Test points are essential in allowing optical circuits on a wafer to be autonomously tested after selected manufacturing steps, hence allowing poor performance or device failures to be detected early and to be either repaired using direct write methods, or a cessation of further processing to reduce fabrication costs.Grating couplers are a commonly used method for efficiently coupling light from an optical fibre to a silicon waveguide. They are relatively easy to fabricate and they allow light to be coupled into/out from any location on the device without the need for polishing, making them good candidates for an optical test point.A fixed test point can be added for this purpose, although traditionally these grating devices are fabricated by etching the silicon waveguide, and hence this permanently adds loss and leads to a poor performing device when placed into use after testing. We demonstrate a similar device utilising a refractive index change induced by lattice disorder. Raman data collected suggests this lattice damage is reversible, allowing a laser to subsequently erase the grating coupler.
Abstract:We report the fabrication of low temperature deposited polysilicon waveguides using a laser annealing process. Micro-Raman and XRD measurements reveal the quasi-single crystal-like quality of the material, which exhibits low optical losses of 5.13 dB/cm.
The intrinsic properties of silicon (Si) make it an excellent material for integrated photonics devices with small footprints [1]. To date, most of the reported devices have been based on crystalline silicon (c-Si), but this material suffers from difficult integration with electronic layers due to fabrication constraints. Subsequently, there has been growing interest in alternative forms of Si, such as hydrogenated amorphous silicon (a-Si:H), silicon nitride (SiN) and polysilicon (poly-Si) [2]. Among these materials, only poly-Si has the potential to exhibit both optical and electronic properties that are equivalent to c-Si. However, to achieve good material quality, poly-Si is typically deposited at temperatures higher than 900°C, rendering it incompatible with most CMOS fabrication processes. Thus there is a growing drive to develop new techniques to deposit poly-Si at low temperatures (<450°C) [2], but so far the optical losses in these materials have been high, limiting its use in all-optical systems employing nonlinear optical processing. In this work, we report the fabrication and characterisation of laser annealed, low temperature deposited silicon waveguides with low optical losses. Our results represent the first demonstration of nonlinear propagation in a poly-Si waveguide suitable for integration.The waveguide fabrication process starts with the deposition of 400 nm of amorphous silicon (a-Si) on a 4.7 µm thick silica box layer using a hot-wire chemical vapor deposition technique, at a temperature of 320°C [3]. Then, using e-beam lithography and dry etching, 2 µm wide wires are patterned on the a-Si film. Next, the pre-patterned waveguides are crystallised using a continuous wave argon ion laser emitting at 488 nm. By adjusting the power and scanning speed of the laser, thermal energy is transferred to the a-Si material, which melts and crystallises, forming large crystal grains along the microstructure. The processed waveguides display an ultra-smooth top surface, as shown in Fig. 1(a), while x-ray diffraction measurements reveal single crystal-like properties over lengths greater than 40 µm. Using a cut back method, we measure linear optical loss as low as 5.13 dB/cm, suitable for the observation of nonlinear dynamics.To assess the nonlinear properties of these waveguides we performed a set of measurements using a passively mode-locked laser emitting 750 fs pulses centred at 1540 nm at a repetition rate of 40 MHz. First, we measured the power at the waveguide output for different input pulse powers. The results are shown in Fig. 1(b), where we can see a clear saturation of the output power due to the nonlinear absorption of the Si material originating from the two-photon absorption [4]. Next, we recorded the optical output spectra for different input powers using an optical spectrum analyser. The recorded spectra, shown in Fig. 1(c), display clear evidence of self-phase modulation induced spectral broadening when the input pulse power increases. Note that the sharp features modulating the spectral s...
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