Hyperbolic Embedding of Graphs and Clustering#

Lead authors: Thomas Gerald and Hadi Zaatiti.

Introduction#

From social networks to parse trees, knowledge graphs to protein interaction networks, Graph-Structured Data is endemic to a wide variety of natural and engineered systems. Often, understanding the structure and/or dynamics of these graphs yields insight into the systems under investigation. Take, for example, the problems of finding key influencers or distinct communities within social networks.

The goal of graph embedding is to find a way of representing the graph in a space which more readily lends itself to analysis/investigation. One approach is to identify points in a vector space with nodes of the graph in such a way that important relations between nodes are preserved via relations between their corresponding points.

There are a wide variety of methods which approach this problem in different ways and for different aims, say for clustering or for link prediction. Recently, the embedding of Graph Structured Data (GSD) on manifolds has received considerable attention. In particular, much work has shown that hyperbolic spaces are beneficial for a wide variety of tasks with GSD [ND2017]. This tutorial shows how to learn such embeddings using the Poincaré Ball manifold and the well-known ‘Karate Club’ social network dataset with geomstats. This data and several others can be found in the datasets.data module of the project’s github repository.

KarateEmbedding Learning a Poincaré disk embedding of the Karate club graph dataset

We start by importing standard tools for logging and visualization, allowing us to draw the embedding of the GSD on the manifold. Next, we import the manifold of interest, visualization tools, and other methods from geomstats.

 In [1]:
import logging
import matplotlib.pyplot as plt

import geomstats.backend as gs
import geomstats.visualization as visualization

from geomstats.datasets.utils import load_karate_graph
from geomstats.geometry.poincare_ball import PoincareBall
INFO: Using numpy backend

Parameters and Initialization#

We define the following parameters needed for embedding:

Parameter

Description

random.seed

An initial manually set number for generating pseudorandom numbers

dim

Dimensions of the manifold used for embedding

max_epochs

Number of iterations for learning the embedding

lr

Learning rate

n_negative

Number of negative samples

context_size

Size of the considered context for each node of the graph

Let us discuss a few things about the parameters of the above table. The number of dimensions should be high (i.e., 10+) for large datasets (i.e., where the number of nodes/edges is significantly large). In this tutorial we consider a dataset that is quite small with only 34 nodes. The Poincaré disk of only two dimensions is therefore sufficient to capture the complexity of the graph and provide a faithful representation. Some parameters are hard to know in advance, such as max_epochs and lr. These should be tuned specifically for each dataset. Visualization can help with tuning the parameters. Also, one can perform a grid search to find values of these parameters which maximize some performance function. In learning embeddings, one can consider performance metrics such as a measure for cluster seperability or normalized mutual information (NMI) or others. Similarly, the number of negative samples and context size can also be thought of as hyperparameters and will be further discussed in the sequel. An instance of the Graph class is created and set to the Karate club dataset.

 In [2]:
gs.random.seed(1234)
dim = 2
max_epochs = 100
lr = 0.05
n_negative = 2
context_size = 1
karate_graph = load_karate_graph()

The Zachary karate club network was collected from the members of a university karate club by Wayne Zachary in 1977. Each node represents a member of the club, and each edge represents an undirected relation between two members. An often discussed problem using this dataset is to find the two groups of people into which the karate club split after an argument between two teachers. 2878968ff4544d4aad62e73a3d78e6c7 Some information about the dataset is displayed to provide insight into its complexity.

