This paper presents the application of Kolmogorov-Arnold Networks (KAN) in classifying metal surface defects. Specifically, steel surfaces are analyzed to detect defects such as cracks, inclusions, patches, pitted sur...
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The dynamics of social relations and the possibility of reaching the state of structural balance (Heider balance) are discussed for various networks of interacting actors under the influence of the temperature modelin...
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The complex magnetic structures, spin reorientation, and associated exchange interactions have been investigated in Er0.5Dy0.5FeO3 using bulk magnetization, neutron diffraction, specific heat measurements, and density...
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The complex magnetic structures, spin reorientation, and associated exchange interactions have been investigated in Er0.5Dy0.5FeO3 using bulk magnetization, neutron diffraction, specific heat measurements, and density functional theory calculations. The Fe3+ spins order as G-type antiferromagnet structure depicted by Γ4(Gx, Ay, Fz) irreducible representation below 700 K, similar to its end compounds. The bulk magnetization data indicate occurrence of the spin-reorientation and rare-earth magnetic moments' polarization below ∼75 K and 10 K, respectively. The neutron diffraction studies confirm an “incomplete” Γ4→ Γ2(Fx, Cy, Gz) spin-reorientation initiated ≤75 K. Although the relative volume fraction of the two magnetic structures varies with decreasing temperature, both coexist even at 1.5 K. Below 10 K, the polarization of Er3+/Dy3+ moments in a cyR arrangement develops, which gradually increases with decreasing temperature. At 2 K, magnetic structure associated with czR arrangement of Er3+/Dy3+ moments also appears. At 1.5 K, while the rare-earth magnetic moments show a cyR+czR-type arrangement, the Fe3+ spins are represented by a combination of a Γ2+Γ4 (Gz,Gx) arrangement. A clear signature of the magnetic structure with Γ1(Gy) representation, symmetrically compatible with the czR-type arrangement of rare-earth moments, is not confirmed from the refinement of the neutron diffraction data. The observed Schottky anomaly at 2.5 K suggests that the “rare-earth ordering” is induced by polarization due to Fe3+ spins. The Er3+−Fe3+ and Er3+−Dy3+ exchange interactions, obtained from first principle calculations, indicate that these interactions primarily cause the complicated spin reorientation and cyR rare-earth ordering in the system, respectively, while the dipolar interactions between rare-earth moments result in the czR type rare-earth ordering at 2 K.
We investigate a nonlinear parabolic reaction-diffusion equation describing the oxygen concentration in encapsulated pancreatic cells with a general core-shell geometry. This geometry introduces a discontinuous diffus...
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The study of interaction between the particle and lattice degrees of freedom is one of the central interests in the quantum many-body systems. The Z2 Bose-Hubbard model has been proposed to describe ultracold bosons i...
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We present results on the Central Exclusive Production of charged particle pairs h+h− (h = π, K, p), pp → p + h+h− + p, obtained with the STAR experiment at RHIC in proton-proton collisions at a center-of-mass energ...
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We determine thresholds pc for random-site percolation on a triangular lattice for all available neighborhoods containing sites from the first to the fifth coordination zones, including their complex combinations. The...
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We study a simple deterministic map that leads a fully connected network to Heider balance. The map is realized by an algorithm that updates all links synchronously in a way depending on the state of the entire networ...
We study fractional Laplace motion (FLM) obtained from subordination of fractional Brownian motion (FBM) to a gamma process in the presence of an external drift that acts on the composite process or of an internal dri...
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We study fractional Laplace motion (FLM) obtained from subordination of fractional Brownian motion (FBM) to a gamma process in the presence of an external drift that acts on the composite process or of an internal drift acting solely on the parental process. We derive the statistical properties of this FLM process and find that the external drift does not influence the mean-squared displacement, whereas the internal drift leads to normal diffusion, dominating at long times in the subdiffusive Hurst exponent regime. We also investigate the intricate properties of the probability density function (PDF), demonstrating that it possesses a central Gaussian region whose expansion in time is influenced by FBM's Hurst exponent. Outside of this region, the PDF follows a non-Gaussian pattern. The kurtosis of this FLM process converges toward the Gaussian limit at long times insensitive to the extreme non-Gaussian tails. Additionally, in the presence of the external drift, the PDF remains symmetric and centered at x=vt. In contrast, for the internal drift this symmetry is broken. The results of our computer simulations are fully consistent with the theoretical predictions. The FLM model is suitable for describing stochastic processes with a non-Gaussian PDF and long-ranged correlations of the motion.
The spectroscopic properties of lead-silicate glass containing $2 \mathrm{~mol}_{2} \mathrm{MoO}_{3}$ and rare earth dopants were investigated in detail. Three glass series were prepared, varying the concentrations of...
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ISBN:
(数字)9798350377323
ISBN:
(纸本)9798350377330
The spectroscopic properties of lead-silicate glass containing $2 \mathrm{~mol}_{2} \mathrm{MoO}_{3}$ and rare earth dopants were investigated in detail. Three glass series were prepared, varying the concentrations of $\mathrm{Pr}, \mathrm{Nd}$, and Er from 0.5 to $1.5 \mathrm{~mol} \%$ each. The addition of MoO
3
was found to have a significant impact on the optical properties of the glass, manifesting in an elevation of the refractive index and a reduction in dispersion [1, 2]. The influence of molybdenum ions and rare earth dopants was examined through absorption, excitation, and luminescence spectra analyses [3]. Luminescence decay times were measured under both ambient conditions and within a temperature range spanning from 10 K to 350 K. Preliminary luminescence data for the glasses at room temperature are illustrated in Fig. 1.
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