For us deep studying practitioners, the world is – not flat, however – linear, principally. Or piecewise linear. Like different
linear approximations, or possibly much more so, deep studying might be extremely profitable at making predictions. However let’s
admit it – generally we simply miss the joys of the nonlinear, of excellent, outdated, deterministic-yet-unpredictable chaos. Can we
have each? It appears like we will. On this put up, we’ll see an utility of deep studying (DL) to nonlinear time collection
prediction – or fairly, the important step that predates it: reconstructing the attractor underlying its dynamics. Whereas this
put up is an introduction, presenting the subject from scratch, additional posts will construct on this and extrapolate to observational

What to anticipate from this put up

In his 2020 paper Deep reconstruction of unusual attractors from time collection (Gilpin 2020), William Gilpin makes use of an
autoencoder structure, mixed with a regularizer implementing the false nearest neighbors statistic
(Kennel, Brown, and Abarbanel 1992), to reconstruct attractors from univariate observations of multivariate, nonlinear dynamical methods. If
you are feeling you fully perceive the sentence you simply learn, you might as nicely straight bounce to the paper – come again for the
code although. If, then again, you’re extra accustomed to the chaos in your desk (extrapolating … apologies) than
chaos concept chaos, learn on. Right here, we’ll first go into what it’s all about, after which, present an instance utility,
that includes Edward Lorenz’s well-known butterfly attractor. Whereas this preliminary put up is primarily alleged to be a enjoyable introduction
to an enchanting matter, we hope to comply with up with functions to real-world datasets sooner or later.

Rabbits, butterflies, and low-dimensional projections: Our drawback assertion in context

In curious misalignment with how we use “chaos” in day-to-day language, chaos, the technical idea, may be very completely different from
stochasticity, or randomness. Chaos might emerge from purely deterministic processes – very simplistic ones, even. Let’s see
how; with rabbits.

Rabbits, or: Delicate dependence on preliminary situations

It’s possible you’ll be accustomed to the logistic equation, used as a toy mannequin for inhabitants progress. Usually it’s written like this –
with (x) being the dimensions of the inhabitants, expressed as a fraction of the maximal measurement (a fraction of attainable rabbits, thus),
and (r) being the expansion charge (the speed at which rabbits reproduce):

x_{n + 1} = r x_n (1 – x_n)

This equation describes an iterated map over discrete timesteps (n). Its repeated utility ends in a trajectory
describing how the inhabitants of rabbits evolves. Maps can have mounted factors, states the place additional operate utility goes
on producing the identical outcome without end. Instance-wise, say the expansion charge quantities to (2.1), and we begin at two (fairly
completely different!) preliminary values, (0.3) and (0.8). Each trajectories arrive at a hard and fast level – the identical mounted level – in fewer
than 10 iterations. Had been we requested to foretell the inhabitants measurement after 100 iterations, we may make a really assured
guess, regardless of the of beginning worth. (If the preliminary worth is (0), we keep at (0), however we might be fairly sure of that as

Trajectory of the logistic map for r = 2.1 and two different initial values.

Determine 1: Trajectory of the logistic map for r = 2.1 and two completely different preliminary values.

What if the expansion charge had been considerably larger, at (3.3), say? Once more, we instantly examine trajectories ensuing from preliminary
values (0.3) and (0.9):

Trajectory of the logistic map for r = 3.3 and two different initial values.

Determine 2: Trajectory of the logistic map for r = 3.3 and two completely different preliminary values.

This time, don’t see a single mounted level, however a two-cycle: Because the trajectories stabilize, inhabitants measurement inevitably is at
one among two attainable values – both too many rabbits or too few, you may say. The 2 trajectories are phase-shifted, however
once more, the attracting values – the attractor – is shared by each preliminary situations. So nonetheless, predictability is fairly
excessive. However we haven’t seen every thing but.

Let’s once more improve the expansion charge some. Now this (actually) is chaos:

Trajectory of the logistic map for r = 3.6 and two different initial values, 0.3 and 0.9.

Determine 3: Trajectory of the logistic map for r = 3.6 and two completely different preliminary values, 0.3 and 0.9.

Even after 100 iterations, there is no such thing as a set of values the trajectories recur to. We will’t be assured about any
prediction we would make.

