Measures of dissimilarities

Classical distances

A distance function or metric a on the space \(\mathbb{R}^n,\:n\geq 1\), is a function \(d:\mathbb{R}^n\times\mathbb{R}^n\rightarrow \mathbb{R}\). It must satisfy some required axioms.

P1. \(d(\mathbf{x},\mathbf{y})= 0\iff \mathbf{x}=\mathbf{y}\) (identity of indiscernibles);

P2. \(d(\mathbf{x},\mathbf{y})= d(\mathbf{y},\mathbf{x})\) (symmetry);

P3. \(d(\mathbf{x},\mathbf{y})+d(\mathbf{y},\mathbf{z})\geq d(\mathbf{x},\mathbf{z})\) (triangle inequality),

where \(\mathbf{x}=(x_1,\cdots,x_n)\), \(\mathbf{y}=(y_1,\cdots,y_n)\) and \(\mathbf{z}=(z_1,\cdots,z_n)\) are any three vectors of \(\mathbb{R}^n\).

Exercice 2: Pove that these three axioms imply the non-negativity condition: \(d(\mathbf{x},\mathbf{y})\geq 0\).

We should use the term dissimilarity instead of distance when not all mathematical axioms for distances, that is P1-P3, are valid.

Let us recall and introduce some useful metrics:

Euclidean distance:

\[d(\mathbf{x},\mathbf{y})=\sqrt{\sum_{i=1}^n (x_i-y_i)^2}.\]

Manhattan distance:

\[d(\mathbf{x},\mathbf{y}) =\sum_{i=1}^n |x_i-y_i|.\]

There exists also a weighted version of the above distance given by:

Canberra distance:

\[d(\mathbf{x},\mathbf{y}) =\sum_{i=1}^n \frac{|x_i-y_i|}{|x_i|+|y_i|}.\]

Note that the term \(|x_i−y_i|/(|x_i|+|y_i|)\) needs to be replaced by zero if both \(x_i\) and \(y_i\) are zero and that the Canberra distance is specially sensitive to small changes near zero.

Exercice 2: Prove that the Canberra distance is a true distance.

Both the Euclidian and Manattan distances are special cases of the Minkowski distance which is now defined:

Minkowski distance:

\[d(\mathbf{x},\mathbf{y}) \left[\sum_{i=1} |x_i-y_i|{p}\right]^{1/p}, \]

Let also us define: \[\|\mathbf{x}\|_p\equiv\left[\sum_{i=1}^n |x_i|^{p}\right]^{1/p},\: p\geq 1,\] where \(\|\mathbf{\cdot}\|_p\) is known as the p-norm or Minkowski norm. Note that the Minkowski distance can be defined as follows: \[ d(\mathbf{x},\mathbf{y})=\|\mathbf{x}-\mathbf{y}\|_p,\:p\geq 1. \] The proof of the triangular inequality P3 is based on the Minkowski inequality which states that for any nonnegative real numbers \(a_1,\cdots,a_n\); \(b_1,\cdots,b_n\), we have:

\[ \left[\sum_{i=1}^n (a_i+b_i)^{p}\right]^{1/p}\leq \left[\sum_{i=1}^n a_i^{p}\right]^{1/p} + \left[\sum_{i=1}^n b_i^{p}\right]^{1/p},\:p\geq 1. \] To prove that the Minkowski distance satisfies P3, notice that

\[ \sum_{i=1}^n|x_i-z_i|^{p}= \sum_{i=1}^n|(x_i-y_i)+(y_i-z_i)|^{p}. \] Noticing then that for any reals \(x,y\), we have \(|x+y|\leq |x|+|y|\), and using the fact that \(a^p\) is increasing in \(a>0\), we obtain

\[ \sum_{i=1}^n|x_i-z_i|^{p}\leq \sum_{i=1}^n(|x_i-y_i|+|y_i-z_i|)^{p}. \] Applying then the Minkowski inequality to the RHS of the above inequality by posing \(a_i=|x_i-y_i|\) and \(b_i=|y_i-z_i|\), \(i=1,\cdots,n\), we get \[ \sum_{i=1}^n|x_i-z_i|^{p}\leq \left(\sum_{i=1}^n |x_i-y_i|^{p}\right)^{1/p}+\left(\sum_{i=1}^n |y_i-z_i|^{p}\right)^{1/p}. \]

