Wavelength switching based on quantum-dot vertical-cavity surface-emitting laser

This study investigates, for the first time, static and dynamic wavelength switching characteristics of the 1.3 ??m quantum-dot vertical-cavity surface-emitting laser (QD VCSEL). The free-running QD VCSEL with ??1 and ??2 state innately is injected by a laser source with ??1 state. When the injection power exceeds the threshold power, the dominant state of the QD VCSEL changes from ??2 to ??1 state. Results of this study demonstrate that the wavelength switching based on a 1.3 ??m QD VCSEL has a simpler and more cost-effective configuration than those of previous systems.     

Structural evolution in the neutron-rich nuclei ¹⁰⁶Zr and ¹⁰⁸Zr

The low-lying states in 1??Zr and 1??Zr have been investigated by means of β-γ and isomer spectroscopy at the radioactive isotope beam factory (RIBF), respectively. A new isomer with a half-life of 620 ± 150 ns has been identified in 1??Zr. For the sequence of even-even Zr isotopes, the excitation energies of the first 2? states reach a minimum at N = 64 and gradually increase as the neutron number increases up to N = 68, suggesting a deformed subshell closure at N = 64. The deformed ground state of 1??Zr indicates that a spherical subshell gap predicted at N = 70 is not large enough to change the ground state of 1??Zr to the spherical shape. The possibility of a tetrahedral shape isomer in 1??Zr is also discussed.     

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利用考虑l能级分裂的屏蔽氢离子模型(SHML),计算高温(T=200~300eV)、高密度(ρ=1g.cm-3)下纯元素Au、Ho、Gd、Sm、Nd、Sn、Ag的Rosseland平均不透明度,以及Au与这些元素混合后的Rosseland平均不透明度,其结果与DCA/UTA及STA模型计算结果吻合较好。     

Linear optical properties of γ-modification of bismuth borate BiB3O6

The refractive index dispersion of the ??-BiB₃O₆ crystal in the wavelength range 0.43?C0.81 ??m has been measured. It has been shown that the principal refractive indices n ₁, n ₂, and n ₃ are on average higher than those of ??-BiB₃O₆, but are slightly lower than those of ??-BiB₃O₆. The temperature dependences of the rotation angle ??(T) of the optical indicatrix and birefringence ??n ₂(T) = (n ₁ ? n ₃)(T) have been studied in the temperature range 100?C963 K. It has been shown that the ??-BiB₃O₆ crystal is stable in this temperature region.     

Nuclear spin effect on recombination of H₃⁺ ions with electrons at 77 K

Utilizing different ratios of para to ortho H? in normal and para enriched hydrogen, we varied the population of para-H?? in an H?? dominated plasma at 77 K. Absorption spectroscopy was used to measure the densities of the two lowest rotational states of H??. Monitoring plasma decays at different populations of para-H?? allowed us to determine the rate coefficients for binary recombination of para-H?? and ortho-H?? ions: (p)α(bin)(77 K) = (1.9 ± 0.4) × 10?? cm3 s?1 and (o)α(bin)(77 K) = (0.2 ± 0.2) × 10?? cm3 s?1.     

Distinct Photoacidity of Honokiol from Magnolol

Honokiol, 5,5??-diallyl-2,4??-dihydroxy- biphenyl, by comparison with its isomer magnolol, 5,5??-diallyl- 2,2??-dihydroxy- biphenyl, has been characterized by steady-state and time-resolved spectroscopy as well as ¹H NMR. Honokiol shows more complex pH dependence of absorption and fluorescence characteristics compared with magnolol. Honokiol possesses much weaker acidity than magnolol both in the ground and excited states. Its weak photoacidity is similar to that of 4-hydroxy- biphenyl or 4, 4??-dihydroxy- biphenyl rather than 2-hydroxy- biphenyl or 2, 2??-hydroxy- biphenyl. The electron effect and geometry configuration of substitution has been discussed.     

The Dirac particle in a one-dimensional “hydrogen atom”

Specific features of the behavior of the spectrum of steady states of the Dirac particle in a regularized ??Coulomb?? potential V??(z) = ?q/(|z| + ??) as a function of the cutting parameter of ?? in 1 + 1 D are investigated. It is shown that in such a one-dimensional relativistic ??hydrogen atom?? at ?? ? 1, the discrete spectrum becomes a quasi-periodic function of ??; this effect depends on the bonding constant analytically and has no nonrelativistic analog. This property of the Dirac spectral problem clearly demonstrates the presence of a physically containable energy spectrum at arbitrary small ?? > 0 and simultaneously the absence of the regular limiting transition to ?? ?? 0. Thus, the necessity of extension of a definition for the Dirac Hamiltonian with irregularized potential in 1 + 1 D is confirmed at all nonzero values of the bonding constant q. It is also noted that the three-dimensional Coulomb problem possesses a similar property at q = Z?? > 1, i.e., when the selfconsistent extension is required for the Dirac Hamiltonian with an irregularized potential.     

