Critical currents due to flux pinning in cylinders of type I superconductor (Pb-Ag)

Some preliminary studies of flux pinning in cylinders of type I superconductors are reported (12 μ silver powder in lead). These show that when a magnetic field appreciably greater than $\text{1}\text{2}\text{H}{}_{\mathrm{c}}$ is applied perpendicular to the sample axis, the critical current densities are fairly small (e.g. 5.5 × 10⁶ Am^-2 at $\text{3}\text{4}\text{H}{}_{\mathrm{c}}$), but are of the same order that one might expect in a low κ type II superconductor with similar pinning, and that the critical current density is directly proportional to the density of pinning centres in the material, surface currents playing no important role.     

Critical current density and flux pinning in an unconventional superconductor

The functional dependence of the critical current density on magnetic field, Jc(H), observed at fixed temperatures in the unconventional type-II superconductor, LaAg1−cMnc (c=0.1,0.2,0.3) alloys, but not the relative magnitude of Jc in different alloy compositions at any given temperature and field, is adequately described by the exponential-decay critical state model. In accordance with the predictions of the Kramer's flux-pinning model, the peak value of the pinning force density with the exponent 1.7?m?2.8 and scales with h=H/Hc₂, where Hc₂ is the upper critical field. Irrespective of sample composition and temperature in the superconducting state, the pinning of the flux line lattice (FLL) dominates over the plastic FLL shear.     

Correlation between vortex lattice and crystal lattice in type II superconductors due to elastic interaction

In an elastic anisotropic crystal certain orientations of the vortex lattice with respect to the crystal lattice are favoured due to the magneto-elastic strain fields of the vortex lattice.     

Flux flow current-voltage characteristics and their magnetic field dependence in a type II superconductor

Experimental flux flow V-I characteristics are compared with our previous model which assumes flux motion is interrupted by local pinning interactions. Quantitative changes in these characteristics occur at the field at which the peak in the pinning force occurs.     

Unstable flux flow due to heated electrons in superconducting films

A flux instability occurs in superconductors at low temperatures, where e-e scattering is more rapid than e-ph, whereby the dissipation significantly elevates the electronic temperature while maintaining a thermal-like distribution function. The reduction in condensate and rise in resistivity produce a nonmonotonic current-voltage response. In contrast to the Larkin-Ovchinnikov instability where the vortex shrinks, in this scenario the vortex expands and the quasiparticle population rises. Measurements in Y(1)Ba(2)Cu(3)O(7-delta) agree quantitatively with the distinct predictions of this mechanism.     

Observation of record flux pinning in melt-textured NEG-123 superconductor doped by Nb, Mo, and Ti nanoparticles

Flux pinning in melt-processed (Nd_0.33Eu_0.33Gd_0.33)Ba₂Cu₃O_y “NEG-123” + 35 mol% Gd₂BaCuO₅ “NEG-211” (70 nm in size) composite doped by TiO₃, MoO₃ and Nb₂O₅ achieved record values. The optimum values of all three dopands were found to be around 0.1 mol%. Transmission electron microscope (TEM) analysis found clouds of <10 nm sized particles in the NEG-123 matrix, shifting the pinning particle size distribution to significantly lower values. TEM by energy dispersive X-ray spectroscopy (EDX) analysis clarified that these nanoparticles contained a significant amount of Nb, Mo, and Ti. Appearance of nanometer-sized defects correlated with a significantly improved flux pining at low and medium magnetic fields, which was particularly significant at high temperatures. In the Nb-doped sample, a record J_c value of 925 kA/cm² at the secondary peak field (4.5 T) was achieved at 65 K, 640 kA/cm² at zero field at 77 K, and 100 kA/cm² at 90.2 K, the last value having been up to now considered as a good standard for REBa₂Cu₃O_y “RE-123” materials at 77 K. The greatly improved J_c–B performance in Nb/Mo/Ti doped samples can be easily translated to large-scale LRE-123 (LRE = light rare earths, Nd, Eu, Gd, Sm) blocks intended for real superconducting super-magnets applications.     

Irreversibility line and flux pinning properties in iron-based high-Tc superconductor SmFeAsO0.85

The irreversibility line and flux pinning properties of high-T_c superconductor SmFeAsO_0.85 were studied using DC magnetization data. Polycrystalline SmFeAsO_0.85 was prepared in a high pressure synthesis apparatus under the pressure of 6 GPa. The results of DC susceptibility showed the superconducting transition at about 55 K. A critical current density J_c(B) was calculated using Bean’s critical state model. At low temperatures (20 K), J_c(B) showed a relatively high value with weak dependence on an applied magnetic field. At higher temperatures, a stronger dependence of the magnetic field was observed, which resulted from decrease in a critical current density probably due to the flux creep effect. The irreversibility line (IL) agreed well with the flux creep theory of Matsushita et al. A comparison of normalized pinning force density with the theoretical models showed that the irreversible behavior in SmFeAsO_0.85 is dominated mainly by normal point pinning (δT_c) and surface pinning mechanisms.     

All-optical bistability due to charge transfer in a type II heterostructure

We report bistability of low temperature photoluminescence in a n-i-n type II GaAs/AlGaAs/AlAs heterostructure. The luminescence intensity ratio between the two states reaches 50, and no external bias is needed. The bistability range lies between 40 and 280 W/cm². The two states are thought to correspond to different charge accumulations in the structure. The redistribution of charges is due to competition between slow type II and fast type I recombination in the center of the structure.     

