Transport, magnetic, and thermal properties of phase-separated ${\mathrm{La}}_{0.8}{\mathrm{Ca}}_{0.2}\mathrm{Mn}{\mathrm{O}}_3$ crystal were studied in a wide temperature range down to $10\mathrm{K}$. At low temperatures below the Curie point $T_C=184\mathrm{K}$, the sample resistance is characterized by spontaneous transitions to higher resistivity metastable states. Metastability becomes more pronounced when enforced by the application of current pulses at low temperatures. Metastable states are characterized by long-term memory surviving even thermal cycling to room temperatures. Only heating to $T>T_e\approx 350\mathrm{K}$ erases the previously imprinted state of the system. At temperatures close to the low temperature resistivity maximum, a slow relaxation of the resistance has been observed following changes in the bias current. Ac susceptibility, low-field magnetization, and specific heat data indicate that there is a spin-cluster glass-like transition at temperatures corresponding to the maximum of the relaxation time. Phase separation and coexistence of metallic and insulating ferromagnetic phases with different orbital order at a wide temperature range are claimed to be responsible for the observed electric-field and current effects. The disappearance of the resistance memory effects at temperatures above $T_e$ may be considered an indirect proof for the existence of one more temperature scale in disordered manganites.

• Received 13 April 2004

DOI:https://doi.org/10.1103/PhysRevB.70.064414