{"title":"Defect-mode ternary MgF2/SiON/TiO2 photonic crystal for theoretical NIR discrimination of literature-derived skin-cancer refractive-index scenarios","authors":"Emadelden Fouad, Arafa H. Aly","doi":"10.1007/s11082-026-09179-3","DOIUrl":null,"url":null,"abstract":"<div><p>One-dimensional photonic crystal (1D-PhC) defect-mode resonators offer a compact and tunable platform for optical biosensing, yet achieving reliable discrimination of closely spaced analytes within a single photonic bandgap (PBG) remains challenging because the resonance characteristics depend jointly on the mirror materials, defect-cavity thickness, and number of periods. We present a ternary 1D-PhC biosensor, Air/(MgF<sub>2</sub>/SiON/TiO<sub>2</sub>)<span>\\({}^{N}\\)</span>/D/(MgF<sub>2</sub>/SiON/TiO<sub>2</sub>)<span>\\({}^{N}\\)</span>/Glass, evaluated by the transfer matrix method against literature-derived refractive indices for melanoma (ME), basal cell carcinoma (BCC), and squamous cell carcinoma (SCC), yielding simulated <span>\\(S=646\\)</span>–652 nm RIU<span>\\({}^{-1}\\)</span>, <span>\\(Q=31248\\)</span>–31644, and FOM = 19785–19966 RIU<span>\\({}^{-1}\\)</span> with the mirror pair lossless (<span>\\(k=0\\)</span>) to experimental precision; these are loss-consistent, not idealized, values, still simulated and unfabricated, with defect-layer and sample losses unmodeled. Within a 905.0–1342.3 nm PBG, the three subtypes’ defect modes separate by 5.83–46.93 nm, or 178–1654 times the mode linewidth. The primary discrimination claims are BCC<span>\\(\\rightarrow \\)</span>ME and SCC<span>\\(\\rightarrow \\)</span>ME (Monte Carlo reversal probability <span>\\(\\le 12.6\\%\\)</span>), spanning different modalities, not only biology; SCC<span>\\(\\rightarrow \\)</span>BCC is excluded and reported only as an exploratory observation, since its oral-mucosa-proxy SCC index carries a <span>\\(20.7\\%\\)</span> reversal probability exceeding the discrimination gap. The ternary architecture and TMM formalism are established in prior literature, not claimed as new; the contribution is a skin-specific triple-subtype application with an explicit two-tier validity framework separating supported claims from exploratory and calibration comparisons, within which the ternary-over-binary benefit is quantified (FOM 3.12–<span>\\(3.14\\times \\)</span> higher at the ME mode) rather than assumed. The results demonstrate optical distinguishability of the literature-derived refractive indices used, not clinical distinguishability of skin lesions, requiring dedicated skin-specific measurement and validation.</p></div>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":"58 12","pages":""},"PeriodicalIF":4.0000,"publicationDate":"2026-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optical and Quantum Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s11082-026-09179-3","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
One-dimensional photonic crystal (1D-PhC) defect-mode resonators offer a compact and tunable platform for optical biosensing, yet achieving reliable discrimination of closely spaced analytes within a single photonic bandgap (PBG) remains challenging because the resonance characteristics depend jointly on the mirror materials, defect-cavity thickness, and number of periods. We present a ternary 1D-PhC biosensor, Air/(MgF2/SiON/TiO2)\({}^{N}\)/D/(MgF2/SiON/TiO2)\({}^{N}\)/Glass, evaluated by the transfer matrix method against literature-derived refractive indices for melanoma (ME), basal cell carcinoma (BCC), and squamous cell carcinoma (SCC), yielding simulated \(S=646\)–652 nm RIU\({}^{-1}\), \(Q=31248\)–31644, and FOM = 19785–19966 RIU\({}^{-1}\) with the mirror pair lossless (\(k=0\)) to experimental precision; these are loss-consistent, not idealized, values, still simulated and unfabricated, with defect-layer and sample losses unmodeled. Within a 905.0–1342.3 nm PBG, the three subtypes’ defect modes separate by 5.83–46.93 nm, or 178–1654 times the mode linewidth. The primary discrimination claims are BCC\(\rightarrow \)ME and SCC\(\rightarrow \)ME (Monte Carlo reversal probability \(\le 12.6\%\)), spanning different modalities, not only biology; SCC\(\rightarrow \)BCC is excluded and reported only as an exploratory observation, since its oral-mucosa-proxy SCC index carries a \(20.7\%\) reversal probability exceeding the discrimination gap. The ternary architecture and TMM formalism are established in prior literature, not claimed as new; the contribution is a skin-specific triple-subtype application with an explicit two-tier validity framework separating supported claims from exploratory and calibration comparisons, within which the ternary-over-binary benefit is quantified (FOM 3.12–\(3.14\times \) higher at the ME mode) rather than assumed. The results demonstrate optical distinguishability of the literature-derived refractive indices used, not clinical distinguishability of skin lesions, requiring dedicated skin-specific measurement and validation.
期刊介绍:
Optical and Quantum Electronics provides an international forum for the publication of original research papers, tutorial reviews and letters in such fields as optical physics, optical engineering and optoelectronics. Special issues are published on topics of current interest.
Optical and Quantum Electronics is published monthly. It is concerned with the technology and physics of optical systems, components and devices, i.e., with topics such as: optical fibres; semiconductor lasers and LEDs; light detection and imaging devices; nanophotonics; photonic integration and optoelectronic integrated circuits; silicon photonics; displays; optical communications from devices to systems; materials for photonics (e.g. semiconductors, glasses, graphene); the physics and simulation of optical devices and systems; nanotechnologies in photonics (including engineered nano-structures such as photonic crystals, sub-wavelength photonic structures, metamaterials, and plasmonics); advanced quantum and optoelectronic applications (e.g. quantum computing, memory and communications, quantum sensing and quantum dots); photonic sensors and bio-sensors; Terahertz phenomena; non-linear optics and ultrafast phenomena; green photonics.