Show that
\begin{eqnarray*}
c_{1} &=& m_{1}=\mu \\
c_{2} &=& m_{2} - m_{1}^{2}=\sigma^{2}.
\end{eqnarray*}
That is, show that the first and second cumulants of a distribution are equal to the mean ($\mu$) and variance ($\sigma^{2}$), respectively.
Proof:
The $n$th moment of a continuous distribution, $m_{n}$ is defined as:
\begin{eqnarray*}
m_{n} &=& E[x^{n}]\\
&=& \int_{-\infty}^{\infty}x^{n}p\left(x\right)\,dx.
\end{eqnarray*}
A function that generates any moment is called a moment-generating function and is defined as $$E[e^{tX}].$$ where $X$ is a random variable and $E[f\left(X\right)]$ is the expected value of a function, $f$, of a random variable $X$.
If we expand the definition of $E[e^{tX}]$ we can see that
\begin{eqnarray*}
E[e^{tX}] &=&
\int_{-\infty}^{\infty}p\left(X\right)\left(\sum_{n=0}^{\infty}\frac{t^{n}X^{n}}{n!}\right)\,\,\mathrm{d}x\\
&=& \int_{-\infty}^{\infty}p\left(X\right)\left(1 + tX + \frac{t^{2}X^{2}}{2!} + \cdots +
\frac{t^{n}X^{n}}{n!}\right)\,\,\mathrm{d}x\\
&=& 1 + tm_{1} + \frac{t^{2}m_{2}}{2!} + \cdots + \frac{t^{n}m_{n}}{n!}.
\end{eqnarray*}
If we evaluate the $n$th derivative of $E[e^{tX}]$ with respect to $t$ at $t=0$, that is, $$\left(\frac{\mathrm{d}^{n}}{\mathrm{d}t^{n}}E[e^{tX}]\right)_{t=0} =
\frac{\mathrm{d}^{n}}{\mathrm{d}t^{n}}\left(m_{0} + tm_{1} +
\frac{t^{2}m_{2}}{2!} + \cdots + \frac{t^{n}m_{n}}{n!}\right)$$ we get the $n$th moment of a probability distribution.
The $n$th cumulant, $c_{n}$, of a continuous distribution is defined as:
$$\ln\left(E[e^{tX}]\right).$$
Since the power series definition of the natural logarithm of $x$ is
$$\ln\left(x\right) = \sum_{n=1}^{\infty}\frac{\left(-1\right)^{n+1}}{n}\left(x - 1\right)^{n},$$
we can rewrite the definition of the $n$th cumulant, $c_{n}$, as
\begin{eqnarray*}
\ln\left(E[e^{tX}]\right) &=&
\sum_{n=1}^{\infty}\frac{\left(-1\right)^{n+1}}{n}\left(tm_{1} +
\frac{t^{2}m_{2}}{2!} + \cdots\right)^{n}
\end{eqnarray*}
Expanding the terms from the previous equation we see that,
\begin{eqnarray*}
\ln\left(E[e^{tX}]\right) &=& \left(tm_{1} +
\frac{t^{2}m_{2}}{2!} + \cdots\right) - \frac{1}{2}\left(tm_{1} +
\frac{t^{2}m_{2}}{2!} + \cdots\right)^{2} + \cdots\\
&=&\left(tm_{1} +
\frac{t^{2}m_{2}}{2!} + \cdots\right)-\frac{1}{2}\left(t^{2}m_{1}^{2}+\frac{t^{3}m_{1}m_{2}}{2}+\cdots\right) + \cdots.
\end{eqnarray*}
Now do a little algebra on the second term of $\ln\left(E[e^{tX}]\right)$ to get
$$\left(tm_{1}+\frac{t^{2}m_{2}}{2!}+\cdots\right)-\frac{t^{2}m_{1}^{2}}{2}-\frac{t^{3}m_{1}m_{2}}{4}+\cdots$$
The first derivative, with respect to $t$, evaluated at 0 gives $m_{1}$. The second derivative evaluated at 0 gives
$$\frac{\mathrm{d}^{2}}{\mathrm{d}t^{2}}\left(\frac{t^{2}m_{2}}{2!}\right) =m_{2}.$$
Then we see that $m_{2} - m_{1}^{2}$ gives the variance.
Thus it is shown that the first two cumulants of a distribution are the mean and variance, respectively.
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