First-order nature of the ferromagnetic phase transition in (La-Ca)MnO_3 near optimal doping

TL;DR

This study demonstrates that the ferromagnetic transition in (La-Ca)MnO_3 near optimal doping is first-order, characterized by discontinuous changes and relaxation effects, with significant isotope effects influencing the transition temperature.

Contribution

It provides direct neutron scattering evidence that the ferromagnetic transition in these manganites is first-order and highlights the role of polarons and isotope effects in this transition.

Findings

Discontinuous change in neutron scattering at T_C

Large oxygen isotope effect on T_C

Polaron formation truncates ferromagnetic phase

Abstract

Neutron scattering has been used to study the nature of the ferromagnetic transition in single crystals of La_0.7Ca_0.3MnO_3 and La_0.8Ca_0.2MnO_3, and polycrystalline samples of La_0.67Ca_0.33MnO_3 and La_5/8Ca_3/8MnO_3 where the naturally occurring O-16 can be replaced with the O-18 isotope. Small angle neutron scattering on the x=0.3 single crystal reveals a discontinuous change in the scattering at the Curie temperature for wave vectors below ~0.065 A^-1. Strong relaxation effects are observed for this domain scattering, for the magnetic order parameter, and for the quasielastic scattering, demonstrating that the transition is not continuous in nature. There is a large oxygen isotope effect observed for the T_C in the polycrystalline samples. For the optimally doped x=3/8 sample we observed T_C(O-16)=266.5 K and T_C(O-18)=261.5 K at 90% O-18 substitution. The temperature dependence of the spin-wave stiffness is found to be identical for the two samples despite changes in T_C. Hence, T_C is not solely determined by the magnetic subsystem, but instead the ferromagnetic phase is truncated by the formation of polarons which cause an abrupt transition to the paramagnetic, insulating state. Application of uniaxial stress in the x=0.3 single crystal sharply enhances the polaron scattering at room temperature. Measurements of the phonon density-of-states show only modest differences above and below T_C and between the two different isotopic samples.