N. E. Shaik
École Polytechnique Fédérale de Lausanne
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by N. E. Shaik.
Physical Review B | 2015
C. G. Fatuzzo; Marcus Dantz; Sara Fatale; P. Olalde-Velasco; N. E. Shaik; B. Dalla Piazza; S. Toth; Jonathan Pelliciari; R. Fittipaldi; A. Vecchione; N. Kikugawa; J. S. Brooks; Henrik M. Rønnow; M. Grioni; Ch. Rüegg; Thorsten Schmitt; J. Chang
High-resolution resonant inelastic x-ray scattering (RIXS) at the oxygen K edge has been used to study the orbital excitations of Ca2RuO4 and Sr2RuO4. In combination with linear dichroism x-ray absorption spectroscopy, the ruthenium 4d-orbital occupation and excitations were probed through their hybridization with the oxygen p orbitals. These results are described within a minimal model, taking into account crystal field splitting and a spin-orbit coupling λso=200 meV. The effects of spin-orbit interaction on the electronic structure and implications for the Mott and superconducting ground states of (Ca,Sr)2RuO4 are discussed.
Physical Review B | 2017
O. Ivashko; N. E. Shaik; X. Lu; C. G. Fatuzzo; Marcus Dantz; Paul Gregory Freeman; D. E. Mcnally; D. Destraz; N. B. Christensen; T. Kurosawa; N. Momono; M. Oda; C. E. Matt; Claude Monney; Henrik M. Rønnow; Thorsten Schmitt; J. Chang
A resonant inelastic x-ray scattering study of overdamped spin excitations in slightly underdoped La2−x Srx CuO4 (LSCO) with x = 0.12 and 0.145 is presented. Three high-symmetry directions have been investigated: (1) the antinodal (0,0) → ( 1 ,0), (2) the nodal (0,0) → ( 1 , 1 ), and (3) the zone-boundary direction 2 4 4 ( 1 1 1 2 ,0) → ( 4 ,4 ) connecting these two. The overdamped excitations exhibit strong dispersions along (1) and (3), whereas a much more modest dispersion is found along (2). This is in strong contrast to the undoped compound La2CuO4 (LCO) for which the strongest dispersions are found along (1) and (2). The t − t i − t ii − U Hubbard model used to explain the excitation spectrum of LCO predicts—for constant U/t —that the dispersion along (3) scales with (t i/t )2. However, the diagonal hopping t i extracted on LSCO using single-band models is low (t i/t ∼ −0.16) and decreasing with doping. We therefore invoked a two-orbital (dx2 −y2 and dz2 ) model which implies that t i is enhanced. This effect acts to enhance the zone-boundary dispersion within the Hubbard model. We thus conclude that hybridization of dx2 −y2 and dz2 states has a significant impact on the zone-boundary dispersion in LSCO.
RSC Advances | 2015
Farzaneh Fadaee; Mehdi Amirnasr; Krunoslav Prsa; Philip Pattison; N. E. Shaik; Henrik M. Rønnow; Mehdi D. Esrafili; Arash Alahgholipour Omrani; Ahmad Amiri; Kurt Schenk-Joß
A 1D, end-on azido- and phenoxo-bridged, coordination polymer, [Cu2(μ-NAPPR)(μ1,1-N3)2]n (1), (NAPPR2− = 1,3-bis(naphthylideneimino)propane dianion), was synthesized and characterized. The 1D branched-chain is built of two types of slightly different, square-pyramidal, Cu(II) ions with different sets of donor atoms. Temperature- and field-dependent magnetic analyses reveal an antiferromagnetic interaction between copper centres in the main chain (Cu2) mediated by EO-azide bridges along the chain. The interaction between the copper centres Cu1 (in the branches of the main chain) and Cu2 is very weak and is included by means of an own Weiss constant θ′. The electron density map of 1 from synchrotron data shows that the dx2−y2 orbitals of Cu2 are not well described by the procrystal model, a difference which might be meaningful for the magnetic properties. Cyclic voltammetry studies show two different redox waves with a large difference between the redox potentials of the two types of copper centres (1.21 V). The resulting data are consistent with the crystal structure of this complex determined by single crystal X-ray diffraction.
