Abstract
We report the suppression of the ferromagnetic phase transition in close to the localized-to-itinerant electronic transition, i.e., at and . A new crossover temperature can be defined for these compositions instead of . Unlike in common continuous magnetic phase transition the susceptibility does not diverge at and a spontaneous magnetization cannot be defined below it. We propose that the proximity to the doping-induced metal-insulator transition breaks up the electronic/magnetic homogeneity of the system and explains these effects.
- Received 31 August 2004
DOI:https://doi.org/10.1103/PhysRevB.70.172410
©2004 American Physical Society