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Surface plasmon resonance from metallic columnar thin films

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Surface plasmon resonance from metallic columnar thin films. / Shalabney, A.; Lakhtakia, A.; Abdulhalim, I. et al.
In: Photonics and Nanostructures-Fundamentals and Applications, Vol. 7, No. 4, 31.12.2009, p. 176-185.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Shalabney, A, Lakhtakia, A, Abdulhalim, I, Lahav, A, Patzig, C, Hazek, I, Karabchevsky, A, Rauschenbach, B, Zhang, F & Xu, J 2009, 'Surface plasmon resonance from metallic columnar thin films', Photonics and Nanostructures-Fundamentals and Applications, vol. 7, no. 4, pp. 176-185. https://doi.org/10.1016/j.photonics.2009.03.003

APA

Shalabney, A., Lakhtakia, A., Abdulhalim, I., Lahav, A., Patzig, C., Hazek, I., Karabchevsky, A., Rauschenbach, B., Zhang, F., & Xu, J. (2009). Surface plasmon resonance from metallic columnar thin films. Photonics and Nanostructures-Fundamentals and Applications, 7(4), 176-185. https://doi.org/10.1016/j.photonics.2009.03.003

Vancouver

Shalabney A, Lakhtakia A, Abdulhalim I, Lahav A, Patzig C, Hazek I et al. Surface plasmon resonance from metallic columnar thin films. Photonics and Nanostructures-Fundamentals and Applications. 2009 Dec 31;7(4):176-185. Epub 2009 May 18. doi: 10.1016/j.photonics.2009.03.003

Author

Shalabney, A. ; Lakhtakia, A. ; Abdulhalim, I. et al. / Surface plasmon resonance from metallic columnar thin films. In: Photonics and Nanostructures-Fundamentals and Applications. 2009 ; Vol. 7, No. 4. pp. 176-185.

Bibtex

@article{400ce2cd8ba448759bfbf13088fe5058,
title = "Surface plasmon resonance from metallic columnar thin films",
abstract = "Surface plasmon (SP) waves on the interface of a dielectric (such as water) and a metallic columnar thin film (CTF) of porosity as high as 0.55 were experimentally and theoretically investigated. The CTFs were made of Al, Au, Ag, or Cr. As the porosity increases, the SP resonance (SPR) dip was found to widen, shift to higher wave numbers, and become asymmetric due to increasing scattering losses. With further increase of porosity, the SPR dip was found to disappear, leaving behind only a peak near the onset to the total internal reflection regime. The shape of the nanoislands constituting the CTF is better described as ellipsoidal than as spherical or spheroidal, indicating thereby the existence of orientational biaxial anisotropy even for CTFs thinner than 60 nm. For a best fit between the theoretical calculations and the experimental data, the CTF was divided into two layers having different porosity and nanoisland shape, particularly for the Ag- and Au-CTFs. The sensitivity of the CTF-based SPR signal to refractive index variations of an analyte infiltrating the nanopores of and in the region adjoining the metallic CTF was found to be doubly enhanced compared to that for the SPR signal from a nonporous metallic film.",
author = "A. Shalabney and A. Lakhtakia and I. Abdulhalim and A. Lahav and Christian Patzig and I. Hazek and A. Karabchevsky and Bernd Rauschenbach and F. Zhang and J. Xu",
year = "2009",
month = dec,
day = "31",
doi = "10.1016/j.photonics.2009.03.003",
language = "English",
volume = "7",
pages = "176--185",
journal = "Photonics and Nanostructures-Fundamentals and Applications",
number = "4",

}

RIS

TY - JOUR

T1 - Surface plasmon resonance from metallic columnar thin films

AU - Shalabney, A.

AU - Lakhtakia, A.

AU - Abdulhalim, I.

AU - Lahav, A.

AU - Patzig, Christian

AU - Hazek, I.

AU - Karabchevsky, A.

AU - Rauschenbach, Bernd

AU - Zhang, F.

AU - Xu, J.

PY - 2009/12/31

Y1 - 2009/12/31

N2 - Surface plasmon (SP) waves on the interface of a dielectric (such as water) and a metallic columnar thin film (CTF) of porosity as high as 0.55 were experimentally and theoretically investigated. The CTFs were made of Al, Au, Ag, or Cr. As the porosity increases, the SP resonance (SPR) dip was found to widen, shift to higher wave numbers, and become asymmetric due to increasing scattering losses. With further increase of porosity, the SPR dip was found to disappear, leaving behind only a peak near the onset to the total internal reflection regime. The shape of the nanoislands constituting the CTF is better described as ellipsoidal than as spherical or spheroidal, indicating thereby the existence of orientational biaxial anisotropy even for CTFs thinner than 60 nm. For a best fit between the theoretical calculations and the experimental data, the CTF was divided into two layers having different porosity and nanoisland shape, particularly for the Ag- and Au-CTFs. The sensitivity of the CTF-based SPR signal to refractive index variations of an analyte infiltrating the nanopores of and in the region adjoining the metallic CTF was found to be doubly enhanced compared to that for the SPR signal from a nonporous metallic film.

AB - Surface plasmon (SP) waves on the interface of a dielectric (such as water) and a metallic columnar thin film (CTF) of porosity as high as 0.55 were experimentally and theoretically investigated. The CTFs were made of Al, Au, Ag, or Cr. As the porosity increases, the SP resonance (SPR) dip was found to widen, shift to higher wave numbers, and become asymmetric due to increasing scattering losses. With further increase of porosity, the SPR dip was found to disappear, leaving behind only a peak near the onset to the total internal reflection regime. The shape of the nanoislands constituting the CTF is better described as ellipsoidal than as spherical or spheroidal, indicating thereby the existence of orientational biaxial anisotropy even for CTFs thinner than 60 nm. For a best fit between the theoretical calculations and the experimental data, the CTF was divided into two layers having different porosity and nanoisland shape, particularly for the Ag- and Au-CTFs. The sensitivity of the CTF-based SPR signal to refractive index variations of an analyte infiltrating the nanopores of and in the region adjoining the metallic CTF was found to be doubly enhanced compared to that for the SPR signal from a nonporous metallic film.

UR - http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=ORCID&SrcApp=OrcidOrg&DestLinkType=FullRecord&DestApp=WOS_CPL&KeyUT=WOS:000273379700003&KeyUID=WOS:000273379700003

U2 - 10.1016/j.photonics.2009.03.003

DO - 10.1016/j.photonics.2009.03.003

M3 - Journal article

VL - 7

SP - 176

EP - 185

JO - Photonics and Nanostructures-Fundamentals and Applications

JF - Photonics and Nanostructures-Fundamentals and Applications

IS - 4

ER -