6,900 research outputs found
Maxwell-Hydrodynamic Model for Simulating Nonlinear Terahertz Generation from Plasmonic Metasurfaces
The interaction between the electromagnetic field and plasmonic
nanostructures leads to both the strong linear response and inherent nonlinear
behavior. In this paper, a time-domain hydrodynamic model for describing the
motion of electrons in plasmonic nanostructures is presented, in which both
surface and bulk contributions of nonlinearity are considered. A coupled
Maxwell-hydrodynamic system capturing full-wave physics and free electron
dynamics is numerically solved with the parallel finite-difference time-domain
(FDTD) method. The validation of the proposed method is presented to simulate
linear and nonlinear responses from a plasmonic metasurface. The linear
response is compared with the Drude dispersion model and the nonlinear
terahertz emission from a difference-frequency generation process is validated
with theoretical analyses. The proposed scheme is fundamentally important to
design nonlinear plasmonic nanodevices, especially for efficient and broadband
THz emitters.Comment: 8 pages, 7 figures, IEEE Journal on Multiscale and Multiphysics
Computational Techniques, 201
Full Hydrodynamic Model of Nonlinear Electromagnetic Response in Metallic Metamaterials
Applications of metallic metamaterials have generated significant interest in
recent years. Electromagnetic behavior of metamaterials in the optical range is
usually characterized by a local-linear response. In this article, we develop a
finite-difference time-domain (FDTD) solution of the hydrodynamic model that
describes a free electron gas in metals. Extending beyond the local-linear
response, the hydrodynamic model enables numerical investigation of nonlocal
and nonlinear interactions between electromagnetic waves and metallic
metamaterials. By explicitly imposing the current continuity constraint, the
proposed model is solved in a self-consistent manner. Charge, energy and
angular momentum conservation laws of high-order harmonic generation have been
demonstrated for the first time by the Maxwell-hydrodynamic FDTD model. The
model yields nonlinear optical responses for complex metallic metamaterials
irradiated by a variety of waveforms. Consequently, the multiphysics model
opens up unique opportunities for characterizing and designing nonlinear
nanodevices.Comment: 11 pages, 14 figure
Application of nursing core competency standard education in the training of nursing undergraduates
AbstractPurposeTo evaluate the effectiveness of nursing core competency standard education in undergraduate nursing training.MethodsForty-two nursing undergraduates from the class of 2007 were recruited as the control group receiving conventional teaching methods, while 31 students from the class of 2008 were recruited as the experimental group receiving nursing core competency standard education. Teaching outcomes were evaluated using comprehensive theoretical knowledge examination and objective structured clinical examination.ResultsThe performance in the health information collection, physical assessment, scenario simulation and communication in the experimental group were significantly higher than those of the control group (p < 0.05).ConclusionsNursing core competency standard education is helpful for the training of nursing students' core competencies
(4-CarbÂoxy-2-sulfonatoÂbenzoato-Îş2 O 1,O 2)bisÂ(1,10-phenanthroline-Îş2 N,N′)manganese(II)
In the title complex, [Mn(C8H4O7S)(C12H8N2)2], the MnII atom is chelated by one 4-carbÂoxy-2-sulfonatoÂbenzoate anion and two phenathroline (phen) ligands in a distorted octaÂhedral MnN4O2 geometry. The benzene ring of the 4-carbÂoxy-2-sulfonatoÂbenzoate anion is twisted with respect to the two phen ring systems at dihedral angles of 66.38 (9) and 53.56 (9)°. In the crystal, interÂmolecular O—Hâ‹ŻO and C—Hâ‹ŻO hydrogen bonding links the molÂecules into chains running parallel to [100]. InterÂmolecular π–π stacking is also observed between parallel phen ring systems, the face-to-face distance being 3.432 (6) Å
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