Or can we? In spite of everything, now we have the governing equation, which is deterministic. So we should always be capable of calculate the dimensions of
the inhabitants at, say, time (150)? In precept, sure; however this presupposes now we have an correct measurement for the beginning

How correct? Let’s examine trajectories for preliminary values (0.3) and (0.301):

Trajectory of the logistic map for r = 3.6 and two different initial values, 0.3 and 0.301.

Determine 4: Trajectory of the logistic map for r = 3.6 and two completely different preliminary values, 0.3 and 0.301.

At first, trajectories appear to leap round in unison; however in the course of the second dozen iterations already, they dissociate extra and
extra, and more and more, all bets are off. What if preliminary values are actually shut, as in, (0.3) vs. (0.30000001)?

It simply takes a bit longer for the disassociation to floor.

Trajectory of the logistic map for r = 3.6 and two different initial values, 0.3 and 0.30000001.

Determine 5: Trajectory of the logistic map for r = 3.6 and two completely different preliminary values, 0.3 and 0.30000001.

What we’re seeing right here is delicate dependence on preliminary situations, an important precondition for a system to be chaotic.
In an nutshell: Chaos arises when a deterministic system reveals delicate dependence on preliminary situations. Or as Edward
Lorenz is said to have put it,

When the current determines the longer term, however the approximate current doesn’t roughly decide the longer term.

Now if these unstructured, random-looking level clouds represent chaos, what with the all-but-amorphous butterfly (to be
displayed very quickly)?

Butterflies, or: Attractors and unusual attractors

Truly, within the context of chaos concept, the time period butterfly could also be encountered in numerous contexts.

Firstly, as so-called “butterfly impact,” it’s an instantiation of the templatic phrase “the flap of a butterfly’s wing in
_________ profoundly impacts the course of the climate in _________.” On this utilization, it’s principally a
metaphor for delicate dependence on preliminary situations.

Secondly, the existence of this metaphor led to a Rorschach-test-like identification with two-dimensional visualizations of
attractors of the Lorenz system. The Lorenz system is a set of three first-order differential equations designed to explain
atmospheric convection:

& frac{dx}{dt} = sigma (y – x)
& frac{dy}{dt} = rho x – x z – y
& frac{dz}{dt} = x y – beta z

This set of equations is nonlinear, as required for chaotic conduct to seem. It additionally has the required dimensionality, which
for easy, steady methods, is not less than 3. Whether or not we truly see chaotic attractors – amongst which, the butterfly –
is dependent upon the settings of the parameters (sigma), (rho) and (beta). For the values conventionally chosen, (sigma=10),
(rho=28), and (beta=8/3) , we see it when projecting the trajectory on the (x) and (z) axes:

Two-dimensional projections of the Lorenz attractor for sigma = 10, rho = 28, beta = 8 / 3. On the right: the butterfly.

Determine 6: Two-dimensional projections of the Lorenz attractor for sigma = 10, rho = 28, beta = 8 / 3. On the precise: the butterfly.

The butterfly is an attractor (as are the opposite two projections), however it’s neither some extent nor a cycle. It’s an attractor
within the sense that ranging from a wide range of completely different preliminary values, we find yourself in some sub-region of the state house, and we
don’t get to flee no extra. That is simpler to see when watching evolution over time, as on this animation:

How the Lorenz attractor traces out the famous "butterfly" shape.

Determine 7: How the Lorenz attractor traces out the well-known “butterfly” form.

Now, to plot the attractor in two dimensions, we threw away the third. However in “actual life,” we don’t normally have too a lot
data (though it might generally look like we had). We’d have loads of measurements, however these don’t normally replicate
the precise state variables we’re all in favour of. In these instances, we might need to truly add data.

