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Review CSPs are a special kind of search problems. Here we don't treat the space as a black box but the state has a particular form and we use that to our advantage to tweak our algorithms to be more suited to the problems. A CSP State is defined by a set of variables which can take values from corresponding domains. T...
%psource CSP
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The _ init _ method parameters specify the CSP. Variable can be passed as a list of strings or integers. Domains are passed as dict where key specify the variables and value specify the domains. The variables are passed as an empty list. Variables are extracted from the keys of the domain dictionary. Neighbor is a di...
s = UniversalDict(['R','G','B']) s[5]
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
For our CSP we also need to define a constraint function f(A, a, B, b). In this what we need is that the neighbors must not have the same color. This is defined in the function different_values_constraint of the module.
%psource different_values_constraint
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The CSP class takes neighbors in the form of a Dict. The module specifies a simple helper function named parse_neighbors which allows to take input in the form of strings and return a Dict of the form compatible with the CSP Class.
%pdoc parse_neighbors
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The MapColoringCSP function creates and returns a CSP with the above constraint function and states. The variables our the keys of the neighbors dict and the constraint is the one specified by the different_values_constratint function. australia, usa and france are three CSPs that have been created using MapColoringCSP...
%psource MapColoringCSP australia, usa, france
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
NQueens The N-queens puzzle is the problem of placing N chess queens on a N×N chessboard so that no two queens threaten each other. Here N is a natural number. Like the graph coloring, problem NQueens is also implemented in the csp module. The NQueensCSP class inherits from the CSP class. It makes some modifications in...
%psource queen_constraint
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The NQueensCSP method implements methods that support solving the problem via min_conflicts which is one of the techniques for solving CSPs. Because min_conflicts hill climbs the number of conflicts to solve the CSP assign and unassign are modified to record conflicts. More details about the structures rows, downs, ups...
%psource NQueensCSP
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The _ init _ method takes only one parameter n the size of the problem. To create an instance we just pass the required n into the constructor.
eight_queens = NQueensCSP(8)
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Helper Functions We will now implement few helper functions that will help us visualize the Coloring Problem. We will make some modifications to the existing Classes and Functions for additional book keeping. To begin with we modify the assign and unassign methods in the CSP to add a copy of the assignment to the assin...
import copy class InstruCSP(CSP): def __init__(self, variables, domains, neighbors, constraints): super().__init__(variables, domains, neighbors, constraints) self.assingment_history = [] def assign(self, var, val, assignment): super().assign(var,val, assignment) se...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Next, we define make_instru which takes an instance of CSP and returns a InstruCSP instance.
def make_instru(csp): return InstruCSP(csp.variables, csp.domains, csp.neighbors, csp.constraints)
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
We will now use a graph defined as a dictonary for plotting purposes in our Graph Coloring Problem. The keys are the nodes and their corresponding values are the nodes are they are connected to.
neighbors = { 0: [6, 11, 15, 18, 4, 11, 6, 15, 18, 4], 1: [12, 12, 14, 14], 2: [17, 6, 11, 6, 11, 10, 17, 14, 10, 14], 3: [20, 8, 19, 12, 20, 19, 8, 12], 4: [11, 0, 18, 5, 18, 5, 11, 0], 5: [4, 4], 6: [8, 15, 0, 11, 2, 14, 8, 11, 15, 2, 0, 14], 7: [13, 16, 13, 16], 8: [19, 15...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Backtracking Search For solving a CSP the main issue with Naive search algorithms is that they can continue expanding obviously wrong paths. In backtracking search, we check constraints as we go. Backtracking is just the above idea combined with the fact that we are dealing with one variable at a time. Backtracking Sea...
result = backtracking_search(coloring_problem1) result # A dictonary of assingments.
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Let us also check the number of assingments made.
coloring_problem1.nassigns
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Now let us check the total number of assingments and unassingments which is the lentgh ofour assingment history.
len(coloring_problem1.assingment_history)
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Now let us explore the optional keyword arguments that the backtracking_search function takes. These optional arguments help speed up the assignment further. Along with these, we will also point out to methods in the CSP class that help make this work. The first of these is select_unassigned_variable. It takes in a fu...
%psource mrv %psource num_legal_values %psource CSP.nconflicts
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Another ordering related parameter order_domain_values governs the value ordering. Here we select the Least Constraining Value which is implemented by the function lcv. The idea is to select the value which rules out the fewest values in the remaining variables. The intuition behind selecting the lcv is that it leaves ...
