| dc.contributor.author | Tekbas, Kenan | |
| dc.contributor.author | Berenger, Jean-Pierre | |
| dc.date.accessioned | 2024-03-12T19:29:14Z | |
| dc.date.available | 2024-03-12T19:29:14Z | |
| dc.date.issued | 2023 | |
| dc.identifier.issn | 0021-9991 | |
| dc.identifier.issn | 1090-2716 | |
| dc.identifier.uri | https://doi.org/10.1016/j.jcp.2023.112266 | |
| dc.identifier.uri | https://hdl.handle.net/20.500.12450/2238 | |
| dc.description.abstract | With the objective of reducing the overall number of FDTD cells in applications where the objects of interest are given as sets of voxels, as in bio-electromagnetism, a subcell technique is introduced to allow the FDTD method to account for non-homogeneous cells composed with voxels of different permittivity's. Numerical experiments with dielectric objects are reported to illustrate the effectiveness and the limitations of the method. & COPY; 2023 Elsevier Inc. All rights reserved. | en_US |
| dc.language.iso | eng | en_US |
| dc.publisher | Academic Press Inc Elsevier Science | en_US |
| dc.relation.ispartof | Journal Of Computational Physics | en_US |
| dc.rights | info:eu-repo/semantics/closedAccess | en_US |
| dc.subject | FDTD | en_US |
| dc.subject | Subcell | en_US |
| dc.subject | Voxel | en_US |
| dc.subject | Multigrid | en_US |
| dc.title | Finite-difference time-domain (FDTD) method with non-homogeneous cells filled with voxels | en_US |
| dc.type | article | en_US |
| dc.department | Amasya Üniversitesi | en_US |
| dc.identifier.volume | 489 | en_US |
| dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
| dc.identifier.scopus | 2-s2.0-85162180641 | en_US |
| dc.identifier.doi | 10.1016/j.jcp.2023.112266 | |
| dc.department-temp | [Tekbas, Kenan] Amasya Univ, Dept Elect & Elect Engn, TR-05100 Amasya, Turkiye; [Tekbas, Kenan] Univ Granada, Dept Electromagnetism & Matter Phys, Granada 18071, Spain; [Berenger, Jean-Pierre] Univ Manchester, Dept Elect & Elect Engn, Manchester M139PL, England | en_US |
| dc.identifier.wos | WOS:001024045400001 | en_US |
