We study existence and uniqueness of weak solutions to (F) ∂tu+(−Δ)αu+h(t,u)=0 in (0,∞)×RN, with initial condition u(0,⋅)=ν in RN, where N≥2, the operator (−Δ)α is the fractional Laplacian with α∈(0,1), ν is a bounded Radon measure and h:(0,∞)×R→R is a continuous function satisfying a subcritical integrability condition.
In particular, if h(t,u)=tβup with β>−1 and , we prove that there exists a unique weak solution uk to (F) with ν=kδ0, where δ0 is the Dirac mass at the origin. We obtain that uk→∞ in (0,∞)×RN as k→∞ for p∈(0,1] and the limit of uk exists as k→∞ when , we denote it by u∞. When , u∞ is the minimal self-similar solution of (F)∞∂tu+(−Δ)αu+tβup=0 in (0,∞)×RN with the initial condition u(0,⋅)=0 in RN∖{0} and it satisfies u∞(0,x)=0 for x≠0. While if , then u∞≡Up, where Up is the maximal solution of the differential equation y′+tβyp=0 on R+.