%psource lcv
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Finally, the third parameter inference can make use of one of the two techniques called Arc Consistency or Forward Checking. The details of these methods can be found in the Section 6.3.2 of the book. In short the idea of inference is to detect the possible failure before it occurs and to look ahead to not make mistake...
solve_simple = copy.deepcopy(usa) solve_parameters = copy.deepcopy(usa) backtracking_search(solve_simple) backtracking_search(solve_parameters, order_domain_values=lcv, select_unassigned_variable=mrv, inference=mac ) solve_simple.nassigns solve_parameters.nassigns
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Graph Coloring Visualization Next, we define some functions to create the visualisation from the assingment_history of coloring_problem1. The reader need not concern himself with the code that immediately follows as it is the usage of Matplotib with IPython Widgets. If you are interested in reading more about these vis...
%matplotlib inline import networkx as nx import matplotlib.pyplot as plt import matplotlib import time
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The ipython widgets we will be using require the plots in the form of a step function such that there is a graph corresponding to each value. We define the make_update_step_function which return such a function. It takes in as inputs the neighbors/graph along with an instance of the InstruCSP. This will be more clear w...
def make_update_step_function(graph, instru_csp): def draw_graph(graph): # create networkx graph G=nx.Graph(graph) # draw graph pos = nx.spring_layout(G,k=0.15) return (G, pos) G, pos = draw_graph(graph) def update_step(iteration): # here iterat...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Finally let us plot our problem. We first use the function above to obtain a step function.
step_func = make_update_step_function(neighbors, coloring_problem1)
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Next we set the canvas size.
matplotlib.rcParams['figure.figsize'] = (18.0, 18.0)
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Finally our plot using ipywidget slider and matplotib. You can move the slider to experiment and see the coloring change. It is also possible to move the slider using arrow keys or to jump to the value by directly editing the number with a double click. The Visualize Button will automatically animate the slider for you...
import ipywidgets as widgets from IPython.display import display iteration_slider = widgets.IntSlider(min=0, max=len(coloring_problem1.assingment_history)-1, step=1, value=0) w=widgets.interactive(step_func,iteration=iteration_slider) display(w) visualize_callback = make_visualize(iteration_slider) visualize_button ...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
NQueens Visualization Just like the Graph Coloring Problem we will start with defining a few helper functions to help us visualize the assignments as they evolve over time. The make_plot_board_step_function behaves similar to the make_update_step_function introduced earlier. It initializes a chess board in the form of ...
def label_queen_conflicts(assingment,grid): ''' Mark grid with queens that are under conflict. ''' for col, row in assingment.items(): # check each queen for conflict row_conflicts = {temp_col:temp_row for temp_col,temp_row in assingment.items() if temp_row == row and temp_col ...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Now let us visualize a solution obtained via backtracking. We use of the previosuly defined make_instru function for keeping a history of steps.
twelve_queens_csp = NQueensCSP(12) backtracking_instru_queen = make_instru(twelve_queens_csp) result = backtracking_search(backtracking_instru_queen) backtrack_queen_step = make_plot_board_step_function(backtracking_instru_queen) # Step Function for Widgets
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Now finally we set some matplotlib parameters to adjust how our plot will look. The font is necessary because the Black Queen Unicode character is not a part of all fonts. You can move the slider to experiment and observe the how queens are assigned. It is also possible to move the slider using arrow keys or to jump to...
matplotlib.rcParams['figure.figsize'] = (8.0, 8.0) matplotlib.rcParams['font.family'].append(u'Dejavu Sans') iteration_slider = widgets.IntSlider(min=0, max=len(backtracking_instru_queen.assingment_history)-1, step=0, value=0) w=widgets.interactive(backtrack_queen_step,iteration=iteration_slider) display(w) visualize...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
The visualization has same features as the above. But here it also highlights the conflicts by labeling the conflicted queens with a red background.
iteration_slider = widgets.IntSlider(min=0, max=len(conflicts_instru_queen.assingment_history)-1, step=0, value=0) w=widgets.interactive(conflicts_step,iteration=iteration_slider) display(w) visualize_callback = make_visualize(iteration_slider) visualize_button = widgets.ToggleButton(desctiption = "Visualize", value ...