The proof of the Minkowski inequality itself requires the Hölder inequality which states that for any nonnegative real numbers \(a_1,\cdots,a_n\); \(b_1,\cdots,b_n\), and any \(p,q>1\) with \(1/p+1/q=1\), we have

\[ \sum_{i=1}^n a_ib_i\leq \left[\sum_{i=1}^n a_i^{p}\right]^{1/p} \left[\sum_{i=1}^n b_i^{q}\right]^{1/q} \] The proof of the above displayed Hölder inequality relies on the Young’s inequality: For any \(a,b>0\) we have \[ ab\leq \frac{a^p}{p}+\frac{b^q}{q}, \] with equality occuring iff: \(a^p=b^q\). To prove the Young’s inequality, one can use the (strict) convexity of the exponential function which tels us that for any reals \(x,y\), then

\[ e^{\frac{x}{p}+\frac{y}{q} }\leq \frac{e^{x}}{p}+\frac{e^{y}}{q}. \] We then set \(x=p\ln a\) and \(y=q\ln b\) to get the Young’s inequality. A good reference on the inequalities topic is: Z. Cvetkovski, Inequalities: theorems, techniques and selected problems, 2012, Springer Science & Business Media.

Note that the triangular inequality for the Minkowski distance implies

\[ \sum_{i=1}^n |x_i|\leq \left[\sum_{i=1}^n |x_i|^{p}\right]^{1/p} ,\:p\geq 1. \]

Note that for \(p=2\), we have \(q=2\). The Hölder inequality implies for that special case \[ \sum_{i=1}^n|x_iy_i|\leq\sqrt{\sum_{i=1}^n x_i^2}\sqrt{\sum_{i=1}^n y_i^2}. \]

Since the LHS od thes above inequality is greater then \(|\sum_{i=1}^nx_iy_i|\), we get the Cauchy-Schwartz inequality \[ |\sum_{i=1}^nx_iy_i|\leq\sqrt{\sum_{i=1}^n x_i^2}\sqrt{\sum_{i=1}^n y_i^2}. \] Using the dot product noation called also scalar product noation \(\mathbf{x\cdot y}=\sum_{i=1}^nx_iy_i\), and the norm notation \(\|\mathbf{\cdot}\|_2 \|\), the Cauchy-Schwart inequality is:

\[|\mathbf{x\cdot y} | \leq \|\mathbf{x}\|_2 \| \mathbf{y}\|_2 \]

Correlation-based distances;

Cosine correlation distance.

The cosine of the angle \(\theta\) between two vectors \(\mathbf{x}\) and \(\mathbf{y}\) is a measure of similarity given by: \[ \cos(\theta)=\frac{\mathbf{x}\cdot \mathbf{y}}{\|\mathbf{x}\|_2\|\mathbf{y}\|_2}=\frac{\sum_{i=1}^n x_i y_i}{{\sqrt{\sum_{i=1}^n x_i^2\sum_{i=1}^n y_i^2}}}. \] Note that the cosine of the angle between the two centred vectors \((x_1-\bar{\mathbf{x}},\cdots,x_n-\bar{\mathbf{x}})\) and \((y_1-\bar{\mathbf{y}},\cdots,y_n-\bar{\mathbf{y}})\) coincides with the Pearson correlation coefficient of \(\mathbf{x}\) and \(\mathbf{y}\).

The cosine correlation distance is defined by: \[ d(\mathbf{x},\mathbf{y})=1-\cos(\theta). \] It shares similar properties than the Pearson correlation distance. Likewise, Axioms P1 and P3 are not satisfied.