Embeddings (as a non-DL time period), or: Undoing the projection

Assume that as an alternative of all three variables of the Lorenz system, we had measured only one: (x), the speed of convection. Usually
in nonlinear dynamics, the strategy of delay coordinate embedding (Sauer, Yorke, and Casdagli 1991) is used to boost a collection of univariate

On this technique – or household of strategies – the univariate collection is augmented by time-shifted copies of itself. There are two
choices to be made: What number of copies so as to add, and the way massive the delay ought to be. As an instance, if we had a scalar collection,

1 2 3 4 5 6 7 8 9 10 11 ...

a three-dimensional embedding with time delay 2 would appear to be this:

1 3 5
2 4 6
3 5 7
4 6 8
5 7 9
6 8 10
7 9 11

Of the 2 choices to be made – variety of shifted collection and time lag – the primary is a call on the dimensionality of
the reconstruction house. Numerous theorems, comparable to Taken’s theorem,
point out bounds on the variety of dimensions required, supplied the dimensionality of the true state house is thought – which,
in real-world functions, usually is just not the case.The second has been of little curiosity to mathematicians, however is essential
in apply. Actually, Kantz and Schreiber (Kantz and Schreiber 2004) argue that in apply, it’s the product of each parameters that issues,
because it signifies the time span represented by an embedding vector.

How are these parameters chosen? Concerning reconstruction dimensionality, the reasoning goes that even in chaotic methods,
factors which are shut in state house at time (t) ought to nonetheless be shut at time (t + Delta t), supplied (Delta t) may be very
small. So say now we have two factors which are shut, by some metric, when represented in two-dimensional house. However in three
dimensions, that’s, if we don’t “undertaking away” the third dimension, they’re much more distant. As illustrated in
(Gilpin 2020):

In the two-dimensional projection on axes x and y, the red points are close neighbors. In 3d, however, they are separate. Compare with the blue points, which stay close even in higher-dimensional space. Figure from Gilpin (2020).

Determine 8: Within the two-dimensional projection on axes x and y, the crimson factors are shut neighbors. In 3d, nonetheless, they’re separate. Evaluate with the blue factors, which keep shut even in higher-dimensional house. Determine from Gilpin (2020).

If this occurs, then projecting down has eradicated some important data. In second, the factors had been false neighbors. The
false nearest neighbors (FNN) statistic can be utilized to find out an satisfactory embedding measurement, like this:

For every level, take its closest neighbor in (m) dimensions, and compute the ratio of their distances in (m) and (m+1)
dimensions. If the ratio is bigger than some threshold (t), the neighbor was false. Sum the variety of false neighbors over all
factors. Do that for various (m) and (t), and examine the ensuing curves.

At this level, let’s look forward on the autoencoder method. The autoencoder will use that very same FNN statistic as a
regularizer, along with the standard autoencoder reconstruction loss. This can lead to a brand new heuristic relating to embedding
dimensionality that includes fewer choices.

Going again to the traditional technique for an prompt, the second parameter, the time lag, is much more troublesome to type out
(Kantz and Schreiber 2004). Often, mutual data is plotted for various delays after which, the primary delay the place it falls beneath some
threshold is chosen. We don’t additional elaborate on this query as it’s rendered out of date within the neural community method.
Which we’ll see now.

Studying the Lorenz attractor

Our code intently follows the structure, parameter settings, and information setup used within the reference
William supplied. The loss operate, particularly, has been ported

The overall thought is the next. An autoencoder – for instance, an LSTM autoencoder as introduced right here – is used to compress
the univariate time collection right into a latent illustration of some dimensionality, which can represent an higher certain on the
dimensionality of the realized attractor. Along with imply squared error between enter and reconstructions, there shall be a
second loss time period, making use of the FNN regularizer. This ends in the latent models being roughly ordered by significance, as
measured by their variance. It’s anticipated that someplace within the itemizing of variances, a pointy drop will seem. The models
earlier than the drop are then assumed to encode the attractor of the system in query.

On this setup, there’s nonetheless a option to be made: tips on how to weight the FNN loss. One would run coaching for various weights
(lambda) and search for the drop. Certainly, this might in precept be automated, however given the novelty of the strategy – the
paper was printed this 12 months – it is smart to deal with thorough evaluation first.

