1978
DOI: 10.1109/map.1978.27344
|View full text |Cite
|
Sign up to set email alerts
|

Reviews and abstracts - Electromagnetic scattering from a homogeneous body of revolution

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
153
0

Year Published

1998
1998
2021
2021

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 76 publications
(160 citation statements)
references
References 0 publications
3
153
0
Order By: Relevance
“…The resulting sets of simultaneous equations may be represented in matrix form as (17) where is the moment matrix, is a column vector containing the unknown basis function coefficients, and is the driving vector for the th Fourier mode [21]- [23], [25]- [26]. Details regarding the calculation of the impedance matrix or the driving vector can be found in the literature.…”
Section: B Surface Integral Equation and Mommentioning
confidence: 99%
See 1 more Smart Citation
“…The resulting sets of simultaneous equations may be represented in matrix form as (17) where is the moment matrix, is a column vector containing the unknown basis function coefficients, and is the driving vector for the th Fourier mode [21]- [23], [25]- [26]. Details regarding the calculation of the impedance matrix or the driving vector can be found in the literature.…”
Section: B Surface Integral Equation and Mommentioning
confidence: 99%
“…Assuming poles of single order, which is true for the conducting and permeable targets of interest here [3], [19], the system function in the Laplace domain and the corresponding impulse response are given by (24) where the excitation coefficients for pairs of conjugate complex poles satisfy Therefore the components of the signal vector can be written as (25) with where represents the time increment for the sampling and, hence, the total observation time. The vector of the unknown parameters (excluding the noise variance ) is given by (26) and the likelihood function is [33]- [34] (27)…”
Section: Cramer-rao Lower Boundmentioning
confidence: 99%
“…To demonstrate the usefulness of the AWE method, we implemented it into the MOM code described by Chao In addition to PEC objects treated above, the AWE method is also applicable to dielectric objects. A formulation that is widely used for scattering by a dielectric object is the so-called PMCHW [Mautz and Harrington, 1979 …”
Section: Numerical Examplesmentioning
confidence: 99%
“…The field decomposition approach [1] is employed to split the homogeneous BI medium into two uncoupled isotropic media. We formulate the surface integral equations (SIE) using the PaggioMiller-Chang-Harrington-Wu-Tsai (PMCHWT) approach [27,28] for multiple homogeneous isotropic media and the electric field approach for conducting objects. The resultant integral equations are discretized by MoM.…”
Section: Introductionmentioning
confidence: 99%