)

for (epoch in 1:200) {
 cat("Epoch: ", epoch, " -----------n")
 training_loop(ds_train)
 
 test_batch <- as_iterator(ds_test) %>% iter_next()
 encoded <- encoder(test_batch[[1]]) 
 test_var <- tf$math$reduce_variance(encoded, axis = 0L)
 print(test_var %>% as.numeric() %>% spherical(5))
}

On to what we’ll use as a baseline for comparability.

Vanilla LSTM

Right here is the vanilla LSTM, stacking two layers, every, once more, of dimension 32. Dropout and recurrent dropout had been chosen individually per dataset, as was the training price.

lstm <- operate(n_latent, n_timesteps, n_features, n_recurrent, dropout, recurrent_dropout,
                 optimizer = optimizer_adam(lr =  1e-3)) {
  
  mannequin <- keras_model_sequential() %>%
    layer_lstm(
      models = n_recurrent,
      input_shape = c(n_timesteps, n_features),
      dropout = dropout, 
      recurrent_dropout = recurrent_dropout,
      return_sequences = TRUE
    ) %>% 
    layer_lstm(
      models = n_recurrent,
      dropout = dropout,
      recurrent_dropout = recurrent_dropout,
      return_sequences = TRUE
    ) %>% 
    time_distributed(layer_dense(models = 1))
  
  mannequin %>%
    compile(
      loss = "mse",
      optimizer = optimizer
    )
  mannequin
  
}

mannequin <- lstm(n_latent, n_timesteps, n_features, n_hidden, dropout = 0.2, recurrent_dropout = 0.2)

Information preparation

For all experiments, knowledge had been ready in the identical manner.

In each case, we used the primary 10000 measurements out there within the respective .pkl recordsdata offered by Gilpin in his GitHub repository. To avoid wasting on file dimension and never rely upon an exterior knowledge supply, we extracted these first 10000 entries to .csv recordsdata downloadable immediately from this weblog’s repo:

geyser <- obtain.file(
  "https://uncooked.githubusercontent.com/rstudio/ai-blog/grasp/docs/posts/2020-07-20-fnn-lstm/knowledge/geyser.csv",
  "knowledge/geyser.csv")

electrical energy <- obtain.file(
  "https://uncooked.githubusercontent.com/rstudio/ai-blog/grasp/docs/posts/2020-07-20-fnn-lstm/knowledge/electrical energy.csv",
  "knowledge/electrical energy.csv")

ecg <- obtain.file(
  "https://uncooked.githubusercontent.com/rstudio/ai-blog/grasp/docs/posts/2020-07-20-fnn-lstm/knowledge/ecg.csv",
  "knowledge/ecg.csv")

mouse <- obtain.file(
  "https://uncooked.githubusercontent.com/rstudio/ai-blog/grasp/docs/posts/2020-07-20-fnn-lstm/knowledge/mouse.csv",
  "knowledge/mouse.csv")

Must you wish to entry the whole time sequence (of significantly better lengths), simply obtain them from Gilpin’s repo and cargo them utilizing reticulate:

Right here is the information preparation code for the primary dataset, geyser – all different datasets had been handled the identical manner.

# the primary 10000 measurements from the compilation offered by Gilpin
geyser <- read_csv("geyser.csv", col_names = FALSE) %>% choose(X1) %>% pull() %>% unclass()

# standardize
geyser <- scale(geyser)

# varies per dataset; see under 
n_timesteps <- 60
batch_size <- 32

# remodel into [batch_size, timesteps, features] format required by RNNs
gen_timesteps <- operate(x, n_timesteps) {
  do.name(rbind,
          purrr::map(seq_along(x),
                     operate(i) {
                       begin <- i
                       finish <- i + n_timesteps - 1
                       out <- x[start:end]
                       out
                     })
  ) %>%
    na.omit()
}

n <- 10000
practice <- gen_timesteps(geyser[1:(n/2)], 2 * n_timesteps)
check <- gen_timesteps(geyser[(n/2):n], 2 * n_timesteps) 

dim(practice) <- c(dim(practice), 1)
dim(check) <- c(dim(check), 1)

# break up into enter and goal  
x_train <- practice[ , 1:n_timesteps, , drop = FALSE]
y_train <- practice[ , (n_timesteps + 1):(2*n_timesteps), , drop = FALSE]

x_test <- check[ , 1:n_timesteps, , drop = FALSE]
y_test <- check[ , (n_timesteps + 1):(2*n_timesteps), , drop = FALSE]

# create tfdatasets
ds_train <- tensor_slices_dataset(record(x_train, y_train)) %>%
  dataset_shuffle(nrow(x_train)) %>%
  dataset_batch(batch_size)

ds_test <- tensor_slices_dataset(record(x_test, y_test)) %>%
  dataset_batch(nrow(x_test))

Now we’re prepared to have a look at how forecasting goes on our 4 datasets.

