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deposited onto various bond pad sizes
                                                                              to determine and maintain a consistent
                                                                              height for efficient optical coupling to
                                                                              grating couplers. The translational and
                                                                              angular tolerances for both the free-form
                                                                              couplers and tapered waveguides were
                                                                              determined via simulation.

                                                                              Simulation
                                                                                3D finite difference time domain
                                                                              (FDTD) simulations were performed
                                                                              to determine the coupling efficiency
                                                                              (CE) for both presented approaches. The
                                                                              alignment tolerances of the structure
                                                                              as a function of translation between
                                                                              the two chips were calculated. For
                                                                              the evanescent coupling approach,
                                                                              si mulat ion result s usi ng A nsys-
                                                                              Lumerical’s 3D FDTD solver are shown
                                                                              in Figure 2. The gap length in the Z
                                                                              direction was input to be 0µm for the
                                                                              X/Y tolerance results and 500nm for
                                                                              both tilt and twist tolerance simulations.
                                                                                The results from the data in Figure
                                                                              2 show this design has a lateral (Y)
                                                                              tolerance  of  ±2.7μm,  vertical  (Z)
                                                                              tolerance of 2.8μm, longitudinal (X)
                                                                              tolerance of over ±150μm, twist rotation
                                                                              tolerance of  ±2.3°,  and tilt rotation
                                                                              tolerance of ±0.4°. For this simulation,
                                                                              the underfill epoxy refractive index
                                                                              is assumed to be 1.457 to match the
                                                                              refractive index of silica being used
                                                                              [10]. Further simulations indicated the
                                                                              Z-tolerance can be extended to near
                                                                              3.75µm if an epoxy with refractive
                                                                              index closer to 1.5 is used. However, as
                                                                              the epoxy refractive index increases,
                                                                              the light becomes less confined in the
                                                                              waveguides and will require longer
                                                                              tapers to compensate for the scattering
                                                                              loss. This simulation data demonstrates
                                                                              this design has comparable lateral
                                                                              a nd a ng u la r tole r a nces to t hose
                                                                              achievable using high-speed pick-and-
                                                                              place die bonders (approximately ±3-
                                                                              10µm) and has a vertical tolerance
                                                                              comparable to back-end-of-line (BEOL)
                                                                              thicknesses typical of active PICs. This
                                                                              indicates there is potential use for this
                                                                              evanescent coupler design in flip-chip
                                                                              bonded packages.
                                                                                In the case of chip-to-chip freeform
                                                                              reflectors, possible misalignments or
                                                                              tilts that may be introduced during
                                                                              assembly are necessary to determine as
                                                                              they are important metrics to evaluate
        Figure 2: 3D FDTD simulation results showing: a) coupler parameter definitions where the red is Si and the   the practicality of the device. FDTD
        blue is Si 3 N 4 , b) the translational alignment tolerance in X/Y/Z, and c) the rotational alignment tolerance where   simulations indicate that the reflectors
        tilt indicates rotation about the Y-axis and twist indicates rotation about the Z-axis. Reprinted with permission   are very tolerant to both translation and
        from [1] © The Optical Society

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