Reconstruction of the coordinate dependences of quadratic susceptibility tensor \hat \chi ^{(2)} (z, ω1 ± ω2; ω1, ±ω2) components for the one-dimensionally inhomogeneous absorbing medium

A method for the unambiguous reconstruction of the spatial profiles of all components (except for ?? _zzz ) of the quadratic susceptibility complex tensor {ie165-2} (z, ??₁ + ??₂; ??₁, ??₂), which is responsible for the sumfrequency generation in a one-dimensionally inhomogeneous plate is proposed and proven for the first time. Such reconstruction is possible if the symmetry of the medium provides the diagonal character of the linear permittivity tensor {ie165-3} (z, ??). The procedure involves the measurement of the complex amplitude of the new wave with the frequency ??₁ + ??₂ that is reflected from the plate for a certain interval of the angles of incidence of the wave with the frequency ??₂. The reflected wave results from the nonlinear interaction of the wave with frequency ??₂ and the wave with frequency ??₁ that exhibits the normal incidence. A similar approach can be used to determine the profiles of the components of the quadratic susceptibility tensor {ie165-4}(z, ??₁ ? ??₂; ??₁, ? ??₂), which is responsible for the difference-frequency generation.     

Anchoring energy and orientational elasticity of a ferroelectric liquid crystal

The dielectric susceptibility of a helix-free ferroelectric liquid crystal layer has been experimentally and theoretically studied as a function of the layer thickness. The investigation has been performed on the inner branch of the polarization hysteresis loop, in the region of a linear dependence of the polarization on the electric field. The experimental results are explained using the notion of effective layer thickness, which involves the characteristic distance ?? over which the orienting effect of interfaces is operative. Comparison of the experimental data and theoretical results made it possible to estimate this distance as ?? = 41 ??m and evaluate the anchoring energy (W = 2.8 × 10^?3?1.1 × 10^?2 J/m²) and the intralayer elastic constant (K?? ?? 1 × 10^?8?3 × 10^?7 N).     

Systematics of M4 transitions

Reduced probabilities of known ?? transitions of M4 multipolarity are analyzed. Hindrance factors of 95 M4 transitions are calculated and presented. It is shown that the investigated M4 transitions are inhibited in regard to estimates using Moszkovsky formulas, and their mean hindrance factor is 5.5. The factors are close to unity in two cases only, but the intensity of a weak M4 transition could be overestimated in an experiment due to the summation effect. Dependences of the hindrance factors on the number of protons and neutrons are shown for M4 transitions between states with dominant single-particle components ??1g9/2 ?? ??2p1/2, ??1h11/2 ?? ??2d3/2, and ??1i13/2 ?? ??2f5/2.     

Heat capacity of the 0.7PbNi1/3Nb2/3O3-0.3PbTiO3 ferroelectric ceramics

The temperature dependence of the heat capacity of the 0.7PbNi_1/3Nb_2/3O₃-0.3PbTiO₃ compound has been studied in the temperature range 120?C800 K. The temperature dependence of the heat capacity C _p has two diffuse anomalies in the temperature ranges 250?C450 K and 450?C650 K and a ?? anomaly at temperatures T ?? 225 K. The results are discussed with inclusion of the dielectric and structural data.     

Dielectric properties and specific heat of the (1 ? x)PbNi1/3Nb2/3O3-xPbTiO3 ferroelectric ceramics

The temperature dependences of the permittivity and specific heat of a mixed (1 ? x)PbNi_1/3Nb_2/3O₃-xPbTiO₃ system (where x = 0.3, 0.4, 0.5) have been studied over a wide temperature range 290?C700 K. It has been shown that the composition with x = 0.3 undergoes a diffuse phase transition at T _m ?? 315 K. A specific heat anomaly that is characteristic of the phase transition has been revealed at T ?? 315 K in all the compositions under study.     

