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annealing_hand_written_digits.ipynb
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annealing_hand_written_digits.ipynb
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{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Problem setting: Recognizing hand-written digits.\n",
"\n",
"Recognizing hand-written digits is a classification problem, in which the aim is to assign each input vector to one of a finite number of discrete categories, to learn observed data points from already labeled data how to predict the class of unlabeled data. In the usecase of hand-written digits dataset, the task is to predict, given an image, which digit it represents.\n",
"\n",
"Training model learn features of each number between 0 and 9. The model will be given samples of each of the 10 possible classes on which we fit an estimator to be able to predict the classes to which unseen samples belong.\n",
"\n",
"## Problem solution: Supervised learning and predicting\n",
"\n",
"In this simple problem, there can be no need to use *state-of-the-art* Machine Learning library and to implement deep neural network. We use a simple algorithm as the estimator for the purpose of convenience. An example of the estimator is the class [sklearn.neural_network.MLPClassifier](http://scikit-learn.org/stable/modules/generated/sklearn.neural_network.MLPClassifier.html#sklearn-neural-network-mlpclassifier) that implements Multi-layer Perceptron classifier. The constructor of an estimator takes as arguments the parameters of the model, but for the time being, we will consider the estimator as a black box."
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import matplotlib.pyplot as plt\n",
"from sklearn import datasets, metrics\n",
"from sklearn.neural_network import MLPClassifier"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {},
"outputs": [
{
"name": "stderr",
"output_type": "stream",
"text": [
"/usr/local/bin/.pyenv/versions/anaconda3-5.1.0/lib/python3.6/site-packages/sklearn/neural_network/multilayer_perceptron.py:564: ConvergenceWarning: Stochastic Optimizer: Maximum iterations (100) reached and the optimization hasn't converged yet.\n",
" % self.max_iter, ConvergenceWarning)\n"
]
},
{
"name": "stdout",
"output_type": "stream",
"text": [
"Classification report for classifier MLPClassifier(activation='relu', alpha=1e-05, batch_size=100, beta_1=0.9,\n",
" beta_2=0.999, early_stopping=False, epsilon=1e-08,\n",
" hidden_layer_sizes=(1000,), learning_rate='constant',\n",
" learning_rate_init=1e-05, max_iter=100, momentum=0.9,\n",
" nesterovs_momentum=True, power_t=0.5, random_state=None,\n",
" shuffle=True, solver='adam', tol=0.0001, validation_fraction=0.1,\n",
" verbose=False, warm_start=False):\n",
" precision recall f1-score support\n",
"\n",
" 0 0.89 0.94 0.92 88\n",
" 1 0.88 0.81 0.85 91\n",
" 2 0.96 0.95 0.96 86\n",
" 3 0.83 0.87 0.85 91\n",
" 4 0.98 0.91 0.94 92\n",
" 5 0.80 0.95 0.87 91\n",
" 6 0.98 0.98 0.98 91\n",
" 7 0.89 0.96 0.92 89\n",
" 8 0.88 0.72 0.79 88\n",
" 9 0.80 0.78 0.79 92\n",
"\n",
"avg / total 0.89 0.89 0.89 899\n",
"\n",
"\n",
"Confusion matrix:\n",
"[[83 0 1 0 0 3 1 0 0 0]\n",
" [ 0 74 1 8 0 0 0 0 3 5]\n",
" [ 1 0 82 0 0 0 0 0 0 3]\n",
" [ 0 3 0 79 0 0 0 6 2 1]\n",
" [ 4 0 0 0 84 1 0 0 2 1]\n",
" [ 0 1 0 0 0 86 1 0 0 3]\n",
" [ 0 2 0 0 0 0 89 0 0 0]\n",
" [ 0 0 0 0 2 2 0 85 0 0]\n",
" [ 0 4 1 6 0 7 0 2 63 5]\n",
" [ 5 0 0 2 0 8 0 3 2 72]]\n"
]
},
{
"data": {
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\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7ea20828f6a0>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"from sklearn.neural_network import MLPClassifier\n",
"\n",
"# The digits dataset\n",
"digits = datasets.load_digits()\n",
"\n",
"# The data that we are interested in is made of 8x8 images of digits, let's\n",
"# have a look at the first 4 images, stored in the `images` attribute of the\n",
"# dataset. If we were working from image files, we could load them using\n",
"# matplotlib.pyplot.imread. Note that each image must have the same size. For these\n",
"# images, we know which digit they represent: it is given in the 'target' of\n",
"# the dataset.\n",
"images_and_labels = list(zip(digits.images, digits.target))\n",
"for index, (image, label) in enumerate(images_and_labels[:4]):\n",
" plt.subplot(2, 4, index + 1)\n",
" plt.axis('off')\n",
" plt.imshow(image, cmap=plt.cm.gray_r, interpolation='nearest')\n",
" plt.title('Training: %i' % label)\n",
"\n",
"# To apply a classifier on this data, we need to flatten the image, to\n",
"# turn the data in a (samples, feature) matrix:\n",
"n_samples = len(digits.images)\n",
"data = digits.images.reshape((n_samples, -1))\n",
"\n",
"classifier = MLPClassifier(\n",
" # Activation function in the hidden layer.\n",
" activation=\"relu\",\n",
