We have fabricated 3D photonic crystals based on the woodpile structure by means of the two-photon polymerization technique. The crystals have a photonic bandgap at a wavelength of 1.2 lm and show superprism effects at wavelengths slightly below their PBG. We have demonstrated these wavelength-dependent dispersion properties experimentally, and they are in good agreement with our theoretical calculations. We were able to observe a change in the propagating angle of more than 10°for a wavelength tuning range of 20 nm. This effect is two orders of magnitude larger than in conventional prisms. The results show the great potential of low-refractive-index 3D PCs, fabricated in a very fast and single-step process, to serve directly as functional micro-optical devices in the NIR wavelength regime.
ExperimentalFor the fabrication of the woodpile structures, organic/inorganic hybrid polymers of high optical quality, called Ormocers, were used. After laser irradiation, the samples were developed in a mixture of 4-methyl-2-pentanone and isopropyl alcohol (volume ratio of 1:2) for approx. 1 min and subsequently rinsed in isopropyl alcohol. To fabricate the structures by means of 2PP, we used an optical parametric oscillator (Coherent Mira OPO) at a wavelength of 580 nm, a repetition rate of 90 MHz, and pulse duration of 100 fs. The pulses were focused into a thin Ormocer film with an immersion oil objective lens (Olympus; numerical aperture, NA= 1.4, 100×). In order to move the laser focus three-dimensionally through the resin, the sample was mounted on a computer-controlled piezo-driven nanoscanner (PI). The transmission spectra were measured with a FTIR spectrometer (Thermo Nicolet) in combination with an IR microscope. The IR light was focused onto the sample using a 32× reflective microscope objective. The superprism characterization was performed with a tunable Ti:sapphire laser operated in continuous-wave mode (Spectra Tsunami), allowing for a maximum wavelength of approx. 1020 nm. The light was focused onto the crystals with a 6.3× objective lens (NA= 0.2), leading to a focal size of approx. 10 lm. The angles of propagation were derived quantitatively by computational analysis of the CCD images of the propagating light (a Gaussian function was fitted to the recorded light distribution at different positions inside the crystal. The accuracy of the fitting determined the size of the error bars). All of the band structures shown were calculated using the freely available MIT Photonic Bands software package [23]. Calculations of the transmittance and reflectance of the woodpile structures were not performed.