Beats of quantum oscillations of the hall coefficient and resistivity in semiconductor alloys n-Bi0.93Sb0.07 at a small deviation of the magnetic field direction from the trigonal axis

Quantum oscillations of the resistivity ??₂₂ and Hall coefficient R _12.3 in the semiconductor alloy n-Bi_0.93Sb_0.07 have been studied at H ?? C ₃ and j ?? C ₁ in magnetic fields to 14 T and at temperatures of 1.5, 4.5, 10, and 20 K. At temperatures of 1.5 and 4.5 K, beats of quantum oscillations of ??₂₂ and R _12.3 due to a small deviation of the magnetic field H from the crystallographic C ₃ axis have been observed. To determine the oscillation period ?? _i , cyclotron mass m _ci , cyclotron frequency ?? _ci , and extreme section S _extri, experimentally measured quantum oscillation beats have been compared with the model beats of oscillations of three harmonic functions, two of which have close frequencies. The deviation of the parameters ?? _i , m _ci , and S _extri from the same parameters when the magnetic field H exactly coincides with the trigonal C ₃ axis has made it possible to estimate the magnetic field H deflection angle from the trigonal C ₃ axis, which is ??1°.     

Effect of contamination with iron on the electron-beam-induced current contrast of extended defects in multicrystalline silicon

The effect of contamination with iron on the recombination activity of extended defects in multicrystalline silicon has been studied by the electron-beam-induced current (EBIC) technique. It has been shown that this process does not lead to the appearance of EBIC contrast of the ??3 and ??9 grain boundaries. It has been revealed that iron diffusion results in a significant increase in the contrast of dislocations introduced by plastic deformation and of traces behind the dislocations in single-crystal silicon, while the dislocation contrast in multicrystalline silicon remains practically unchanged.     

Splitting of the electromagnetically induced transparency resonance on 85Rb atoms in strong magnetic fields up to the Paschen-Back regime

Electromagnetically induced transparency (EIT) resonance in strong magnetic fields of up to 1.7 kG has been investigated with the use of a 30-??m cell filled with an atomic rubidium vapor and neon as a buffer gas. The EIT resonance in the ?? system of the D₁ line of ⁸⁵Rb atoms has been formed with the use of two narrowband (??1 MHz) 795-nm diode lasers. The EIT resonance in a longitudinal magnetic field is split into five components. It has been demonstrated that the frequencies of the five EIT components are either blue- or red-shifted with an increase in the magnetic field, depending on the frequency ??_P of the probe laser. In has been shown that in both cases the ⁸⁵Rb atoms enter the hyperfine Paschen-Back regime in magnetic fields of >1 kG. The hyperfine Paschen-Back regime is manifested by the frequency slopes of all five EIT components asymptotically approaching the same fixed value. The experiment agrees well with the theory.     

Disturbed oscillatory brain dynamics in subcortical ischemic vascular dementia

Background

This study examined the effects of dietary polyunsaturated fatty acids (PUFA) as different n-6: n-3 ratios on spatial learning and gene expression of peroxisome- proliferator-activated receptors (PPARs) in the hippocampus of rats. Thirty male Sprague?CDawley rats were randomly allotted into 3 groups of ten animals each and received experimental diets with different n-6: n-3 PUFA ratios of either 65:1, 22:1 or 4.5:1. After 10?weeks, the spatial memory of the animals was assessed using the Morris Water Maze test. The expression of PPAR?? and PPAR?? genes were determined using real-time PCR.

Results

Decreasing dietary n-6: n-3 PUFA ratios improved the cognitive performance of animals in the Morris water maze test along with the upregulation of PPAR?? and PPAR?? gene expression. The animals with the lowest dietary n-6: n-3 PUFA ratio presented the highest spatial learning improvement and PPAR gene expression.

Conclusion

It can be concluded that modulation of n-6: n-3 PUFA ratios in the diet may lead to increased hippocampal PPAR gene expression and consequently improved spatial learning and memory in rats.     

Preparation of cytocompatible luminescent and magnetic nanohybrids based on ZnO, Zn0.95Ni0.05O and core@shell ZnO@Fe2O3 polymer grafted nanoparticles for biomedical imaging

ZnO, Zn_0.95Ni_0.05O and core@shell ZnO@??-Fe₂O₃ nanoparticles (NPs) have been prepared by forced hydrolysis in polyol medium and then coated via the ??grafting from?? approach with poly(sodium-4-styrenesulfonate) and poly(sodium-4-styrenesulfonate?Cco?Csodium methacrylate) in the case of ZnO. The surface-initiated atom transfer radical polymerization occurred from the surface-functionalized NPs with ??-bromoisobutyric acid as initiator. The polymer chains were grown from the surface to yield hybrid NPs with a 1?C3-nm thick organic shell. FT-IR, TGA and electron microscopy evidenced the presence of a polymer layer on the surface of NPs. Magnetic and optical properties of bare and coated NPs have been measured. Eventually, the weak cytotoxicity of coated NPs on human endothelial cell allows considering their potentialities as new tools for nanomedicine and biomedical imaging.     

