  We have shown that the Landau paradigm based upon both the quasiparticle
concept and the notion of the order parameter can be used to explain the
anomalous behavior of heavy fermion metals. Exploiting this paradigm and the
fermion condensation quantum phase transition (FCQPT) we show that this
anomalous behavior is universal and can be used to capture the essential
aspects of recent experiments on the heavy-fermion metals at low temperatures.
Behind FCQPT a tunneling conductivity between a heavy fermion metal and a
simple metallic point can be noticeably dissymmetrical with respect to the
change of voltage bias. We show that at T=0 and beyond FCQPT the Hall
coefficient undergoes a jump upon magnetic-field tuning HF metals.
