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\chapter{\tr{Maximum likelihood estimation}{Maximum-Likelihood-Sch\"atzer}}
\label{maximumlikelihoodchapter}
A common problem in statistics is to estimate from a probability
distribution one or more parameters $\theta$ that best describe the
data $x_1, x_2, \ldots x_n$. \enterm{Maximum likelihood estimators}
(\enterm[mle|see{Maximum likelihood estimators}]{mle},
\determ{Maximum-Likelihood-Sch\"atzer}) choose the parameters such
that they maximize the likelihood of the data $x_1, x_2, \ldots x_n$
to originate from the distribution.
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\section{Maximum Likelihood}
Let $p(x|\theta)$ (to be read as ``probability(density) of $x$ given
$\theta$.'') the probability (density) distribution of $x$ given the
parameters $\theta$. This could be the normal distribution
\begin{equation}
\label{normpdfmean}
p(x|\mu, \sigma) = \frac{1}{\sqrt{2\pi \sigma^2}}e^{-\frac{(x-\mu)^2}{2\sigma^2}}
\end{equation}
defined by the mean $\mu$ and the standard deviation $\sigma$ as
parameters $\theta$. If the $n$ independent observations of $x_1,
x_2, \ldots x_n$ originate from the same probability density
distribution (they are \enterm{i.i.d.} independent and identically
distributed) then the conditional probability $p(x_1,x_2, \ldots
x_n|\theta)$ of observing $x_1, x_2, \ldots x_n$ given a specific
$\theta$ is given by
\begin{equation}
p(x_1,x_2, \ldots x_n|\theta) = p(x_1|\theta) \cdot p(x_2|\theta)
\ldots p(x_n|\theta) = \prod_{i=1}^n p(x_i|\theta) \; .
\end{equation}
Vice versa, the \enterm{likelihood} of the parameters $\theta$
given the observed data $x_1, x_2, \ldots x_n$ is
\begin{equation}
{\cal L}(\theta|x_1,x_2, \ldots x_n) = p(x_1,x_2, \ldots x_n|\theta) \; .
\end{equation}
Note: the likelihood ${\cal L}$ is not a probability in the
classic sense since it does not integrate to unity ($\int {\cal
L}(\theta|x_1,x_2, \ldots x_n) \, d\theta \ne 1$).
When applying maximum likelihood estimations we are interested in the
parameter values
\begin{equation}
\theta_{mle} = \text{argmax}_{\theta} {\cal L}(\theta|x_1,x_2, \ldots x_n)
\end{equation}
that maximize the likelihood. $\text{argmax}_xf(x)$ is the value of
the argument $x$ of the function $f(x)$ for which the function $f(x)$
assumes its global maximum. Thus, we search for the value of $\theta$
at which the likelihood ${\cal L}(\theta)$ reaches its maximum.
The position of a function's maximum does not change when the values
of the function are transformed by a strictly monotonously rising
function such as the logarithm. For numerical and reasons that we will
discuss below, we commonly search for the maximum of the logarithm of
the likelihood (\enterm{log-likelihood}):
\begin{eqnarray}
\theta_{mle} & = & \text{argmax}_{\theta}\; {\cal L}(\theta|x_1,x_2, \ldots x_n) \nonumber \\
& = & \text{argmax}_{\theta}\; \log {\cal L}(\theta|x_1,x_2, \ldots x_n) \nonumber \\
& = & \text{argmax}_{\theta}\; \log \prod_{i=1}^n p(x_i|\theta) \nonumber \\
& = & \text{argmax}_{\theta}\; \sum_{i=1}^n \log p(x_i|\theta) \label{loglikelihood}
\end{eqnarray}
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\subsection{Example: the arithmetic mean}
Suppose that the measurements $x_1, x_2, \ldots x_n$ originate from a
normal distribution \eqnref{normpdfmean} and we consider the mean
$\mu$ as the only parameter $\theta$. Which value of $\theta$
maximizes the likelihood of the data?