Spearman correlation distance

To calculate the Spearman rank-order correlation or Spearman correlation coefficient for short, we need to map seperately each of the vectors to ranked data values: \(\mathbf{x}\rightarrow \mathbf{x}^r=(x_1^r,\cdots,x_n^r)\). Here, \(x_i^r\) is the rank of \(x_i\) among the set of values of \(\mathbf{x}\). We illustrate this transformation with a simple example. If \(\mathbf{x}=(3, 1, 4, 15, 92)\), then the rank-order vector is \(\mathbf{x}^r=(2,1,3,4,5)\).

x=c(3, 1, 4, 15, 92)
rank(x)

The Spearman correlation of two numerical variables \(\mathbf{x}\) and \(\mathbf{y}\) is simply the Pearson correlation of the two correspnding rank-oerder variables \(\mathbf{x}^r\) and \(\mathbf{y}^r\), i.e. \(\rho(\mathbf{x}^r,\mathbf{y}^r)\). This measure is is useful because it is more robust against outliers than the Pearson correlation. The spearman distance is then defined by: \[ d(\mathbf{x},\mathbf{y})=1-\rho(\mathbf{x^r},\mathbf{y^r}).\]

Kendall correlation distance


---
title: "Cluster Analysis"
output: 
  html_notebook: 
    toc: yes
---



# Measures of dissimilarities


## Classical distances

A distance function or metric a on the space $\mathbb{R}^n,\:n\geq 1$, is a function $d:\mathbb{R}^n\times\mathbb{R}^n\rightarrow \mathbb{R}$. It must satisfy some required axioms. 

P1. $d(\mathbf{x},\mathbf{y})= 0\iff \mathbf{x}=\mathbf{y}$ (identity of indiscernibles);

P2. $d(\mathbf{x},\mathbf{y})= d(\mathbf{y},\mathbf{x})$ (symmetry);

P3. $d(\mathbf{x},\mathbf{y})+d(\mathbf{y},\mathbf{z})\geq d(\mathbf{x},\mathbf{z})$ (triangle inequality),

where $\mathbf{x}=(x_1,\cdots,x_n)$, $\mathbf{y}=(y_1,\cdots,y_n)$ and $\mathbf{z}=(z_1,\cdots,z_n)$ are any three vectors of $\mathbb{R}^n$.

**Exercice 2:** Pove that these three axioms imply the non-negativity condition: $d(\mathbf{x},\mathbf{y})\geq 0$.

We should use the term dissimilarity instead of distance when not all mathematical axioms for distances, that is P1-P3, are valid.

Let us recall and introduce some useful metrics:
 
### Euclidean distance:

$$d(\mathbf{x},\mathbf{y})=\sqrt{\sum_{i=1}^n (x_i-y_i)^2}.$$

### Manhattan distance:

$$d(\mathbf{x},\mathbf{y})
=\sum_{i=1}^n |x_i-y_i|.$$

There exists also a  weighted version  of the above distance given by:


### Canberra distance:

$$d(\mathbf{x},\mathbf{y})
=\sum_{i=1}^n \frac{|x_i-y_i|}{|x_i|+|y_i|}.$$

Note that the term $|x_i−y_i|/(|x_i|+|y_i|)$ needs to be replaced by zero if both $x_i$ and $y_i$ are zero and that the Canberra distance is specially sensitive to small changes near zero.

**Exercice 2:** Prove that the Canberra distance is a true distance.

Both the Euclidian and Manattan distances are special cases of the Minkowski distance which is now defined:

