190 research outputs found

    Local breaking of four-fold rotational symmetry by short-range magnetic order in heavily overdoped Ba(Fe1βˆ’x_{1-x}Cux_{x})2_{2}As2_{2}

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    We investigate Cu-doped Ba(Fe1βˆ’x_{1-x}Cux_x)2_2As2_2 with transport, magnetic susceptibility, and elastic neutron scattering measurements. In the heavily Cu-doped regime where long-range stripe-type antiferromagnetic order in BaFe2_2As2_2 is suppressed, Ba(Fe1βˆ’x_{1-x}Cux_x)2_2As2_2 (0.145 ≀x≀\leq x \leq 0.553) samples exhibit spin-glass-like behavior in magnetic susceptibility and insulating-like temperature dependence in electrical transport. Using elastic neutron scattering, we find stripe-type short-range magnetic order in the spin-glass region identified by susceptibility measurements. The persistence of short-range magnetic order over a large doping range in Ba(Fe1βˆ’x_{1-x}Cux_x)2_2As2_2 likely arises from local arrangements of Fe and Cu that favor magnetic order, with Cu acting as vacancies relieving magnetic frustration and degeneracy. These results indicate locally broken four-fold rotational symmetry, suggesting that stripe-type magnetism is ubiquitous in iron pnictides.Comment: accepted by Physical Review B Rapid Communication

    Universal quasiparticle decoherence in hole- and electron-doped high-Tc cuprates

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    We use angle-resolved photoemission to unravel the quasiparticle decoherence process in the high-TcT_c cuprates. The coherent band is highly renormalized, and the incoherent part manifests itself as a nearly vertical ``dive'' in the EE-kk intensity plot that approaches the bare band bottom. We find that the coherence-incoherence crossover energies in the hole- and electron-doped cuprates are quite different, but scale to their corresponding bare bandwidth. This rules out antiferromagnetic fluctuations as the main source for decoherence. We also observe the coherent band bottom at the zone center, whose intensity is strongly suppressed by the decoherence process. Consequently, the coherent band dispersion for both hole- and electron-doped cuprates is obtained, and is qualitatively consistent with the framework of Gutzwiller projection.Comment: 4 pages, 4 figure

    Investigating Behavioural Intention Toward Adopting Artificial Intelligence Service Robots Technology in Hospitality in China

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    The pandemic accelerated the blooming of service robots in the hospitality industry in recent years in China. The researcher drew upon extended UTAUT2 theory and satisfaction to construct the conceptual framework and spent time on smartphones as mediating and moderating roles. Besides, IBM SPSS and SmartPLS were conducted to analyse the collected data with 310 valid responses through questionnaires. The results of this study contributed practical insights for relevant governmental departments and hotel operators as well as restaurant managers in their decision-making on whether to adopt AI unmanned services in the hospitality industry in China

    Impact of Uniaxial Pressure on Structural and Magnetic Phase Transitions in Electron-Doped Iron Pnictides

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    We use neutron resonance spin echo and Larmor diffraction to study the effect of uniaxial pressure on the tetragonal-to-orthorhombic structural (TsT_s) and antiferromagnetic (AF) phase transitions in iron pnictides BaFe2βˆ’x_{2-x}Nix_{x}As2_{2} (x=0,0.03,0.12x=0,0.03,0.12), SrFe1.97_{1.97}Ni0.03_{0.03}As2_2, and BaFe2_2(As0.7_{0.7}P0.3_{0.3})2_2. In antiferromagnetically ordered BaFe2βˆ’x_{2-x}Nix_{x}As2_{2} and SrFe1.97_{1.97}Ni0.03_{0.03}As2_2 with TNT_N and TsT_s (TN≀TsT_N\leq T_s), a uniaxial pressure necessary to detwin the sample also increases TNT_N, smears out the structural transition, and induces an orthorhombic lattice distortion at all temperatures. By comparing temperature and doping dependence of the pressure induced lattice parameter changes with the elastoresistance and nematic susceptibility obtained from transport and ultrasonic measurements, we conclude that the in-plane resistivity anisotropy found in the paramagnetic state of electron underdoped iron pnictides depends sensitively on the nature of the magnetic phase transition and a strong coupling between the uniaxial pressure induced lattice distortion and electronic nematic susceptibility.Comment: 18 pages, 15 figure

    Spin excitations in optimally P-doped BaFe2(As0.7P0.3)2superconductor

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    We use inelastic neutron scattering to study temperature and energy dependence of spin excitations in optimally P-doped BaFe2(As0.7P0.3)2 superconductor (Tc = 30 K) throughout the Brillouin zone. In the undoped state, spin waves and paramagnetic spin excitations of BaFe2As2 stem from antiferromagnetic (AF) ordering wave vector QAF= (1/-1,0) and peaks near zone boundary at (1/-1,1/-1) around 180 meV. Replacing 30% As by smaller P to induce superconductivity, low-energy spin excitations of BaFe2(As0.7P0.3)2form a resonance in the superconducting state and high-energy spin excitations now peaks around 220 meV near (1/-1,1/-1). These results are consistent with calculations from a combined density functional theory and dynamical mean field theory, and suggest that the decreased average pnictogen height in BaFe2(As0.7P0.3)2 reduces the strength of electron correlations and increases the effective bandwidth of magnetic excitations.Comment: 7 pages, 5 figures, with supplementar

    Effect of Li-deficiency impurities on the electron-overdoped LiFeAs superconductor

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    We use transport, inelastic neutron scattering, and angle resolved photoemission experiments to demonstrate that the stoichiometric LiFeAs is an intrinsically electron-overdoped superconductor similar to those of the electron-overdoped NaFe1-xTxAs and BaFe2-xTxAs2 (T = Co,Ni). Furthermore, we show that although transport properties of the stoichiometric superconducting LiFeAs and Li-deficient nonsuperconducting Li1-xFeAs are different, their electronic and magnetic properties are rather similar. Therefore, the nonsuperconducting Li1-xFeAs is also in the electron overdoped regime, where small Li deficiencies near the FeAs octahedra can dramatically suppress superconductivity through the impurity scattering effect.Comment: 5 figures,5 page
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