306 research outputs found

    Spin dynamics of strongly-doped La_{1-x}Sr_xMnO_3

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    Cold neutron triple-axis measurements have been used to investigate the nature of the long-wavelength spin dynamics in strongly-doped La1−x_{1-x}Srx_{x}MnO3_3 single crystals with xx=0.2 and 0.3. Both systems behave like isotropic ferromagnets at low T, with a gapless (E0<0.02E_0 < 0.02 meV) quadratic dispersion relation E=E0+Dq2E = E_0 + Dq^2. The values of the spin-wave stiffness constant DD are large (DT=0D_{T=0} = 166.77 meVA˚2 \AA^2 for xx=0.2 and DT=0_{T=0} = 175.87 meVA˚2 \AA^2 for xx=0.3), which directly shows that the electron transfer energy for the dd band is large. DD exhibits a power law behavior as a function of temperature, and appears to collapse as T -> T_C. Nevertheless, an anomalously strong quasielastic central component develops and dominates the fluctuation spectrum as T -> T_C. Bragg scattering indicates that the magnetization near TCT_C exhibits power law behavior, with β≃0.30\beta \simeq 0.30 for both systems, as expected for a three-dimensional ferromagnet.Comment: 4 pages (RevTex), 3 figures (encapsulated postscript

    Structure and Spin Dynamics of La0.85_{0.85}Sr0.15_{0.15}MnO3_3

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    Neutron scattering has been used to study the structure and spin dynamics of La0.85_{0.85}Sr0.15_{0.15}MnO3_3. The magnetic structure of this system is ferromagnetic below T_C = 235 K. We see anomalies in the Bragg peak intensities and new superlattice peaks consistent with the onset of a spin-canted phase below T_{CA} = 205 K, which appears to be associated with a gap at q = (0, 0, 0.5) in the spin-wave spectrum. Anomalies in the lattice parameters indicate a concomitant lattice distortion. The long-wavelength magnetic excitations are found to be conventional spin waves, with a gapless (< 0.02 meV) isotropic dispersion relation E=Dq2E = Dq^2. The spin stiffness constant D has a T5/2T^{5/2} dependence at low T, and the damping at small q follows q4T2q^4T^{2}. An anomalously strong quasielastic component, however, develops at small wave vector above 200 K and dominates the fluctuation spectrum as T -> T_C. At larger q, on the other hand, the magnetic excitations become heavily damped at low temperatures, indicating that spin waves in this regime are not eigenstates of the system, while raising the temperature dramatically increases the damping. The strength of the spin-wave damping also depends strongly on the symmetry direction in the crystal. These anomalous damping effects are likely due to the itinerant character of the ege_g electrons.Comment: 8 pages (RevTex), 9 figures (encapsulated postscript

    Structures and Heats of Formation of Simple Alkaline Earth Metal Compounds II: Fluorides, Chlorides, Oxides, and Hydroxides for Ba, Sr, and Ra

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    Geometry parameters, vibrational frequencies, heats of formation, bond dissociation energies, cohesive energies, and selected fluoride affinities (difluorides) are predicted for the late alkaline earth (Sr, Ba and Ra) oxides, fluorides, chlorides, and hydroxides at the coupled cluster theory [CCSD(T)] level. Additional corrections (scalar relativistic and pseudopotential corrections, vibrational zero-point energies, and atomic spin-orbit effects) were included to accurately calculate the total atomization energies and heats of formation following the Feller-Peterson-Dixon methodology. The calculated values are compared to the experimental data where available. In some cases, especially for Ra compounds, there are no experimental results or the experimental energetics and geometries are not reliable or have very large error bars. All of the Sr, Ba and Ra difluorides, dichlorides and dihydroxides are bent structures with the OMO bond angles decreasing going down the group. The cohesive energy of bulk Be dihalides are predicted to be quite low while those of Ra are relatively large. The fluoride affinities show that the difluorides are moderately strong Lewis acids and that such trifluorides may form under the appropriate experimental conditions

    Novel stripe-type charge ordering in the metallic A-type antiferromagnet Pr{0.5}Sr{0.5}MnO{3}

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    We demonstrate that an A-type antiferromagnetic (AFM) state of Pr{0.5}Sr{0.5}MnO{3} exhibits a novel charge ordering which governs the transport property. This charge ordering is stripe-like, being characterized by a wave vector q ~ (0,0,0.3) with very anisotropic correlation parallel and perpendicular to the stripe direction. This charge ordering is specific to the manganites with relatively wide one-electron band width (W) which often exhibit a metallic A-type AFM state, and should be strictly distinguished from the CE-type checkerboard-like charge ordering which is commonly observed in manganites with narrower W such as La{1-x}Ca{x}MnO{3} and Pr{1-x}Ca{x}MnO{3}.Comment: REVTeX4, 5 pages, 4 figure

