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024 | 7 | _ | |2 DOI |a 10.1088/0953-8984/17/41/L02 |
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041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
100 | 1 | _ | |a Bowen, M. |b 0 |0 P:(DE-HGF)0 |
245 | _ | _ | |a Half-metallicity proven using fully spin-polarized tunneling |
260 | _ | _ | |a Bristol |b IOP Publ. |c 2005 |
300 | _ | _ | |a L407 - 409 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
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336 | 7 | _ | |a article |2 DRIVER |
440 | _ | 0 | |a Journal of Physics: Condensed Matter |x 0953-8984 |0 3703 |v 17 |
500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
520 | _ | _ | |a A half-metal has been defined as a material with propagating electron states at the Fermi energy only for one of the spin directions. But is it fully half-metallic, that is without electrons with opposite spin at that energy? We have studied the spin-conserving process of tunnelling between La0.7Sr0.3MnO3 half-metallic electrodes across an ultrathin SrTiO3 insulator. This experiment demonstrates that the class of half-metallic materials indeed exists at non-zero temperatures, even at interfaces. It also shows that a fully spin-polarized tunnelling current may persist at large bias. |
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700 | 1 | _ | |a Barthélémy, A. |b 1 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Bibes, M. |b 2 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Jacquet, E. |b 3 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Contour, J. P. |b 4 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Fert, A. |b 5 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Wortmann, D. |b 6 |u FZJ |0 P:(DE-Juel1)131042 |
700 | 1 | _ | |a Blügel, S. |b 7 |u FZJ |0 P:(DE-Juel1)130548 |
773 | _ | _ | |a 10.1088/0953-8984/17/41/L02 |g Vol. 17, p. L407 - 409 |p L407 - 409 |q 17 |t Journal of physics / Condensed matter |v 17 |y 2005 |x 0953-8984 |
856 | 7 | _ | |u http://dx.doi.org/10.1088/0953-8984/17/41/L02 |
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914 | 1 | _ | |a Nachtrag |y 2005 |
915 | _ | _ | |0 StatID:(DE-HGF)0010 |a JCR/ISI refereed |
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