2019
DOI: 10.1049/iet-map.2018.5208
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Implementation of higher order CNAD CFS‐PML for truncating unmagnetised plasma

Abstract: An unconditionally stable implementation of the higher order complex frequency‐shifted (CFS) perfectly matched layer (PML) is proposed for the Crank–Nicolson‐approximate‐decoupling (CNAD) finite‐difference time‐domain (FDTD) scheme. The proposed higher order CFS‐PML, which is implemented by the auxiliary differential equation (ADE) method, not only has better performance than the first‐order PML but also maintains the unconditional stability of the origin Crank–Nicolson (CN) algorithm. The unmagnetised plasma,… Show more

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Cited by 11 publications
(5 citation statements)
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“…48 Based on the CN procedure, several implementations are developed. [49][50][51] However, they cannot be directly extended to three-dimensions. 52 Recently, higher order convolutional PML is carried out for unmagnetized simulation.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…48 Based on the CN procedure, several implementations are developed. [49][50][51] However, they cannot be directly extended to three-dimensions. 52 Recently, higher order convolutional PML is carried out for unmagnetized simulation.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…However, the absorption capacity of CFS-PML to low frequency propagation waves is poor. For the purpose of solving the above PML problems, the higher order PML with the advantages of SC-PML and CFS-PML was proposed in [6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%
“…The most prominent disadvantage is the significant increment of auxiliary variables and coefficients resulting in decrement of efficiency [22][23][24]. Thus, unconditionally stable algorithms are introduced into the higher order PML implementations [25][26][27][28][29].…”
Section: Introductionmentioning
confidence: 99%