4.5 Article

Sensitive Evanescence-Field Waveguide Interferometer for Aqueous Nitro-Explosive Sensing

Journal

CHEMOSENSORS
Volume 11, Issue 4, Pages -

Publisher

MDPI
DOI: 10.3390/chemosensors11040246

Keywords

polymer waveguide; MZI sensor; nitro-explosive detection; dipolar polycarbonate

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In this study, a polymer waveguide Mach-Zehnder interferometer (MZI) sensor was designed and fabricated to detect 2,4-dinitrotoluene (DNT) in water. The theoretical sensitivity of the MZI sensor can reach up to 24,696 nm/RIU. The fabricated sensor had a maximum wavelength shift of 4.465 nm and good linear relation between the wavelength shift and a concentration ranging from 3.5 x 10(-5) to 6.3 x 10(-4) mol/L, with a sensitivity of 6821.6 nm/(mol/L). The unbalanced MZI sensor design, together with the sensing material, provides a new approach to low-cost, compact, and highly sensitive explosive detection.
The development of novel chemical nitro-explosive sensors with high sensitivity, low cost and a compact size is essential for homeland security, environmental protection and addressing military challenges. Polymeric optical waveguides based on refractive index sensing are widely used in biochemical detection due to their advantages of large-scale integration, low cost, high sensitivity and anti-electromagnetic interference. In this study, we designed and fabricated a polymer waveguide Mach-Zehnder interferometer (MZI) sensor to detect 2,4-dinitrotoluene (DNT) in water. One phase shifter of the MZI waveguide was functionalized by coating a thin cladding layer of polycarbonate with dipolar chromophores and used as the sensing arm; the other arm was coated with passive epoxy resin cladding and used as the reference arm. The phase difference between the two arms of the MZI was modulated using the refractive index (RI) change in the polycarbonate cladding when dipolar chromophores interacted with electro-deficient DNT. The theoretical sensitivity of the designed MZI can reach up to 24,696 nm/RIU. When used for explosive detection, our fabricated sensor had a maximum wavelength shift of 4.465 nm and good linear relation, with an R-2 of 0.96 between the wavelength shift and a concentration ranging from 3.5 x 10(-5) to 6.3 x 10(-4) mol/L. The sensitivity of our device was 6821.6 nm/(mol/L). The design of an unbalanced MZI sensor, together with the sensing material, provides a new approach to using low-cost, compact and highly sensitive devices for in-field explosive detection.

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