" # L2 penalty (regularization term) parameter.\n",
" alpha=0.00001,\n",
" # Bath size.\n",
" batch_size=100,\n",
" # The ith element represents the number of neurons in the ith hidden layer.\n",
" hidden_layer_sizes=(1000,), \n",
" # The initial learning rate used.\n",
" learning_rate_init=0.00001,\n",
" # Maximum number of iterations.\n",
" max_iter=100,\n",
" # Solver.\n",
" solver=\"adam\",\n",
" shuffle=True,\n",
" verbose=False\n",
")\n",
"\n",
"# We learn the digits on the first half of the digits\n",
"classifier.fit(data[:n_samples // 2], digits.target[:n_samples // 2])\n",
"\n",
"# Now predict the value of the digit on the second half:\n",
"expected = digits.target[n_samples // 2:]\n",
"predicted = classifier.predict(data[n_samples // 2:])\n",
"\n",
"print(\"Classification report for classifier %s:\\n%s\\n\"\n",
" % (classifier, metrics.classification_report(expected, predicted)))\n",
"print(\"Confusion matrix:\\n%s\" % metrics.confusion_matrix(expected, predicted))\n",
"\n",
"images_and_predictions = list(zip(digits.images[n_samples // 2:], predicted))\n",
"for index, (image, prediction) in enumerate(images_and_predictions[:4]):\n",
" plt.subplot(2, 4, index + 5)\n",
" plt.axis('off')\n",
" plt.imshow(image, cmap=plt.cm.gray_r, interpolation='nearest')\n",
" plt.title('Prediction: %i' % prediction)\n",
"\n",
"plt.show()\n",
"plt.close()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Issue: Complexity of hyperparameters, or how can be hyperparameters decided? \n",
"\n",
"There are many hyperparameters that we have to set before the actual training process begins. Each parameter should be decided in relation to machine learning theory and it cause side effects in training model. Because of this complexity of hyperparameters, so-called the *hyperparameter tuning* must become a burden of Data scientists and R & D engineers from the perspective of not only a theoretical point of view but also implementation level. \n",
"\n",
"Beginners or end users who are inclined to use *state-of-the-art* Machine Learning Library as a mere blackbox and spend all one's time doing blackbox test may regard this problem setting as a kind of paradox or a bitter irony. Even if hyperparameters were chosen at random, the training for indefinitely long times makes it possible to predict with high precision to serve end user's aim. \n",
"\n",
"In a sense, such endless *hyperparameter tuning* implicates a behavior that supports **the infinite monkey theorem**. This theorem states that a monkey hitting keys at random on a typewriter keyboard for an infinite amount of time will almost surely type a given natural sentence, such as the complete works of William Shakespeare. Although we can believe the illimitable possibilities of human beings, but time is limited.\n",
"\n",
"# Problem re-setting: Combinatorial optimization problem.\n",
"\n",
"This issue can be considered as Combinatorial optimization problem which is an optimization problem, where an optimal solution has to be identified from a finite set of solutions. The solutions are normally discrete or can be converted into discrete. This is an important topic studied in operations research such as software engineering, artificial intelligence(AI), and machine learning. For instance, travelling sales man problem is one of the popular combinatorial optimization problem.\n",
"\n",
"Considering that the *hyperparameter tuning* can be formed into Combinatorial optimization problem, the optimal solution to be searched is estimation accuracy, precision, recall, or F-value and so on. Conversely, estimation error such as Mean Squared Error(MSE), Root Mean Squared Error(RMSE), or Mean Absolute Error(MAE) can be a value of penalty, which must be reduced by searching and learning.\n",
"\n",
"In this problem setting, combination of the hyperparameters are explanatory variables for the optimal solution. Each parameter can be generated from random sampling like Monte Carlo method."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Problem solution: Simulated Annealing.\n",
"\n",
"Simulated Annealing is a probabilistic single solution based search method inspired by the annealing process in metallurgy. Annealing is a physical process referred to as tempering certain alloys of metal, glass, or crystal by heating above its melting point, holding its temperature, and then cooling it very slowly until it solidifies into a perfect crystalline structure. The simulation of this process is known as simulated annealing. \n",
"\n",
"### Conceptual perspective.\n",
"\n",
"The simulated annealing is a generic algorithm. Combinatorial optimization is an one of the various functions of simulated annealing. \n",
"\n",
"#### Boltzmann distribution.\n",
"\n",
"According to statistical mechanics and thermodynamics, $P_{\\alpha}$, the probability of a physical system\n",