Physical Review B | 2017
L. Yang; M. Jeong; P. Babkevich; Vamshi M. Katukuri; Bálint Náfrádi; N. E. Shaik; Arnaud Magrez; H. Berger; J. Schefer; E. Ressouche; M. Kriener; Ivica Živković; Oleg V. Yazyev; László Forró; Henrik M. Rønnow
We report magnetic and thermodynamic properties of a 4d1 (Mo5+) magnetic insulator MoOPO4 single crystal, which realizes a J1−J2 Heisenberg spin-1/2 model on a stacked square lattice. The specific-heat measurements show a magnetic transition at 16 K which is also confirmed by magnetic susceptibility, ESR, and neutron diffraction measurements. Magnetic entropy deduced from the specific heat corresponds to a two-level degree of freedom per Mo5+ ion, and the effective moment from the susceptibility corresponds to the spin-only value. Using ab initio quantum chemistry calculations, we demonstrate that the Mo5+ ion hosts a purely spin-1/2 magnetic moment, indicating negligible effects of spin-orbit interaction. The quenched orbital moments originate from the large displacement of Mo ions inside the MoO6 octahedra along the apical direction. The ground state is shown by neutron diffraction to support a collinear Neel-type magnetic order, and a spin-flop transition is observed around an applied magnetic field of 3.5 T. The magnetic phase diagram is reproduced by a mean-field calculation assuming a small easy-axis anisotropy in the exchange interactions. Our results suggest 4d molybdates as an alternative playground to search for model quantum magnets.
Physical Review B | 2017
Sara Fatale; C. G. Fatuzzo; P. Babkevich; N. E. Shaik; Jonathan Pelliciari; X. Lu; D. E. McNally; Thorsten Schmitt; Akiko Kikkawa; Y. Taguchi; Y. Tokura; B. Normand; Henrik M. Rønnow; M. Grioni
We use resonant inelastic x-ray scattering (RIXS) at the Cu L3 edge to measure the charge and spin excitations in the “half-stuffed” Cu-O planes of the cuprate antiferromagnet Ba2Cu3O4Cl2. The RIXS line shape reveals distinct contributions to the dd excitations from the two structurally inequivalent Cu sites, which have different out-of-plane coordinations. The low-energy response exhibits magnetic excitations. We find a spin-wave branch whose dispersion follows the symmetry of a CuO2 sublattice, similar to the case of the “fully stuffed” planes of tetragonal CuO (T-CuO). Its bandwidth is closer to that of a typical cuprate material, such as Sr2CuO2Cl2, than it is to that of T-CuO. We interpret this result as arising from the absence of the effective four-spin inter-sublattice interactions that act to reduce the bandwidth in T-CuO.
Physical Review B | 2017
P. Babkevich; N. E. Shaik; D. Lançon; Akiko Kikkawa; M. Enderle; R. A. Ewings; H. C. Walker; D. T. Adroja; P. Manuel; D. D. Khalyavin; Y. Taguchi; Y. Tokura; Minoru Soda; Takatsugu Masuda; Henrik M. Rønnow
We report detailed neutron scattering studies on Ba
Physical Review B | 2016
L. Yang; M. Jeong; Alla Arakcheeva; Ivica Zivkovic; Bálint Náfrádi; Arnaud Magrez; A. Pisoni; Jaćim Jaćimović; Vamshi M. Katukuri; S. Katrych; N. E. Shaik; Oleg V. Yazyev; László Forró; Henrik M. Rønnow
_2
Physical Review B | 2015
Simon Moser; N. E. Shaik; D. Samal; Sara Fatale; B. Dalla Piazza; Marcus Dantz; Jonathan Pelliciari; P. Olalde-Velasco; Thorsten Schmitt; G. Koster; Frederic Mila; Henrik M. Rønnow; M. Grioni
Cu
European Journal of Inorganic Chemistry | 2018
José L. Bila; Mathieu Marmier; Konstantin O. Zhurov; Rosario Scopelliti; Ivica Živković; Henrik M. Rønnow; N. E. Shaik; Andrzej Sienkiewicz; Cornel Fink; Kay Severin
_3
Physical Review B | 2015
C. G. Fatuzzo; Marcus Dantz; Sara Fatale; P. Olalde-Velasco; N. E. Shaik; B. Dalla Piazza; S. Toth; Jonathan Pelliciari; R. Fittipaldi; A. Vecchione; N. Kikugawa; J. S. Brooks; H. M. Rønnow; M. Grioni; Ch. Rüegg; Thorsten Schmitt; J. Chang
O