.ipynb_checkpoints/csp-checkpoint.ipynb
nikodtbVf/aima-si
mit
Configuring MNE python This tutorial gives a short introduction to MNE configurations.
import os.path as op import mne from mne.datasets.sample import data_path fname = op.join(data_path(), 'MEG', 'sample', 'sample_audvis_raw.fif') raw = mne.io.read_raw_fif(fname).crop(0, 10) original_level = mne.get_config('MNE_LOGGING_LEVEL', 'INFO')
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
MNE-python stores configurations to a folder called .mne in the user's home directory, or to AppData directory on Windows. The path to the config file can be found out by calling :func:mne.get_config_path.
print(mne.get_config_path())
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
These configurations include information like sample data paths and plotter window sizes. Files inside this folder should never be modified manually. Let's see what the configurations contain.
print(mne.get_config())
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
We see fields like "MNE_DATASETS_SAMPLE_PATH". As the name suggests, this is the path the sample data is downloaded to. All the fields in the configuration file can be modified by calling :func:mne.set_config. Logging Configurations also include the default logging level for the functions. This field is called "MNE_LOG...
mne.set_config('MNE_LOGGING_LEVEL', 'INFO') print(mne.get_config(key='MNE_LOGGING_LEVEL'))
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
The default value is now set to INFO. This level will now be used by default every time we call a function in MNE. We can set the global logging level for only this session by calling :func:mne.set_log_level function.
mne.set_log_level('WARNING') print(mne.get_config(key='MNE_LOGGING_LEVEL'))
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
Notice how the value in the config file was not changed. Logging level of WARNING only applies for this session. Let's see what logging level of WARNING prints for :func:mne.compute_raw_covariance.
cov_raw = mne.compute_raw_covariance(raw)
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
Nothing. This means that no warnings were emitted during the computation. If you look at the documentation of :func:mne.compute_raw_covariance, you notice the verbose keyword. Setting this parameter does not touch the configurations, but sets the logging level for just this one function call. Let's see what happens wit...
cov = mne.compute_raw_covariance(raw, verbose=True)
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
As you see there is some info about what the function is doing. The logging level can be set to 'DEBUG', 'INFO', 'WARNING', 'ERROR' or 'CRITICAL'. It can also be set to an integer or a boolean value. The correspondence to string values can be seen in the table below. verbose=None uses the default value from the configu...
mne.set_config('MNE_LOGGING_LEVEL', original_level) print('Config value restored to: %s' % mne.get_config(key='MNE_LOGGING_LEVEL'))
0.18/_downloads/8a8a7b741ef485e4d3d3772b252fcb81/plot_configuration.ipynb
mne-tools/mne-tools.github.io
bsd-3-clause
Running TFLite models <table class="tfo-notebook-buttons" align="left"> <td> <a target="_blank" href="https://colab.research.google.com/github/tensorflow/examples/blob/master/courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb"> <img src="https://www.tensorflow.org/images/colab_logo_32...
import tensorflow as tf import pathlib import numpy as np import matplotlib.pyplot as plt from tensorflow.keras.models import Model from tensorflow.keras.layers import Input
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Create a basic model of the form y = mx + c
# Create a simple Keras model. x = [-1, 0, 1, 2, 3, 4] y = [-3, -1, 1, 3, 5, 7] model = tf.keras.models.Sequential([ tf.keras.layers.Dense(units=1, input_shape=[1]) ]) model.compile(optimizer='sgd', loss='mean_squared_error') model.fit(x, y, epochs=200, verbose=1)
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Generate a SavedModel
export_dir = 'saved_model/1' tf.saved_model.save(model, export_dir)
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Convert the SavedModel to TFLite
# Convert the model. converter = tf.lite.TFLiteConverter.from_saved_model(export_dir) tflite_model = converter.convert() tflite_model_file = pathlib.Path('model.tflite') tflite_model_file.write_bytes(tflite_model)
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Initialize the TFLite interpreter to try it out
# Load TFLite model and allocate tensors. interpreter = tf.lite.Interpreter(model_content=tflite_model) interpreter.allocate_tensors() # Get input and output tensors. input_details = interpreter.get_input_details() output_details = interpreter.get_output_details() # Test the TensorFlow Lite model on random input data...
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Visualize the model
plt.plot(inputs, outputs, 'r') plt.show()
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Download the TFLite model file
try: from google.colab import files files.download(tflite_model_file) except: pass
courses/udacity_intro_to_tensorflow_lite/tflite_c01_linear_regression.ipynb
tensorflow/examples
apache-2.0
Part 3.a The first machine learning algorithm for classifying spam emails is the Naive Bayes model. First we trained the model using the MATRIX.TRAIN data file.
df_train = rm.read_data('spam_data/MATRIX.TRAIN') nb_model = nb_train.train(df_train)
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Next we ran the model against the testing data.
df_test = rm.read_data('spam_data/MATRIX.TEST') nb_predictions = nb_test.test(nb_model, df_test)
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
The following is the testing error.