"being in state $\\alpha$ with energy $E_{\\alpha}$ at absolute temperature $T$ satisfies the Boltzmann distribution as follow.\n",
"\n",
"$$P_{\\alpha} = \\frac{1}{Z}e^{\\frac{E_{\\alpha}}{k_{B}}}T$$\n",
"\n",
"where $k_{B}$ is the Boltzmann’s constant and $Z$ is the partition function, defined by\n",
"\n",
"$$Z = \\sum_{\\beta}^{}e^{\\frac{E_{\\beta}}{k_{B}}}T$$\n",
"\n",
"#### Meaning of partition function.\n",
"\n",
"To simplify, this partition function can be considered as the summation being taken over all states $\\alpha = \\{0, 1, ..., \\beta \\}$ with energy $E_{\\alpha}$ at temperature $T$ . At high $T$ , the Boltzmann distribution exhibits uniform preference for all the states, regardless of the energy. The system ignores small changes in\n",
"the energy and approaches thermal equilibrium rapidly. On the other hand, when $T$ approaches zero or very low, only the states with minimum energy have non-zero probability of occurrence. The system can respond to small changes in the energy.\n",
"\n",
"#### To find a better minimum\n",
"\n",
"According to statistical mechanics, gradually decreasing temperature corresponds to gradually decreasing information entropy. So this system can perform a fine search in the neighborhood of the already determined minimum and finds a better minimum.\n",
"\n",
"#### Cost function\n",
"\n",
"The function of Combinatorial optimization algorithm is minimization of the penalty that cost function returns. Typically, the cost function is defined by\n",
"\n",
"$$f(p_k, y_k) = Loss_{MSE} =\\frac{1}{n}\\sum_{k=1}^n(p_k - y_k)^2$$\n",
"\n",
"where $p_k$ is a set of predicted labels and $y_k$ is a set of correct labels."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### Specification perspective.\n",
"\n",
"There are various Simulated Annealing such as Boltzmann Annealing, Adaptive Simulated Annealing(SAS), and Quantum Simulated Annealing. On the premise of Combinatorial optimization problem, these annealing methods can be considered as functionally equivalent. The *Commonality/Variability* in these methods are able to keep responsibility of objects all straight as the class diagram below indicates.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/class_diagram_annealing_model.png\" />"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"An abstract class `AnnealingModel` is responsible for common annealing methods. And a concrete class `SimulatedAnnealing` is-a `AnnealingModel` to behave as Simulated Annealing. `CostFunctionable` is an interface which performs as cost function. Implementation of this interface depends on user's problem settings.\n",
"\n",
"`AdaptiveSimulatedAnnealing` is a functionally extended version of `SimulatedAnnealing`. `QuantumMonteCarlo` is a functional equivalent of `SimulatedAnnealing`. The interface `DistanceComputable` can be distance function for `QuantumMonteCarlo`. For instance, `CostAsDistance` is-a `DistanceComputable` to obtain cost as distance by `CostFunctionable`."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### Implementation perspective.\n",
"\n",
"In order to implement `CostFunctionable` and use `AnnealingModel` in this problem setting, let us adhere fundamentally to an introduction with scikit-learn.\n",
"\n",
"- [An introduction to machine learning with scikit-learn — scikit-learn 0.19.1 documentation](http://scikit-learn.org/stable/tutorial/basic/tutorial.html)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Dataset.\n",
"\n",
"The data that we are interested in is made of 8x8 images of digits, let's have a look at the first 4 images, stored in the `images` attribute of the dataset. If we were working from image files, we could load them using matplotlib.pyplot.imread. Note that each image must have the same size. For these images, we know which digit they represent: it is given in the 'target' of the dataset."
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {},
"outputs": [
{
"data": {
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"text/plain": [
"<matplotlib.figure.Figure at 0x7ea2082da908>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# The digits dataset\n",
"digits = datasets.load_digits()\n",
"\n",
"images_and_labels = list(zip(digits.images, digits.target))\n",
"for index, (image, label) in enumerate(images_and_labels[:4]):\n",
" plt.subplot(2, 4, index + 1)\n",
" plt.axis('off')\n",
" plt.imshow(image, cmap=plt.cm.gray_r, interpolation='nearest')\n",
" plt.title('Training: %i' % label)\n",
"\n",
"# To apply a classifier on this data, we need to flatten the image, to\n",
"# turn the data in a (samples, feature) matrix:\n",
"n_samples = len(digits.images)\n",
"data = digits.images.reshape((n_samples, -1))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Implement cost function.\n",
"\n",
"Let us implement `CostFunctionable` as follow."
