Abstract

The influence of hydrostatic pressure, magnetic field and temperature on resistivity behaviour of bulk and film samples La 0.9Mn 1.1O 3 and La 0.56Ca 0.24Mn 1.2O 3 at action of magnetic field and temperature has been analysed. It is established that the maximum of magnetoresistive and the revealed baroresistive, magnetobaroresistive effects coincide at the same temperature T pp. This temperature is equal to the “metal-semiconductor” phase transition temperature T ms. “Cooling” and “heating” effects of pressure and magnetic field have been revealed. A mutual correspondence of T– P– H (6.2 K, 1 kbar, 2.7 kOe) influence on polycrystalline sample La 0.9Mn 1.1O 3 resistivity has been determined. The linear change of T ms( P) and T ms( H) in La 0.9Mn 1.1O 3, La 0.56Ca 0.24Mn 1.2O 3 resistivity have been found. An importance of the regularities of elastic-deforming correspondence of T– H– P influence on magnetic, resistivity properties, phase transitions and effects was elucidated and explained. An alternating influence of T– H– P and its role in resistivity has been pointed. A correlation between structural, elastic and resistive properties is specified.

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