y = df_test.iloc[:,0] nb_error = nb_test.compute_error(y, nb_predictions) print('NB Test error: {}'.format(nb_error))
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Part 3.b. The five most indicative words of a spam message are the following.
words = nb_test.k_most_indicative_words(5, nb_model.to_dataframe().iloc[:,1:]) print('The {} most spam-worthy words are: {}'.format(len(words), words))
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Part 3.c. To test the convergence properties of the Naive Bayes classifier on the email data set, it needs to be run on different training set sizes. Here we use six different sized training sets to see how the error rate progresses.
training_set_files = { 50 : 'spam_data/MATRIX.TRAIN.50', 100 : 'spam_data/MATRIX.TRAIN.100', 200 : 'spam_data/MATRIX.TRAIN.200', 400 : 'spam_data/MATRIX.TRAIN.400', 800 : 'spam_data/MATRIX.TRAIN.800', 1400 : 'spam_data/MATRIX.TRAIN.1400' }
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Estimate the models and compute the errors.
nb_models = {} for size, filename in training_set_files.items(): df_next = rm.read_data(filename) m = nb_train.train(df_next) nb_models[size] = m nb_errors = {} for size, model in nb_models.items(): guessed_y = nb_test.test(model, df_test) err = nb_test.compute_error(y, guessed_y) nb_errors[siz...
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
The resulting errors are
print('Naive Bayes') for size, error in nb_errors.items(): print('size: {}; error: {}'.format(size, error))
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
As the training set size increases, the error rate for the Naive Bayes classifier decreases. It converges above a training set size of about 1000 emails. Part 3.d. The second model used to classify the emails is a support vector machine. As in part (a), we train the SVM model using the MATRIX.TRAIN data.
tau = 8 max_iters = 40 svm_model = svm_train.train(df_train, tau, max_iters)
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Next, we run the trained SVM model against the testing data.
svm_predictions = svm_test.test(svm_model, df_test) print(svm_predictions.shape)
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
The testing error is:
ytest = 2 * df_test.iloc[:,0].as_matrix() - 1 svm_error = svm_test.compute_error(ytest, svm_predictions) print('SVM Test Error: {}'.format(svm_error))
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
For the varying sized training sets, we estimate an SVM model.
svm_models = {} for size, filename in training_set_files.items(): df_next = rm.read_data(filename) m = svm_train.train(df_next, tau, max_iters) svm_models[size] = m
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
And we compute the errors for each model.
svm_errors = {} for size, model in svm_models.items(): guessed_y = svm_test.test(model, df_test) err = svm_test.compute_error(ytest, guessed_y) svm_errors[size] = err
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
The resulting errors are
print('Support Vector Machine') for size, error in svm_errors.items(): print('size: {}; error: {}'.format(size, error))
src/homework2/q3/homework2_3.ipynb
stallmanifold/cs229-machine-learning-stanford-fall-2016
apache-2.0
Modifying the isotopic yields of a specific stellar model
# Select an isotope and a stellar model (the model needs to be in the yields table). iso = "Si-28" M = 15.0 Z = 0.02 # Run SYGMA with no yields modification. s1 = sygma.sygma(iniZ=Z) # Run SYGMA where the yield is multiplied by 2. factor = 2.0 yield_modifier = [ [iso, M, Z, "multiply", factor] ] s2 = sygma.sygma(iniZ...
DOC/Capabilities/Modifying_yields.ipynb
NuGrid/NuPyCEE
bsd-3-clause
Modifying the isotopic yields of several stellar models
# Select an isotope iso = "Si-28" # Define the list of multiplication factor for each stellar model factor_list = [2, 4, 8, 16] M_list = [12.0, 15.0, 20.0, 25.0] Z = 0.02 # Fill the yield_modifier array yield_modifier = [] for M, factor in zip(M_list, factor_list): yield_modifier.append([iso, M, Z, "multiply", fa...
DOC/Capabilities/Modifying_yields.ipynb
NuGrid/NuPyCEE
bsd-3-clause
Example with OMEGA
# Import the NuPyCEE galactic chemical evolution code from NuPyCEE import omega # Print the list of available M and Z in the yields table print("M:",s1.M_table) print("Z:",s1.Z_table) # Boost the Mg-24 yields of all massive stars by a factor of 2 iso = "Mg-24" yield_modifier = [] for M in [12.0, 15.0, 20.0, 25.0]: ...