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {},
"outputs": [],
"source": [
"from pyqlearning.annealingmodel.simulated_annealing import SimulatedAnnealing\n",
"from pyqlearning.annealingmodel.cost_functionable import CostFunctionable\n",
"import numpy as np\n",
"import pandas as pd\n",
"from sklearn.metrics import mean_squared_error"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {},
"outputs": [],
"source": [
"class DigitClfCost(CostFunctionable):\n",
" '''\n",
" is-a `CostFunctionable` in relation to `SimulatedAnnealing`.\n",
" '''\n",
"\n",
" # The list of activation function in the hidden layer.\n",
" __activation_list = [\"relu\", \"logistic\", \"tanh\"]\n",
" # The solver for weight optimization.\n",
" __solver_list = [\"lbfgs\", \"sgd\", \"adam\"]\n",
" \n",
" def compute(self, x):\n",
" '''\n",
" Compute cost.\n",
" \n",
" Args:\n",
" x: `np.ndarray` of explanatory variables.\n",
" \n",
" Returns:\n",
" cost\n",
" '''\n",
" classifier = MLPClassifier(\n",
" # Activation function in the hidden layer.\n",
" activation=self.__activation_list[int(x[0])],\n",
" # L2 penalty (regularization term) parameter.\n",
" alpha=x[1],\n",
" # Bath size.\n",
" batch_size=int(x[2]),\n",
" # The ith element represents the number of neurons in the ith hidden layer.\n",
" hidden_layer_sizes=(int(x[3]),), \n",
" # The initial learning rate used.\n",
" learning_rate_init=x[4],\n",
" # Maximum number of iterations.\n",
" max_iter=int(x[5]),\n",
" # Solver.\n",
" solver=self.__solver_list[int(x[6])],\n",
" shuffle=True,\n",
" verbose=False\n",
" )\n",
"\n",
" # We learn the digits on the first half of the digits\n",
" classifier.fit(data[:n_samples // 2], digits.target[:n_samples // 2])\n",
"\n",
" # Now predict the value of the digit on the second half:\n",
" expected = digits.target[n_samples // 2:]\n",
" predicted = classifier.predict(data[n_samples // 2:])\n",
" \n",
" cost = mean_squared_error(expected, predicted)\n",
" \n",
" return cost\n",
"\n",
" def get_activation_list(self):\n",
" return self.__activation_list\n",
"\n",
" def get_solver_list(self):\n",
" return self.__solver_list\n",
"\n",
" def set_readonly(self, value):\n",
" raise TypeError()\n",
"\n",
" activation_list = property(get_activation_list, set_readonly)\n",
" solver_list = property(get_solver_list, set_readonly)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Sampling hyperparameters.\n",
"\n",
"Like Monte Carlo method, let us draw random samples from a normal (Gaussian) or unifrom distribution."
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [],
"source": [
"cost_functionable = DigitClfCost()\n",
"\n",
"activation_arr = np.random.randint(low=0, high=len(cost_functionable.activation_list), size=1000)\n",
"alpha_arr = np.random.normal(loc=0.0001, scale=0.00001, size=1000)\n",
"batch_size_arr = np.random.normal(loc=200, scale=10, size=1000).astype(int)\n",
"hidden_arr = np.random.normal(loc=1000, scale=100, size=1000).astype(int)\n",
"learning_rate_arr = np.random.normal(loc=0.01, scale=0.0005, size=1000)\n",
"max_iter_arr = np.random.normal(loc=1000, scale=200, size=1000)\n",
"solver_arr = np.random.randint(low=0, high=len(cost_functionable.solver_list), size=1000)\n",
"\n",
"params_arr = np.c_[\n",
" activation_arr,\n",
" alpha_arr,\n",
" batch_size_arr,\n",
" hidden_arr,\n",
" learning_rate_arr,\n",
" max_iter_arr,\n",
" solver_arr\n",
"]\n",
"\n",
"params_arr = pd.DataFrame(params_arr, columns=[\n",
" \"activation\",\n",
" \"alpha\",\n",
" \"batch_size\",\n",
" \"hidden\",\n",
" \"learning_rate\",\n",
" \"max_iter\",\n",
" \"solver\"\n",
"]).sort_values(by=[\n",
" \"learning_rate\",\n",
" \"batch_size\",\n",
" \"max_iter\",\n",
" \"hidden\",\n",
" \"alpha\",\n",
" \"activation\",\n",
" \"solver\"\n",
"]).values"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Use `AnnealingModel`.\n",
"\n",
"Instantiate `DigitClfCost` and delegate it to `SimulatedAnnealing.__init__()`. Then call the method `fit_dist_mat` to fit the combination of hyperparameters. Finally, call the method `annealing`."
