Abstract

We have investigated the effect of large in-plane compressive strain on the electrical transport in La0.88Sr0.12MnO3 in thin films. For achieving large compressive strain, films have been deposited on single crystal LaAlO3 (LAO, a = 3.798 Å) substrate from a polycrystalline bulk target having average in-plane lattice parameter aav = (ab + bb)/2 = 3.925 Å. The compressive strain was further relaxed by varying the film thickness in the range ∼6–75 nm. In the film having least thickness (∼6 nm) large increase (c = 3.929 Å) in the out-of-plane lattice parameter is observed which gradually decreases towards the bulk value (cbulk = 3.87 Å) for ∼75 nm thick film. This shows that the film having the least thickness is under large compressive strain, which partially relaxes with increasing film thickness. The TIM of the bulk target ∼145 K goes up to ∼235 K for the ∼6 nm thin film and even for partially strain relaxed ∼75 nm thick film TIM is as high as ∼200 K. This enhancement in TIM is explained in terms of suppression of Jahn–Teller distortion of the MnO6 octahedra by the large in-plane compressive strain. We observe a large enhancement in the low field magnetoresistance (MR) just below TIM in the films having partial strain relaxation. Thick films of 6 and 20 nm have MR ∼14% at 3 kOe that almost doubles in 35 nm film to ∼27%. Similar enhancement is also obtained in the case of the temperature coefficient of resistivity. The near doubling of low field MR is explained in terms of delocalization of weakly localized carriers around TIM by small magnetic fields.

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