DOC/Capabilities/Modifying_yields.ipynb
NuGrid/NuPyCEE
bsd-3-clause
Unobserved Components The unobserved components model available in Statsmodels can be written as: $$ y_t = \underbrace{\mu_{t}}{\text{trend}} + \underbrace{\gamma{t}}{\text{seasonal}} + \underbrace{c{t}}{\text{cycle}} + \sum{j=1}^k \underbrace{\beta_j x_{jt}}{\text{explanatory}} + \underbrace{\varepsilon_t}{\text{irreg...
# Datasets from pandas.io.data import DataReader # Get the raw data start = '1948-01' end = '2008-01' us_gnp = DataReader('GNPC96', 'fred', start=start, end=end) us_gnp_deflator = DataReader('GNPDEF', 'fred', start=start, end=end) us_monetary_base = DataReader('AMBSL', 'fred', start=start, end=end).resample('QS') rece...
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
To get a sense of these three variables over the timeframe, we can plot them:
# Plot the data ax = dta.plot(figsize=(13,3)) ylim = ax.get_ylim() ax.xaxis.grid() ax.fill_between(dates, ylim[0]+1e-5, ylim[1]-1e-5, recessions, facecolor='k', alpha=0.1);
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
Model Since the data is already seasonally adjusted and there are no obvious explanatory variables, the generic model considered is: $$ y_t = \underbrace{\mu_{t}}{\text{trend}} + \underbrace{c{t}}{\text{cycle}} + \underbrace{\varepsilon_t}{\text{irregular}} $$ The irregular will be assumed to be white noise, and the cy...
# Model specifications # Unrestricted model, using string specification unrestricted_model = { 'level': 'local linear trend', 'cycle': True, 'damped_cycle': True, 'stochastic_cycle': True } # Unrestricted model, setting components directly # This is an equivalent, but less convenient, way to specify a # local lin...
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
We now fit the following models: Output, unrestricted model Prices, unrestricted model Prices, restricted model Money, unrestricted model Money, restricted model
# Output output_mod = sm.tsa.UnobservedComponents(dta['US GNP'], **unrestricted_model) output_res = output_mod.fit(method='powell', disp=False) # Prices prices_mod = sm.tsa.UnobservedComponents(dta['US Prices'], **unrestricted_model) prices_res = prices_mod.fit(method='powell', disp=False) prices_restricted_mod = sm....
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
Once we have fit these models, there are a variety of ways to display the information. Looking at the model of US GNP, we can summarize the fit of the model using the summary method on the fit object.
print(output_res.summary())
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
For unobserved components models, and in particular when exploring stylized facts in line with point (2) from the introduction, it is often more instructive to plot the estimated unobserved components (e.g. the level, trend, and cycle) themselves to see if they provide a meaningful description of the data. The plot_com...
fig = output_res.plot_components(legend_loc='lower right', figsize=(15, 9));
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
Finally, Harvey and Jaeger summarize the models in another way to highlight the relative importances of the trend and cyclical components; below we replicate their Table I. The values we find are broadly consistent with, but different in the particulars from, the values from their table.
# Create Table I table_i = np.zeros((5,6)) start = dta.index[0] end = dta.index[-1] time_range = '%d:%d-%d:%d' % (start.year, start.quarter, end.year, end.quarter) models = [ ('US GNP', time_range, 'None'), ('US Prices', time_range, 'None'), ('US Prices', time_range, r'$\sigma_\eta^2 = 0$'), ('US monet...
examples/notebooks/statespace_structural_harvey_jaeger.ipynb
YihaoLu/statsmodels
bsd-3-clause
Load Iris Dataset
# Load data iris = datasets.load_iris() X = iris.data y = iris.target
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Create Logistic Regression
# Create logistic regression logistic = linear_model.LogisticRegression()
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Create Hyperparameter Search Space
# Create regularization penalty space penalty = ['l1', 'l2'] # Create regularization hyperparameter space C = np.logspace(0, 4, 10) # Create hyperparameter options hyperparameters = dict(C=C, penalty=penalty)
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Create Grid Search
# Create grid search using 5-fold cross validation clf = GridSearchCV(logistic, hyperparameters, cv=5, verbose=0)
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Conduct Grid Search
# Fit grid search best_model = clf.fit(X, y)
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
View Hyperparameter Values Of Best Model
# View best hyperparameters print('Best Penalty:', best_model.best_estimator_.get_params()['penalty']) print('Best C:', best_model.best_estimator_.get_params()['C'])
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Predict Using Best Model
# Predict target vector best_model.predict(X)
machine-learning/hyperparameter_tuning_using_grid_search.ipynb
tpin3694/tpin3694.github.io
mit
Python for Probability, Statistics, and Machine Learning
from __future__ import division %pylab inline
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
As we have seen, outside of some toy problems, it can be very difficult or impossible to determine the probability density distribution of the estimator of some quantity. The idea behind the bootstrap is that we can use computation to approximate these functions which would otherwise be impossible to solve for anal...
import numpy as np _=np.random.seed(123456) import numpy as np from scipy import stats rv = stats.beta(3,2) xsamples = rv.rvs(50)
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Because this is simulation data, we already know that the mean is $\mu_1 = 3/5$ and the standard deviation of the sample mean for $n=50$ is $\bar{\sigma} =1/\sqrt {1250}$, which we will verify this later.