Experiments

Geyser dataset

Individuals working with time sequence could have heard of Previous Devoted, a geyser in Wyoming, US that has frequently been erupting each 44 minutes to 2 hours because the yr 2004. For the subset of knowledge Gilpin extracted,

geyser_train_test.pkl corresponds to detrended temperature readings from the principle runoff pool of the Previous Devoted geyser in Yellowstone Nationwide Park, downloaded from the GeyserTimes database. Temperature measurements begin on April 13, 2015 and happen in one-minute increments.

Like we stated above, geyser.csv is a subset of those measurements, comprising the primary 10000 knowledge factors. To decide on an ample timestep for the LSTMs, we examine the sequence at numerous resolutions:


Geyer dataset. Top: First 1000 observations. Bottom: Zooming in on the first 200.

Determine 1: Geyer dataset. High: First 1000 observations. Backside: Zooming in on the primary 200.

It looks like the conduct is periodic with a interval of about 40-50; a timestep of 60 thus appeared like strive.

Having educated each FNN-LSTM and the vanilla LSTM for 200 epochs, we first examine the variances of the latent variables on the check set. The worth of fnn_multiplier equivalent to this run was 0.7.

test_batch <- as_iterator(ds_test) %>% iter_next()
encoded <- encoder(test_batch[[1]]) %>%
  as.array() %>%
  as_tibble()

encoded %>% summarise_all(var)
   V1     V2        V3          V4       V5       V6       V7       V8       V9      V10
0.258 0.0262 0.0000627 0.000000600 0.000533 0.000362 0.000238 0.000121 0.000518 0.000365

There’s a drop in significance between the primary two variables and the remainder; nonetheless, not like within the Lorenz system, V1 and V2 variances additionally differ by an order of magnitude.

Now, it’s fascinating to check prediction errors for each fashions. We’re going to make a remark that can carry by to all three datasets to come back.

Maintaining the suspense for some time, right here is the code used to compute per-timestep prediction errors from each fashions. The identical code will likely be used for all different datasets.

calc_mse <- operate(df, y_true, y_pred) {
  (sum((df[[y_true]] - df[[y_pred]])^2))/nrow(df)
}

get_mse <- operate(test_batch, prediction) {
  
  comp_df <- 
    knowledge.body(
      test_batch[[2]][, , 1] %>%
        as.array()) %>%
        rename_with(operate(identify) paste0(identify, "_true")) %>%
    bind_cols(
      knowledge.body(
        prediction[, , 1] %>%
          as.array()) %>%
          rename_with(operate(identify) paste0(identify, "_pred")))
  
  mse <- purrr::map(1:dim(prediction)[2],
                        operate(varno)
                          calc_mse(comp_df,
                                   paste0("X", varno, "_true"),
                                   paste0("X", varno, "_pred"))) %>%
    unlist()
  
  mse
}

prediction_fnn <- decoder(encoder(test_batch[[1]]))
mse_fnn <- get_mse(test_batch, prediction_fnn)

prediction_lstm <- mannequin %>% predict(ds_test)
mse_lstm <- get_mse(test_batch, prediction_lstm)

mses <- knowledge.body(timestep = 1:n_timesteps, fnn = mse_fnn, lstm = mse_lstm) %>%
  collect(key = "sort", worth = "mse", -timestep)

ggplot(mses, aes(timestep, mse, shade = sort)) +
  geom_point() +
  scale_color_manual(values = c("#00008B", "#3CB371")) +
  theme_classic() +
  theme(legend.place = "none") 

And right here is the precise comparability. One factor particularly jumps to the attention: FNN-LSTM forecast error is considerably decrease for preliminary timesteps, at the start, for the very first prediction, which from this graph we anticipate to be fairly good!


Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Green: LSTM. Blue: FNN-LSTM.

Determine 2: Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Inexperienced: LSTM. Blue: FNN-LSTM.

