Angular and Intensity Modes Self-Referenced Refractive Index Sensor Based on Thin Dielectric Grating Combined With Thin Metal Film

The combination of a thin dielectric grating with a thin metal film is shown to reveal the existence of multiple plasmons, some are short range and others long range both represented by resonant dips in the reflectivity. Usually the plasmons come in pairs, where one is excited at the substrate metal interface while the other at the grating metal interface. One of these dips is sensitive to the refractive index (RI) of the medium adjacent to the metal surface while the other to that near the grating interfaces. Using an optimum design it is possible to obtain high sensitivity to the RI variations of one of the adjacent media but not to the other, hence a self-referenced biosensor can be built using this design. Two configurations are shown to reveal unique features in the angular mode: 1) the possibility of using both angular and intensity sensitivity to detect variations in the RI of the analyte, 2) the possibility of using the excited multiple sharp plasmons that cause multiple resonances (dips) in the reflectivity, where part of these resonances are red-shifted due to variations in the RI of the analyte, while the others are blue shifted. Hence, by measuring the shift of one with respect to the other the angular sensitivity is improved, 3) multiple dips can be used for reference, and 4) high figure of merit is obtained. The thin dielectric grating is shown to have two roles, one to provide the momentum matching whereas the other is to act effectively as a dielectric layer underneath the metal film to enable the excitation of both the long and short range surface plasmons.

[1]  Pei Wang,et al.  Improving the sensitivity of SPR sensors based on gratings by double-dips method (DDM). , 2008, Optics express.

[2]  Kevin Barraclough,et al.  I and i , 2001, BMJ : British Medical Journal.

[3]  Ibrahim Abdulhalim,et al.  Electromagnetic fields distribution in multilayer thin film structures and the origin of sensitivity enhancement in surface plasmon resonance sensors , 2010 .

[4]  Ibrahim Abdulhalim,et al.  Sensitivity‐enhancement methods for surface plasmon sensors , 2011 .

[5]  M. Vala,et al.  Diffraction grating-coupled surface plasmon resonance sensor based on spectroscopy of long-range and short-range surface plasmons , 2007, SPIE Optics + Optoelectronics.

[6]  I. Abdulhalim,et al.  Simplified optical scatterometry for periodic nanoarrays in the near-quasi-static limit. , 2007, Applied optics.

[7]  Donghyun Kim,et al.  Grating-coupled transmission-type surface plasmon resonance sensors based on dielectric and metallic gratings. , 2007, Applied optics.

[8]  Jing Guo,et al.  Dual-mode surface-plasmon-resonance sensors using angular interrogation. , 2008 .

[9]  Sergiy Patskovsky,et al.  Phase and amplitude sensitivities in surface plasmon resonance bio and chemical sensing. , 2009, Optics express.

[10]  Deming Liu,et al.  High-performance Grating Coupled Surface Plasmon Resonance Sensor Based on Al-Au Bimetallic Layer , 2010 .

[11]  Byeong Ha Lee,et al.  Thermo-optic coefficient measurement of liquids based on simultaneous temperature and refractive index sensing capability of a two-mode fiber interferometric probe. , 2012, Optics express.

[12]  J. Kondoh,et al.  Tuning and sensitivity enhancement of surface plasmon resonance sensor , 2007 .

[13]  Ibrahim Abdulhalim,et al.  Self-referenced biosensor based on thin dielectric grating combined with thin metal film. , 2015, Optics express.

[14]  I. Abdulhalim,et al.  Critical-angle-based sensor with improved figure of merit using dip detection. , 2015, Optics letters.