I am a student who is writing a little thesis belonged in the applied mathematics category.
I choose a "Levy distribution" defined as, \begin{equation} \lambda(t;u,c) = \begin{cases} \sqrt{\frac{c}{2\pi}}\frac{ e^{-\frac{c} {2(t-u)} }} {(t-u)^{3/2}} & \text{if } t>u \\ 0 & \text{otherwise} \end{cases} \end{equation} to examine the behavior of the variables.
Now I thought I had to apply the MLE to obtain the good estimation of the parameter: $c,u $
However, after calculating the derivative of logarithm of the levy distribution. I obtained only \begin{equation} \frac{d\lambda(t;u,c)} {dc} = \frac{c-t+u} {2ct-2cu} = 0 \iff c = t-u \end{equation} and \begin{equation} \frac{d\lambda(t;u,c)} {du} = -\frac{c-3t+3u} {2(t-u)^{2}} = 0 \iff u = t-\frac{c}{3} \end{equation}
However, both the parameters $c$ and $u$ are dependent on each other. Could somebody suggest me the better method for estimating?
Thank you very much.
Parameter $u$ in your Levy pdf is just a shift parameter that adjusts the lower bound from 0. It is equivalent to the transformation $X = T + u$, where random variable $T$ has pdf $f(t)$:
The following plot illustrates the pdf, as parameter $c$ changes:
From the plot, the lower bound parameter will generally be clearly defined by the data itself (unless parameter $c$ is very large) ... So, the way I would proceed would be to:
a) zero-shift your data so that the lower bound is 0; i.e. newdata = data - min[data]
b) then your problem reduces to finding the MLE of parameter $c$, for the single parameter model.
That can be solved by hand (if you prefer), or get a computer to do the work for you. Here I am using the
mathStaticaadd-on to Mathematica (I am one of the authors of the former).mathStaticahas a specialSuperLogfunction specially designed for formulating log-likelihood problems:Then, for a random sample of size $n$ drawn on $T$, the log-likelihood function is:
The score function is the gradient of the log-likelihood with respect to $c$:
Setting the score to zero and solving for $c$ corresponds to the first-order conditions:
Finally, check the second-order condition, evaluated at
solc:... reveals that the Hessian is strictly negative at the FOC.
Therefore, the MLE of $c$ is:
$$\hat{c}=\frac{n}{\underset{i=1}{\overset{n}{\sum }}\frac{1}{T_i}.}$$