Curiously, we see “jumps” in prediction error, for FNN-LSTM, between the very first forecast and the second, after which between the second and the following ones, reminding of the same jumps in variable significance for the latent code! After the primary ten timesteps, vanilla LSTM has caught up with FNN-LSTM, and we received’t interpret additional improvement of the losses based mostly on only a single run’s output.

As a substitute, let’s examine precise predictions. We randomly decide sequences from the check set, and ask each FNN-LSTM and vanilla LSTM for a forecast. The identical process will likely be adopted for the opposite datasets.

given <- knowledge.body(as.array(tf$concat(record(
  test_batch[[1]][, , 1], test_batch[[2]][, , 1]
),
axis = 1L)) %>% t()) %>%
  add_column(sort = "given") %>%
  add_column(num = 1:(2 * n_timesteps))

fnn <- knowledge.body(as.array(prediction_fnn[, , 1]) %>%
                    t()) %>%
  add_column(sort = "fnn") %>%
  add_column(num = (n_timesteps  + 1):(2 * n_timesteps))

lstm <- knowledge.body(as.array(prediction_lstm[, , 1]) %>%
                     t()) %>%
  add_column(sort = "lstm") %>%
  add_column(num = (n_timesteps + 1):(2 * n_timesteps))

compare_preds_df <- bind_rows(given, lstm, fnn)

plots <- 
  purrr::map(pattern(1:dim(compare_preds_df)[2], 16),
             operate(v) {
               ggplot(compare_preds_df, aes(num, .knowledge[[paste0("X", v)]], shade = sort)) +
                 geom_line() +
                 theme_classic() +
                 theme(legend.place = "none", axis.title = element_blank()) +
                 scale_color_manual(values = c("#00008B", "#DB7093", "#3CB371"))
             })

plot_grid(plotlist = plots, ncol = 4)

Listed here are sixteen random picks of predictions on the check set. The bottom fact is displayed in pink; blue forecasts are from FNN-LSTM, inexperienced ones from vanilla LSTM.


60-step ahead predictions from FNN-LSTM (blue) and vanilla LSTM (green) on randomly selected sequences from the test set. Pink: the ground truth.

Determine 3: 60-step forward predictions from FNN-LSTM (blue) and vanilla LSTM (inexperienced) on randomly chosen sequences from the check set. Pink: the bottom fact.

What we anticipate from the error inspection comes true: FNN-LSTM yields considerably higher predictions for quick continuations of a given sequence.

Let’s transfer on to the second dataset on our record.

Electrical energy dataset

This can be a dataset on energy consumption, aggregated over 321 completely different households and fifteen-minute-intervals.

electricity_train_test.pkl corresponds to common energy consumption by 321 Portuguese households between 2012 and 2014, in models of kilowatts consumed in fifteen minute increments. This dataset is from the UCI machine studying database.

Right here, we see a really common sample:


Electricity dataset. Top: First 2000 observations. Bottom: Zooming in on 500 observations, skipping the very beginning of the series.

Determine 4: Electrical energy dataset. High: First 2000 observations. Backside: Zooming in on 500 observations, skipping the very starting of the sequence.

With such common conduct, we instantly tried to foretell the next variety of timesteps (120) – and didn’t need to retract behind that aspiration.

For an fnn_multiplier of 0.5, latent variable variances seem like this:

V1          V2            V3       V4       V5            V6       V7         V8      V9     V10
0.390 0.000637 0.00000000288 1.48e-10 2.10e-11 0.00000000119 6.61e-11 0.00000115 1.11e-4 1.40e-4

We positively see a pointy drop already after the primary variable.

How do prediction errors examine on the 2 architectures?


Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Green: LSTM. Blue: FNN-LSTM.

Determine 5: Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Inexperienced: LSTM. Blue: FNN-LSTM.

Right here, FNN-LSTM performs higher over a protracted vary of timesteps, however once more, the distinction is most seen for quick predictions. Will an inspection of precise predictions verify this view?


60-step ahead predictions from FNN-LSTM (blue) and vanilla LSTM (green) on randomly selected sequences from the test set. Pink: the ground truth.

Determine 6: 60-step forward predictions from FNN-LSTM (blue) and vanilla LSTM (inexperienced) on randomly chosen sequences from the check set. Pink: the bottom fact.

It does! In truth, forecasts from FNN-LSTM are very spectacular on all time scales.