\begin{figure}[t]
\includegraphics[width=1\textwidth]{mlemean}
\titlecaption{\label{mlemeanfig} Maximum likelihood estimation of
the mean.}{Top: The measured data (blue dots) together with three
different possible normal distributions with different means
(arrows) the data could have originated from. Bottom left: the
likelihood as a function of $\theta$ i.e. the mean. It is maximal
at a value of $\theta = 2$. Bottom right: the
log-likelihood. Taking the logarithm does not change the position
of the maximum.}
\end{figure}
The log-likelihood \eqnref{loglikelihood}
\begin{eqnarray*}
\log {\cal L}(\theta|x_1,x_2, \ldots x_n)
& = & \sum_{i=1}^n \log \frac{1}{\sqrt{2\pi \sigma^2}}e^{-\frac{(x_i-\theta)^2}{2\sigma^2}} \\
& = & \sum_{i=1}^n - \log \sqrt{2\pi \sigma^2} -\frac{(x_i-\theta)^2}{2\sigma^2} \; .
\end{eqnarray*}
Since the logarithm is the inverse function of the exponential
($\log(e^x)=x$), taking the logarithm removes the exponential from the
normal distribution. To calculate the maximum of the log-likelihood,
we need to take the derivative with respect to $\theta$ and set it to
zero:
\begin{eqnarray*}
\frac{\text{d}}{\text{d}\theta} \log {\cal L}(\theta|x_1,x_2, \ldots x_n) & = & \sum_{i=1}^n - \frac{2(x_i-\theta)}{2\sigma^2} \;\; = \;\; 0 \\
\Leftrightarrow \quad \sum_{i=1}^n x_i - \sum_{i=1}^n \theta & = & 0 \\
\Leftrightarrow \quad n \theta & = & \sum_{i=1}^n x_i \\
\Leftrightarrow \quad \theta & = & \frac{1}{n} \sum_{i=1}^n x_i \;\; = \;\; \bar x
\end{eqnarray*}
Thus, the maximum likelihood estimator is the arithmetic mean. That
is, the arithmetic mean maximizes the likelihood that the data
originate from a normal distribution centered at the arithmetic mean
(\figref{mlemeanfig}). Equivalently, the standard deviation computed
from the data, maximizes the likelihood that the data were generated
from a normal distribution with this standard deviation.
\begin{exercise}{mlemean.m}{mlemean.out}
Draw $n=50$ random numbers from a normal distribution with a mean of
$\ne 0$ and a standard deviation of $\ne 1$.
Plot the likelihood (the product of the probabilities) and the
log-likelihood (given by the sum of the logarithms of the
probabilities) for the mean as parameter. Compare the position of
the maxima with the mean calculated from the data.
\end{exercise}
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\section{Fitting probability distributions}
Consider normally distributed data with unknown mean and standard
deviation. From the considerations above we just have seen that a
Gaussian distribution with mean at the arithmetic mean and standard
deviation equal to the standard deviation computed from the data is
the best Gaussian distribution that fits the data best in a maximum
likelihood sense, i.e. the likelihood that the data were generated
from this distribution is the largest. Fitting a Gaussian distribution
to data is very simple: just compute the two parameter of the Gaussian
distribution as the arithmetic mean and a standard deviation directly
from the data.
For non-Gaussian distributions (e.g. a Gamma-distribution), however,
such simple analytical expressions for the parameters of the
distribution do not exist, e.g. the shape parameter of a
\enterm{Gamma-distribution}. How do we fit such a distribution to
some data? That is, how should we compute the values of the parameters
of the distribution, given the data?
