Brahim Dkhil
Université Paris-Saclay
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Featured researches published by Brahim Dkhil.
Physical Review B | 2002
Jean-Michel Kiat; Yoshiaki Uesu; Brahim Dkhil; Masaaki Matsuda; Charlotte Malibert; G. Calvarin
Evidences of a monoclinic phase in unpoled (PbMg1/3Nb2/3O3)1-x-(PbTiO3)x with x=0.35 (PMN-PT 35%) and unpoled (PbZn1/3Nb2/3O3)1-x-(PbTiO3)x with x=0.09 (PZN-PT 9%) are presented from a neutron Rietveld analysis. This monoclinic phase is different from the phase recently evidenced by Noheda and coworkers in PbZr1-xTixO3 with x=0.481 but is identical to the phase observed in poled PZN-PT with x=0.102 by the same authors. The structural resolutions allowed us to compare both structures and to deduce the direction and magnitude of polarization. In PMN-PT 35% and PZN-PT 9% this phase is characterised by a weak value of polarization, a strong deformation of oxygen polyhedra and weak cationic shifts.
Journal of the American Chemical Society | 2011
Emilio Pardo; Cyrille Train; Geoffrey Gontard; Kamal Boubekeur; Oscar Fabelo; Hongbo Liu; Brahim Dkhil; Francesc Lloret; Kosuke Nakagawa; Hiroko Tokoro; Shin-ichi Ohkoshi; Michel Verdaguer
A complex-as-ligand strategy to get a multifunctional molecular material led to a metal-organic framework with the formula (NH(4))(4)[MnCr(2)(ox)(6)]·4H(2)O. Single-crystal X-ray diffraction revealed that the anionic bimetallic coordination network adopts a chiral three-dimensional quartz-like architecture. It hosts ammonium cations and water molecules in functionalized channels. In addition to ferromagnetic ordering below T(C) = 3.0 K related to the host network, the material exhibits a very high proton conductivity of 1.1 × 10(-3) S cm(-1) at room temperature due to the guest molecules.
Nature Materials | 2014
Ryan O. Cherifi; V. V. Ivanovskaya; L. C. Phillips; Alberto Zobelli; Ingrid C. Infante; Eric Jacquet; Vincent Garcia; S. Fusil; P.R. Briddon; Nicolas Guiblin; A. Mougin; Ahmet A. Ünal; Florian Kronast; S. Valencia; Brahim Dkhil; A. Barthélémy; M. Bibes
Controlling magnetism by means of electric fields is a key issue for the future development of low-power spintronics. Progress has been made in the electrical control of magnetic anisotropy, domain structure, spin polarization or critical temperatures. However, the ability to turn on and off robust ferromagnetism at room temperature and above has remained elusive. Here we use ferroelectricity in BaTiO3 crystals to tune the sharp metamagnetic transition temperature of epitaxially grown FeRh films and electrically drive a transition between antiferromagnetic and ferromagnetic order with only a few volts, just above room temperature. The detailed analysis of the data in the light of first-principles calculations indicate that the phenomenon is mediated by both strain and field effects from the BaTiO3. Our results correspond to a magnetoelectric coupling larger than previous reports by at least one order of magnitude and open new perspectives for the use of ferroelectrics in magnetic storage and spintronics.
Journal of Physics: Condensed Matter | 1997
Charlotte Malibert; Brahim Dkhil; Jean-Michel Kiat; D Durand; J.-F. Berar; A Spasojević-de Biré
We report a structural evolution analysis of the long-range and local order and disorder of lead scandium niobate (PSN) down to 10 K, using a combination of neutron and x-ray diffraction on powder and single crystals. The structure of PSN is discussed and compared with those of simple perovskite compounds and . In PSN the existence of a long-range but still disordered ferroelectric phase, different from those of simple perovskites, is evidenced. The disorder of lead and scandium/niobium atoms on short-, medium- and long-range scales is discussed in connection with the dielectric properties of these materials.
Angewandte Chemie | 2012
Emilio Pardo; Cyrille Train; Hongbo Liu; Lise-Marie Chamoreau; Brahim Dkhil; Kamal Boubekeur; Francesc Lloret; Keitaro Nakatani; Hiroko Tokoro; Shin-ichi Ohkoshi; Michel Verdaguer
Multiferroics (MF) are materials that exhibit simultaneouslyseveral ferroic order parameters. Among the multiferroicmaterials, those combining antiferro- or ferroelectricity (FE)and antiferro-, ferri-, or ferromagnetism (FM) within thesame material are highly desirable: the coexistence of thepolar and magnetic orders paves the way towards four-levelmemories while their interactions through the magnetoelec-tric effect makes it possible to control the magnetization byelectric fields and hence to develop electronically tuneablemagnetic devices, which are an essential feature for spin-tronics.
Journal of Physics: Condensed Matter | 2004
Ph. Sciau; A. Kania; Brahim Dkhil; E. Suard; Alicja Ratuszna
The structures and phase transitions of AgNbO3 were investigated using neutron powder diffraction and restricted single-crystal x-ray diffraction. Both methods have revealed the high temperature M3–O1, O2–T and T–C phase transitions but have not given any significant evidence of low temperature M1–M2 and M2–M3 ones. The refinements of neutron diffraction patterns allowed us to determine the symmetry, space group and crystal structure for all phases except the O1 one. The existence of structural disorder in the T and probably O2 phases was found. The high temperature paraelectric phase transitions can be interpreted on the basis of consecutive condensation of oxygen octahedron tilts around the main axis. The ferroelectric and antiferroelectric behaviour has been associated with Ag and Nb cations. The reason why phase transitions between low temperature ferroelectric and antiferroelectric phases are not detectable by diffraction methods is discussed. The sequence of phase transitions in AgNbO3 can then be understood in the framework of a long range and/or local order–disorder type arrangement.
Applied Physics Letters | 2010
Jie Wei; R. Haumont; Romain Jarrier; Patrik Berhtet; Brahim Dkhil
In this paper, we show that a pure single phase by doping Fe-site of BiFeO3 (BFO) using tetravalent Zr4+ ions can be achieved by introducing cation (Bi3+) vacancies. The structural analysis reveals that the ferroelectric nature of BFO should be weakly affected by 10% of Zr4+ doping as the c/a ratio and the Curie temperature TC remain roughly unchanged compared to that of pure BFO. In contrast, the magnetic properties are affected as a weak ferromagnetism and a change of Neel temperature TN are observed. Beyond the double-exchange interactions arising from the creation of Fe2+, we propose another simple model inducing a local ferromagnetic coupling rather than an antiferromagnetic which considers the replacement of the magnetically active Fe3+, time to time, by a nonactive Zr4+.
Physical Review B | 2009
Brahim Dkhil; P. Gemeiner; A. Al-Barakaty; L. Bellaiche; E. Dul’kin; E. Mojaev; M. Roth
Via a combination of various experimental and theoretical techniques, a peculiar, identical temperature scale
Physical Review B | 2009
R. Haumont; P. Bouvier; Alexej Pashkin; K. Rabia; S. Frank; Brahim Dkhil; Wilson A. Crichton; C. A. Kuntscher; J. Kreisel
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New Journal of Physics | 2010
Philip Liu; J. L. Wang; Xiangju Meng; Jing Yang; Brahim Dkhil; J. H. Chu
is found to exist in all complex lead-based relaxor ferroelectrics studied by us.