Now that we’ve seen the straightforward and predictable, let’s strategy the bizarre and troublesome.

ECG dataset

Says Gilpin,

ecg_train.pkl and ecg_test.pkl correspond to ECG measurements for 2 completely different sufferers, taken from the PhysioNet QT database.

How do these look?


ECG dataset. Top: First 1000 observations. Bottom: Zooming in on the first 400 observations.

Determine 7: ECG dataset. High: First 1000 observations. Backside: Zooming in on the primary 400 observations.

To the layperson that I’m, these don’t look almost as common as anticipated. First experiments confirmed that each architectures will not be able to coping with a excessive variety of timesteps. In each strive, FNN-LSTM carried out higher for the very first timestep.

That is additionally the case for n_timesteps = 12, the ultimate strive (after 120, 60 and 30). With an fnn_multiplier of 1, the latent variances obtained amounted to the next:

     V1        V2          V3        V4         V5       V6       V7         V8         V9       V10
  0.110  1.16e-11     3.78e-9 0.0000992    9.63e-9  4.65e-5  1.21e-4    9.91e-9    3.81e-9   2.71e-8

There is a spot between the primary variable and all different ones; however not a lot variance is defined by V1 both.

Aside from the very first prediction, vanilla LSTM reveals decrease forecast errors this time; nonetheless, we have now so as to add that this was not persistently noticed when experimenting with different timestep settings.


Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Green: LSTM. Blue: FNN-LSTM.

Determine 8: Per-timestep prediction error as obtained by FNN-LSTM and a vanilla stacked LSTM. Inexperienced: LSTM. Blue: FNN-LSTM.

precise predictions, each architectures carry out finest when a persistence forecast is ample – in reality, they produce one even when it’s not.


60-step ahead predictions from FNN-LSTM (blue) and vanilla LSTM (green) on randomly selected sequences from the test set. Pink: the ground truth.

Determine 9: 60-step forward predictions from FNN-LSTM (blue) and vanilla LSTM (inexperienced) on randomly chosen sequences from the check set. Pink: the bottom fact.

On this dataset, we actually would wish to discover different architectures higher capable of seize the presence of excessive and low frequencies within the knowledge, akin to combination fashions. However – had been we pressured to stick with considered one of these, and will do a one-step-ahead, rolling forecast, we’d go together with FNN-LSTM.

Talking of blended frequencies – we haven’t seen the extremes but …

Mouse dataset

“Mouse,” that’s spike charges recorded from a mouse thalamus.

mouse.pkl A time sequence of spiking charges for a neuron in a mouse thalamus. Uncooked spike knowledge was obtained from CRCNS and processed with the authors’ code with the intention to generate a spike price time sequence.


Mouse dataset. Top: First 2000 observations. Bottom: Zooming in on the first 500 observations.

Determine 10: Mouse dataset. High: First 2000 observations. Backside: Zooming in on the primary 500 observations.

Clearly, this dataset will likely be very laborious to foretell. How, after “lengthy” silence, have you learnt {that a} neuron goes to fireside?

As typical, we examine latent code variances (fnn_multiplier was set to 0.4):

Whereas it’s straightforward to acquire these estimates, utilizing, as an example, the nonlinearTseries package deal explicitly modeled after practices described in Kantz & Schreiber’s basic (Kantz and Schreiber 2004), we don’t wish to extrapolate from our tiny pattern of datasets, and go away such explorations and analyses to additional posts, and/or the reader’s ventures :-). In any case, we hope you loved the demonstration of sensible usability of an strategy that within the previous submit, was primarily launched by way of its conceptual attractivity.

Thanks for studying!

Gilpin, William. 2020. “Deep Reconstruction of Unusual Attractors from Time Collection.” https://arxiv.org/abs/2002.05909.
Grassberger, Peter, and Itamar Procaccia. 1983. “Measuring the Strangeness of Unusual Attractors.” Physica D: Nonlinear Phenomena 9 (1): 189–208. https://doi.org/https://doi.org/10.1016/0167-2789(83)90298-1.

Kantz, Holger, and Thomas Schreiber. 2004. Nonlinear Time Collection Evaluation. Cambridge College Press.

Sauer, Tim, James A. Yorke, and Martin Casdagli. 1991. Embedology.” Journal of Statistical Physics 65 (3-4): 579–616. https://doi.org/10.1007/BF01053745.

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