### Minkowski distance: 

$$d(\mathbf{x},\mathbf{y})
\left[\sum_{i=1} |x_i-y_i|{p}\right]^{1/p},
$$



Let also us define: 
$$\|\mathbf{x}\|_p\equiv\left[\sum_{i=1}^n |x_i|^{p}\right]^{1/p},\: p\geq 1,$$
where $\|\mathbf{\cdot}\|_p$ is known as the p-norm or Minkowski norm. Note that the Minkowski distance can be defined as follows:
$$
d(\mathbf{x},\mathbf{y})=\|\mathbf{x}-\mathbf{y}\|_p,\:p\geq 1.
$$
The proof of the triangular inequality P3 is based on the Minkowski inequality which states that for any nonnegative real numbers $a_1,\cdots,a_n$; $b_1,\cdots,b_n$, we have:

$$
\left[\sum_{i=1}^n (a_i+b_i)^{p}\right]^{1/p}\leq
\left[\sum_{i=1}^n a_i^{p}\right]^{1/p}
+
\left[\sum_{i=1}^n b_i^{p}\right]^{1/p},\:p\geq 1.
$$
To prove that the Minkowski distance satisfies P3, notice that 

$$
 \sum_{i=1}^n|x_i-z_i|^{p}= \sum_{i=1}^n|(x_i-y_i)+(y_i-z_i)|^{p}.
$$
Noticing then that for any reals $x,y$, we have $|x+y|\leq |x|+|y|$, and using the fact that $a^p$ is increasing in $a>0$, we obtain

$$
 \sum_{i=1}^n|x_i-z_i|^{p}\leq \sum_{i=1}^n(|x_i-y_i|+|y_i-z_i|)^{p}.
$$
Applying then the Minkowski inequality to the RHS of the above inequality by posing $a_i=|x_i-y_i|$ and $b_i=|y_i-z_i|$, $i=1,\cdots,n$, we get
$$
 \sum_{i=1}^n|x_i-z_i|^{p}\leq \left(\sum_{i=1}^n |x_i-y_i|^{p}\right)^{1/p}+\left(\sum_{i=1}^n |y_i-z_i|^{p}\right)^{1/p}.
$$

The proof of the Minkowski inequality itself requires the Hölder inequality which states that for any nonnegative real numbers $a_1,\cdots,a_n$; $b_1,\cdots,b_n$, and any $p,q>1$ with $1/p+1/q=1$, we have

$$
\sum_{i=1}^n a_ib_i\leq
\left[\sum_{i=1}^n a_i^{p}\right]^{1/p}
\left[\sum_{i=1}^n b_i^{q}\right]^{1/q}
$$
The proof of the above displayed Hölder inequality relies on the Young's  inequality: For any $a,b>0$ we have
$$
ab\leq \frac{a^p}{p}+\frac{b^q}{q},
$$
with equality occuring iff: $a^p=b^q$.  To prove the Young's inequality, one can use the (strict) convexity of the exponential function which tels us that for any reals $x,y$, then 

$$
e^{\frac{x}{p}+\frac{y}{q} }\leq \frac{e^{x}}{p}+\frac{e^{y}}{q}. 
$$
We then set $x=p\ln a$ and $y=q\ln b$ to get the Young's inequality.
 A good reference on the inequalities topic is: Z. Cvetkovski,  Inequalities: theorems, techniques and selected problems, 2012, Springer Science & Business Media.

Note that the triangular inequality for the Minkowski distance implies 

$$
\sum_{i=1}^n |x_i|\leq
\left[\sum_{i=1}^n |x_i|^{p}\right]^{1/p}
,\:p\geq 1.
$$

Note that for $p=2$, we have $q=2$. The Hölder inequality implies for that special case
$$
\sum_{i=1}^n|x_iy_i|\leq\sqrt{\sum_{i=1}^n x_i^2}\sqrt{\sum_{i=1}^n y_i^2}. 
$$

