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91.
Si-Qi Li Chao-Hai Du Da-Li Yin Xin-Wei Cai Tie-Quan Xu Yue Wang Fan-Hong Li Yu Zhu Feng Zhang 《Advanced functional materials》2023,33(47):2305789
Recently, skyrmions are constructed in the system of localized spoof surface plasmons (LSSPs), showing topological robustness and near-equidistant multi-resonant response. Guided wave excitation of the LSSP skyrmions plays an elementary role in large-scale planar integration and construction of complex networks. However, it is not investigated. In this study, the LSSP skyrmions are excited by guided waves supported by two kinds of widely used transmission lines, microstrip line and coplanar waveguide. Space-coiling meta-structures with different shapes that support LSSP skyrmions are etched on the ground planes as defected ground structures (DGSs). All structures including resonator, transmission line, input and output ports are in one plane. The structures are fabricated on printed circuit boards (PCBs) and the near-equidistant multi-resonant spectra of the LSSP skyrmions are measured. Moreover, to reduce the material loss, the structure is made on MgB2 superconducting film, and the quality factor (Q-factor) is increased by seven times compared to the corresponding mode on PCB. This study paves the way for the massive planar integration of the LSSP skyrmions and the construction of complex networks with the LSSP skyrmions, and provides an idea for developing metasurfaces with low material loss in the microwave and terahertz bands. 相似文献
92.
Wu Shi Yu 《Transport in Porous Media》1987,2(2):103-127
This paper deals with the flow through a layered medium that has alternate sand and clay strata. The solutions of plane, axisymmetric and spatial cases are given. Research results in this paper can be applied to seepage calculations and hydraulic engineering designs in flood areas and reclaimed marsh land.List of Symbols
A
n
Upward leakage factor of the nth sand stratum
-
A
n
Downward leakage factor of the nth sand stratum
- [B]
Matrix of eigenvector
-
B
nm
Element of [B] corresponding to the nth sand stratum and the mth eigenvalue
-
C
m
, C
N+m
Arbitrary constants belonging to the terms contained the mth eigenvalue
- Cmj
Arbitrary constant belonging to the term contained the mth eigenvalue due to a line source in the jth sand stratum
- [D]
Inverse matrix of [B]
-
d
f0
sup+
Additional length of the seepage path for ditches in symmetric flow
-
F,
F
m
Area and dimensionless area corresponding to the mth eigenvalue (
F
m
=
fm
sup2
F)
-
f
0
Coefficient of additional resistance of partially penetrating well
-
H
Total water head; upstream water head
-
h, h
n
Water head and water head of the nth sand stratum
-
h
nj
Water head of the nth sand stratum due to a line source in the jth sand stratum
-
h
0
Surface water head
-
h/H × 100%
Potential
-
i, j
Number
-
k, k
Permeability coefficient of the sand stratum and clay stratum, respectively
-
k
n
, k
n
Permeability coefficient of the nth sand stratum and the nth clay stratum, respectively
-
L
Length
-
m
Number
-
N
Total number of sand or clay strata
-
n
Number
-
Q
j
Discharge of a line source distributed along a vertical line in the jth sand stratum
-
Q
ji
The partial discharge of the ith well (or line source), which flows through the screen pipe penetrating the jth sand stratum
-
qj
Discharge of a face source distributed on an area - unit breadth multiplied by the thickness of the jth sand stratum. The abbreviation is: unit discharge of a face source in the jth sand stratum
-
qji
Unit discharge of a face source on the ith surface element in the jth sand stratum
-
R
Constant radius
-
S
Distance; length of a curve
-
S
m
Dimensionless length of a curve corresponding to the mth eigenvalue (
S
m
=
m
S)
-
s
Number
-
T
n
, T
n
Thickness of the nth sand stratum and the nth clay stratum, respectively
-
t
Number; thickness
-
x, y, z
Cartesian coordinates
-
y
Polar coordinate; radius; distance
-
y
m
Dimensionless distance corresponding to the mth eigenvalue (
y
m
=
m
y)
-
y
0
Radius of well
-
y
0
Radius of equivalent completely penetrating well
-
Infinitesimal half breadth
-
Infinitesimal area
-
Angle
-
Eigenvalue 相似文献
93.
S. C. Bradley R. Bulla A. C. Hewson G -M. Zhang 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,11(4):535-550
The O(3) symmetric Anderson model is an example of a system which has a stable low energy marginal Fermi liquid fixed point
for a certain choice of parameters. It is also exactly equivalent, in the large U limit, to a localized model which describes the spin degrees of freedom of the linear dispersion two channel Kondo model.
We first use an argument based on conformal field theory to establish this precise equivalence with the two channel model.
We then use the numerical renormalization group (NRG) approach to calculate both one-electron and two-electron response functions
for a range of values of the interaction strength U. We compare the behaviours about the marginal Fermi liquid and Fermi liquid fixed points and interpret the results in terms
of a renormalized Majorana fermion picture of the elementary excitations. In the marginal Fermi liquid case the spectral densities
of all the Majorana fermion modes display a dependence on the lowest energy scale, and in addition the zero Majorana mode has a delta function contribution. The weight
of this delta function is studied as a function of the interaction U and is found to decrease exponentially with U for large U. Using the equivalence with the two channel Kondo model in the large U limit, we deduce the dynamical spin susceptibility of the two channel Kondo model over the full frequency range. We use renormalized
perturbation theory to interpret the results and to calculate the coefficient of the ln divergence found in the low frequency behaviour of the T=0 dynamic susceptibility.