高温超导体磁通钉扎和磁通动力学研究简介

ψ=ψ0eiφ行为用统一的波函数进行描述,其相位φ在宏观尺度上是相同的.当磁场低于一定值的时候,在超Φ0=h/2e保证最大的界面面积,降低系统能量.该最小的磁通束被称为磁通量子,其磁通量是(h为普朗克超导态是一个宏观量子相干态,其载流子是库珀对.在没有外加磁场和电流的时候,这些库珀对的运动导体的边界处穿透深度内会出现一...     

Direct observation of the flux-line vortex glass phase in a type II superconductor

The order of the vortex state in La1.9Sr0.1CuO4 is probed using muon-spin rotation and small-angle neutron scattering. A transition from a Bragg glass to a vortex glass is observed, where the latter is composed of disordered vortex lines. In the vicinity of the transition the microscopic behavior reflects a delicate interplay of thermally induced and pinning-induced disorder.     

The non-linear dynamics of vortices subjected to correlated and random pinning disorders in a quasi-2D superconductor

Understanding the dynamics of vortex matter subjected to random and correlated pinning disorders in layered superconductors remains a topic of considerable interest. The dynamical behavior of vortices in these systems shows a rich variety of effects due to many competing interactions. Here, we study the ac response of as-grown as well as heavy-ion-irradiated Tl₂Ba₂CaCu₂O₈ (Tl-2212) thin films by using a micro Hall-probe susceptometer. We find that the dynamics of vortices in the high-temperature, low-field regime of the H-T phase diagram investigated here depends on the nature of pinning defects. While the decay of screening currents J(t) indicates a glassy behavior in both types of samples, the nature of the glassy phase is different in the two cases. Samples with columnar defects show distinct signature of a Bose glass in the measurement of J(t) and the angular dependence of the irreversibility field (B irr).     

Estimate of the core size of a vortex in an extreme type II superconductor

The core size of a single straight vortex in an extreme type II superconductor is estimated at zero temperature. The free energy is expressed as a non-local functional of the order parameter and vector potential associated with the vortex. Profiles for the order parameter and vector potential that depend on the length scales ξ and λ, respectively, are assumed. For an order parameter profile that achieves its bulk value after the finite distance, ξ, the free energy approximately separates into a sum of two contributions, one depending on the order parameter and the other on the magnetic field. Using two different approximation schemes the two parts of the free energy are minimised. For an order parameter profile that, in its region of change, varies linearly with distance from the vortex axis, the length scale ξ is found to be comparable with the zero temperature coherence length, in agreement with the findings of Ullah et al. (Phys. Rev. B 42 (1990), 9950) for a one-parameter fit to the order parameter. The length scale associated with the magnetic field is also estimated.     

Relationship between low-frequency aircraft noise and annoyance due to rattle and vibration

A near-replication of a study of the annoyance of rattle and vibration attributable to aircraft noise [Fidell et al., J. Acoust. Soc. Am. 106, 1408-1415 (1999)] was conducted in the vicinity of Minneapolis-St. Paul International Airport (MSP). The findings of the current study were similar to those reported earlier with respect to the types of objects cited as sources of rattle in homes, frequencies of notice of rattle, and the prevalence of annoyance due to aircraft noise-induced rattle. A reliably lower prevalence rate of annoyance (but not of complaints) with rattle and vibration was noted among respondents living in homes that had been treated to achieve a 5-dB improvement in A-weighted noise reduction than among respondents living in untreated homes. This difference is not due to any substantive increase in low-frequency noise reduction of acoustically treated homes, but may be associated with installation of nonrattling windows. Common interpretations of the prevalence of a consequential degree of annoyance attributable to low-frequency aircraft noise may be developed from the combined results of the present and prior studies.     

Correlation between structural changes and luminescent properties of ZnMgS:Mn thin film phosphor with annealing temperature

With varying rapid thermal annealing temperature, luminescent properties of Zn_0.75Mg_0.25S:Mn thin film deposited by RF-magnetron sputtering technique were investigated. Although all samples were deposited from identical source composition, it was found that a main peak wavelength of photoluminescence of Zn_0.75Mg_0.25S:Mn depended on RTA temperatures and it shifted toward shorter wavelength upon the increase of RTA temperature. The same dependence of wavelength on RTA temperature was also observed in cathodoluminescence as well as electroluminescence measurements. It is noticeable that Zn_0.75Mg_0.25S:Mn thin film phosphor in this study showed more reddish emission than those of the previous studies.It was revealed that changes of the luminescent properties were originated from structural changes in Zn_0.75Mg_0.25S:Mn thin film phosphor from cubic to hexagonal phases using X-ray pole figure mapping, and the growing up of hexagonal phase mainly caused cracks and porous morphology on the surface of thin films. It is suggested that the phase transition would be the origin of luminescent property changes with respect to rapid thermal annealing temperature.     

Correlation between amplitude and phase noise in a mode-locked Cr:LiSAF laser

The coherence function between the amplitude and phase fluctuations of a mode-locked Cr:LiSAF laser has been measured with a time-domain demodulation technique. A relatively large correlation has been found for the noise components that originate in the pump-power fluctuation. Through an examination of the modulation-induced change in the noise power spectral densities, the influences of pump-power and cavity-length variations on these fluctuations have been investigated.     

Dephasing of a qubit due to quantum and classical noise

The qubit (or a system of two quantum dots) has become a standard paradigm for studying quantum information processes. Our focus is decoherence due to interaction of the qubit with its environment, leading to noise. We consider quantum noise generated by a dissipative quantum bath. A detailed comparative study with the results for a classical noise source such as generated by a telegraph process, enables us to set limits on the applicability of this process vis à vis its quantum counterpart, as well as lend handle on the parameters that can be tuned for analysing decoherence. Both Ohmic and non-Ohmic dissipations are treated and appropriate limits are analysed for facilitating comparison with the telegraph process.