Information technology

We use the deSolve package deal to generate information from the Lorenz equations.


parameters <- c(sigma = 10,
                rho = 28,
                beta = 8/3)

initial_state <-
  c(x = -8.60632853,
    y = -14.85273055,
    z = 15.53352487)

lorenz <- operate(t, state, parameters) {
  with(as.list(c(state, parameters)), {
    dx <- sigma * (y - x)
    dy <- x * (rho - z) - y
    dz <- x * y - beta * z
    list(c(dx, dy, dz))

instances <- seq(0, 500, size.out = 125000)

lorenz_ts <-
    y = initial_state,
    instances = instances,
    func = lorenz,
    parms = parameters,
    technique = "lsoda"
  ) %>% as_tibble()

# A tibble: 10 x 4
      time      x     y     z
     <dbl>  <dbl> <dbl> <dbl>
 1 0        -8.61 -14.9  15.5
 2 0.00400  -8.86 -15.2  15.9
 3 0.00800  -9.12 -15.6  16.3
 4 0.0120   -9.38 -16.0  16.7
 5 0.0160   -9.64 -16.3  17.1
 6 0.0200   -9.91 -16.7  17.6
 7 0.0240  -10.2  -17.0  18.1
 8 0.0280  -10.5  -17.3  18.6
 9 0.0320  -10.7  -17.7  19.1
10 0.0360  -11.0  -18.0  19.7

We’ve already seen the attractor, or fairly, its three two-dimensional projections, in determine 6 above. However now our situation is
completely different. We solely have entry to (x), a univariate time collection. Because the time interval used to numerically combine the
differential equations was fairly tiny, we simply use each tenth commentary.

obs <- lorenz_ts %>%
  choose(time, x) %>%
  filter(row_number() %% 10 == 0)

ggplot(obs, aes(time, x)) +
  geom_line() +
  coord_cartesian(xlim = c(0, 100)) +

Convection rates as a univariate time series.

Determine 9: Convection charges as a univariate time collection.


The primary half of the collection is used for coaching. The information is scaled and remodeled into the three-dimensional kind anticipated
by recurrent layers.


# scale observations
obs <- obs %>% mutate(
  x = scale(x)

# generate timesteps
n <- nrow(obs)
n_timesteps <- 10

gen_timesteps <- operate(x, n_timesteps) {,
             operate(i) {
               begin <- i
               finish <- i + n_timesteps - 1
               out <- x[start:end]
  ) %>%

# practice with begin of time collection, check with finish of time collection 
x_train <- gen_timesteps(as.matrix(obs$x)[1:(n/2)], n_timesteps)
x_test <- gen_timesteps(as.matrix(obs$x)[(n/2):n], n_timesteps) 

# add required dimension for options (now we have one)
dim(x_train) <- c(dim(x_train), 1)
dim(x_test) <- c(dim(x_test), 1)

# some batch measurement (worth not essential)
batch_size <- 100

# rework to datasets so we will use customized coaching
ds_train <- tensor_slices_dataset(x_train) %>%

ds_test <- tensor_slices_dataset(x_test) %>%


With newer variations of TensorFlow (>= 2.0, definitely if >= 2.2), autoencoder-like fashions are greatest coded as customized fashions,
and educated in an “autographed” loop.

The encoder is centered round a single LSTM layer, whose measurement determines the utmost dimensionality of the attractor. The
decoder then undoes the compression – once more, primarily utilizing a single LSTM.

# measurement of the latent code
n_latent <- 10L
n_features <- 1

encoder_model <- operate(n_timesteps,
                          title = NULL) {
  keras_model_custom(title = title, operate(self) {
    self$noise <- layer_gaussian_noise(stddev = 0.5)
    self$lstm <-  layer_lstm(
      models = n_latent,
      input_shape = c(n_timesteps, n_features),
      return_sequences = FALSE
    self$batchnorm <- layer_batch_normalization()
    operate (x, masks = NULL) {
      x %>%
        self$noise() %>%
        self$lstm() %>%

decoder_model <- operate(n_timesteps,
                          title = NULL) {
  keras_model_custom(title = title, operate(self) {
    self$repeat_vector <- layer_repeat_vector(n = n_timesteps)
    self$noise <- layer_gaussian_noise(stddev = 0.5)
    self$lstm <- layer_lstm(
        models = n_latent,
        return_sequences = TRUE,
        go_backwards = TRUE
    self$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() %>%

encoder <- encoder_model(n_timesteps, n_features, n_latent)
decoder <- decoder_model(n_timesteps, n_features, n_latent)


As already defined above, the loss operate we practice with is twofold. On the one hand, we examine the unique inputs with
the decoder outputs (the reconstruction), utilizing imply squared error:

