Abstract
The specific heat coefficient and magnetic susceptibility for different concentrations of the heavy fermion alloy are calculated in the slave boson mean-field scheme. The results show that the system undergoes a smooth variation from incoherent dilute limit to the coherent dense limit as the concentration of the alloy increases from zero to unity.
Full Text 
Sign-in/Register to access full text options
Sign-in/Register to access full text options 
Paper version not known
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a call
