Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors

The total internal reflection ellipsometry (TIRE) method was used for the excitation and study of the sensitivity features of surface plasmon polariton (SPP) and Bloch surface waves (BSWs) resonances. For the BSWs generation distributed Bragg gratings were formed on the tops of the substrates (BK7 g...

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Main Authors: Zigmas Balevicius, Algirdas Baskys
Format: Article
Language:English
Published: MDPI AG 2019-09-01
Series:Materials
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Online Access:https://www.mdpi.com/1996-1944/12/19/3147
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spelling doaj-5f351340474a469781e24765da868cc62020-11-24T21:55:32ZengMDPI AGMaterials1996-19442019-09-011219314710.3390/ma12193147ma12193147Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced BiosensorsZigmas Balevicius0Algirdas Baskys1Faculty of Electronics, Vilnius Gediminas Technical University, Naugarduko st. 41, 03227 Vilnius, LithuaniaFaculty of Electronics, Vilnius Gediminas Technical University, Naugarduko st. 41, 03227 Vilnius, LithuaniaThe total internal reflection ellipsometry (TIRE) method was used for the excitation and study of the sensitivity features of surface plasmon polariton (SPP) and Bloch surface waves (BSWs) resonances. For the BSWs generation distributed Bragg gratings were formed on the tops of the substrates (BK7 glass substrate), which had six bilayers of ~120 nm SiO<sub>2</sub> and ~40 nm TiO<sub>2</sub> and 40 nm of TiO<sub>2</sub> on the top. The SPP sample consisted of the BK7 glass prism and a gold layer (45 nm). Numerical calculations of the optical dispersions and the experimental TIRE data have shown that SPP resonance overtake the BSWs in wavelength scanning by a factor of about 17. However, for the ellipsometric parameters <i>&#936;</i> and <i>&#916;</i> in the vicinity of excitations, the BSW sensitivity is comparable with SPP. The obtained resolutions were <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#916;</mi> <mrow> <mi>S</mi> <mi>P</mi> <mi>P</mi> </mrow> </msub> <mo>=</mo> <mn>7.14</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>6</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula>, <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#936;</mi> <mrow> <mi>S</mi> <mi>P</mi> <mi>P</mi> </mrow> </msub> <mo>=</mo> <mn>1.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>5</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula> for the SPP and <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#916;</mi> <mrow> <mi>B</mi> <mi>S</mi> <mi>W</mi> </mrow> </msub> <mo>=</mo> <mn>8.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>6</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula>, <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#936;</mi> <mrow> <mi>B</mi> <mi>S</mi> <mi>W</mi> </mrow> </msub> <mo>=</mo> <mn>2.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>5</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula> for the BSW. The capabilities of both surface excitations are discussed from the sensitivity point of view in the design of these advanced biosensors.https://www.mdpi.com/1996-1944/12/19/3147bloch surface wavessurface plasmon polaritonoptical biosensorsphotonic crystalssilicon oxidetitanium oxide
collection DOAJ
language English
format Article
sources DOAJ
author Zigmas Balevicius
Algirdas Baskys
spellingShingle Zigmas Balevicius
Algirdas Baskys
Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
Materials
bloch surface waves
surface plasmon polariton
optical biosensors
photonic crystals
silicon oxide
titanium oxide
author_facet Zigmas Balevicius
Algirdas Baskys
author_sort Zigmas Balevicius
title Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
title_short Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
title_full Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
title_fullStr Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
title_full_unstemmed Optical Dispersions of Bloch Surface Waves and Surface Plasmon Polaritons: Towards Advanced Biosensors
title_sort optical dispersions of bloch surface waves and surface plasmon polaritons: towards advanced biosensors
publisher MDPI AG
series Materials
issn 1996-1944
publishDate 2019-09-01
description The total internal reflection ellipsometry (TIRE) method was used for the excitation and study of the sensitivity features of surface plasmon polariton (SPP) and Bloch surface waves (BSWs) resonances. For the BSWs generation distributed Bragg gratings were formed on the tops of the substrates (BK7 glass substrate), which had six bilayers of ~120 nm SiO<sub>2</sub> and ~40 nm TiO<sub>2</sub> and 40 nm of TiO<sub>2</sub> on the top. The SPP sample consisted of the BK7 glass prism and a gold layer (45 nm). Numerical calculations of the optical dispersions and the experimental TIRE data have shown that SPP resonance overtake the BSWs in wavelength scanning by a factor of about 17. However, for the ellipsometric parameters <i>&#936;</i> and <i>&#916;</i> in the vicinity of excitations, the BSW sensitivity is comparable with SPP. The obtained resolutions were <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#916;</mi> <mrow> <mi>S</mi> <mi>P</mi> <mi>P</mi> </mrow> </msub> <mo>=</mo> <mn>7.14</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>6</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula>, <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#936;</mi> <mrow> <mi>S</mi> <mi>P</mi> <mi>P</mi> </mrow> </msub> <mo>=</mo> <mn>1.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>5</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula> for the SPP and <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#916;</mi> <mrow> <mi>B</mi> <mi>S</mi> <mi>W</mi> </mrow> </msub> <mo>=</mo> <mn>8.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>6</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula>, <inline-formula> <math display="inline"> <semantics> <mrow> <msub> <mi>&#936;</mi> <mrow> <mi>B</mi> <mi>S</mi> <mi>W</mi> </mrow> </msub> <mo>=</mo> <mn>2.7</mn> <mo>&#215;</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>&#8722;</mo> <mn>5</mn> </mrow> </msup> <mi>R</mi> <mi>I</mi> <mi>U</mi> </mrow> </semantics> </math> </inline-formula> for the BSW. The capabilities of both surface excitations are discussed from the sensitivity point of view in the design of these advanced biosensors.
topic bloch surface waves
surface plasmon polariton
optical biosensors
photonic crystals
silicon oxide
titanium oxide
url https://www.mdpi.com/1996-1944/12/19/3147
work_keys_str_mv AT zigmasbalevicius opticaldispersionsofblochsurfacewavesandsurfaceplasmonpolaritonstowardsadvancedbiosensors
AT algirdasbaskys opticaldispersionsofblochsurfacewavesandsurfaceplasmonpolaritonstowardsadvancedbiosensors
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