A first guess could be to fit the probability density function by
minimization of the squared difference to a histogram of the measured
data. For several reasons this is, however, not the method of choice:
(i) Probability densities can only be positive which leads, for small
values in particular, to asymmetric distributions. (ii) The values of
a histogram estimating the density are not independent because the
integral over a density is unity. The two basic assumptions of
normally distributed and independent samples, which are a prerequisite
make the minimization of the squared difference \eqnref{chisqmin} to a
maximum likelihood estimation, are violated. (iii) The histogram
strongly depends on the chosen bin size \figref{mlepdffig}).
\begin{figure}[t]
\includegraphics[width=1\textwidth]{mlepdf}
\titlecaption{\label{mlepdffig} Maximum likelihood estimation of a
probability density.}{Left: the 100 data points drawn from a 2nd
order Gamma-distribution. The maximum likelihood estimation of the
probability density function is shown in orange, the true pdf is
shown in red. Right: normalized histogram of the data together
with the real (red) and the fitted probability density
functions. The fit was done by minimizing the squared difference
to the histogram.}
\end{figure}
Instead we should stay with maximum-likelihood estimation. Exactly in
the same way as we estimated the mean value of a Gaussian distribution
above, we can numerically fit the parameter of any type of
distribution directly from the data by means of maximizing the
likelihood. We simply search for the parameter $\theta$ of the
desired probability density function that maximizes the
log-likelihood. In general this is a non-linear optimization problem
that is solved with numerical methods such as the gradient descent
\matlabfun{mle()}.
\begin{exercise}{mlegammafit.m}{mlegammafit.out}
Generate a sample of gamma-distributed random numbers and apply the
maximum likelihood method to estimate the parameters of the gamma
function from the data.
\end{exercise}
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\section{Curve fitting}
When fitting a function of the form $f(x;\theta)$ to data pairs
$(x_i|y_i)$ one tries to adapt the parameter $\theta$ such that the
function best describes the data. With maximum likelihood we search
for the parameter value $\theta$ for which the likelihood that the data
were drawn from the corresponding function is maximal. If we assume
that the $y_i$ values are normally distributed around the function
values $f(x_i;\theta)$ with a standard deviation $\sigma_i$, the
log-likelihood is
\begin{eqnarray*}
\log {\cal L}(\theta|(x_1,y_1,\sigma_1), \ldots, (x_n,y_n,\sigma_n))
& = & \sum_{i=1}^n \log \frac{1}{\sqrt{2\pi \sigma_i^2}}e^{-\frac{(y_i-f(x_i;\theta))^2}{2\sigma_i^2}} \\
& = & \sum_{i=1}^n - \log \sqrt{2\pi \sigma_i^2} -\frac{(y_i-f(x_i;\theta))^2}{2\sigma_i^2} \\
\end{eqnarray*}
The only difference to the previous example is that the averages in
the equations above are now given as the function values
$f(x_i;\theta)$. The parameter $\theta$ should be the one that
maximizes the log-likelihood. The first part of the sum is independent
of $\theta$ and can thus be ignored when computing the the maximum:
\begin{eqnarray*}
& = & - \frac{1}{2} \sum_{i=1}^n \left( \frac{y_i-f(x_i;\theta)}{\sigma_i} \right)^2
\end{eqnarray*}
We can further simplify by inverting the sign and then search for the
minimum. Also the factor $1/2$ can be ignored since it does not affect
the position of the minimum:
\begin{equation}
\label{chisqmin}
\theta_{mle} = \text{argmin}_{\theta} \; \sum_{i=1}^n \left( \frac{y_i-f(x_i;\theta)}{\sigma_i} \right)^2 \;\; = \;\; \text{argmin}_{\theta} \; \chi^2
\end{equation}
The sum of the squared differences normalized by the standard
deviation is also called $\chi^2$. The parameter $\theta$ which
minimizes the squared differences is thus the one that maximizes the
likelihood that the data actually originate from the given
function. Minimizing $\chi^2$ therefore is a maximum likelihood
estimation.
From the mathematical considerations above we can see that the
minimization of the squared difference is a maximum-likelihood
estimation only if the data are normally distributed around the
function. In case of other distributions, the log-likelihood
\eqnref{loglikelihood} needs to be adapted accordingly and be
maximized respectively.
