Beilstein J. Nanotechnol.2011,2, 585–592, doi:10.3762/bjnano.2.62
counts/ppm for λmax = 684, 764 and 935 nm, respectively. From the plot, the maximum sensitivity is seen for λmax = 684 nm.
Here, it is proposed that the gassensing mechanism follows the changes in the refractive index and evanescent wave absorption. For h-MoO3, the oxygen vacancies and interstitial
molybdenum atoms play a major role in gassensing operation. The reaction between ethanol gas and the chemisorbed oxygen (O2−, O− and O2−) at the surface of the MoO3 material changes the refractive index of the clad structure. Due to this change, the light wave travelling through the removed and coated
linearly as a function of ethanol concentration in the range of 0 to 500 ppm. In the present study, changes in the refractive index and the evanescent wave absorption phenomenon were proposed to explain the gassensing mechanism. The reaction between ethanol gas and the chemisorbed oxygen (O2−, O− and O2