Enhanced the sensitivity of one-dimensional photonic crystals infiltrated with cancer cells
In this work, we use a one-dimensional photonic crystal as a biosensor composed of alternating GaAs and air layers. Within the cavity where they are infiltrated, the Normal, Jurkat, HeLa, PC-12, MDA-MB-231, and MCF-7 cells are bounded by layers of nanocomposite and graphene to increase biosensor sen...
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description | In this work, we use a one-dimensional photonic crystal as a biosensor composed of alternating GaAs and air layers. Within the cavity where they are infiltrated, the Normal, Jurkat, HeLa, PC-12, MDA-MB-231, and MCF-7 cells are bounded by layers of nanocomposite and graphene to increase biosensor sensitivity. The transmission spectrum was calculated using the transfer matrix method. We observed that, when the structural periodicity is broken, defect modes that characterize each cell are created. These defect modes move at a wavelength as the dielectric constant increases. Additionally, the separation between defect modes and bandwidth determines sensitivity, Q factor, and FOM, in which average values of 406.84 nm/RIU, 1765.53, and 535.44 were obtained, respectively, for normal light incidence. Regarding Transverse-Electric (TE) and Transverse-Magnetic (TM) polarization, the defect modes shift toward shorter wavelengths as the angle of incidence increases. For TE polarization, transmittance decreased and the distance between the modes increased. At a 50° angle, sensitivity, Q factor, and FOM increased up to 497.55 nm/RIU, 3182.02, and 1401.25, respectively. Conversely, at a 50° angle in TM polarization, sensitivity remained constant at a value of 407 nm/RIU, along with increased transmittance and decreased performance. Finally, sensitivity and performance were optimized by modifying the cavity thickness value at an incidence angle of 30° for TE polarization, and at an incidence angle of 10° for TM polarization. In both cases, the increased cavity thickness shifted the defect modes toward longer wavelengths while increasing sensitivity up to 495.75 nm/RIU for TE and 451.33 nm/RIU for TM. |
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Within the cavity where they are infiltrated, the Normal, Jurkat, HeLa, PC-12, MDA-MB-231, and MCF-7 cells are bounded by layers of nanocomposite and graphene to increase biosensor sensitivity. The transmission spectrum was calculated using the transfer matrix method. We observed that, when the structural periodicity is broken, defect modes that characterize each cell are created. These defect modes move at a wavelength as the dielectric constant increases. Additionally, the separation between defect modes and bandwidth determines sensitivity, Q factor, and FOM, in which average values of 406.84 nm/RIU, 1765.53, and 535.44 were obtained, respectively, for normal light incidence. Regarding Transverse-Electric (TE) and Transverse-Magnetic (TM) polarization, the defect modes shift toward shorter wavelengths as the angle of incidence increases. For TE polarization, transmittance decreased and the distance between the modes increased. At a 50° angle, sensitivity, Q factor, and FOM increased up to 497.55 nm/RIU, 3182.02, and 1401.25, respectively. Conversely, at a 50° angle in TM polarization, sensitivity remained constant at a value of 407 nm/RIU, along with increased transmittance and decreased performance. Finally, sensitivity and performance were optimized by modifying the cavity thickness value at an incidence angle of 30° for TE polarization, and at an incidence angle of 10° for TM polarization. In both cases, the increased cavity thickness shifted the defect modes toward longer wavelengths while increasing sensitivity up to 495.75 nm/RIU for TE and 451.33 nm/RIU for TM.</description><identifier>ISSN: 2053-1591</identifier><identifier>EISSN: 2053-1591</identifier><identifier>DOI: 10.1088/2053-1591/acb907</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Biosensors ; cancer cell ; cavity ; Crystal defects ; Graphene ; Incidence angle ; Matrix methods ; Nanocomposites ; one-dimensional photonic crystal ; Photonic crystals ; Polarization ; Q factors ; Sensitivity enhancement ; Thickness ; Transfer matrices ; Transmittance ; transmittance spectrum ; Wavelengths</subject><ispartof>Materials research express, 2023-02, Vol.10 (2), p.26202</ispartof><rights>2023 The Author(s). Published by IOP Publishing Ltd</rights><rights>2023 The Author(s). Published by IOP Publishing Ltd. 