filters, [3] polarizers with embedded photon emitters, [4] label-free optical biosensors, [5,6] fluorophore enhancers, [7] and amplifiers for surface-enhanced Raman scattering (SERS). [8] Many of these applications would benefit from increasing the interaction between surface-confined resonant electromagnetic fields and the materials being probed such as biomolecules, [9] cells, [10] viral particles, [11] Raman tags, [8] liquid crystals, and fluorophores [7] that reside on the PC surface. Open-faced PC slabs that interface with liquid media, such as those used for label-free biosensing applications, are generally comprised of a subwavelength, periodic surface structure within a low refractive index material (such as polymer or SiO 2 ) that is subsequently coated with a layer of high refractive index material (such as TiO 2 or Si 3 N 4 ), which is then immersed into the sensing medium. [12] The spatial electromagnetic field profile of the device mainly resides within the higher refractive index regions, but exponentially decays into its lower refractive index surroundings. Modulation of the PC's resonant wavelength derives from perturbations of the local refractive index (for example, displacing water with cells/biomolecules, or changing the orientation of a liquid crystal film) within the evanescent tail of the electromagnetic field. However, the short penetration depth of the electromagnetic field leaves the device sensitive to change only in close proximity to the surface. [13] In order to increase the penetration depth of the evanescent field profile into the sensing medium, which is desirable for improved sensitivity to bulk refractive index changes, a thinner waveguide layer can be used to weaken the confinement of the mode and enhance the leakage of the evanescent field into the sensing medium. Meanwhile, a drastic reduction of the refractive index of the cladding layer such that it is less than that of the sensing medium works in a more straightforward and universal manner. Our hypothesis is that if the grating structure is comprised of a cladding material with a lower refractive index than the media coving the PC surface, then the mode structure of the electromagnetic standing wave will relocate its spatial distribution to reside mainly in the sensing medium, and thus a greater degree of resonant wavelength modulation can be achieved for a given change of refractive index in the surrounding medium. In order to achieve this more sensitive optical architecture, conventional low refractive index bulk materials utilized for the PC cladding can be Porous SiO 2 (PSiO 2 ) with ultralow refractive index (n = 1.09) is incorporated as the cladding of a photonic crystal (PC) refractive index sensor with enhanced sensitivity through the establishment of resonant modes that principally reside in the liquid medium covering the PC surface. PSiO 2 , obtained by thermal oxidation of porous Si that has been transferred to a transparent substrate, is transparent at visible and near infrared wavelengths with a refractive ind...