]
},
{
"cell_type": "code",
"execution_count": 22,
"metadata": {},
"outputs": [
{
"name": "stderr",
"output_type": "stream",
"text": [
"/media/removable/rum/accel-brain-code/Reinforcement-Learning/pyqlearning/annealing_model.py:30: FutureWarning: This property will be removed in future version. Use `var_arr`.\n",
" warnings.warn(\"This property will be removed in future version. Use `var_arr`.\", FutureWarning)\n"
]
}
],
"source": [
"annealing_model = SimulatedAnnealing(\n",
" cost_functionable=cost_functionable,\n",
" cycles_num=33,\n",
" trials_per_cycle=3,\n",
" accepted_sol_num=0.0,\n",
" init_prob=0.7,\n",
" final_prob=0.001,\n",
" start_pos=0,\n",
" move_range=3\n",
")\n",
"annealing_model.fit_dist_mat(params_arr)\n",
"annealing_model.annealing()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Get and plot result data.\n",
"\n",
"As shown by the figure below, the energy has been decreasing gradually."
]
},
{
"cell_type": "code",
"execution_count": 23,
"metadata": {},
"outputs": [
{
"name": "stderr",
"output_type": "stream",
"text": [
"/media/removable/rum/accel-brain-code/Reinforcement-Learning/pyqlearning/annealing_model.py:112: FutureWarning: This property will be removed in future version. Use `predicted_log_arr`.\n",
" warnings.warn(\"This property will be removed in future version. Use `predicted_log_arr`.\", FutureWarning)\n"
]
}
],
"source": [
"# Extract list: [(Cost, Delta energy, Mean of delta energy, probability, accept)]\n",
"predicted_log_list = annealing_model.predicted_log_list\n",
"predicted_log_arr = np.array(predicted_log_list)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Get and plot result data.\n",
"\n",
"As shown by the figure below, the energy has been decreasing gradually."
]
},
{
"cell_type": "code",
"execution_count": 24,
"metadata": {},
"outputs": [
{
"data": {
"image/png": 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\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7ea200962128>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# Plot delta_e_avg\n",
"fig = plt.figure(figsize=(15, 12))\n",
"plt.plot(predicted_log_arr[:, 2])\n",
"plt.show()\n",
"plt.close()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Dicide optimal solution\n",
"\n",
"The optimal combination of hyperparameters can be confirmed as follow."
]
},
{
"cell_type": "code",
"execution_count": 25,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Activation: logistic\n",
"Alpha: 9.07558440806e-05\n",
"Batch size: 193\n",
"The number of units in hidden layer: 968\n",
"Init of Learning rate: 0.00905655735841\n",
"Max iter: 862\n",
"Solver: lbfgs\n"
]
}
],
"source": [
"min_e_v_arr = annealing_model.var_arr[np.argmin(predicted_log_arr[:, 0])]\n",
"\n",
"activation = cost_functionable.activation_list[int(min_e_v_arr[0])]\n",
"alpha = min_e_v_arr[1]\n",
"batch_size = int(min_e_v_arr[2])\n",
"hidden_n = int(min_e_v_arr[3])\n",
"learning_rate_init = min_e_v_arr[4]\n",
"max_iter = int(min_e_v_arr[5])\n",
"solver = cost_functionable.solver_list[int(min_e_v_arr[6])]\n",
"\n",
"print(\"Activation: \" + str(activation))\n",
"print(\"Alpha: \" + str(alpha))\n",
"print(\"Batch size: \" + str(batch_size))\n",
"print(\"The number of units in hidden layer: \" + str(hidden_n))\n",
"print(\"Init of Learning rate: \" + str(learning_rate_init))\n",
"print(\"Max iter: \" + str(max_iter))\n",
"print(\"Solver: \" + str(solver))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Training by optimal hyperparameters.\n",
"\n",
"Then this optimal solution makes it possible for machine learning model to learn by optimal hyperparameters."
