79 research outputs found

    Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-x_\mathrm{1\text{-}x}Sx_\mathrm{x}

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    We report muon spin rotation (μ\muSR) and magnetization measurements under pressure on Fe1+δ_{1+\delta}Se1-x_\mathrm{1\text{-}x}Sx_\mathrm{x} with x 0.11\approx 0.11.Above p0.6p\approx0.6 GPa we find microscopic coexistence of superconductivity with an extended dome of long range magnetic order that spans a pressure range between previously reported separated magnetic phases. The magnetism initially competes on an atomic scale with the coexisting superconductivity leading to a local maximum and minimum of the superconducting Tc(p)T_\mathrm{c}(p). The maximum of TcT_\mathrm{c} corresponds to the onset of magnetism while the minimum coincides with the pressure of strongest competition. A shift of the maximum of Tc(p)T_\mathrm{c}(p) for a series of single crystals with x up to 0.14 roughly extrapolates to a putative magnetic and superconducting state at ambient pressure for x 0.2\geq0.2.Comment: 10 pages, 6 figures, including supplemental materia

    Gradual Enhancement of Stripe-Type Antiferromagnetism in Spin Ladder Material BaFe2_2S3_3 Under Pressure

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    We report pressure-dependent neutron diffraction and muon spin relaxation/rotation measurements combined with first-principles calculations to investigate the structural, magnetic, and electronic properties of BaFe2_2S3_3 under pressure. The experimental results reveal a gradual enhancement of the stripe-type ordering temperature with increasing pressure up to 2.6 GPa and no observable change in the size of the ordered moment. The ab initio calculations suggest that the magnetism is highly sensitive to the Fe-S bond lengths and angles, clarifying discrepancies with previously published results. In contrast to our experimental observations, the calculations predict a monotonic reduction of the ordered moment with pressure. We suggest that the robustness of the stripe-type antiferromagnetism is due to strong electron correlations not fully considered in the calculations

    Spin pseudogap in Ni-doped SrCuO2

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    The S=1/2 spin chain material SrCuO2 doped with 1% S=1 Ni-impurities is studied by inelastic neutron scattering. At low temperatures, the spectrum shows a pseudogap \Delta ~ 8 meV, absent in the parent compound, and not related to any structural phase transition. The pseudogap is shown to be a generic feature of quantum spin chains with dilute defects. A simple model based on this idea quantitatively accounts for the exprimental data measured in the temperature range 2-300 K, and allows to represent the momentum-integrated dynamic structure factor in a universal scaling form.Comment: 5 pages, 3 figure

    Universal fluctuating regime in triangular chromate antiferromagnets

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    We report x-ray diffraction, magnetic susceptibility, heat capacity, 1^{1}H nuclear magnetic resonance (NMR), and muon spin relaxation (μ\muSR) measurements, as well as density-functional band-structure calculations for the frustrated S=3/2S=3/2 triangular lattice Heisenberg antiferromagnet (TLHAF) α\alpha-HCrO2_{2} (trigonal, space group: R3ˉmR\bar{3}m). This compound undergoes a clear magnetic transition at TN22.5T_{\rm N} \simeq 22.5~K, as seen from the drop in the muon paramagnetic fraction and concurrent anomalies in the magnetic susceptibility and specific heat. Local probes (NMR and μ\muSR) reveal a broad regime with slow fluctuations down to 0.7TN0.7\,T_{\rm N}, this temperature corresponding to the maximum in the μ\muSR relaxation rate and in the NMR wipe-out. From the comparison with NaCrO2_{2} and α\alpha-KCrO2_{2}, the fluctuating regime and slow dynamics below TNT_{\rm N} appear to be hallmarks of the TLHAF with ABCABC stacking that leads to a frustration of interlayer couplings between the triangular planes. This interlayer frustration is a powerful lever to generate spin states with persistent dynamics and may bear implications to spin-liquid candidates with the triangular geometry.Comment: 14 pages, 11 figures, 2 table

    Disordered ground state in the spin-orbit coupled Jeff = 1/2 distorted honeycomb magnet BiYbGeO5

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    We delineate quantum magnetism in the strongly spin-orbit coupled distorted honeycomb lattice antiferromagnet BiYbGeO5. Our magnetization and heat capacity measurements reveal that its low-temperature behavior is well described by an effective Jeff=12 Kramers doublet of Yb3+. The ground state is nonmagnetic with a tiny spin gap. Temperature-dependent magnetic susceptibility, magnetization isotherm, and heat capacity can be modeled well assuming isolated spin dimers with anisotropic exchange interactions JZ≃2.6 K and JXY≃1.3 K. Heat capacity measurements backed by muon spin relaxation suggest the absence of magnetic long-range order down to at least 80 mK both in zero field and in applied fields. This sets BiYbGeO5 apart from Yb2Si2O7, with its unusual regime of magnon Bose-Einstein condensation, and suggests negligible interdimer couplings, despite only a weak structural deformation of the honeycomb lattice
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