 In [3]:
nb_vertices_by_edges = [len(e_2) for _, e_2 in karate_graph.edges.items()]
logging.info("Number of vertices: %s", len(karate_graph.edges))
logging.info(
    "Mean edge-vertex ratio: %s",
    (sum(nb_vertices_by_edges, 0) / len(karate_graph.edges)),
)
INFO: Number of vertices: 34
INFO: Mean edge-vertex ratio: 4.588235294117647

Denote \(V\) as the set of nodes and \(E \subset V\times V\) the set of edges. The goal of embedding GSD is to provide a faithful and exploitable representation of the graph structure. It is mainly achieved by preserving first-order proximity that enforces nodes sharing edges to be close to each other. It can additionally preserve second-order proximity that enforces two nodes sharing the same context (i.e., nodes that share neighbors but are not necessarily directly connected) to be close. Let \(\mathbb{B}^m\) be the Poincaré Ball of dimension \(m\) equipped with the distance function \(d\). The below figure shows geodesics between pairs of points on \(\mathbb{B}^2\). Geodesics are the shortest path between two points. The distance function \(d\) of two points is the length of the geodesic that links them.

3a22eca3ac134a8b8d9fd39e1a69cd0e

Declaring an instance of the PoincareBall manifold of two dimensions in geomstats is straightforward:

 In [4]:
hyperbolic_manifold = PoincareBall(2)

first and second-order proximities can be achieved by optimising the following loss functions:

Loss function.#

To preserve first and second-order proximities we adopt a loss function similar to (Nickel, 2017) and consider the negative sampling approach as in (Mikolov, 2013) :

\[\mathcal{L} = - \sum_{v_i\in V} \sum_{v_j \in C_i} \bigg[ log(\sigma(-d^2(\phi_i, \phi_j'))) + \sum_{v_k\sim \mathcal{P}_n} log(\sigma(d^2(\phi_i, \phi_k'))) \bigg]\]

where \(\sigma(x)=\frac{1}{1+e^{-x}}\) is the sigmoid function and \(\phi_i \in \mathbb{B}^m\) is the embedding of the \(i\)-th node of \(V\), \(C_i\) the nodes in the context of the \(i\)-th node, \(\phi_j'\in \mathbb{B}^m\) the embedding of \(v_j\in C_i\) and \(\mathcal{P}_n\) the negative sampling distribution over \(V\): \(\mathcal{P}_n(v)=\frac{deg(v)^{3/4}}{\sum_{v_i\in V}deg(v_i)^{3/4}}\). Intuitively one can see that to minimizing \(L\), the distance between \(v_i\) and \(v_j\) should get smaller, while the one between \(v_i\) and \(v_k\) would get larger. 4823661e0304459c9d3440498d0de491

Riemannian optimization.#

Following the idea of (Ganea, 2018) we use the following formula to optimize \(L\):

\[\phi^{t+1} = \text{Exp}_{\phi^t} \left( -lr \frac{\partial L}{\partial \phi} \right)\]

where \(\phi\) is a parameter of \(L\), \(t\in\{1,2,\cdots\}\) is the epoch iteration number and \(lr\) is the learning rate. The formula consists of first computing the usual gradient of the loss function giving the direction in which the parameter should move. The Riemannian exponential map \(\text{Exp}\) is a function that takes a base point \(\phi^t\) and some direction vector \(T\) and returns the point \(\phi^{t+1}\) such that \(\phi^{t+1}\) belongs to the geodesic initiated from \(\phi{t}\) in the direction of \(T\) and the length of the geoedesic curve between \(\phi^t\) and \(\phi^{t+1}\) is of 1 unit. The Riemannian exponential map is implemented as a method of the PoincareBallMetric class in the geometry module of geomstats.

Therefore to minimize \(L\) we will need to compute its gradient. Several steps are required to do so, 1. Compute the gradient of the squared distance 2. Compute the gradient of the log sigmoid 3. Compute the gradient of the composision of 1. and 2.

For 1., we use the formula proposed by (Arnaudon, 2013) which uses the Riemannian logarithmic map to compute the gradient of the distance. This is implemented as

 In [5]:
def grad_squared_distance(point_a, point_b):
    """Gradient of squared hyperbolic distance.

    Gradient of the squared distance based on the
    Ball representation according to point_a

    Parameters
    ----------
    point_a : array-like, shape=[n_samples, dim]
        First point in hyperbolic space.
    point_b : array-like, shape=[n_samples, dim]
        Second point in hyperbolic space.