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

As well as, we attempt to hold the variety of false neighbors small, via the next regularizer.

loss_false_nn <- operate(x) {
  # unique values utilized in Kennel et al. (1992)
  rtol <- 10 
  atol <- 2
  k_frac <- 0.01
  okay <- max(1, floor(k_frac * batch_size))
  tri_mask <-
        form = c(n_latent, n_latent),
        dtype = tf$float32
      num_lower = -1L,
      num_upper = 0L
   batch_masked <- tf$multiply(
     tri_mask[, tf$newaxis,], x[tf$newaxis, reticulate::py_ellipsis()]
  x_squared <- tf$reduce_sum(
    batch_masked * batch_masked,
    axis = 2L,
    keepdims = TRUE

  pdist_vector <- x_squared +
    x_squared, perm = c(0L, 2L, 1L)
  ) -
  2 * tf$matmul(
    tf$transpose(batch_masked, perm = c(0L, 2L, 1L))

  all_dists <- pdist_vector
  all_ra <-
    tf$sqrt((1 / (
      batch_size * tf$vary(1, 1 + n_latent, dtype = tf$float32)
    )) *
        batch_masked - tf$reduce_mean(batch_masked, axis = 1L, keepdims = TRUE)
      ), axis = c(1L, 2L)))
  all_dists <- tf$clip_by_value(all_dists, 1e-14, tf$reduce_max(all_dists))

  top_k <- tf$math$top_k(-all_dists, tf$forged(okay + 1, tf$int32))
  top_indices <- top_k[[1]]

  neighbor_dists_d <- tf$collect(all_dists, top_indices, batch_dims = -1L)
  neighbor_new_dists <- tf$collect(
    all_dists[2:-1, , ],
    top_indices[1:-2, , ],
    batch_dims = -1L
  # Eq. 4 of Kennel et al. (1992)
  scaled_dist <- tf$sqrt((
    tf$sq.(neighbor_new_dists) -
      tf$sq.(neighbor_dists_d[1:-2, , ])) /
      tf$sq.(neighbor_dists_d[1:-2, , ])
  # Kennel situation #1
  is_false_change <- (scaled_dist > rtol)
  # Kennel situation #2
  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)
  total_false_neighbors <-
    tf$forged(is_false_neighbor, tf$int32)[reticulate::py_ellipsis(), 2:(k + 2)]
  reg_weights <- 1 -
    tf$reduce_mean(tf$forged(total_false_neighbors, tf$float32), axis = c(1L, 2L))
  reg_weights <- tf$pad(reg_weights, list(list(1L, 0L)))
  activations_batch_averaged <-
    tf$sqrt(tf$reduce_mean(tf$sq.(x), axis = 0L))
  loss <- tf$reduce_sum(tf$multiply(reg_weights, activations_batch_averaged))

MSE and FNN are added , with FNN loss weighted in response to the important hyperparameter of this mannequin:

This worth was experimentally chosen because the one greatest conforming to our look-for-the-highest-drop heuristic.

Mannequin coaching

The coaching loop intently follows the aforementioned recipe on tips on how to
practice with customized fashions and tfautograph.

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

train_step <- operate(batch) {
  with (tf$GradientTape(persistent = TRUE) %as% tape, {
    code <- encoder(batch)
    reconstructed <- decoder(code)
    l_mse <- mse_loss(batch, reconstructed)
    l_fnn <- loss_false_nn(code)
    loss <- l_mse + fnn_weight * l_fnn
  encoder_gradients <- tape$gradient(loss, encoder$trainable_variables)
  decoder_gradients <- tape$gradient(loss, decoder$trainable_variables)
    purrr::transpose(list(encoder_gradients, encoder$trainable_variables))
    purrr::transpose(list(decoder_gradients, decoder$trainable_variables))

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

optimizer <- optimizer_adam(lr = 1e-3)

for (epoch in 1:200) {
  cat("Epoch: ", epoch, " -----------n")

After 2 hundred epochs, general loss is at 2.67, with the MSE element at 1.8 and FNN at 0.09.