\begin{figure}[t]
\includegraphics[width=1\textwidth]{mlepropline}
\titlecaption{\label{mleproplinefig} Maximum likelihood estimation
of the slope of line through the origin.}{The data (blue and
left histogram) originate from a straight line $y=mx$ trough the origin
(red). The maximum-likelihood estimation of the slope $m$ of the
regression line (orange), \eqnref{mleslope}, is close to the true
one. The residuals, the data minus the estimated line (right), reveal
the normal distribution of the data around the line (right histogram).}
\end{figure}
\subsection{Example: simple proportionality}
The function of a line with slope $\theta$ through the origin is
\[ f(x) = \theta x \; . \]
The $\chi^2$-sum is thus
\[ \chi^2 = \sum_{i=1}^n \left( \frac{y_i-\theta x_i}{\sigma_i} \right)^2 \; . \]
To estimate the minimum we again take the first derivative with
respect to $\theta$ and equate it to zero:
\begin{eqnarray}
\frac{\text{d}}{\text{d}\theta}\chi^2 & = & \frac{\text{d}}{\text{d}\theta} \sum_{i=1}^n \left( \frac{y_i-\theta x_i}{\sigma_i} \right)^2 \nonumber \\
& = & \sum_{i=1}^n \frac{\text{d}}{\text{d}\theta} \left( \frac{y_i-\theta x_i}{\sigma_i} \right)^2 \nonumber \\
& = & -2 \sum_{i=1}^n \frac{x_i}{\sigma_i} \left( \frac{y_i-\theta x_i}{\sigma_i} \right) \nonumber \\
& = & -2 \sum_{i=1}^n \left( \frac{x_i y_i}{\sigma_i^2} - \theta \frac{x_i^2}{\sigma_i^2} \right) \;\; = \;\; 0 \nonumber \\
\Leftrightarrow \quad \theta \sum_{i=1}^n \frac{x_i^2}{\sigma_i^2} & = & \sum_{i=1}^n \frac{x_i y_i}{\sigma_i^2} \nonumber
\end{eqnarray}
\begin{eqnarray}
\Leftrightarrow \quad \theta & = & \frac{\sum_{i=1}^n \frac{x_i y_i}{\sigma_i^2}}{ \sum_{i=1}^n \frac{x_i^2}{\sigma_i^2}} \label{mleslope}
\end{eqnarray}
This is an analytical expression for the estimation of the slope
$\theta$ of the regression line (\figref{mleproplinefig}).
A gradient descent, as we have done in the previous chapter, is not
necessary for fitting the slope of a straight line, because the slope
can be directly computed via \eqnref{mleslope}. More generally, this
is the case also for fitting the coefficients of linearly combined
basis functions as for example the slope $m$ and the y-intercept $b$
of a straight line
\[ y = m \cdot x +b \]
or the coefficients $a_k$ of a polynomial
\[ y = \sum_{k=0}^N a_k x^k = a_o + a_1x + a_2x^2 + a_3x^4 + \ldots \]
\matlabfun{polyfit()}.
Parameters that are non-linearly combined can not be calculated
analytically. Consider for example the rate $\lambda$ of the
exponential decay
\[ y = c \cdot e^{\lambda x} \quad , \quad c, \lambda \in \reZ \; . \]
Such cases require numerical solutions for the optimization of the
cost function, e.g. the gradient descent \matlabfun{lsqcurvefit()}.
Let us have a closer look on \eqnref{mleslope}. If the standard
deviation of the data $\sigma_i$ is the same for each data point,
i.e. $\sigma_i = \sigma_j \; \forall \; i, j$, the standard deviation drops
out of \eqnref{mleslope} and we get
\begin{equation}
\label{whitemleslope}
\theta = \frac{\sum_{i=1}^n x_i y_i}{\sum_{i=1}^n x_i^2}
\end{equation}
To see what this expression is, we need to standardize the data. We
make the data mean free and normalize them to their standard
deviation, i.e. $x \mapsto (x - \bar x)/\sigma_x$. The resulting
numbers are also called \enterm{$z$-values} or $z$-scores and they
have the property $\bar x = 0$ and $\sigma_x = 1$. $z$-scores are
often used in Biology to make quantities that differ in their units
comparable. For standardized data the variance
\[ \sigma_x^2 = \frac{1}{n} \sum_{i=1}^n (x_i - \bar x)^2 = \frac{1}{n} \sum_{i=1}^n x_i^2 = 1 \]
is given by the mean squared data and equals one.