    Returns
    -------
    dist : array-like, shape=[n_samples, 1]
        Geodesic squared distance between the two points.
    """
    log_map = PoincareBall(2).metric.log(point_b, point_a)

    return -2 * log_map

For 2. define the log_sigmoid corresponding as follows:

 In [6]:
def log_sigmoid(vector):
    """Logsigmoid function.

    Apply log sigmoid function

    Parameters
    ----------
    vector : array-like, shape=[n_samples, dim]

    Returns
    -------
    result : array-like, shape=[n_samples, dim]
    """
    return gs.log((1 / (1 + gs.exp(-vector))))

The gradient of the logarithm of sigmoid function is implemented as:

 In [7]:
def grad_log_sigmoid(vector):
    """Gradient of log sigmoid function.

    Parameters
    ----------
    vector : array-like, shape=[n_samples, dim]

    Returns
    -------
    gradient : array-like, shape=[n_samples, dim]
    """
    return 1 / (1 + gs.exp(vector))

For 3., apply the composition rule to obtain the gradient of \(L\). The following function given \(\phi_i\), \(\phi'_j\) and \(\phi'_k\) returns the total value of \(L\) and its gradient vector at \(\phi_i\). For the value of \(L\) the loss function formula is simply applied. For the gradient, we apply the composition of grad_log_sigmoid with grad_squared_distance while paying attention to the signs.

 In [8]:
def loss(example_embedding, context_embedding, negative_embedding, manifold):
    """Compute loss and grad.

    Compute loss and grad given embedding of the current example,
    embedding of the context and negative sampling embedding.
    """
    n_edges, dim = negative_embedding.shape[0], example_embedding.shape[-1]
    example_embedding = gs.expand_dims(example_embedding, 0)
    context_embedding = gs.expand_dims(context_embedding, 0)
    positive_distance = manifold.metric.squared_dist(
        example_embedding, context_embedding
    )
    positive_loss = log_sigmoid(-positive_distance)

    reshaped_example_embedding = gs.repeat(example_embedding, n_edges, axis=0)
    negative_distance = manifold.metric.squared_dist(
        reshaped_example_embedding, negative_embedding
    )
    negative_loss = log_sigmoid(negative_distance)

    total_loss = -(positive_loss + negative_loss.sum())

    positive_log_sigmoid_grad = -grad_log_sigmoid(-positive_distance)

    positive_distance_grad = grad_squared_distance(example_embedding, context_embedding)

    positive_grad = (
        gs.repeat(positive_log_sigmoid_grad, dim, axis=-1) * positive_distance_grad
    )

    negative_distance_grad = grad_squared_distance(
        reshaped_example_embedding, negative_embedding
    )

    negative_distance = gs.to_ndarray(negative_distance, to_ndim=2, axis=-1)
    negative_log_sigmoid_grad = grad_log_sigmoid(negative_distance)

    negative_grad = negative_log_sigmoid_grad * negative_distance_grad
    example_grad = -(positive_grad + negative_grad.sum(axis=0))

    return total_loss, example_grad

Capturing the graph structure#

At this point we have the necessary bricks to compute the resulting gradient of \(L\). We are ready to prepare the nodes \(v_i\), \(v_j\) and \(v_k\) and initialise their embeddings \(\phi_i\), \(\phi^{'}_j\) and \(\phi^{'}_k\). First, initialize an array that will hold embeddings \(\phi_i\) of each node \(v_i\in V\) with random points belonging to the Poincaré disk.

 In [9]:
embeddings = gs.random.normal(size=(karate_graph.n_nodes, dim))
embeddings = embeddings * 0.2

Next, to prepare the context nodes \(v_j\) for each node \(v_i\), we compute random walks initialised from each \(v_i\) up to some length (5 by default). The latter is done via a special function within the Graph class. The nodes \(v_j\) will be later picked from the random walk of \(v_i\).