]
},
{
"cell_type": "code",
"execution_count": 26,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Classification report for classifier MLPClassifier(activation='logistic', alpha=9.0755844080612054e-05,\n",
" batch_size=193, beta_1=0.9, beta_2=0.999, early_stopping=False,\n",
" epsilon=1e-08, hidden_layer_sizes=(968,), learning_rate='constant',\n",
" learning_rate_init=0.009056557358407635, max_iter=862, momentum=0.9,\n",
" nesterovs_momentum=True, power_t=0.5, random_state=None,\n",
" shuffle=True, solver='lbfgs', tol=0.0001, validation_fraction=0.1,\n",
" verbose=False, warm_start=False):\n",
" precision recall f1-score support\n",
"\n",
" 0 1.00 0.95 0.98 88\n",
" 1 0.94 0.92 0.93 91\n",
" 2 0.92 1.00 0.96 86\n",
" 3 0.96 0.87 0.91 91\n",
" 4 0.98 0.88 0.93 92\n",
" 5 0.92 0.96 0.94 91\n",
" 6 0.90 0.98 0.94 91\n",
" 7 0.93 0.93 0.93 89\n",
" 8 0.94 0.88 0.91 88\n",
" 9 0.85 0.96 0.90 92\n",
"\n",
"avg / total 0.93 0.93 0.93 899\n",
"\n",
"\n",
"Confusion matrix:\n",
"[[84 0 0 0 1 1 2 0 0 0]\n",
" [ 0 84 2 0 0 0 0 0 0 5]\n",
" [ 0 0 86 0 0 0 0 0 0 0]\n",
" [ 0 0 2 79 0 2 0 5 3 0]\n",
" [ 0 1 0 0 81 0 7 0 0 3]\n",
" [ 0 0 0 0 0 87 1 0 1 2]\n",
" [ 0 2 0 0 0 0 89 0 0 0]\n",
" [ 0 0 2 0 1 0 0 83 1 2]\n",
" [ 0 2 1 2 0 3 0 0 77 3]\n",
" [ 0 0 0 1 0 2 0 1 0 88]]\n"
]
},
{
"data": {
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"text/plain": [
"<matplotlib.figure.Figure at 0x7ea205d0f128>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"classifier = MLPClassifier(\n",
" # Activation function in the hidden layer.\n",
" activation=activation,\n",
" # L2 penalty (regularization term) parameter.\n",
" alpha=alpha,\n",
" # Bath size.\n",
" batch_size=batch_size,\n",
" # The ith element represents the number of neurons in the ith hidden layer.\n",
" hidden_layer_sizes=(hidden_n,), \n",
" # The initial learning rate used.\n",
" learning_rate_init=learning_rate_init,\n",
" # Maximum number of iterations.\n",
" max_iter=max_iter,\n",
" # Solver.\n",
" solver=solver,\n",
" shuffle=True,\n",
" verbose=False\n",
")\n",
"\n",
"# We learn the digits on the first half of the digits\n",
"classifier.fit(data[:n_samples // 2], digits.target[:n_samples // 2])\n",
"\n",
"# Now predict the value of the digit on the second half:\n",
"expected = digits.target[n_samples // 2:]\n",
"predicted = classifier.predict(data[n_samples // 2:])\n",
"\n",
"print(\"Classification report for classifier %s:\\n%s\\n\"\n",
" % (classifier, metrics.classification_report(expected, predicted)))\n",
"print(\"Confusion matrix:\\n%s\" % metrics.confusion_matrix(expected, predicted))\n",
"\n",
"images_and_predictions = list(zip(digits.images[n_samples // 2:], predicted))\n",
"for index, (image, prediction) in enumerate(images_and_predictions[:4]):\n",
" plt.subplot(2, 4, index + 5)\n",
" plt.axis('off')\n",
" plt.imshow(image, cmap=plt.cm.gray_r, interpolation='nearest')\n",
" plt.title('Prediction: %i' % prediction)\n",
"\n",
"plt.show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Functional equivalent: Adaptive Simulated Annealing.\n",
"\n",
"Adaptive simulated annealing, also known as the very fast simulated reannealing, is a very efficient version of simulated annealing."
]
},
{
"cell_type": "code",
"execution_count": 12,
"metadata": {},
"outputs": [
{
"name": "stderr",
"output_type": "stream",
"text": [
"/media/removable/rum/accel-brain-code/Reinforcement-Learning/pyqlearning/annealing_model.py:30: FutureWarning: This property will be removed in future version. Use `var_arr`.\n",
" warnings.warn(\"This property will be removed in future version. Use `var_arr`.\", FutureWarning)\n"
]
}
],
"source": [
"from pyqlearning.annealingmodel.simulatedannealing.adaptive_simulated_annealing import AdaptiveSimulatedAnnealing\n",
"\n",
"cost_functionable = DigitClfCost()\n",
"annealing_model = AdaptiveSimulatedAnnealing(\n",
" cost_functionable=cost_functionable,\n",
" cycles_num=33,\n",
" trials_per_cycle=3,\n",
" accepted_sol_num=0.0,\n",
" init_prob=0.7,\n",
" final_prob=0.001,\n",
" start_pos=0,\n",
" move_range=3\n",
")\n",
"annealing_model.adaptive_set(\n",
" reannealing_per=50,\n",
" thermostat=0.,\n",
" t_min=0.001,\n",
" t_default=1.0\n",
")\n",
"annealing_model.fit_dist_mat(params_arr)\n",
"annealing_model.annealing()"
]
},
{
"cell_type": "code",
"execution_count": 13,
"metadata": {},
"outputs": [
{
"name": "stderr",
"output_type": "stream",
"text": [
"/media/removable/rum/accel-brain-code/Reinforcement-Learning/pyqlearning/annealing_model.py:112: FutureWarning: This property will be removed in future version. Use `predicted_log_arr`.\n",
" warnings.warn(\"This property will be removed in future version. Use `predicted_log_arr`.\", FutureWarning)\n"
]
}
],
"source": [
"# Extract list: [(Cost, Delta energy, Mean of delta energy, probability, accept)]\n",
"predicted_log_list = annealing_model.predicted_log_list\n",
"predicted_log_arr = np.array(predicted_log_list)"
]
},
{
"cell_type": "code",
"execution_count": 14,
"metadata": {},
"outputs": [
{
"data": {
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\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7ea200eb4748>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"# Plot delta_e_avg\n",
"fig = plt.figure(figsize=(15, 12))\n",
"plt.plot(predicted_log_arr[:, 2])\n",
"plt.show()\n",
"plt.close()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Dicide optimal solution\n",
"\n",
"The optimal combination of hyperparameters can be confirmed as follow."
