<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     naa a22        4500</leader>
  <controlfield tag="001">510817610</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180411083515.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">180411e20130601xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/s11468-013-9526-x</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s11468-013-9526-x</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Analysis and Optimum Design of Hybrid Plasmonic Slab Waveguides</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Mahmoud Talafi Noghani, Mohammad Vadjed Samiei]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">Propagation properties of hybrid plasmonic slab waveguides are studied in detail using transfer matrix method considering structural and material aspects. Hybrid metal-insulator, hybrid metal-insulator-metal, and hybrid insulator-metal-insulator waveguides are considered. Propagation length (L p), spatial length (L s), and mode length (L m) are utilized as three common figures of merit to compare and optimize the waveguides according to the layer thicknesses and metal/dielectric materials. The effect of constituting materials including metals (such as silver, gold, copper, and aluminum) and dielectrics (common dielectric materials used in photonic integrated circuit technologies such as silicon and silicon compounds, III-V compounds, and polymers) are discussed. It is found that hybrid waveguides are partially to completely superior to conventional plasmonic waveguides, providing a better balance between confinement and loss.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Springer Science+Business Media New York, 2013</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Plasmonics</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Hybrid plasmonic slab waveguide</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Transfer matrix method</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Talafi Noghani</subfield>
   <subfield code="D">Mahmoud</subfield>
   <subfield code="u">School of Electrical Engineering, Iran University of Science and Technology, 1684613114, Tehran, Iran</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Vadjed Samiei</subfield>
   <subfield code="D">Mohammad</subfield>
   <subfield code="u">School of Electrical Engineering, Iran University of Science and Technology, 1684613114, Tehran, Iran</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Plasmonics</subfield>
   <subfield code="d">Springer US; http://www.springer-ny.com</subfield>
   <subfield code="g">8/2(2013-06-01), 1155-1168</subfield>
   <subfield code="x">1557-1955</subfield>
   <subfield code="q">8:2&lt;1155</subfield>
   <subfield code="1">2013</subfield>
   <subfield code="2">8</subfield>
   <subfield code="o">11468</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/s11468-013-9526-x</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="908" ind1=" " ind2=" ">
   <subfield code="D">1</subfield>
   <subfield code="a">research-article</subfield>
   <subfield code="2">jats</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">856</subfield>
   <subfield code="E">40</subfield>
   <subfield code="u">https://doi.org/10.1007/s11468-013-9526-x</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Talafi Noghani</subfield>
   <subfield code="D">Mahmoud</subfield>
   <subfield code="u">School of Electrical Engineering, Iran University of Science and Technology, 1684613114, Tehran, Iran</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Vadjed Samiei</subfield>
   <subfield code="D">Mohammad</subfield>
   <subfield code="u">School of Electrical Engineering, Iran University of Science and Technology, 1684613114, Tehran, Iran</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">773</subfield>
   <subfield code="E">0-</subfield>
   <subfield code="t">Plasmonics</subfield>
   <subfield code="d">Springer US; http://www.springer-ny.com</subfield>
   <subfield code="g">8/2(2013-06-01), 1155-1168</subfield>
   <subfield code="x">1557-1955</subfield>
   <subfield code="q">8:2&lt;1155</subfield>
   <subfield code="1">2013</subfield>
   <subfield code="2">8</subfield>
   <subfield code="o">11468</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="898" ind1=" " ind2=" ">
   <subfield code="a">BK010053</subfield>
   <subfield code="b">XK010053</subfield>
   <subfield code="c">XK010000</subfield>
  </datafield>
  <datafield tag="949" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="F">NATIONALLICENCE</subfield>
   <subfield code="b">NL-springer</subfield>
  </datafield>
 </record>
</collection>