 In [10]:
random_walks = karate_graph.random_walk()

Negatively sampled nodes \(v_k\) are chosen according to the previously defined probability distribution function \(\mathcal{P}_n(v_k)\) implemented as

 In [11]:
negative_table_parameter = 5
negative_sampling_table = []

for i, nb_v in enumerate(nb_vertices_by_edges):
    negative_sampling_table += (
        [i] * int((nb_v ** (3.0 / 4.0))) * negative_table_parameter
    )

negative_sampling_table = gs.array(negative_sampling_table)

Numerically optimizing the loss function#

Optimising the loss function is performed numerically over the number of epochs. At each iteration, we will compute the gradient of \(L\). Then the graph nodes are moved in the direction pointed by the gradient. The movement of the nodes is performed by following geodesics in the gradient direction. The key to obtain an embedding representing accurately the dataset, is to move the nodes smoothly rather than brutal movements. This is done by tuning the learning rate, such as at each epoch all the nodes made small movements.

A first level loop iterates over the epochs, the table total_loss will record the value of \(L\) at each iteration and help us track the minimization of \(L\).

A second level nested loop iterates over each path in the previously computed random walks. Observing these walks, notice that nodes having many edges appear more often. Such nodes can be considered as important crossroads and will therefore be subject to a greater number of embedding updates. This is one of the main reasons why random walks have proven to be effective in capturing the structure of graphs. The context of each \(v_i\) will be the set of nodes \(v_j\) belonging to the random walk from \(v_i\). The context_size specified earlier will limit the length of the walk to be considered. Similarly, we use the same context_size to limit the number of negative samples. We find \(\phi_i\) from the embeddings array.

A third level nested loop will iterate on each \(v_j\) and \(v_k\). From within, we find \(\phi'_j\) and \(\phi'_k\) then call the loss function to compute the gradient. Then the Riemannian exponential map is applied to find the new value of \(\phi_i\) as we mentioned before.

 In [12]:
for epoch in range(max_epochs):
    total_loss = []
    for path in random_walks:
        for example_index, one_path in enumerate(path):
            context_index = path[
                max(0, example_index - context_size) : min(
                    example_index + context_size, len(path)
                )
            ]
            negative_index = gs.random.randint(
                negative_sampling_table.shape[0], size=(len(context_index), n_negative)
            )
            negative_index = negative_sampling_table[negative_index]

            example_embedding = embeddings[one_path]
            for one_context_i, one_negative_i in zip(context_index, negative_index):
                context_embedding = embeddings[one_context_i]
                negative_embedding = embeddings[one_negative_i]
                l, g_ex = loss(
                    example_embedding,
                    context_embedding,
                    negative_embedding,
                    hyperbolic_manifold,
                )
                total_loss.append(l)

                example_to_update = embeddings[one_path]
                embeddings[one_path] = hyperbolic_manifold.metric.exp(
                    -lr * g_ex, example_to_update
                )
    logging.info(
        "iteration %d loss_value %f", epoch, sum(total_loss, 0) / len(total_loss)
    )
INFO: iteration 0 loss_value 1.819745
INFO: iteration 1 loss_value 1.757333
INFO: iteration 2 loss_value 1.727391
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Plotting results#

Once the max_epochs iterations of epochs is achieved, we can plot the resulting embeddings array and the true labels shown as two colors. At 100 epochs we can see that the two group of nodes with different labels are moving away from each other on the manifold. If one increases the max_epochs, then further separability is achieved.