The covariance between $x$ and $y$ also simplifies to
\[ \text{cov}(x, y) = \frac{1}{n} \sum_{i=1}^n (x_i - \bar x)(y_i -
\bar y) =\frac{1}{n} \sum_{i=1}^n x_i y_i \]
the averaged product between pairs of $x$ and $y$ values. Recall that
the correlation coefficient $r_{x,y}$,
\eqnref{correlationcoefficient}, is the covariance normalized by the
product of the standard deviations of $x$ and $y$,
respectively. Therefore, in case the standard deviations equal one,
the correlation coefficient equals the covariance. Consequently, for
standardized data the slope of the regression line
\eqnref{whitemleslope} simplifies to
\begin{equation}
\theta = \frac{1}{n} \sum_{i=1}^n x_i y_i = \text{cov}(x,y) = r_{x,y}
\end{equation}
For standardized data the slope of the regression line equals the
correlation coefficient!
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\section{Neural coding}
In sensory systems certain aspects of the environment are encoded in
the neuronal activity of populations of neurons. One example of such a
population code is the tuning of neurons in the primary visual cortex
(V1) to the orientation of an edge or bar in the visual
stimulus. Different neurons respond best to different edge
orientations. Traditionally, such a tuning is measured by analyzing
the neuronal response strength (e.g. the firing rate) as a function of
the orientation of a black bar and is illustrated and summarized
with the so called \enterm{tuning-curve} (\determ{Abstimmkurve},
figure~\ref{mlecodingfig}, top).
\begin{figure}[tp]
\includegraphics[width=1\textwidth]{mlecoding}
\titlecaption{\label{mlecodingfig} Maximum likelihood estimation of
a stimulus parameter from neuronal activity.}{Top: Tuning curve of
an individual neuron as a function of the stimulus orientation (a
dark bar in front of a white background). The stimulus that evokes
the strongest activity in that neuron is the bar with the vertical
orientation (arrow, $\phi_i=90$\,\degree). The red area indicates
the variability of the neuronal activity $p(r|\phi)$ around the
tuning curve. Center: In a population of neurons, each neuron may
have a different tuning curve (colors). A specific stimulus (the
vertical bar) activates the individual neurons of the population
in a specific way (dots). Bottom: The log-likelihood of the
activity pattern will be maximized close to the real stimulus
orientation.}
\end{figure}
The brain, however, is confronted with the inverse problem: given a
certain activity pattern in the neuronal population, what is the
stimulus (here the orientation of an edge)? In the sense of maximum
likelihood, a possible answer to this question would be: the stimulus
for which the particular activity pattern is most likely given the
tuning of the neurons.
Let's stay with the example of the orientation tuning in V1. The
tuning $\Omega_i(\phi)$ of the neurons $i$ to the preferred edge
orientation $\phi_i$ can be well described using a van-Mises function
(the Gaussian function on a cyclic x-axis) (\figref{mlecodingfig}):
\[ \Omega_i(\phi) = c \cdot e^{\cos(2(\phi-\phi_i))} \quad , \quad c \in \reZ \]
If we approximate the neuronal activity by a normal distribution
around the tuning curve with a standard deviation $\sigma=\Omega/4$,
which is proportional to $\Omega$, then the probability $p_i(r|\phi)$
of the $i$-th neuron showing the activity $r$ given a certain
orientation $\phi$ of an edge is given by
\[ p_i(r|\phi) = \frac{1}{\sqrt{2\pi}\Omega_i(\phi)/4} e^{-\frac{1}{2}\left(\frac{r-\Omega_i(\phi)}{\Omega_i(\phi)/4}\right)^2} \; . \]
The log-likelihood of the edge orientation $\phi$ given the
activity pattern in the population $r_1$, $r_2$, ... $r_n$ is thus
\[ {\cal L}(\phi|r_1, r_2, \ldots r_n) = \sum_{i=1}^n \log p_i(r_i|\phi) \]
The angle $\phi$ that maximizes this likelihood is then an estimate of
the orientation of the edge.