“…A direct inspection shows that the Green's function for this equation is given byĤ z (x; y) = i 4 H (1)…”
Section: Z +1mentioning
confidence: 99%
“…where H (1) n is the Hankel function of rst kind and order zero, and x = exp(i ). This series converges uniformly for r a 0 9].…”
Section: Z +1mentioning
confidence: 99%
“…Suppose~ = r + i~ i where~ r and~ i are real. The desired asymptotic behavior of the Hankel functions is H (1) m…”
Section: Z +1mentioning
confidence: 99%
“…This approach is easy to implement and is very e ective. It has already been the subject of numerous of papers 18,1,5,12,11,13,25,26,23,21,15,7,4,24,3]. However, to our knowledge, there has been very little theoretical analysis of the method.…”
In 1994 B erenger showed how to construct a perfectly matched absorbing layer for the Maxwell system in rectilinear coordinates. This layer absorbs waves of any wavelength and any frequency without re ection and thus can be used to arti cially terminate the domain of scattering calculations. In this paper we show how to derive and implement the B erenger layer in curvilinear coordinates (in two space dimensions). We prove that an in nite layer of this type can be used to solve time harmonic scattering problems. We also show that the truncated B erenger problem has a solution except at a discrete set of exceptional frequencies (which might be empty). Finally numerical results show that the curvilinear layer can produce accurate solutions in the time and frequency domain.
“…A direct inspection shows that the Green's function for this equation is given byĤ z (x; y) = i 4 H (1)…”
Section: Z +1mentioning
confidence: 99%
“…where H (1) n is the Hankel function of rst kind and order zero, and x = exp(i ). This series converges uniformly for r a 0 9].…”
Section: Z +1mentioning
confidence: 99%
“…Suppose~ = r + i~ i where~ r and~ i are real. The desired asymptotic behavior of the Hankel functions is H (1) m…”
Section: Z +1mentioning
confidence: 99%
“…This approach is easy to implement and is very e ective. It has already been the subject of numerous of papers 18,1,5,12,11,13,25,26,23,21,15,7,4,24,3]. However, to our knowledge, there has been very little theoretical analysis of the method.…”
In 1994 B erenger showed how to construct a perfectly matched absorbing layer for the Maxwell system in rectilinear coordinates. This layer absorbs waves of any wavelength and any frequency without re ection and thus can be used to arti cially terminate the domain of scattering calculations. In this paper we show how to derive and implement the B erenger layer in curvilinear coordinates (in two space dimensions). We prove that an in nite layer of this type can be used to solve time harmonic scattering problems. We also show that the truncated B erenger problem has a solution except at a discrete set of exceptional frequencies (which might be empty). Finally numerical results show that the curvilinear layer can produce accurate solutions in the time and frequency domain.
“…The PML technique involves the application of a nonphysical absorbing material adjacent to the computational boundary. The PML material has characteristics that permit electromagnetic waves of arbitraq frequency and angle of incidence to be absorbed while maintaining the impedance and velocity of a lossless dielectric [3]. This technique has shown its effectiveness and generality of handling a large class of problems in discrete domain techniques.…”
An artificial lossy absorbing boundary condition is proposed for use in the method of lines for simulating unbounded electromagnetic structures. It is found, through the modeling results of a microstrip line, that the proposed absorbing boundary condition could be effective and a simple rule of application may be established.
Figure 4 Comparison of normalized power density calculated using w x Ž . the recursive T-matrix algorithm with 11 a Tessellated geometry Ž . showing the scattering for 45Њ slanted metallic rectangle b Polar Ž . plot showing the normalized power density vs. for geometry of a
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