Optical: systems and elements – Diffraction – From grating
Reexamination Certificate
2000-09-29
2002-06-04
Spyrou, Cassandra (Department: 2872)
Optical: systems and elements
Diffraction
From grating
C359S569000, C359S572000, C359S574000, C359S576000, C359S199200, C359S900000
Reexamination Certificate
active
06400509
ABSTRACT:
TECHNICAL FIELD
The present invention is directed toward optical communications, and more particularly toward reduction of polarization sensitivity in optical multiplexers/demultiplexers using bulk diffraction gratings.
BACKGROUND ART
At the inception of fiber optic communications, typically a fiber was used to carry a single channel of data at a single wavelength. Dense wavelength division multiplexing (DWDM) enables multiple channels at distinct wavelengths within a given wavelength band to be sent over a single mode fiber, thus greatly expanding the volume of data that can be transmitted per optical fiber. The wavelength of each channel is selected so that the channels do not interfere with each other and the transmission losses to the fiber are minimized. Typical DWDM allows up to 40 channels to be simultaneously transmitted by a fiber.
DWDM requires two conceptually symmetric devices: a multiplexer and a demultiplexer. A multiplexer takes multiple beams or channels of light, each at a discrete wavelength and from a discrete source and combines the channels into a single multi-channel or polychromatic beam. The input typically is a linear array of waveguides such as a linear array of optical fibers, a linear array of laser diodes or some other optical source. The output is typically a single waveguide such as an optical fiber. A demultiplexer specially separates a polychromatic beam into separate channels according to wavelength. Input is typically a single input fiber and the output is typically a linear array of waveguides such as optical fibers or a linear array of photodetectors.
In order to meet the requirements of DWDM, multiplexers and demultiplexers require certain inherent features. First, dispersive devices must be able to provide for a high angular dispersion of closely spaced channels so that individual channels from a multi-channel or multiplexed beam can be separated sufficiently over relatively short distances to couple with a linear array of single channel fibers. Multiplexers and demultiplexers are preferably reversible so that a single device can perform both multiplexing and demultiplexing functions (hereinafter, a “(de)multiplexer”). Furthermore, the (de)multiplexer must be able to accommodate channels over a free spectral range commensurate with fiber optic communications bandwidth. Moreover, the devices must provide high resolution to minimize cross talk and must further be highly efficient to minimize signal loss. The ideal device would also be small, durable, inexpensive, and scalable.
Diffraction grating based multiplexers and demultiplexers have significant advantages over other technologies for dense wavelength division multiplexing applications because of their relatively low cost, high yield, low insertion loss and cross talk, uniformity of loss as well as their ability to multiplex a large number of channels concurrently. Representative diffraction grating based (de)multiplexer configurations are disclosed on applicant's commonly assigned co-pending U.S. patent application Ser. No. 09/628,774, filed Jul. 29, 2000, entitled “Echelle Grating Dense Wavelength Division Multiplexer/Demultiplexer”, the contacts of which are incorporated herein in their entirety. However, diffraction gratings have an intrinsic polarization sensitivity that can limit their usefulness in (de)multiplexing applications. That is, an optical signal propagating through an optical fiber has an indeterminate polarization state, requiring that the (de)multiplexer be substantially polarization insensitive so as to minimize polarization dependent losses, a measure of diffraction efficiency that is dependent on the polarization state of the optical signal.
There are numerous methods and apparatus for reducing the polarization sensitivity of diffraction grating fiber optic (de)multiplexers. Chowdhury, U.S. Pat. Nos. 5,966,483 and 6,097,863 (collectively “Chowdhury”), the disclosure of which is incorporated in its entirely by reference, describes a diffraction grating with reduced polarization sensitivity. Chowdhury teaches that polarization sensitivity can be minimized by orienting the reflective faces of a diffraction grating at a blaze angle “&thgr;
b
” for retro-reflecting normal incident light of a wavelength “&lgr;
b
” that is different from a median wavelength “&lgr;
o
” of a transmission bandwidth “&Dgr;&lgr;”. The blaze angle &thgr;
b
is chosen to reduce the difference between first and second diffraction efficiencies of a wavelength &lgr; within the transmission bandwidth &Dgr;&lgr;. This solution for minimizing differences in diffraction efficiency can be of limited utility because it requires limitations on election of blaze angles and blaze wavelengths that can inhibit the overriding goal of providing a diffraction grating for a (de)multiplexer accommodating a large number of closely spaced channels with high resolution, minimal cross talk and little signal loss.
Chowdhury further teaches that diffraction grating polarization sensitivity can be reduced by providing concave and convex corners between adjacent reflective steps and risers of a diffraction grating. More particularly, Chowdhury teaches that polarization sensitivity can be reduced by varying the radius of concave corners between adjacent steps and risers. While this proposal has the advantage of not placing an unwarranted restraint of selection of a blaze wavelength and blaze angle for a grating, accurately controlling the concave and convex radii on a nanometer scale could be both difficult and expensive. It can also limit the absolute efficiency of the grating.
Chowdhury also teaches that maximizing the pitch (or groove spacing) can help to minimize polarization sensitivity. However, as with Chowdhury's proposal of manipulating blaze angle and blaze wavelength to minimize polarization sensitivity, this proposal puts constraints on grating pitch that can degrade other important objectives of the diffraction grating, such as achieving suitable channel separation for DWDM signals.
McMahon, U.S. Pat. No. 4,736,360, teaches that polarization sensitivity in a bulk optic grating can be minimized by assuring that the width of the reflective surface is sufficiently large as compared to the operating wavelength of the grating. This is effectively similar to maximizing pitch as taught by Chowdhury. While this solution may have limited application, it also places what can be an unnecessary restraint on grating design choices and thus may limit the ability of the grating to perform its wavelength division (de)multiplexing function for signals having a close channel spacing.
He, U.S. Pat. No. 5,937,113, teaches yet another way to minimize polarization dependent losses for an optical waveguide diffraction grating. He teaches a diffraction grating device having an output region with a plurality of predetermined light receiving locations, A first slab waveguide region has a first birefringence, the first slab guide region being optically coupled with input and output regions of the device. A second slab waveguide region adjacent to the first slab waveguide region has a predetermined shape and predetermined dimensions providing a second different birefringence than the first slab waveguide region to provide polarization compensation for the device. This solution requires providing first and second slab waveguides and thus is not readily applicable to bulk optic devices. In any event, providing at least two slab waveguides increases product complexity and cost.
Another known method for reducing polarization sensitivity is providing a polarization separator followed by a half wave plate on one of the separated beams between a collimating optic and a grating. The polarization separator splits an incident beam into first and second beams of light, with each beam being linearly polarized along different orthogonal directions. The half wave plate located on one of the beams results in both beams having the same orthogonal polarization. While this method has the advantage of not placing limitations on the design of the
Bach Bernhard W.
Sappey Andrew D.
Jr. John Juba
Spyrou Cassandra
Swanson & Bratschun LLC
Zolo Technologies, Inc.
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