695 research outputs found

    L\'evy-like behavior in deterministic models of intelligent agents exploring heterogeneous environments

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    Many studies on animal and human movement patterns report the existence of scaling laws and power-law distributions. Whereas a number of random walk models have been proposed to explain observations, in many situations individuals actually rely on mental maps to explore strongly heterogeneous environments. In this work we study a model of a deterministic walker, visiting sites randomly distributed on the plane and with varying weight or attractiveness. At each step, the walker minimizes a function that depends on the distance to the next unvisited target (cost) and on the weight of that target (gain). If the target weight distribution is a power-law, p(k)∼kβˆ’Ξ²p(k)\sim k^{-\beta}, in some range of the exponent Ξ²\beta, the foraging medium induces movements that are similar to L\'evy flights and are characterized by non-trivial exponents. We explore variations of the choice rule in order to test the robustness of the model and argue that the addition of noise has a limited impact on the dynamics in strongly disordered media.Comment: 15 pages, 7 figures. One section adde

    Universal magneto-orbital ordering in the divalent AA-site quadruple perovskite manganites AAMn7_7O12_{12} (AA = Ca, Sr, Cd, and Pb)

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    Through analysis of variable temperature neutron powder diffraction data, we present solutions for the magnetic structures of SrMn7_7O12_{12}, CdMn7_7O12_{12}, and PbMn7_7O12_{12} in all long-range ordered phases. The three compounds were found to have magnetic structures analogous to that reported for CaMn7_7O12_{12}. They all feature a higher temperature lock-in phase with \emph{commensurate} magneto-orbital coupling, and a delocked, multi-\textbf{k} magnetic ground state where \emph{incommensurate} magneto-orbital coupling gives rise to a constant-moment magnetic helix with modulated spin helicity. CdMn7_7O12_{12} represents a special case in which the orbital modulation is commensurate with the crystal lattice and involves stacking of fully and partially polarized orbital states. Our results provide a robust confirmation of the phenomenological model for magneto-orbital coupling previously presented for CaMn7_7O12_{12}. Furthermore, we show that the model is universal to the A2+A^{2+} quadruple perovskite manganites synthesised to date, and that it is tunable by selection of the AA-site ionic radius

    Magnetic ground state and multiferroicity in BiMnO3_3

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    We argue that the centrosymmetric C2/cC2/c symmetry in BiMnO3_3 is spontaneously broken by antiferromagnetic (AFM) interactions existing in the system. The true symmetry is expected to be CcCc, which is compatible with the noncollinear magnetic ground state, where the ferromagnetic order along one crystallographic axis coexists with the the hidden AFM order and related to it ferroelectric polarization along two other axes. The C2/cC2/c symmetry can be restored by the magnetic field B∼35B \sim 35 Tesla, which switches off the ferroelectric polarization. Our analysis is based on the solution of the low-energy model constructed for the 3d-bands of BiMnO3_3, where all the parameters have been derived from the first-principles calculations. Test calculations for isostructural BiCrO3_3 reveal an excellent agreement with experimental data.Comment: 5 pages, 5 figure

    Π‘ΠΈΠ½Ρ‚Π΅Π· ΠΈ свойства силикатов висмута, ΠΏΡ€ΠΈΠ³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ мСханичСской Π°ΠΊΡ‚ΠΈΠ²Π°Ρ†ΠΈΠΈ

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    Π’ настоящСй Ρ€Π°Π±ΠΎΡ‚Π΅ Π±Ρ‹Π»ΠΈ синтСзированы сСрии силикатов висмута мСтодоммСханичСской Π°ΠΊΡ‚ΠΈΠ²Π°Ρ†ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ исслСдованы ΠΈΡ… свойства Ρ‚Π°ΠΊΠΈΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ, ΠΊΠ°ΠΊ Π’Π“-Π”Π‘Πš Π°Π½Π°Π»ΠΈΠ· ΠΈ РЀА-спСктроскопия. УстановлСно, Ρ‡Ρ‚ΠΎ для сСрии, ΠΏΡ€ΠΈΠ³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π½ΠΎΠΉ с ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠ΅ΠΌ Ρ€Π΅Π°Π³Π΅Π½Ρ‚ΠΎΠ² Bi:Si = 2:1 послС 800 Β°Π‘ наступаСт ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅, Ρ‚ΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ для сСрии с эквиатомным ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠ΅ΠΌ Bi ΠΈ Si Π² исходных Ρ€Π΅Π°Π³Π΅Π½Ρ‚Π°Ρ… плавлСния Π² этом Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠΌ ΠΈΠ½Ρ‚Π΅Ρ€Π²Π°Π»Π΅ Π½Π΅ Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ. Показано, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠΈ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ прокаливания с 500˚Б Π΄ΠΎ 700 Β°Π‘ Ρ„Π°Π·Π° мСтасиликата висмута (Bi2SiO5) ΠΏΠΎΠ»Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ΠΈΡ‚ Π² ортосиликат висмута (Bi4Si3O12), Π° доля Ρ„Π°Π·Ρ‹ силлСнита (Bi12SiO20) увСличиваСтся ΠΏΡ€ΠΈ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠΈ ΡΠΎΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ Bi:Si
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