We study the thermodynamic properties associated with the black hole event
horizon and the cosmological horizon for black hole solutions in asymptotically
de Sitter spacetimes. We examine thermodynamics of these horizons on the basis
of the conserved charges according to Teitelboim's method. In particular, we
have succeeded in deriving the generalized Smarr formula among thermodynamical
quantities in a simple and natural way. We then show that cosmological constant
must decrease when one takes into account the quantum effect. These
observations have been obtained if and only if cosmological constant plays the
role of a thermodynamical state variable. We also touch upon the relation
between inflation of our universe and a phase transition of black holes.Comment: Revtex4, 11page