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dc.contributor.authorGuérin, Bastien
dc.contributor.authorVillena, Jorge F
dc.contributor.authorPolimeridis, Athanasios G
dc.contributor.authorRosen, Bruce R
dc.contributor.authorAdalsteinsson, Elfar
dc.contributor.authorDaniel, Luca
dc.contributor.authorWhite, Jacob K.
dc.contributor.authorRosen, Bruce R.
dc.contributor.authorWald, Lawrence
dc.date.accessioned2022-07-12T19:13:55Z
dc.date.available2021-10-27T20:29:10Z
dc.date.available2022-07-12T19:13:55Z
dc.date.issued2018
dc.identifier.urihttps://hdl.handle.net/1721.1/135761.2
dc.description.abstract© 2017 Informa UK Limited, trading as Taylor & Francis Group. Purpose: We introduce a method for calculation of the ultimate specific absorption rate (SAR) amplification factors (uSAF) in non-uniform body models. The uSAF is the greatest possible SAF achievable by any hyperthermia (HT) phased array for a given frequency, body model and target heating volume. Methods: First, we generate a basis-set of solutions to Maxwell’s equations inside the body model. We place a large number of electric and magnetic dipoles around the body model and excite them with random amplitudes and phases. We then compute the electric fields created in the body model by these excitations using an ultra-fast volume integral solver called MARIE. We express the field pattern that maximises the SAF in the target tumour as a linear combination of these basis fields and optimise the combination weights so as to maximise SAF (concave problem). We compute the uSAFs in the Duke body models at 10 frequencies in the 20–900 MHz range and for twelve 3 cm-diameter tumours located at various depths in the head and neck. Results: For both shallow and deep tumours, the frequency yielding the greatest uSAF was ∼900 MHz. Since this is the greatest frequency that we simulated, we hypothesise that the globally optimal frequency is actually greater. Conclusions: The uSAFs computed in this work are very large (40–100 for shallow tumours and 4–17 for deep tumours), indicating that there is a large room for improvement of the current state-of-the-art head and neck HT devices.en_US
dc.language.isoen
dc.publisherInforma UK Limiteden_US
dc.relation.isversionof10.1080/02656736.2017.1319077en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourcePMCen_US
dc.titleComputation of ultimate SAR amplification factors for radiofrequency hyperthermia in non-uniform body models: impact of frequency and tumour locationen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Research Laboratory of Electronicsen_US
dc.contributor.departmentHarvard University--MIT Division of Health Sciences and Technologyen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Electrical Engineering and Computer Scienceen_US
dc.relation.journalInternational Journal of Hyperthermiaen_US
dc.eprint.versionAuthor's final manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2019-05-01T16:16:38Z
dspace.orderedauthorsGuérin, B; Villena, JF; Polimeridis, AG; Adalsteinsson, E; Daniel, L; White, JK; Rosen, BR; Wald, LLen_US
dspace.date.submission2019-05-01T16:16:39Z
mit.journal.volume34en_US
mit.journal.issue1en_US
mit.metadata.statusPublication Information Neededen_US


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