%matplotlib inline from matplotlib.pylab import subplots fig,ax = subplots() fig.set_size_inches(8,4) _=ax.hist(xsamples,normed=True,color='gray') ax2 = ax.twinx() _=ax2.plot(np.linspace(0,1,100),rv.pdf(np.linspace(0,1,100)),lw=3,color='k') _=ax.set_xlabel('$x$',fontsize=28) _=ax2.set_ylabel(' $y$',fontsize=28,rotati...
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
<!-- dom:FIGURE: [fig-statistics/Bootstrap_001.png, width=500 frac=0.85] The $\beta(3,2)$ distribution and the histogram that approximates it. <div id="fig:Bootstrap_001"></div> --> <!-- begin figure --> <div id="fig:Bootstrap_001"></div> <p>The $\beta(3,2)$ distribution and the histogram that approximates it.</p> <im...
yboot = np.random.choice(xsamples,(100,50)) yboot_mn = yboot.mean()
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
and the bootstrap estimate is therefore,
np.std(yboot.mean(axis=1)) # approx sqrt(1/1250)
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Figure shows the distribution of computed sample means from the bootstrap samples. As promised, the next block shows how to use sympy.stats to compute the $\beta(3,2)$ parameters we quoted earlier.
fig,ax = subplots() fig.set_size_inches(8,4) _=ax.hist(yboot.mean(axis=1),normed=True,color='gray') _=ax.set_title('Bootstrap std of sample mean %3.3f vs actual %3.3f'% (np.std(yboot.mean(axis=1)),np.sqrt(1/1250.))) fig.tight_layout() #fig.savefig('fig-statistics/Bootstrap_002.png')
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
<!-- dom:FIGURE: [fig-statistics/Bootstrap_002.png, width=500 frac=0.85] For each bootstrap draw, we compute the sample mean. This is the histogram of those sample means that will be used to compute the bootstrap estimate of the standard deviation. <div id="fig:Bootstrap_002"></div> --> <!-- begin figure --> <div id="f...
import sympy as S import sympy.stats for i in range(50): # 50 samples # load sympy.stats Beta random variables # into global namespace using exec execstring = "x%d = S.stats.Beta('x'+str(%d),3,2)"%(i,i) exec(execstring) # populate xlist with the sympy.stats random variables # from above xlist = [eval(...
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Programming Tip. Using the exec function enables the creation of a sequence of Sympy random variables. Sympy has the var function which can automatically create a sequence of Sympy symbols, but there is no corresponding function in the statistics module to do this for random variables. <!-- @@@CODE src-statistics/Boots...
import numpy as np np.random.seed(123) from scipy import stats import numpy as np p= 0.25 # true head-up probability x = stats.bernoulli(p).rvs(10) print x
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
The maximum likelihood estimator of $p$ is $\hat{p}=\sum X_i/n$,
phat = x.mean() print phat
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Then, plugging this into the delta method approximant above,
print (1-2*phat)**2*(phat)**2/10.
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Now, let's try this using the bootstrap estimate of the variance
phat_b=np.random.choice(x,(50,10)).mean(1) print np.var(phat_b*(1-phat_b))
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
This shows that the delta method's estimated variance is different from the bootstrap method, but which one is better? For this situation we can solve for this directly using Sympy
import sympy as S from sympy.stats import E, Bernoulli xdata =[Bernoulli(i,p) for i in S.symbols('x:10')] ph = sum(xdata)/float(len(xdata)) g = ph*(1-ph)
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Programming Tip. The argument in the S.symbols('x:10') function returns a sequence of Sympy symbols named x1,x2 and so on. This is shorthand for creating and naming each symbol sequentially. Note that g is the $g(\hat{p})=\hat{p}(1- \hat{p})$ whose variance we are trying to estimate. Then, we can plug in for the estim...
print E(g**2) - E(g)**2
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
This case is generally representative --- the delta method tends to underestimate the variance and the bootstrap estimate is better here. Parametric Bootstrap In the previous example, we used the $\lbrace x_1, x_2, \ldots, x_n \rbrace $ samples themselves as the basis for $\hat{F}$ by weighting each with $1/n$. An alte...
