This invention relates generally to well structures for hybrid optical waveguides.
An optical waveguide is a structure that conveys an optical light signal. Conventionally, an optical waveguide may include a substrate and a core encased within an upper and lower cladding. The bulk of the light signal typically travels within the core along the axis of the waveguide structure.
In order to access the core, a well may be formed through the upper cladding. This well may be formed by etching the upper cladding. Sometimes such etching does not completely expose the core of the waveguide, resulting in reduced access to the light signal. In other cases, the core of the waveguide might not only be exposed but it may be damaged by the etching process, resulting in reduced transmission of the light signal.
After the well is formed, the well may be filled with a polymer. If the well is not appropriately formed, voids may be formed within the well where the polymer cannot completely fill the well, also resulting in reduced transmission of the light signal.
Thus, there is a need to form wells for accessing optical cores in hybrid optical circuits that are less prone to forming voids or bubbles or cuts or other damage to the core itself.
Referring to the transverse cross-sectional view of
As shown in
After removal of any masking materials, the thickness of the etch stop layer 16a may be increased by plating additional metal, such as nickel, up to a thickness of 2 microns in one embodiment of the present invention shown in
Referring next to
The etch stop layer 16a is then completely removed as shown in
Provided that the opening produced by the second mask is smaller than the etch stop 16a pattern produced by the first mask, the dimensions of the well 24 are determined, in its upper region 26, by the dimensions of the second mask and its process parameters and, in the lower region 20, by the first mask and its process parameters.
As shown in
A polymer 22 may be dispensed into the well 24 as shown in
The effect of such a bubble can be very negative on the performance of the finished waveguide. The index of refraction difference between the inside and the outside of the bubble is typically 0.5, resulting in strong optical scattering and refraction. Any bubbles within the optical path of the waveguide may degrade the insertion loss.
By enlarging the size of the well 24 until any bubbles trapped at its edge lay outside the optical path, the problem may be reduced. However, such a method may leave the problem unchanged at the ends of the waveguide where bubbles may be trapped directly between the core 12 and the upper cladding 18. By making the etch stop layer 16a thick enough so that the dynamics of the polymer 22 spreading produces full wetting under the overhang 28, bubble formation may be reduced.
A cut is the opposite type of problem. If the second mask is displaced along the direction of the waveguide so that the overhang 28 becomes negative, the etch of the top cladding 18 produces a cut in the core 12. The depth of this cut will depend on the process parameters. This imperfection may produce scatter and refraction loss just as a bubble does, although with a refractive index difference corresponding to the core 12 to polymer 22 refractive index difference. Since the cut is located within the core, its optical effects can be severe.
By using a two-step fabrication for the etch stop layer 16a, both bubbles and cuts may be reduced. Cuts may be reduced by making the second mask pattern smaller than the first so that the alignment errors in the process do not permit etching of the core. Unfortunately, this approach creates the possibility of bubbles trapped into the resultant overhang 28. Bubbles may be reduced by using an etch stop layer 16a that is thick enough to raise the overhang 28 above a threshold level where complete wetting occurs at the edge of the well and under the overhang 28.
The dual layer metal etch stop 16a is used because the seed layer 16 may be very thin and is reproducibly patterned with a wet etch step that removes traces of the metal (and thereby optical loss) from the waveguide. The dual metal etch stop 16a may also be advantageous because the thickness of the patterned etch stop layer can be reproducibly manufactured by controlling the deposition process and time.
While the present invention has been described with respect to a limited number of embodiments, those skilled in the art will appreciate numerous modifications and variations therefrom. It is intended that the appended claims cover all such modifications and variations as fall within the true spirit and scope of this present invention.
This application is a divisional of U.S. patent application Ser. No. 10/609,803, filed on Jun. 30, 2003 now U.S. Pat. No. 7,146,086.
Number | Name | Date | Kind |
---|---|---|---|
5540346 | Fujimoto et al. | Jul 1996 | A |
6002823 | Chandross et al. | Dec 1999 | A |
6031957 | Suzuki et al. | Feb 2000 | A |
6044190 | Kashyap | Mar 2000 | A |
6120693 | Petti et al. | Sep 2000 | A |
6477295 | Lang et al. | Nov 2002 | B1 |
6732550 | Won | May 2004 | B2 |
7058265 | Amparan et al. | Jun 2006 | B2 |
20010046363 | Purchase et al. | Nov 2001 | A1 |
20020151168 | Wang et al. | Oct 2002 | A1 |
20020186950 | Muleā² et al. | Dec 2002 | A1 |
Number | Date | Country | |
---|---|---|---|
20070041691 A1 | Feb 2007 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 10609803 | Jun 2003 | US |
Child | 11586790 | US |