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Res. Express</addtitle><description>In this work, we use a one-dimensional photonic crystal as a biosensor composed of alternating GaAs and air layers. Within the cavity where they are infiltrated, the Normal, Jurkat, HeLa, PC-12, MDA-MB-231, and MCF-7 cells are bounded by layers of nanocomposite and graphene to increase biosensor sensitivity. The transmission spectrum was calculated using the transfer matrix method. We observed that, when the structural periodicity is broken, defect modes that characterize each cell are created. These defect modes move at a wavelength as the dielectric constant increases. Additionally, the separation between defect modes and bandwidth determines sensitivity, Q factor, and FOM, in which average values of 406.84 nm/RIU, 1765.53, and 535.44 were obtained, respectively, for normal light incidence. Regarding Transverse-Electric (TE) and Transverse-Magnetic (TM) polarization, the defect modes shift toward shorter wavelengths as the angle of incidence increases. For TE polarization, transmittance decreased and the distance between the modes increased. At a 50° angle, sensitivity, Q factor, and FOM increased up to 497.55 nm/RIU, 3182.02, and 1401.25, respectively. Conversely, at a 50° angle in TM polarization, sensitivity remained constant at a value of 407 nm/RIU, along with increased transmittance and decreased performance. Finally, sensitivity and performance were optimized by modifying the cavity thickness value at an incidence angle of 30° for TE polarization, and at an incidence angle of 10° for TM polarization. In both cases, the increased cavity thickness shifted the defect modes toward longer wavelengths while increasing sensitivity up to 495.75 nm/RIU for TE and 451.33 nm/RIU for TM.</description><subject>Biosensors</subject><subject>cancer cell</subject><subject>cavity</subject><subject>Crystal defects</subject><subject>Graphene</subject><subject>Incidence angle</subject><subject>Matrix methods</subject><subject>Nanocomposites</subject><subject>one-dimensional photonic crystal</subject><subject>Photonic crystals</subject><subject>Polarization</subject><subject>Q factors</subject><subject>Sensitivity enhancement</subject><subject>Thickness</subject><subject>Transfer matrices</subject><subject>Transmittance</subject><subject>transmittance spectrum</subject><subject>Wavelengths</subject><issn>2053-1591</issn><issn>2053-1591</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>DOA</sourceid><recordid>eNp9kUtLxTAQhYsoKOreZcCFG6t5NE2yFPEFghtduQjTNPHm0tvUJD7uv7e1oi7EzWQ4nPMNmSmKA4JPCJbylGLOSsIVOQXTKCw2ip1vafNXv13sp7TEGFOhGKf1TvF40S-gN7ZFeWFRsn3y2b_6vEbBodDbsvWrSQw9dGhYhBx6b5CJ65ShS8j3znc5Qh4Bbz4vkJlgERnbdWmv2HKjye5_vbvFw-XF_fl1eXt3dXN-dlsaJmQuLUhSucrxhjeuMsoRA4xLY2nDVIuVMw4qY1wruLU1qzijjRSY1y1xDZGU7RY3M7cNsNRD9CuIax3A608hxCcNMXvTWd04JjDjynIJlQUr3VgcblStAECQkXU4s4YYnl9synoZXuL4-aSpEHUtOWHV6MKzy8SQUrTueyrBerqInlaup5Xr-SJj5HiO-DD8MP-xH_1hX8X3KUI1pjXFVA-tYx_97Jue</recordid><startdate>20230201</startdate><enddate>20230201</enddate><creator>Segovia-Chaves, Francis</creator><creator>Carlos Trujillo, Juan</creator><creator>Trabelsi, Youssef</creator><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0002-3232-5796</orcidid></search><sort><creationdate>20230201</creationdate><title>Enhanced the sensitivity of one-dimensional photonic crystals infiltrated with cancer cells</title><author>Segovia-Chaves, Francis ; 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Res. Express</addtitle><date>2023-02-01</date><risdate>2023</risdate><volume>10</volume><issue>2</issue><spage>26202</spage><pages>26202-</pages><issn>2053-1591</issn><eissn>2053-1591</eissn><abstract>In this work, we use a one-dimensional photonic crystal as a biosensor composed of alternating GaAs and air layers. Within the cavity where they are infiltrated, the Normal, Jurkat, HeLa, PC-12, MDA-MB-231, and MCF-7 cells are bounded by layers of nanocomposite and graphene to increase biosensor sensitivity. The transmission spectrum was calculated using the transfer matrix method. We observed that, when the structural periodicity is broken, defect modes that characterize each cell are created. These defect modes move at a wavelength as the dielectric constant increases. Additionally, the separation between defect modes and bandwidth determines sensitivity, Q factor, and FOM, in which average values of 406.84 nm/RIU, 1765.53, and 535.44 were obtained, respectively, for normal light incidence. Regarding Transverse-Electric (TE) and Transverse-Magnetic (TM) polarization, the defect modes shift toward shorter wavelengths as the angle of incidence increases. For TE polarization, transmittance decreased and the distance between the modes increased. At a 50° angle, sensitivity, Q factor, and FOM increased up to 497.55 nm/RIU, 3182.02, and 1401.25, respectively. Conversely, at a 50° angle in TM polarization, sensitivity remained constant at a value of 407 nm/RIU, along with increased transmittance and decreased performance. Finally, sensitivity and performance were optimized by modifying the cavity thickness value at an incidence angle of 30° for TE polarization, and at an incidence angle of 10° for TM polarization. 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subjects | Biosensors cancer cell cavity Crystal defects Graphene Incidence angle Matrix methods Nanocomposites one-dimensional photonic crystal Photonic crystals Polarization Q factors Sensitivity enhancement Thickness Transfer matrices Transmittance transmittance spectrum Wavelengths |
title | Enhanced the sensitivity of one-dimensional photonic crystals infiltrated with cancer cells |
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