Aqueous
solutions of alcohols are used in several applications,
from pharmaceutics and biology, to chemical, biofuel, and food industries.
Nonetheless, development of a simple, inexpensive, and portable sensing
device for the quantification of water in water–ethanol mixtures
remains a significant challenge. Photonic crystals (PhCs) operating
at very high-order photonic bandgaps (PBGs) offer remarkable opportunities
for the realization of chemical sensors with high sensitivity and
low detection limit. However, high-order PhC structures have been
mostly confined to mere theoretical speculations so far, their effective
realization requiring microfabrication tools enabling the control
of periodic refractive index modulations at the submicrometric scale
with extremely high accuracy and precision. Here, we report both experimental
and theoretical results on high-sensitivity chemical analysis using
vertical, silicon/air 1D-PhCs with spatial period of 10 and 20 μm
(namely, over 10 times the operation wavelength) featuring ultra-high-order
PBGs in the near-infrared region (namely, up to 50th at 1.1 μm).
Fabrication of high-order 1D-PhCs was carried out by electrochemical
micromachining (ECM) of silicon, which allowed both surface roughness
and deviation from vertical of etched structures to be controlled
below 5 nm and 0.1%, respectively. Optical characterization of ECM-fabricated
1D-PhCs, which was performed by acquiring reflectivity spectra over
the wavelength range 1–1.7 μm, highlighted the presence
of ultra-high-order PBGs with minor optical losses (i.e., <1 dB
in reflectivity) separated by deep reflectivity notches with high
Q-factors (i.e., >6000), in good agreement with theoretical calculations.
Remarkably, the use of high-order 1D-PhCs as refractometric transducers
for the quantitative detection of traces of water in water–ethanol
mixtures, allowed high sensitivity (namely, either 1000 nm/RIU or
∼0.4 nm/% of water), good detection limit (namely, 5 ×
10–3 RIU or ∼10% water), and excellent resolution
(namely, either 6 × 10–4 RIU or 1.6% of water)
to be reliably achieved on a detection volume of about 168 fL.