]
},
{
"cell_type": "code",
"execution_count": 15,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Activation: relu\n",
"Alpha: 0.000105971020366\n",
"Batch size: 211\n",
"The number of units in hidden layer: 933\n",
"Init of Learning rate: 0.00870026005571\n",
"Max iter: 1316\n",
"Solver: lbfgs\n"
]
}
],
"source": [
"min_e_v_arr = annealing_model.var_arr[np.argmin(predicted_log_arr[:, 0])]\n",
"\n",
"activation = cost_functionable.activation_list[int(min_e_v_arr[0])]\n",
"alpha = min_e_v_arr[1]\n",
"batch_size = int(min_e_v_arr[2])\n",
"hidden_n = int(min_e_v_arr[3])\n",
"learning_rate_init = min_e_v_arr[4]\n",
"max_iter = int(min_e_v_arr[5])\n",
"solver = cost_functionable.solver_list[int(min_e_v_arr[6])]\n",
"\n",
"print(\"Activation: \" + str(activation))\n",
"print(\"Alpha: \" + str(alpha))\n",
"print(\"Batch size: \" + str(batch_size))\n",
"print(\"The number of units in hidden layer: \" + str(hidden_n))\n",
"print(\"Init of Learning rate: \" + str(learning_rate_init))\n",
"print(\"Max iter: \" + str(max_iter))\n",
"print(\"Solver: \" + str(solver))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"#### Training by optimal hyperparameters.\n",
"\n",
"Then this optimal solution makes it possible for machine learning model to learn by optimal hyperparameters."
]
},
{
"cell_type": "code",
"execution_count": 16,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"Classification report for classifier MLPClassifier(activation='relu', alpha=0.00010597102036595624, batch_size=211,\n",
" beta_1=0.9, beta_2=0.999, early_stopping=False, epsilon=1e-08,\n",
" hidden_layer_sizes=(933,), learning_rate='constant',\n",
" learning_rate_init=0.008700260055708401, max_iter=1316,\n",
" momentum=0.9, nesterovs_momentum=True, power_t=0.5,\n",
" random_state=None, shuffle=True, solver='lbfgs', tol=0.0001,\n",
" validation_fraction=0.1, verbose=False, warm_start=False):\n",
" precision recall f1-score support\n",
"\n",
" 0 1.00 0.97 0.98 88\n",
" 1 0.93 0.89 0.91 91\n",
" 2 0.99 1.00 0.99 86\n",
" 3 0.98 0.87 0.92 91\n",
" 4 0.95 0.88 0.92 92\n",
" 5 0.88 0.93 0.90 91\n",
" 6 0.89 0.98 0.93 91\n",
" 7 0.98 0.94 0.96 89\n",
" 8 0.88 0.90 0.89 88\n",
" 9 0.85 0.93 0.89 92\n",
"\n",
"avg / total 0.93 0.93 0.93 899\n",
"\n",
"\n",
"Confusion matrix:\n",
"[[85 0 0 0 1 0 2 0 0 0]\n",
" [ 0 81 0 1 1 4 1 0 1 2]\n",
" [ 0 0 86 0 0 0 0 0 0 0]\n",
" [ 0 0 0 79 0 3 0 0 8 1]\n",
" [ 0 1 0 0 81 0 7 0 0 3]\n",
" [ 0 0 1 0 0 85 1 0 0 4]\n",
" [ 0 2 0 0 0 0 89 0 0 0]\n",
" [ 0 0 0 0 1 0 0 84 1 3]\n",
" [ 0 3 0 0 1 3 0 0 79 2]\n",
" [ 0 0 0 1 0 2 0 2 1 86]]\n"
]
},
{
"data": {
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"text/plain": [
"<matplotlib.figure.Figure at 0x7ea208134ef0>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"classifier = MLPClassifier(\n",
" # Activation function in the hidden layer.\n",
" activation=activation,\n",
" # L2 penalty (regularization term) parameter.\n",
" alpha=alpha,\n",
" # Bath size.\n",
" batch_size=batch_size,\n",
" # The ith element represents the number of neurons in the ith hidden layer.\n",
" hidden_layer_sizes=(hidden_n,), \n",
" # The initial learning rate used.\n",
" learning_rate_init=learning_rate_init,\n",
" # Maximum number of iterations.\n",
" max_iter=max_iter,\n",
" # Solver.\n",
" solver=solver,\n",
" shuffle=True,\n",
" verbose=False\n",
")\n",
"\n",
"# We learn the digits on the first half of the digits\n",
"classifier.fit(data[:n_samples // 2], digits.target[:n_samples // 2])\n",
"\n",
"# Now predict the value of the digit on the second half:\n",
"expected = digits.target[n_samples // 2:]\n",
"predicted = classifier.predict(data[n_samples // 2:])\n",
"\n",
"print(\"Classification report for classifier %s:\\n%s\\n\"\n",
" % (classifier, metrics.classification_report(expected, predicted)))\n",
"print(\"Confusion matrix:\\n%s\" % metrics.confusion_matrix(expected, predicted))\n",
"\n",
"images_and_predictions = list(zip(digits.images[n_samples // 2:], predicted))\n",
"for index, (image, prediction) in enumerate(images_and_predictions[:4]):\n",
" plt.subplot(2, 4, index + 5)\n",
" plt.axis('off')\n",
" plt.imshow(image, cmap=plt.cm.gray_r, interpolation='nearest')\n",
" plt.title('Prediction: %i' % prediction)\n",
"\n",
"plt.show()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Functional equivalent: Quantum Monte Carlo Method\n",
"\n",
"Generally, Quantum Monte Carlo is a stochastic method to solve the Schrödinger equation. This algorithm is one of the earliest types of solution in order to simulate the Quantum Annealing in classical computer. In summary, one of the function of this algorithm is to solve the ground state search problem which is known as logically equivalent to combinatorial optimization problem.\n",
