Dresden 2006 – scientific programme
Parts | Days | Selection | Search | Downloads | Help
MA: Magnetismus
MA 20: Poster: Films(1-36) Transp(37-56) Ex.Bias(57-67) Spindyn(68-80) Micromag(81-95) Particle(96-109) Imag.+Surface(110-113) Spinelectr(114-122) Theory+Micromag(123-131) Spinstr+Aniso(132-142) MagMat(143-156) Meas(157,158) MolMag+Kondo(159-162) Postdead(163-)
MA 20.47: Poster
Tuesday, March 28, 2006, 15:15–19:15, P1
Magnetoresistive effects in LSMO:MgO TMR-systems — •Markus Esseling1, Stephanie Raabe1, Vasily Moshnyagy1, Achim Marx2, Rudolf Gross2, and Konrad Samwer1 — 1I. Physikalisches Institut, Universität Göttingen, Friedrich-Hund-Platz 1, D-37077 Göttingen — 2Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, Walther-Meissner-Str. 8, D-85748 Garching
The TMR effect is known to be very sensitive to the quality of the interface ferromagnet/insulator. The influence of the interfacial properties on the spin-dependent transport can be studied by using different ways to prepare the tunnel junction, namely i) a nanocomposite film consisting of ferromagnetic metallic grains separated by an insulator ii) a well defined grain-boundary of the ferromagnet doped with the insulator due to a chemical phase separation using a bicrystal-substrate and iii) an artificial multilayer structure. Using the highly spin-polarized manganite La0.7Sr0.3MnO3 (LSMO) and the insulating MgO, which is an ideal candidate to achieve high TMR-values, it is possible to prepare these different systems mentioned above. We present results of the structural and electronic characterization of the bicrystal samples, which were prepared on symmetric 24∘ [001] tilted SrTiO3- and MgO-substrates to trigger an epitaxial growth of the LSMO on both sides of the grain-boundary of the bicrystal. The results are compared with the nanocomposite, which was characterized using low-frequency 1/f-noise measurements [1].
[1] M. Esseling et al., Appl. Phys. Lett. 87 (2005) 082509
Supported by SFB 602, TP A2 and DFG Sa 339/9