rv = stats.norm(0,2) xsamples = rv.rvs(45) # estimate mean and var from xsamples mn_ = np.mean(xsamples) std_ = np.std(xsamples) # bootstrap from assumed normal distribution with # mn_,std_ as parameters rvb = stats.norm(mn_,std_) #plug-in distribution yboot = rvb.rvs(1000)
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
<!-- @@@CODE src-statistics/Bootstrap.py from-to:^# In\[7\]:@^yboot --> Recall the sample variance estimator is the following: $$ S^2 = \frac{1}{n-1} \sum (X_i-\bar{X})^2 $$ Assuming that the samples are normally distributed, this means that $(n-1)S^2/\sigma^2$ has a chi-squared distribution with $n-1$ degrees of free...
# MLE-Plugin Variance of the sample mean print 2*(std_**2)**2/9. # MLE plugin # Bootstrap variance of the sample mean print yboot.var() # True variance of sample mean print 2*(2**2)**2/9.
chapters/statistics/notebooks/Bootstrap.ipynb
unpingco/Python-for-Probability-Statistics-and-Machine-Learning
mit
Para exemplificar o caso unidimensional, vamos pegar uma imagem bidimensional (cameraman) e escolher apenas uma linha da imagem para ser nossa função unidimensional.
f1 = mpimg.imread('../data/cameraman.tif')[10,:] plt.plot(f1) F1 = fft(f1) g1 = ifft(F1) print ('comparando g1 e f1:', abs(g1-f1).max())
2S2018/10 A transformada discreta de Fourier - DFT.ipynb
robertoalotufo/ia898
mit
2. Exemplo bidimensional
f2 = mpimg.imread('../data/cameraman.tif') F2 = fft2(f2) g2 = ifft2(F2) print ('comparando g2 e f2:', abs(g2-f2).max()) plt.figure(1, figsize=(8,8)) plt.subplot(1,2,1) plt.imshow(f2, cmap='gray') plt.subplot(1,2,2) plt.imshow(ia.dftview(F2), cmap='gray')
2S2018/10 A transformada discreta de Fourier - DFT.ipynb
robertoalotufo/ia898
mit
In this notebook we will use the Monte Carlo method to find the area under a curve, so first let's define a function $$f(x) = x^2-4x+5$$
f = lambda x:x**2-4*x+5 x = range(0, 11, 1) y = [f(v) for v in x] plt.plot(y)
Monte Carlos Experiments/Monte Carlo Integration.ipynb
victorgcapone/data-science-portifolio
gpl-3.0
Now, we know the probability of a random point being below the curve is equal to $$P_{curve}=\dfrac{A_{curve}}{A_{rectanle}}$$ Where $A_{rectangle}$ is the area of the plot in the given interval, so let's try to integrate it from 0 to 10
#Will use 3000 points number_points=3000 #We want to see the points points=[] below=0 for p in range(0, number_points): x,y=(random.uniform(0,10), random.uniform(0, 70)) # If the function for x is greater then the random y, then the point is under the curve if f(x) >= y: below +=1 points.append(...
Monte Carlos Experiments/Monte Carlo Integration.ipynb
victorgcapone/data-science-portifolio
gpl-3.0
Knowing the ratio of points under the curve, we can now calculate the integral as $$P_{curve}A_{rectangle} = A_{cruve}$$ If we take the integral $$\int_0^{10}x^2-4x+5$$ We have $$\dfrac{x^3}{3}-2x^2+5x\big\lvert_0^{10} = \dfrac{10^3}{3}-200+50 = 333.33 - 200 + 50 = 183.33$$ Which is close to the real area, now, let's ...
def monte_carlo_integration(f, number_points, xlims, ylims): below=0 for p in range(0, number_points): x,y=(random.uniform(*xlims), random.uniform(*ylims)) # If the function for x is greater then the random y, then the point is under the curve if y <= f(x): below +=1 rati...
Monte Carlos Experiments/Monte Carlo Integration.ipynb
victorgcapone/data-science-portifolio
gpl-3.0
As we can see the more points we sample, the more accurate our approximation is to the real values, now what about if we have segments of our curve under the $x$ axis? Let's look at this example $$g(x) = x^2-4x-8$$
g = lambda x:x**2-4*x-8 x = range(0, 11, 1) y = [g(v) for v in x] plt.plot(y) #Will use 3000 points number_points=3000 #We want to see the points points=[] below=0 for p in range(0, number_points): x,y=(random.uniform(0,10), random.uniform(-20, 60)) # If the function for x is greater then the random y, then th...