Since the LHS od thes above inequality is greater then $|\sum_{i=1}^nx_iy_i|$, we get the Cauchy-Schwartz inequality
$$
|\sum_{i=1}^nx_iy_i|\leq\sqrt{\sum_{i=1}^n x_i^2}\sqrt{\sum_{i=1}^n y_i^2}. 
$$
Using the dot product noation called also scalar product noation $\mathbf{x\cdot y}=\sum_{i=1}^nx_iy_i$, and the norm notation $\|\mathbf{\cdot}\|_2 \|$, the Cauchy-Schwart inequality is:

$$|\mathbf{x\cdot y} | \leq \|\mathbf{x}\|_2 \| \mathbf{y}\|_2  $$


## Correlation-based distances;

### Pearson correlation and related distances:

The Pearson correlation coefficient is a similarity measure on $\mathbb{R}^n$ defined by:
$$
\rho(\mathbf{x},\mathbf{y})=
\frac{\sum_{i=1}^n (x_i-\bar{\mathbf{x}})(y_i-\bar{\mathbf{y}})}{{\sqrt{\sum_{i=1}^n (x_i-\bar{\mathbf{x}})^2\sum_{i=1}^n (y_i-\bar{\mathbf{y}})^2}}},
$$
where $\bar{\mathbf{x}}$ is the mean of the vector $\mathbf{x}$ defined by: 
$$\bar{\mathbf{x}}=\frac{1}{n}\sum_{i=1}^n x_i,$$

Note that the Pearson correlation coefficient satisfies P2 and  is invariant to any positive linear transformation, i.e.: $\rho(\alpha\mathbf{x},\mathbf{y})=\rho(\mathbf{x},\mathbf{y})$, for any $\alpha>0$.

The Pearson distance (or correlation distance) is defined by:
$$
d(\mathbf{x},\mathbf{y})=1-\rho(\mathbf{x},\mathbf{y}).$$
Note that the Pearson distance does not satisfy $P1$ since $d(\mathbf{x},\mathbf{x})=0$ for any non-zero vector $\mathbf{x}$. It neither satisfies the triangle inequality. However, the symmetry property is fullfilled. 

### Cosine correlation distance.

The cosine of the angle $\theta$ between two vectors $\mathbf{x}$ and $\mathbf{y}$ is a measure of similarity given by:
$$
\cos(\theta)=\frac{\mathbf{x}\cdot \mathbf{y}}{\|\mathbf{x}\|_2\|\mathbf{y}\|_2}=\frac{\sum_{i=1}^n x_i y_i}{{\sqrt{\sum_{i=1}^n x_i^2\sum_{i=1}^n y_i^2}}}.
$$
Note that the cosine of the angle between the two centred vectors $(x_1-\bar{\mathbf{x}},\cdots,x_n-\bar{\mathbf{x}})$ and $(y_1-\bar{\mathbf{y}},\cdots,y_n-\bar{\mathbf{y}})$ coincides with the Pearson correlation coefficient of $\mathbf{x}$ and $\mathbf{y}$.  

The cosine correlation distance is defined by:
$$
d(\mathbf{x},\mathbf{y})=1-\cos(\theta).
$$
It shares similar properties than the Pearson correlation distance. Likewise, Axioms P1 and P3 are not satisfied.


### Spearman correlation distance

To calculate the Spearman rank-order correlation or Spearman correlation coefficient for short, we need to map seperately each of the vectors to ranked data values: $\mathbf{x}\rightarrow \mathbf{x}^r=(x_1^r,\cdots,x_n^r)$. Here, $x_i^r$ is the rank of $x_i$ among the set of values of $\mathbf{x}$. We illustrate this transformation with a simple example. If $\mathbf{x}=(3, 1, 4, 15, 92)$, then the rank-order vector is $\mathbf{x}^r=(2,1,3,4,5)$.  


```{r}
x=c(3, 1, 4, 15, 92)
rank(x)

```

The Spearman correlation of two numerical variables $\mathbf{x}$  and $\mathbf{y}$ is simply the Pearson correlation of the two correspnding rank-oerder variables $\mathbf{x}^r$ and $\mathbf{y}^r$, i.e. $\rho(\mathbf{x}^r,\mathbf{y}^r)$. This measure is is useful because it is more robust against outliers than the Pearson correlation.
 The spearman distance is then defined by:
$$
d(\mathbf{x},\mathbf{y})=1-\rho(\mathbf{x^r},\mathbf{y^r}).$$



 


### Kendall correlation distance