Acquiring the attractor from the check set

We use the check set to examine the latent code:

# A tibble: 6,242 x 10
      V1    V2         V3        V4        V5         V6        V7        V8       V9       V10
   <dbl> <dbl>      <dbl>     <dbl>     <dbl>      <dbl>     <dbl>     <dbl>    <dbl>     <dbl>
 1 0.439 0.401 -0.000614  -0.0258   -0.00176  -0.0000276  0.000276  0.00677  -0.0239   0.00906 
 2 0.415 0.504  0.0000481 -0.0279   -0.00435  -0.0000970  0.000921  0.00509  -0.0214   0.00921 
 3 0.389 0.619  0.000848  -0.0240   -0.00661  -0.000171   0.00106   0.00454  -0.0150   0.00794 
 4 0.363 0.729  0.00137   -0.0143   -0.00652  -0.000244   0.000523  0.00450  -0.00594  0.00476 
 5 0.335 0.809  0.00128   -0.000450 -0.00338  -0.000307  -0.000561  0.00407   0.00394 -0.000127
 6 0.304 0.828  0.000631   0.0126    0.000889 -0.000351  -0.00167   0.00250   0.0115  -0.00487 
 7 0.274 0.769 -0.000202   0.0195    0.00403  -0.000367  -0.00220  -0.000308  0.0145  -0.00726 
 8 0.246 0.657 -0.000865   0.0196    0.00558  -0.000359  -0.00208  -0.00376   0.0134  -0.00709 
 9 0.224 0.535 -0.00121    0.0162    0.00608  -0.000335  -0.00169  -0.00697   0.0106  -0.00576 
10 0.211 0.434 -0.00129    0.0129    0.00606  -0.000306  -0.00134  -0.00927   0.00820 -0.00447 
# … with 6,232 extra rows

Because of the FNN regularizer, the latent code models ought to be ordered roughly by lowering variance, with a pointy drop
showing some place (if the FNN weight has been chosen adequately).

For an fnn_weight of 10, we do see a drop after the primary two models:

predicted %>% summarise_all(var)
# A tibble: 1 x 10
      V1     V2      V3      V4      V5      V6      V7      V8      V9     V10
   <dbl>  <dbl>   <dbl>   <dbl>   <dbl>   <dbl>   <dbl>   <dbl>   <dbl>   <dbl>
1 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

So the mannequin signifies that the Lorenz attractor might be represented in two dimensions. If we nonetheless need to plot the
full (reconstructed) state house of three dimensions, we should always reorder the remaining variables by magnitude of
variance. Right here, this ends in three projections of the set V1, V2 and V4:

Attractors as predicted from the latent code (test set). The three highest-variance variables were chosen.

Determine 10: Attractors as predicted from the latent code (check set). The three highest-variance variables had been chosen.

Wrapping up (for this time)

At this level, we’ve seen tips on how to reconstruct the Lorenz attractor from information we didn’t practice on (the check set), utilizing an
autoencoder regularized by a customized false nearest neighbors loss. It is very important stress that at no level was the community
introduced with the anticipated resolution (attractor) – coaching was purely unsupervised.

It is a fascinating outcome. In fact, considering virtually, the following step is to acquire predictions on heldout information. Given
how lengthy this textual content has change into already, we reserve that for a follow-up put up. And once more in fact, we’re fascinated by different
datasets, particularly ones the place the true state house is just not recognized beforehand. What about measurement noise? What about
datasets that aren’t fully deterministic? There’s a lot to discover, keep tuned – and as all the time, thanks for

Gilpin, William. 2020. “Deep Reconstruction of Unusual Attractors from Time Sequence.”

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

Kennel, Matthew B., Reggie Brown, and Henry D. I. Abarbanel. 1992. “Figuring out Embedding Dimension for Part-House Reconstruction Utilizing a Geometrical Building.” Phys. Rev. A 45 (March): 3403–11.
Sauer, Tim, James A. Yorke, and Martin Casdagli. 1991. Embedology.” Journal of Statistical Physics 65 (3-4): 579–616.

Strang, Gilbert. 2019. Linear Algebra and Studying from Information. Wellesley Cambridge Press.

Strogatz, Steven. 2015. Nonlinear Dynamics and Chaos: With Functions to Physics, Biology, Chemistry, and Engineering. Westview Press.

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