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Optics Letters

| RAPID, SHORT PUBLICATIONS ON THE LATEST IN OPTICAL DISCOVERIES

  • Editor: Anthony J. Campillo
  • Vol. 32, Iss. 23 — Dec. 1, 2007
  • pp: 3456–3458

Full-field and real-time surface plasmon resonance imaging thermometry

Il Tai Kim and Kenneth David Kihm  »View Author Affiliations


Optics Letters, Vol. 32, Issue 23, pp. 3456-3458 (2007)
http://dx.doi.org/10.1364/OL.32.003456


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Abstract

The feasibility of surface plasmon resonance (SPR) imaging thermometry is tested as a potential tool for full-field and real-time temperature field mapping for thermally transient liquid mediums. Using the well-known Kretschmann’s analysis [ Physik 241, 313 (1971) ]. parametric examinations are performed to delineate the effects of important optical properties, including seven different prism materials with different refractive index values and seven different measured dielectric constants for thin gold (Au) films (approximately 47.5 nm in thickness), on the temperature dependence of SPR reflectance intensity variations. Furthermore, a laboratory-implemented real-time SPR thermometry system demonstrates the full-field mapping capabilities for transient temperature field developments in the near-wall region when a hot water droplet ( 80 ° C ) contacts the Au metal surface ( 20 ° C ) and spreads either in an air- or in a water-surrounded environment.

© 2007 Optical Society of America

OCIS Codes
(120.6780) Instrumentation, measurement, and metrology : Temperature
(240.6680) Optics at surfaces : Surface plasmons

ToC Category:
Instrumentation, Measurement, and Metrology

History
Original Manuscript: September 7, 2007
Revised Manuscript: October 28, 2007
Manuscript Accepted: October 31, 2007
Published: November 29, 2007

Citation
Il Tai Kim and Kenneth David Kihm, "Full-field and real-time surface plasmon resonance imaging thermometry," Opt. Lett. 32, 3456-3458 (2007)
http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-32-23-3456


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References

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  22. Estimated elementary uncertainties: ωdm=47.5 nm×+/-1.25%(=+/-0.59375 nm), ωepsim=+/-0.002115++/-i0.081(epsim=−13.2+i1.25), ωθ=+/-1.0/60°=+/-0.0167°, ωλ=+/-1.5 nm, ωT=+/-0.1°C where dm is the thickness of the Au layer (47.5 nm), θ is the incident SPR angle optimized for water temperature of 80°C (69.47°), and λ is the incident wavelength (632.8 nm).

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