Abstract

AbstractWe report the transport properties of both single‐layer (SL) La0.67Sr0.33MnO3 (SL1), La0.67Ca0.33MnO3 (SL2) and La0.67Sr1.33MnO4 (SL3) each of thickness 135 nm and bilayers (BL) SL1/SL3 (BL1) and SL2/SL3 (BL2) each of thickness 270 nm. All the films are deposited on SrTiO3(001) substrates by the off‐axis RF sputtering process. Compared to SL films, a large enhancement of magnetoresistance (MR) at 1.2 T field is observed in the BL films. Except for the antiferromagnetic (AF) SL3 film, two ferromagnetic (FM) films SL1 and SL2 showed metallic transitions, respectively, at T MI = 248 and 365 K. For the BL films, T MI shifts largely towards a lower temperature than the corresponding T MI of the corresponding SL films due to the increase of disorder and strain effect at the junction of the films. Temperature‐dependent resistivity (ρ ) curves, above T MI, are best fitted by the adiabatic small‐polaron hopping model, i.e. ρ = ρ 0T exp (E a/k BT ) with activation energy E a (BL) > E a(SL). Within the temperature range T D/2 < T < T MI (T D being the Debye temperature), the resistivity curves are well fitted with the variable range hopping (VRH) with effective number of carriers at the Fermi level [N (E F)], being different for BL and SL films. In the SL films, spin ordering completes below a critical temperature (T *, say) and a changeover of the transport mechanism dominated by the electron–electron scattering regime (T < T *) to an electron–magnon‐dominated scattering regime (T > T *) is observed. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

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