Methods and systems relating to optical waveguide tapers
View Patent ↗Photonic integrated circuits required connection to germanium doped silica cored optical fibers or silica cored and fluorine doped silica cladding optical fibers which have low index contrast and large mode field diameters. However, the optical waveguide within a photonic integrated circuit such as formed using silicon-on-insulator or compound semiconductors tends to be high index contrast and small mode field diameter. Accordingly, it is necessary to implement adiabatic waveguide tapers with a high coupling efficiency and small footprint in order to couple into the photonic integrated circuits to/from the optical fiber. Prior art tapers have been generally high loss and absorb valuable die footprint. In contrast the inventors demonstrate a small low loss waveguide taper designed using a methodology they refer to a “constant loss”.
1. A waveguide comprising:
an input waveguide having a first predetermined width and being configured for coupling to a single-mode optical fiber;
an output waveguide having a second predetermined width; and
an optical waveguide taper increasing in width from the first predetermined width to the second predetermined width, the optical waveguide taper decreasing an effective mode area from the input waveguide to the output waveguide, the input waveguide, the output waveguide and the optical waveguide taper being single-mode and having a uniform thickness, wherein an optical loss versus propagation distance from the first predetermined width to the second predetermined width of the optical waveguide taper is approximately constant, the optical waveguide taper comprising a number of waveguide segments of incrementally increasing width from the first predetermined width to the second predetermined width, the waveguide segments contacting each other, each waveguide segment having a given length and a given width along its corresponding length.
2. The waveguide according to claim 1 , wherein
an incremental loss between each consecutive pair of waveguide segments is approximately constant.
3. The waveguide according to claim 1 , wherein
a length of each waveguide segment is constant.
4. A device comprising:
a silicon-on-insulator (SOI) optical waveguide comprising an input of a first predetermined width and an output of a second predetermined width, the input being configured for coupling to a single-mode optical fiber, wherein the SOI optical waveguide increasing in width according to a predetermined profile between the input and the output and decreasing an effective mode area from the input to the output, the SOI optical waveguide being single-mode from the input to the output and having a uniform thickness, an optical loss versus propagation distance from the first predetermined width to the second predetermined width of the predetermined profile is approximately constant, the predetermined profile comprising a number of waveguide segments of incremental increasing width from the first predetermined width to the second predetermined width, each of the waveguide segments having a given length and a given width along its corresponding length, the waveguide of segments contacting each other; and an incremental loss between each consecutive pair of waveguide segments being approximately constant.
5. The device according to claim 4 , wherein
the SOI optical waveguide supports transverse electric (TM) optical signals within a predetermined wavelength range;
the first predetermined width is approximately 155 nm; and
the second predetermined width is approximately 220 nm.
6. The device according to claim 4 , wherein
the SOI optical waveguide supports transverse magnetic (TM) optical signals within a predetermined wavelength range;
the first predetermined width is approximately 100 nm; and
the second predetermined width is approximately 220 nm.
7. The device according to claim 4 , wherein
the predetermined profile is a taper from the first predetermined width to the second predetermined width wherein an optical loss versus propagation distance along the taper is approximately constant.