Efficient Wideband Numerical Simulations for Nanostructures Employing a Drude-Critical Points (DCP) Dispersive Model
暂无分享,去创建一个
D. Werner | P. Werner | Yusheng Bian | Q. Ren | L. Kang | Jogender Nagar
[1] Qing Huo Liu,et al. EB Scheme-Based Hybrid SE-FE DGTD Method for Multiscale EM Simulations , 2016, IEEE Transactions on Antennas and Propagation.
[2] Lei Zhou,et al. Dynamical control on helicity of electromagnetic waves by tunable metasurfaces , 2016, Scientific Reports.
[3] J. Korterik,et al. A phased antenna array for surface plasmons , 2016, Scientific Reports.
[4] Yuebing Zheng,et al. Optimizing plasmonic nanoantennas via coordinated multiple coupling , 2015, Scientific Reports.
[5] D. Werner,et al. Handedness Dependent Electromagnetically Induced Transparency in Hybrid Chiral Metamaterials , 2015, Scientific Reports.
[6] Pierre Berini,et al. On the convergence and accuracy of the FDTD method for nanoplasmonics. , 2015, Optics express.
[7] Qing Huo Liu,et al. A New 3-D Nonspurious Discontinuous Galerkin Spectral Element Time-Domain (DG-SETD) Method for Maxwell’s Equations , 2015, IEEE Transactions on Antennas and Propagation.
[8] Nikolay I. Zheludev,et al. Coherent control of optical polarization effects in metamaterials , 2015, Scientific Reports.
[9] Feng Liu,et al. An integrative analysis of TFBS-clustered regions reveals new transcriptional regulation models on the accessible chromatin landscape , 2015, Scientific Reports.
[10] Qing Huo Liu,et al. A new efficient 3D Discontinuous Galerkin Time Domain (DGTD) method for large and multiscale electromagnetic simulations , 2015, J. Comput. Phys..
[11] Haitao Liu,et al. Role of surface plasmon polaritons and other waves in the radiation of resonant optical dipole antennas , 2015, Scientific Reports.
[12] Q. Gong,et al. Tuning the hybridization of plasmonic and coupled dielectric nanowire modes for high-performance optical waveguiding at sub-diffraction-limited scale , 2014, Scientific Reports.
[13] S. Burger,et al. The spectral shift between near- and far-field resonances of optical nano-antennas. , 2014, Optics express.
[14] N. Zheludev,et al. Coherent control of optical activity and optical anisotropy of thin metamaterials , 2013, 1312.0414.
[15] Arnold F. McKinley,et al. Theory of the circular closed loop antenna in the terahertz, infrared, and optical regions , 2013 .
[16] D. C. Zografopoulos,et al. A Unified FDTD/PML Scheme Based on Critical Points for Accurate Studies of Plasmonic Structures , 2013, Journal of Lightwave Technology.
[17] Jun Shibayama,et al. Frequency-Dependent Formulations of a Drude-Critical Points Model for Explicit and Implicit FDTD Methods Using the Trapezoidal RC Technique , 2012, IEICE Trans. Electron..
[18] S. D. Gedney,et al. A Discontinuous Galerkin Finite Element Time-Domain Method Modeling of Dispersive Media , 2012, IEEE Transactions on Antennas and Propagation.
[19] M. Wegener,et al. Past achievements and future challenges in the development of three-dimensional photonic metamaterials , 2011 .
[20] A. Kildishev,et al. Optical Dispersion Models for Time-Domain Modeling of Metal-Dielectric Nanostructures , 2011, IEEE Transactions on Magnetics.
[21] A. Vial,et al. A new model of dispersion for metals leading to a more accurate modeling of plasmonic structures using the FDTD method , 2011 .
[22] S. Chen,et al. Retardation-effect-induced plasmon modes in a silica-core gold-shell nanocylinder pair , 2010 .
[23] Yaxin Yu,et al. An E-J Collocated 3-D FDTD Model of Electromagnetic Wave Propagation in Magnetized Cold Plasma , 2010, IEEE Transactions on Antennas and Propagation.
