This is not the answer pal, I understand the graph very well. I'm asking physically, I've just put the graph to illustrate the situation.
I got the answer, for who's interested, I thought it over and got something, if you think the answer is wrong tell me.
We're going to use the definition of chemical potential, that it's the energy required to add a particle to the system.
The Fermi distribution at T=0 is a step function, meaning if we want to add any other electron to the system we need to put it after those levels, meaning we need to insert it after the step function, and so the energy required to add this electron to the system is precisely EF(T=0) (Fermi energy at T=0).
http://www.doitpoms.ac.uk/tlplib/semiconductors/images/fermiDirac.jpg
At higher temperature, the distribution loses the step function profile (as we can see in the link), and therefore adding another electron is possible before EF(T=0) since there are vacancies.
At very high temperatures, kT becomes very large that it dominates over EF(T=0), and therefore without consuming any energy, we can find vacancies for new electrons as in the following figure
http://wpcontent.answers.com/wikipedia/commons/thumb/1/15/FD_e_mu.jpg/360px-FD_e_mu.jpg
and so, continuing to increase temperature makes the system extract heat upon adding electron, in other words we get negative Fermi level or chemical potential. The heat extracted is because the system tries to sustain the Fermi distribution function.
I hope this is right, tell me what you think guys.
Thanks for reading :)