Received 29 January 1999 相似文献
94.
95.
Ashraf A. Mohamed 《Monatshefte für Chemie / Chemical Monthly》2001,132(8):919-928
Summary. A new selective, sensitive, and simple kinetic method is developed for the determination of trace amounts of iodide. The
method is based on the catalytic effect of iodide on the reaction of triflupromazine (TFP) with H2O2. The reaction is followed spectrophotometrically by tracing the oxidation product at 498 nm within 1 min after addition of
H2O2. The optimum reaction conditions are TFP (0.4 × 10−3
M), H2SO4 (1.0M), H3PO4 (2.0M), and H2O2 (1.6M) at 30°C. Following this procedure, iodide can be determined with a linear calibration graph up to 4.5 ng ċ cm−3 and a detection limit of 0.04 ng ċ cm−3, based on the 3 Sb criterion. The method can also be applied to the determination of iodate and periodate ions. Determination of as little as
0.2, 1.0, 2.0, and 4.0 ng ċ cm−3 of I−, IO3
-, or IO4
- in aqueous solutions gave an average recovery of 98% with relative standard deviations below 1.6% (n = 5). The method was applied to the determination of iodide in Nile river water and ground waters as well as in various food
samples after alkaline ashing treatment. The method is compared with other catalytic spectrophotometric procedures for iodide
determination.
Received January 19, 2001. Accepted (revised) March 12, 2001 相似文献
96.
A.Yu. Cherny A.A. Shanenko 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,19(4):555-564
The modified Bogoliubov model where the primordial interaction is replaced by the t matrix is reinvestigated. It is shown to provide a negative value of the kinetic energy for a strongly interacting dilute
Bose gas, contrary to the original Bogoliubov model. To clear up the origin of this failure, the correct values of the kinetic
and interaction energies of a dilute Bose gas are calculated. It is demonstrated that both the problem of the negative kinetic
energy and the ultraviolet divergence, dating back to the well-known paper of Lee, Yang and Huang, is connected with an inadequate
picture of the short-range boson correlations. These correlations are reconsidered within the thermodynamically consistent
model proposed earlier by the present authors. Found results are in absolute agreement with the data of the Monte-Carlo calculations
for the hard-sphere Bose gas.
Received 10 February 2000 and Received in final form 28 November 2000 相似文献
97.
This paper examines an asymptotic analysis for predicting sound fields above a rigid-frame porous medium, the so-called non-locally reacting porous medium. Their solutions can be represented by a direct wave term, a reflected wave term and a diffraction wave term. Exact and analytical solutions are available for the direct wave and the reflected wave from a perfectly hard ground. In the contrary, the diffraction wave term can only be cast in an integral form that is amenable to approximate analysis. A modified saddle-point method is explored to evaluate the diffraction integral asymptotically. Three different types of non-locally reacting surfaces, which are an extended reaction, a hard-backed layer, and an impedance-backed layer, were considered. The sound fields above these porous surfaces have the same form but they are different by an augmented diffraction term in the solutions. The analytical formula for the total sound fields, which can be stated in a closed form, offer a physically interpretable solution comprising of a direct wave and ground reflected wave terms. This latter term can further be split into a specularly reflected plane wave and ground wave components. A series of numerical comparisons have been conducted to validate the asymptotic analyses presented in this study. It has been demonstrated that the overall sound fields can be predicted well by the formula for all incidence angles and for a wide range of non-locally reacting porous surfaces. 相似文献
98.
近断层地震作用下钢筋混凝土连续梁桥地震易损性分析 总被引:1,自引:0,他引:1
考虑桥墩、支座构件及主梁的碰撞损伤指标,对钢筋混凝土连续梁桥进行了地震易损性分析.综合考虑了结构参数的不确定性,从太平洋地震工程研究(Paciflc earthquake engineering research,PEER)数据库中随机选取了20条近场地震记录,得到大量的随机地震-结构样本.结合不同破坏状态下的桥梁损伤指标,根据结构的能力与需求得到了桥梁各构件及整体桥梁结构的地震易损性曲线.从概率意义上判断在强烈地震作用下桥梁结构所处的破坏状态,为今后在役的同类型桥梁震害预测提供了参考. 相似文献
99.
选择CaO和纯碱作为激发剂掺入GGBS(粒化高炉矿渣微粉)制备GGBS+CaO+纯碱固化合肥湖积软土,通过无侧限抗压强度试验研究固化黏土的强度变化规律。以GGBS、CaO和纯碱的掺量作为影响因子,以7d和28d固化土的无侧限抗压强度作为响应值,基于Box-Behnken法确定3种外添剂的最佳配合比。研究表明:GGBS掺量的变化对强度响应影响最大,且其敏感程度随龄期的增大而增大;而对于CaO和纯碱,情况则相反。养护7d后,各因素对强度的线性效应和曲面效应均显著,CaO与纯碱的交互作用显著;养护28d后,GGBS与纯碱的交互作用显著。最终得出:GGBS、CaO和纯碱三掺量固化黏土最佳配比分别为13.08%、4.89%和1.25%;在最佳配合比下,7d和28d的预测强度分别达到550.904kPa和665.953kPa。最后对实测值与预测值进行了对比分析。研究成果可为在合肥滨湖地区应用矿渣类软土固化剂提供理论依据。 相似文献
100.
从接地方面分析了干扰对PLC控制系统的影响和破坏,提出了一些提高PLC控制系统的可靠性和安全运行的措施,使之满足工业控制要求。 相似文献