 In [13]:
import matplotlib.patches as mpatches

colors = {1: "b", 2: "r"}
group_1 = mpatches.Patch(color=colors[1], label="Group 1")
group_2 = mpatches.Patch(color=colors[2], label="Group 2")

circle = visualization.PoincareDisk(coords_type="ball")

fig, ax = plt.subplots(figsize=(8, 8))
ax.axes.xaxis.set_visible(False)
ax.axes.yaxis.set_visible(False)
circle.set_ax(ax)
circle.draw(ax=ax)
for i_embedding, embedding in enumerate(embeddings):
    x = embedding[0]
    y = embedding[1]
    pt_id = i_embedding
    plt.scatter(x, y, c=colors[karate_graph.labels[pt_id][0]], s=150)
    ax.annotate(pt_id, (x, y))

plt.tick_params(which="both")
plt.title("Poincare Ball Embedding of the Karate Club Network")
plt.legend(handles=[group_1, group_2])
plt.show()
../_images/notebooks_13_real_world_applications__graph_embedding_and_clustering_in_hyperbolic_space_36_0.png

In geomstats, several unsupervized clustering algorithms on manifolds are implemented such as \(K\)-means and Expectation-Maximization.

Let us apply \(K\)-means to learn the node belonging of the two groups and see how well we predicted the true labels. Lets first import \(K\)-means

 In [14]:
from geomstats.learning.kmeans import RiemannianKMeans

Set the number of groups to 2.

 In [15]:
n_clusters = 2

Initialize an instance of \(K\)-means.

 In [16]:
kmeans = RiemannianKMeans(
    hyperbolic_manifold,
    n_clusters=n_clusters,
    init="random",
)

Fit the embedded nodes

 In [17]:
kmeans.fit(X=embeddings)
cluster_centers = kmeans.cluster_centers_
labels = kmeans.labels_

And plot the resulting labels provided by \(K\)-means

 In [18]:
colors = ["g", "c", "m"]
circle = visualization.PoincareDisk(coords_type="ball")
fig2, ax2 = plt.subplots(figsize=(8, 8))
circle.set_ax(ax2)
circle.draw(ax=ax2)
ax2.axes.xaxis.set_visible(False)
ax2.axes.yaxis.set_visible(False)
group_1_predicted = mpatches.Patch(color=colors[0], label="Predicted Group 1")
group_2_predicted = mpatches.Patch(color=colors[1], label="Predicted Group 2")
group_centers = mpatches.Patch(color=colors[2], label="Cluster centers")

for i in range(n_clusters):
    for i_embedding, embedding in enumerate(embeddings):
        x = embedding[0]
        y = embedding[1]
        pt_id = i_embedding
        if labels[i_embedding] == 0:
            color = colors[0]
        else:
            color = colors[1]
        plt.scatter(x, y, c=color, s=150)
        ax2.annotate(pt_id, (x, y))

for i_centroid, centroid in enumerate(cluster_centers):
    x = centroid[0]
    y = centroid[1]
    plt.scatter(
        x,
        y,
        c=colors[2],
        marker="*",
        s=150,
    )

plt.title("K-means applied to Karate club embedding")
plt.legend(handles=[group_1_predicted, group_2_predicted, group_centers])
plt.show()
../_images/notebooks_13_real_world_applications__graph_embedding_and_clustering_in_hyperbolic_space_46_0.png

By comparing the \(K\)-means labels and the true labels, notice how \(K\)-means accurately finds the two groups of nodes (not perfectly, e.g., nodes 2 and 8). We therefore achieved good performances in predicting the belonging of each member of the Karate club to one of the two groups.

References#

[ABY2013]

Arnaudon, Marc, Frédéric Barbaresco, and Le Yang. “Riemannian medians and means with applications to radar signal processing.” IEEE Journal of Selected Topics in Signal Processing 7.4 (2013): 595-604.

[GBH2018]

Ganea, Octavian, Gary Bécigneul, and Thomas Hofmann. “Hyperbolic neural networks.” Advances in neural information processing systems. 2018.

[M2013]

Mikolov, Tomas, et al. “Distributed representations of words and phrases and their compositionality.” Advances in neural information processing systems. 2013.

[ND2017]

Nickel, Maximillian, and Douwe Kiela. “Poincaré embeddings for learning hierarchical representations.” Advances in neural information processing systems. 2017.