Magnetooptics of magnetic-dipole transitions in the rare-earth paramagnetic garnets

The Faraday effect (FE) of the rare-earth (RE) paramagnetic garnet crystals associated with magnetic-dipole (MD) transitions has been investigated theoretically over a wide temperature range 80 to 300 K. Over this temperature range, the ??gyromagnetic?? Verdet V _gm ^(m) of the Eu₃Ga₅O₁₂ (EuGG) is not a linear function of the magnetic susceptibility ?? measured along the [111] axis. We find that the nontrivial character of the temperature dependence of the MD Verdet constant V _gm ^(m) is associated with the presence of a contribution to the Faraday rotation of the Van Vleck ??mixing?? by an external magnetic field of the Eu³⁺ electronic states. The optical absorption and magnetic circular dichroism (MCD) of Eu³⁺ ion in EuGG at 85 K for the MD transition ⁷ F ₀ ?? ⁵ D ₁ were measured along the [111] axis. We show that the appearance of the MCD feature observed for the absorption line near 526.6 nm for the ⁷ F ₀ ?? ⁵ D ₁ MD absorption band may be well-explained by the contribution of Van Vleck ??mixing?? between the Stark singlet states from the ⁷ F ₀ and ⁷ F ₁ multiplet manifolds mixed by the external magnetic field H.     

Energy migration toward a dye in nanoparticles from complexes with short fluorescent state lifetimes

We have studied regular features of the fluorescence sensitization (cofluorescence) of coumarin 30 and rhodamine 6G introduced into nanoparticles from complexes Ln(PhBTA)₃phen, where PhBTA is p-phenylbenzoyltrifluoroacetone and Ln is a triply charged Pr, Nd, Sm, Eu, Er, or Yb ion, which absorbs in the fluorescence range of ligands of complexes and dyes. We show that both the cofluorescence intensities (I _cofl) of rhodamine 6G in nanoparticles from Sm and Eu complexes and the behavior of intensity I _cofl on the content of rhodamine 6G coincide with the corresponding data obtained for nanoparticles from La and Lu complexes doped with rhodamine 6G molecules. A considerable decrease in I _cofl of rhodamine 6G is observed only in nanoparticles from complexes Nd(PhBTA)₃phen. In nanoparticles from Pr, Nd, Sm, Eu, Er, and Yb complexes doped with coumarin 30, it has been observed that, depending on the choice of the central ion, I _cofl of coumarin 30 is 2 to 80 times lower compared to I _cofl of the dye in nanoparticles from La and Lu complexes. A separate analysis of the influence of these ions on the energy transfer from complexes to coumarin 30 and on the fluorescence intensity of coumarin 30 incorporated into nanoparticles from these ions showed that a decrease in I _cofl of coumarin 30 by a factor of 2?C20 occurs due to the reduction of ??_fl of ligands of complexes under the influence of the interaction with Pr, Nd, Sm, Eu, Er, and Yb ions. Since ??_fl of complexes La(PhBTA)3phen is ??2 ps, while that of complexes Gd(PhBTA)3phen is ??1 ps, then, in nanoparticles with a maximal decrease in I _cofl of coumarin 30, ??_fl of complexes is reduced to ??0.1 ps. It has been found that, in nanoparticles from complexes with this ??_fl, energy migration over complexes takes place. However, as distinct from nanoparticles from La, Lu, and Y complexes, the free path length of singlet excitons in nanoparticles from complexes of absorbing ions is smaller than the nanoparticle size.     

Numerical simulation of nonlinear properties of fullerene-containing one-dimensional photonic crystal

A model of interaction between a one-dimensional photonic crystal (PC) containing a defect (nonlinear optical layer of C₆₀ fullerene) and radiation with a wavelength ??₀= 1064 nm under steady-state conditions has been considered. This structure is a Fabry-Perot microcavity: a fullerene layer (with a thickness multiple of ??₀/2) is placed between the interference mirrors formed by alternating layers ??₀/4 thick. The PC under consideration (1) has a narrow transmission band in the vicinity of ??₀ against the background of a relatively wide 100%-reflection band (photonic band gap) in the linear mode and (2) provides multiple amplification of the radiation intensity in the intermediate layer with respect to the external radiation intensity. Since C₆₀ fullerene exhibits a significant optical Kerr nonlinearity, the optical thickness of the intermediate layer under irradiation deviates from the value multiple of ??₀/2; as a result, 100% transmission for ??₀ changes to almost 100% reflection at a certain radiation intensity. Thus, this structure behaves as a peculiar optical limiter.