-We present Bragg gratings with an effective index change introduced by implanting germanium at only 15KeV. An extinction ratio of 35dB at 1350nm is demonstrated for device lengths of 600μm, furthermore laser annealing is demonstrated.
IntroductionIn the information age current technologies struggle to deliver the data rates required by modern communications and computer bus systems. Silicon photonics has the potential of overcoming some of these obstacles by relying on a well understood material system and technology [1]. However the full adoption of silicon based photonics would require complex integrated optoelectronic systems to be manufactured in high volumes at low costs. These requirements cannot be met without enabling a wafer scale testing [2] strategy in a similar fashion to what has been happening for many decades in the integrated electronics industry. The current challenge for silicon photonics in this area is represented by the inability of the light signal to access a processed wafer without substantially modifying the wafer surface. Most of the solutions presented for light coupling into test samples rely on substantially modifying the structure of the material to enable end fire coupling, prism coupling [3], inverted tapers [4], and cantilever structures [5]. Introducing these kinds of test points, or even wavelength selective test points such as etched or metal gratings on a processed wafer can potentially introduce undesired alterations of the light propagation, such as scattering and losses, as well as interfering with successive processing steps. In order for optical wafer scale testing to become a viable technology, optical wafer scale testing should be implemented as a minimally intrusive technology. The use of ion implanted optical structures is particularly suited for these applications, as the refractive index change can be introduced on the wafer surface without altering the general topography of the wafer. Furthermore, since the planarity of the wafer is retained, it could be possible to employ these structures for applications that require extensive surface interaction such as bonding or flip chip interactions, and sensing. The use of a low energy/low dose implant conditions (10 15 ion/cm 2 , as opposed to general doping densities which can reach 10 19 ion/cm 2 ) potentially allows minimal optical losses to be introduced by the implantation process.