    SOLVENT EFFECTS ON THE ABSORPTION AND FLUORESCENCE SPECTRA OF Er(III) (AZO-DYES AND SCHIFF BASES) COMPLEXES: DETERMINATION OF GROUND AND EXCITED STATE DIPOLE MOMENT

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    Absorption and fluorescence emission spectra of some thermally stable Er(III) mononuclear complexes of azo dyes, namely o, o` -dihydroxy azobenzene (DAB), o, o` -dihydroxy 4-Cl-phenylazonaphatalene (P1) and Schiff bases o, o` -dihydroxy phenylazomethinnaphatalene (D2), o-hidroxy -o` -carboxy (D3), were recorded in solvents with different solvent dielectric constant ε and refractive index n. The solvatochromic shift method was used to determine the experimental ground and excited state dipole moments of the complexes. All the complexes were proved to be more polar in the excited state as compared with the ground state

    The Structure of Nanoscale Polaron Correlations in La1.2Sr1.8Mn2O7

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    A system of strongly-interacting electron-lattice polarons can exhibit charge and orbital order at sufficiently high polaron concentrations. In this study, the structure of short-range polaron correlations in the layered colossal magnetoresistive perovskite manganite, La1.2Sr1.8Mn2O7, has been determined by a crystallographic analysis of broad satellite maxima observed in diffuse X-ray and neutron scattering data. The resulting q=(0.3,0,1) modulation is a longitudinal octahedral-stretch mode, consistent with an incommensurate Jahn-Teller-coupled charge-density-wave fluctuations, that implies an unusual orbital-stripe pattern parallel to the directions.Comment: Reformatted with RevTe

    Tuberculosis in people of Ukrainian origin in the European Union and the European Economic Area, 2019 to 2022.

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    Approximately five million Ukrainians were displaced to the EU/EEA following the Russian invasion of Ukraine. While tuberculosis (TB) notification rates per 100,000 Ukrainians in the EU/EEA remained stable, the number of notified TB cases in Ukrainians increased almost fourfold (mean 2019-2021: 201; 2022: 780). In 2022, 71% cases were notified in three countries, and almost 20% of drug-resistant TB cases were of Ukrainian origin. Targeted healthcare services for Ukrainians are vital for early diagnosis and treatment, and preventing transmission

    Stripes Induced by Orbital Ordering in Layered Manganites

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    Spin-charge-orbital ordered structures in doped layered manganites are investigated using an orbital-degenerate double-exchange model tightly coupled to Jahn-Teller distortions. In the ferromagnetic phase, unexpected diagonal stripes at xx=1/m1/m (mm=integer) are observed, as in recent experiments. These stripes are induced by the orbital degree of freedom, which forms a staggered pattern in the background. A π\pi-shift in the orbital order across stripes is identified, analogous to the π\pi-shift in spin order across stripes in cuprates. At xx=1/4 and 1/3, another non-magnetic phase with diagonal static charge stripes is stabilized at intermediate values of the t2gt_{\rm 2g}-spins exchange coupling.Comment: reordering of figure

    Temperature Dependence of Low-Lying Electronic Excitations of LaMnO_3

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    We report on the optical properties of undoped single crystal LaMnO_3, the parent compound of the colossal magneto-resistive manganites. Near-Normal incidence reflectance measurements are reported in the frequency range of 20-50,000 cm-1 and in the temperature range 10-300 K. The optical conductivity, s_1(w), is derived by performing a Kramers-Kronig analysis of the reflectance data. The far-infrared spectrum of s_1(w) displays the infrared active optical phonons. We observe a shift of several of the phonon to high frequencies as the temperature is lowered through the Neel temperature of the sample (T_N = 137 K). The high-frequency s_1(w) is characterized by the onset of absorption near 1.5 eV. This energy has been identified as the threshold for optical transitions across the Jahn-Teller split e_g levels. The spectral weight of this feature increases in the low-temperature state. This implies a transfer of spectral weight from the UV to the visible associated with the paramagnetic to antiferromagnetic state. We discuss the results in terms of the double exchange processes that affect the optical processes in this magnetic material.Comment: 7 pages, 5 figure
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