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   <subfield code="a">eng</subfield>
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   <subfield code="a">Jun-Sheng Zhao</subfield>
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   <subfield code="a">Integral equation solution of Maxwell's equations from zero frequency to microwave frequencies.</subfield>
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   <subfield code="a">pp. 1635-1645</subfield>
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   <subfield code="a">We develop a new method to precondition the matrix equation resulting from applying the method of moments (MoM) to the electric field integral equation (EFIE). This preconditioning method is based on first applying the loop-tree or loop-star decomposition of the currents to arrive at a Helmholtz decomposition of the unknown currents. However, the MoM matrix thus obtained still cannot be solved efficiently by iterative solvers due to the large number of iterations required. We propose a permutation of the loop-tree or loop-star currents by a connection matrix, to arrive at a current basis that yields a MoM matrix that can be solved efficiently by iterative solvers. Consequently, dramatic reduction in iteration count has been observed. The various steps can be regarded as a rearrangement of the basis functions to arrive at the MoM matrix. Therefore, they are related to the original MoM matrix by matrix transformation, where the transformation requires the inverse of the connection matrix. We have also developed a fast method to invert the connection matrix so that the complexity of the preconditioning procedure is of O(N) and, hence, can be used in fast solvers such as the low-frequency multilevel fast multipole algorithm (LP-MLFMA). This procedure also makes viable the use of fast solvers such as MLFMA to seek the iterative solutions of Maxwell's equations from zero frequency to microwave frequencies</subfield>
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   <subfield code="a">EFIE.</subfield>
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   <subfield code="a">Helmholtz decomposition.</subfield>
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   <subfield code="a">Maxwell's equations.</subfield>
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   <subfield code="a">MoM matrix.</subfield>
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   <subfield code="a">Basis functions.</subfield>
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   <subfield code="a">Complexity.</subfield>
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   <subfield code="a">Conducting bodies.</subfield>
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   <subfield code="a">Connection matrix.</subfield>
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   <subfield code="a">Electric field integral equation.</subfield>
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   <subfield code="a">Fast solvers.</subfield>
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   <subfield code="a">Integral equation solution.</subfield>
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   <subfield code="a">Inverse connection matrix.</subfield>
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   <subfield code="a">Iterative solvers.</subfield>
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   <subfield code="a">Loop-star current.</subfield>
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   <subfield code="a">Loop-star decomposition.</subfield>
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   <subfield code="a">Loop-tree current.</subfield>
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   <subfield code="a">Loop-tree decomposition.</subfield>
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  <datafield tag="653" ind1=" " ind2=" ">
   <subfield code="a">Low-frequency multilevel fast multipole algorithm.</subfield>
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   <subfield code="a">Matrix equation preconditioning.</subfield>
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   <subfield code="a">Matrix transformation.</subfield>
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   <subfield code="a">Method of moments.</subfield>
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   <subfield code="a">Microwave frequencies.</subfield>
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   <subfield code="a">Permutation.</subfield>
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  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">IEEE Transactions on antennas and propagation</subfield>
   <subfield code="g">48, 10 (2000).</subfield>
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   <subfield code="a">FO</subfield>
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   <subfield code="a">UPD</subfield>
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   <subfield code="a">Article</subfield>
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