Roman Grigorev;Faezeh Zarrinkhat;Joel Lamberg;Mikhail Sidorenko;Lufang Guo;Viktar S. Asadchy;Zachary Taylor
{"title":"Corneal Dosimetry in the 200–500 GHz Band Using Generalized Lorenz–Mie Theory","authors":"Roman Grigorev;Faezeh Zarrinkhat;Joel Lamberg;Mikhail Sidorenko;Lufang Guo;Viktar S. Asadchy;Zachary Taylor","doi":"10.1109/JMW.2026.3727126","DOIUrl":null,"url":null,"abstract":"This study presents a comprehensive dosimetric analysis of the human cornea exposed to continuous radiation in the 200–500 GHz frequency range. A semi-analytic approach is developed by combining Bruggeman effective-medium theory of the hydration-graded cornea with Generalized Lorenz–Mie Theory (GLMT) for arbitrary Gaussian-beam illumination, coupled to a Pennes bioheat equation to compute SAR, absorbed power density (<inline-formula><tex-math>$S_{ab}$</tex-math></inline-formula>) averaged over <inline-formula><tex-math>$1\\;\\mathrm{cm^{2}}$</tex-math></inline-formula>, and the temperature rise <inline-formula><tex-math>$\\Delta T$</tex-math></inline-formula>. Validation at 100 GHz against established plane-wave results is obtained in the large-waist limit (<inline-formula><tex-math>$w_{0} = \\text{60}\\;\\text{mm}$</tex-math></inline-formula>). Across 200–500 GHz at <inline-formula><tex-math>$w_{0} = \\text{3}\\;\\text{mm}$</tex-math></inline-formula>, <inline-formula><tex-math>$S_{ab}$</tex-math></inline-formula> and both peak and average temperature rises increase modestly with frequency, whereas the heating factor <inline-formula><tex-math>$\\Delta T_{\\text{peak}}/S_{ab}$</tex-math></inline-formula> varies by less than 0.3%, establishing <inline-formula><tex-math>$S_{ab}$</tex-math></inline-formula> as a frequency-stable surrogate for peak corneal temperature in this band. A beam-size sweep at <inline-formula><tex-math>$\\text{300}\\;\\text{GHz}$</tex-math></inline-formula> (<inline-formula><tex-math>$w_{0} = 2$</tex-math></inline-formula>–<inline-formula><tex-math>$\\text{12}\\;\\text{mm}$</tex-math></inline-formula>) at fixed aperture-averaged incident power density demonstrates that beam geometry is the dominant determinant of peak corneal heating: <inline-formula><tex-math>$\\Delta T_{\\text{peak}}$</tex-math></inline-formula> decreases by roughly a factor of four as the waist increases, while <inline-formula><tex-math>$S_{ab}$</tex-math></inline-formula> increases only slightly. Peak and area-averaged quantities therefore vary in opposite directions as the beam narrows. Across all configurations, the calculated metrics at reference incident power densities of <inline-formula><tex-math>$40\\;\\mathrm{W/m^{2}}$</tex-math></inline-formula> remain more than an order of magnitude below the <inline-formula><tex-math>$5\\;^{\\circ }\\mathrm{C}$</tex-math></inline-formula> Type-1 corneal operational threshold, and no abrupt change in dosimetric behaviour is observed across <inline-formula><tex-math>$\\text{300}\\;\\text{GHz}$</tex-math></inline-formula>. Presented results quantify, for the cornea at sub-terahertz frequencies, the beam-size regime in which area-averaged <inline-formula><tex-math>$S_{ab}$</tex-math></inline-formula> and local peak corneal temperature diverge.","PeriodicalId":93296,"journal":{"name":"IEEE journal of microwaves","volume":"6 5","pages":"1132-1143"},"PeriodicalIF":4.5000,"publicationDate":"2026-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=11700402","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE journal of microwaves","FirstCategoryId":"1085","ListUrlMain":"https://ieeexplore.ieee.org/document/11700402/","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/9/21 0:00:00","PubModel":"Epub","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
This study presents a comprehensive dosimetric analysis of the human cornea exposed to continuous radiation in the 200–500 GHz frequency range. A semi-analytic approach is developed by combining Bruggeman effective-medium theory of the hydration-graded cornea with Generalized Lorenz–Mie Theory (GLMT) for arbitrary Gaussian-beam illumination, coupled to a Pennes bioheat equation to compute SAR, absorbed power density ($S_{ab}$) averaged over $1\;\mathrm{cm^{2}}$, and the temperature rise $\Delta T$. Validation at 100 GHz against established plane-wave results is obtained in the large-waist limit ($w_{0} = \text{60}\;\text{mm}$). Across 200–500 GHz at $w_{0} = \text{3}\;\text{mm}$, $S_{ab}$ and both peak and average temperature rises increase modestly with frequency, whereas the heating factor $\Delta T_{\text{peak}}/S_{ab}$ varies by less than 0.3%, establishing $S_{ab}$ as a frequency-stable surrogate for peak corneal temperature in this band. A beam-size sweep at $\text{300}\;\text{GHz}$ ($w_{0} = 2$–$\text{12}\;\text{mm}$) at fixed aperture-averaged incident power density demonstrates that beam geometry is the dominant determinant of peak corneal heating: $\Delta T_{\text{peak}}$ decreases by roughly a factor of four as the waist increases, while $S_{ab}$ increases only slightly. Peak and area-averaged quantities therefore vary in opposite directions as the beam narrows. Across all configurations, the calculated metrics at reference incident power densities of $40\;\mathrm{W/m^{2}}$ remain more than an order of magnitude below the $5\;^{\circ }\mathrm{C}$ Type-1 corneal operational threshold, and no abrupt change in dosimetric behaviour is observed across $\text{300}\;\text{GHz}$. Presented results quantify, for the cornea at sub-terahertz frequencies, the beam-size regime in which area-averaged $S_{ab}$ and local peak corneal temperature diverge.