[24] Qing Huo Liu,et al. Microwave Imaging in Layered Media: 3-D Image Reconstruction From Experimental Data , 2010, IEEE Transactions on Antennas and Propagation.
[25] M. Wegener,et al. Twisted split-ring-resonator photonic metamaterial with huge optical activity. , 2010, Optics letters.
[26] Y. H. Chang,et al. Optical singularities associated with the energy flow of two closely spaced core-shell nanocylinders. , 2009, Optics express.
[27] F. Capasso,et al. The forces from coupled surface plasmon polaritons in planar waveguides. , 2009, Optics express.
[28] Harald Giessen,et al. Three-dimensional optical metamaterials as model systems for longitudinal and transverse magnetic coupling. , 2008, Optics express.
[29] D. Davidson,et al. Numerical Evaluation of High-Order Finite Element Time Domain Formulations in Electromagnetics , 2008, IEEE Transactions on Antennas and Propagation.
[30] Thierry Laroche,et al. Comparison of gold and silver dispersion laws suitable for FDTD simulations , 2008 .
[31] F. Rachidi,et al. On the Choice Between Transmission Line Equations and Full-Wave Maxwell's Equations for Transient Analysis of Buried Wires , 2008, IEEE Transactions on Electromagnetic Compatibility.
[32] M. J. Lockyear,et al. Optical control over surface-plasmon-polariton-assisted THz transmission through a slit aperture. , 2008, Physical review letters.
[33] F. Teixeira,et al. Mixed Finite-Element Time-Domain Method for Transient Maxwell Equations in Doubly Dispersive Media , 2008, IEEE Transactions on Microwave Theory and Techniques.
[34] A. Vial,et al. Description of dispersion properties of metals by means of the critical points model and application to the study of resonant structures using the FDTD method , 2007 .
[35] Peter Nordlander,et al. Efficient dielectric function for FDTD simulation of the optical properties of silver and gold nanoparticles , 2007 .
[36] Thomas Søndergaard,et al. General properties of slow-plasmon resonant nanostructures: nano-antennas and resonators. , 2007, Optics express.
[37] A. Vial. Implementation of the critical points model in the recursive convolution method for modelling dispersive media with the finite-difference time domain method , 2007 .
[38] S. Maier. Plasmonics: Fundamentals and Applications , 2007 .
[39] F. Teixeira,et al. Mixed $E$–$B$ Finite Elements for Solving 1-D, 2-D, and 3-D Time-Harmonic Maxwell Curl Equations , 2007, IEEE Microwave and Wireless Components Letters.
[40] V. Podolskiy,et al. Compensation of loss in propagating surface plasmon polariton by gain in adjacent dielectric medium. , 2007, Optics express.
[41] P. Etchegoin,et al. An analytic model for the optical properties of gold. , 2006, The Journal of chemical physics.
[42] G. Rodrigue,et al. Vector finite-element modeling of the full-wave Maxwell equations to evaluate power loss in bent optical fibers , 2005, Journal of Lightwave Technology.
[43] Carretera de Valencia,et al. The finite element method in electromagnetics , 2000 .
[44] Qing Huo Liu,et al. The PSTD algorithm: A time-domain method requiring only two cells per wavelength , 1997 .
[45] O. Picon,et al. A finite element method based on Whitney forms to solve Maxwell equations in the time domain , 1995 .
[46] Youngjoo Chung,et al. PLRC AND ADE IMPLEMENTATIONS OF DRUDE- CRITICAL POINT DISPERSIVE MODEL FOR THE FDTD METHOD , 2013 .
[47] Qing Huo Liu,et al. A NEW 2D NON-SPURIOUS DISCONTINUOUS GALERKIN FINITE ELEMENT TIME DOMAIN (DG-FETD) METHOD FOR MAXWELL'S EQUATIONS , 2013 .
[48] V. Shalaev. Optical negative-index metamaterials , 2007 .
[49] J. Lambert. Numerical Methods for Ordinary Differential Equations , 1991 .