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Quantifying the critical thickness of electron hybridization in spintronics materials.
Pincelli, T; Lollobrigida, V; Borgatti, F; Regoutz, A; Gobaut, B; Schlueter, C; Lee, T-L; Payne, D J; Oura, M; Tamasaku, K; Petrov, A Y; Graziosi, P; Granozio, F Miletto; Cavallini, M; Vinai, G; Ciprian, R; Back, C H; Rossi, G; Taguchi, M; Daimon, H; van der Laan, G; Panaccione, G.
  • Pincelli T; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Lollobrigida V; Dipartimento di Fisica, Università di Milano, Via Celoria 16, Milano I-20133, Italy.
  • Borgatti F; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Regoutz A; Dipartimento di Scienze, Università degli Studi Roma Tre, Via della Vasca Navale 84, Roma I-00146, Italy.
  • Gobaut B; Consiglio Nazionale delle Ricerche-Istituto per lo Studio dei Materiali Nanostrutturati (CNR-ISMN), via P. Gobetti 101, Bologna I-40129, Italy.
  • Schlueter C; Department of Materials, Imperial College London, South Kensington, London SW7 2AZ, UK.
  • Lee TL; Sincrotrone Trieste S.C.p.A., S.S. 14 Km 163.5, Area Science Park, Trieste 34149, Italy.
  • Payne DJ; Diamond Light Source, Harwell Science and Innovation Campus, Didcot OX11 0DE, UK.
  • Oura M; Diamond Light Source, Harwell Science and Innovation Campus, Didcot OX11 0DE, UK.
  • Tamasaku K; Department of Materials, Imperial College London, South Kensington, London SW7 2AZ, UK.
  • Petrov AY; RIKEN SPring-8 Center, Kouto 1-1-1, Sayo-cho, Sayo-gun, Hyogo 679-5148, Japan.
  • Graziosi P; RIKEN SPring-8 Center, Kouto 1-1-1, Sayo-cho, Sayo-gun, Hyogo 679-5148, Japan.
  • Granozio FM; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Cavallini M; Consiglio Nazionale delle Ricerche-Istituto per lo Studio dei Materiali Nanostrutturati (CNR-ISMN), via P. Gobetti 101, Bologna I-40129, Italy.
  • Vinai G; CNR-SPIN, Complesso Universitario Monte S. Angelo, Napoli 80126, Italy.
  • Ciprian R; Dipartimento di Fisica, Università 'Federico II' di Napoli, Napoli, 80126, Italy.
  • Back CH; Consiglio Nazionale delle Ricerche-Istituto per lo Studio dei Materiali Nanostrutturati (CNR-ISMN), via P. Gobetti 101, Bologna I-40129, Italy.
  • Rossi G; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Taguchi M; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Daimon H; Institut fur Experimentelle Physik, Universitat Regensburg, Regensburg D-93040, Germany.
  • van der Laan G; Istituto Officina dei Materiali-CNR, Laboratorio TASC, Area Science Park, S.S. 14, Km 163.5, Trieste I-34149, Italy.
  • Panaccione G; Dipartimento di Fisica, Università di Milano, Via Celoria 16, Milano I-20133, Italy.
Nat Commun ; 8: 16051, 2017 07 17.
Article en En | MEDLINE | ID: mdl-28714466
ABSTRACT
In the rapidly growing field of spintronics, simultaneous control of electronic and magnetic properties is essential, and the perspective of building novel phases is directly linked to the control of tuning parameters, for example, thickness and doping. Looking at the relevant effects in interface-driven spintronics, the reduced symmetry at a surface and interface corresponds to a severe modification of the overlap of electron orbitals, that is, to a change of electron hybridization. Here we report a chemically and magnetically sensitive depth-dependent analysis of two paradigmatic systems, namely La1-xSrxMnO3 and (Ga,Mn)As. Supported by cluster calculations, we find a crossover between surface and bulk in the electron hybridization/correlation and we identify a spectroscopic fingerprint of bulk metallic character and ferromagnetism versus depth. The critical thickness and the gradient of hybridization are measured, setting an intrinsic limit of 3 and 10 unit cells from the surface, respectively, for (Ga,Mn)As and La1-xSrxMnO3, for fully restoring bulk properties.