Magnetic droplets in a metal close to a ferromagnetic quantum critical point

Using analytical and path integral Monte Carlo methods, we study the susceptibility χ_dc(T) of a spin-S impurity with XY rotational symmetry embedded in a metal. Close to a ferromagnetic quantum critical point, the impurity polarizes conduction electrons in its vicinity and forms a large magnetic droplet with moment M⪢S. At not too low temperatures, the strongly damping paramagnon modes of the conduction electrons suppress large quantum fluctuations (or spin flips) of this droplet. We show that the susceptibility follows the law χ_dc(T)=(M²∕T)[1−(πg)⁻¹ ln(gE₀∕T)], where the parameter g⪢1 describes the strong damping by conduction electrons, and E₀ is the bandwidth of paramagnon modes. At exponentially low temperatures T⪡T_*∼E₀ exp(−πg∕2) we show that spin flips cannot be ignored. In this regime we find that χ_dc(T)≈χ_dc(0)[1−(2∕3)(T∕T_*)²], where χ_dc(0)∼M²∕T_* is finite and exponentially large in g. We also discuss these effects in the context of the multichannel Kondo impurity model.