"\n",
"According to theory of spin glasses, the ground state search problem can be described as minimization energy determined by the hamiltonian <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/h_0.png\" /> as follow\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/hamiltonian_in_ising_model.png\" />\n",
"\n",
"where <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/pauli_z_i.png\" /> refers to the Pauli spin matrix below for the spin-half particle at lattice point <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/i.gif\" />. In spin glasses, random value is assigned to <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/j_i_j.png\" />. The number of combinations is enormous. If this value is <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/n.png\" />, a trial frequency is <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/2_n.png\" />. This computation complexity makes it impossible to solve the ground state search problem. Then, in theory of spin glasses, the standard hamiltonian is re-described in expanded form.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/hamiltonian_in_t_ising_model.png\" />\n",
"\n",
"where <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/pauli_x_i.png\" /> also refers to the Pauli spin matrix and <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/gamma.png\" /> is so-called annealing coefficient, which is hyperparameter that contains vely high value. Ising model to follow this Hamiltonian is known as the Transverse Ising model.\n",
"\n",
"In relation to this system, thermal equilibrium amount of a physical quantity <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/q.png?1\" /> is as follow.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/langle_q_rangle.png\" />\n",
"\n",
"If <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/h.png\" /> is a diagonal matrix, then also <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/e_beta_h.png\" /> is diagonal matrix. If diagonal element in <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/h.png\" /> is <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/e_i.png\" />, Each diagonal element is <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/e_beta_h_ij_e_i.png\" />. However if <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/h.png\" /> has off-diagonal elements, It is known that <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/e_beta_h_ij_e_i_neq.png\" /> since for any of the exponent <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/i.gif\" /> we must exponentiate the matrix as follow.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/e_matrix_infty.png\" />"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Therefore, a path integration based on Trotter-Suzuki decomposition has been introduced in Quantum Monte Carlo Method. This path integration makes it possible to obtain the partition function <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z.png\" />.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z_in_t_ising_model.png\" />\n",
"\n",
"where if <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/m.png\" /> is large enough, relational expression below is established.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/exp_left_frac_1_m_beta_h_right.png\" /></td></tr>\n",
"\n",
"Then the partition function <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z.png\" /> can be re-descibed as follow.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z_in_t_ising_model_re_described.png\" />"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"where <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/mid_sigma_k_rangle.png\" /> is <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/l.png\" /> topological products (product spaces). Because <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/h_0.png\" /> is the diagonal matrix, <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/tilde_sigma_j_z_mid_sigma.png\" />.\n",
"\n",
"Therefore, \n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/langle_sigma_k_mid.png\" />"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"The partition function <img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z.png\" /> can be re-descibed as follow.\n",
"\n",
"<img src=\"https://storage.googleapis.com/accel-brain-code/Reinforcement-Learning/img/latex/z_in_t_ising_model_re_described_last.png\" />"
]
},