Monte Carlos Experiments/Monte Carlo Integration.ipynb
victorgcapone/data-science-portifolio
gpl-3.0
We can see the area is around 184.0, so let's take the true integral to see if we are close to the real value We have $$\int_0^{10}x^2-4x+5 = \dfrac{x^3}{3}-2x^2-8x\big\lvert_0^{10} = \dfrac{10^3}{3}-200-80 = 333.33 - 200 - 80 = 53.33$$ So, we are off by a lot, that's because we are adding the area under the $x$ axis i...
#Let's adjust our function to deal with points under the x axis def monte_carlo_integration(f, number_points, xlims, ylims): below=0 for p in range(0, number_points): x,y=(random.uniform(*xlims), random.uniform(*ylims)) # If the function for x is greater then the random y, then the point is unde...
Monte Carlos Experiments/Monte Carlo Integration.ipynb
victorgcapone/data-science-portifolio
gpl-3.0
We need to import here the data, modify them if needed and proceed
umat_name = 'MIMTN' #This is the 5 character code for the Mori-Tanaka homogenization for composites with a matrix and ellipsoidal reinforcments nstatev = 0 nphases = 2 #The number of phases num_file = 0 #The num of the file that contains the subphases int1 = 50 int2 = 50 n_matrix = 0 props = np.array([nphases, num_fi...
Examples/MMSP/parametric_analysis/fibre_angle.ipynb
chemiskyy/simmit
gpl-3.0
Now let's study the evolution of the concentration
param_list[0].value = 0.0 param_list[1].value = 100 c = np.arange(0.,1.01,0.01) E_L = np.zeros(len(c)) E_T = np.zeros(len(c)) umat_name = 'MIMTN' #This is the 5 character code for the Mori-Tanaka homogenization for composites with a matrix and ellipsoidal reinforcments for i, x in enumerate (c): param_list[3].v...
Examples/MMSP/parametric_analysis/fibre_angle.ipynb
chemiskyy/simmit
gpl-3.0
量子畳み込みニューラルネットワーク <table class="tfo-notebook-buttons" align="left"> <td><a target="_blank" href="https://www.tensorflow.org/quantum/tutorials/qcnn"><img src="https://www.tensorflow.org/images/tf_logo_32px.png"> TensorFlow.orgで表示</a></td> <td><a target="_blank" href="https://colab.research.google.com/github/tensorfl...
!pip install tensorflow==2.7.0
site/ja/quantum/tutorials/qcnn.ipynb
tensorflow/docs-l10n
apache-2.0
TensorFlow Quantum をインストールします。
!pip install tensorflow-quantum # Update package resources to account for version changes. import importlib, pkg_resources importlib.reload(pkg_resources)
site/ja/quantum/tutorials/qcnn.ipynb
tensorflow/docs-l10n
apache-2.0
次に、TensorFlow とモジュールの依存関係をインポートします。
import tensorflow as tf import tensorflow_quantum as tfq import cirq import sympy import numpy as np # visualization tools %matplotlib inline import matplotlib.pyplot as plt from cirq.contrib.svg import SVGCircuit
site/ja/quantum/tutorials/qcnn.ipynb
tensorflow/docs-l10n
apache-2.0
1. QCNN を構築する 1.1 TensorFlow グラフで回路を組み立てる TensorFlow Quantum(TFQ)には、グラフ内で回路を構築するために設計されたレイヤークラスがあります。たとえば tfq.layers.AddCircuit レイヤーがあり、tf.keras.Layer を継承しています。このレイヤーは、次の図で示すように、回路の入力バッチの前後いずれかに追加できます。 <img src="./images/qcnn_1.png" width="700"> 次のスニペットには、このレイヤーが使用されています。
qubit = cirq.GridQubit(0, 0) # Define some circuits. circuit1 = cirq.Circuit(cirq.X(qubit)) circuit2 = cirq.Circuit(cirq.H(qubit)) # Convert to a tensor. input_circuit_tensor = tfq.convert_to_tensor([circuit1, circuit2]) # Define a circuit that we want to append y_circuit = cirq.Circuit(cirq.Y(qubit)) # Instantiate...
site/ja/quantum/tutorials/qcnn.ipynb
tensorflow/docs-l10n
apache-2.0
入力テンソルを調べます。
print(tfq.from_tensor(input_circuit_tensor))
site/ja/quantum/tutorials/qcnn.ipynb
tensorflow/docs-l10n
apache-2.0