Coherent light generators – Particular beam control device – Tuning
Reexamination Certificate
2000-02-18
2003-02-25
Scott, Jr., Leon (Department: 2828)
Coherent light generators
Particular beam control device
Tuning
C372S019000, C372S092000, C372S098000, C372S102000, C372S107000
Reexamination Certificate
active
06526071
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of Invention
The invention pertains to wavelength-agile laser transmitters for wavelength-division-multiplexed (WDM) optical communications networks. More particularly, the invention pertains to laser transmitters with internal wavelength referencing that can be remotely switched to arbitrarily selectable channels on a standard grid, and to re-configurable optical communications networks.
2. Description of the Related Art
The telecommunications network serving the United States and the rest of the world is presently evolving from analog to digital transmission with ever increasing bandwidth requirements. Fiber optic cable has proved to be a valuable tool, replacing copper cable in nearly every application from large trunks to subscriber distribution plants. Fiber optic cable is capable of carrying much more information than copper with lower attenuation.
The T-1 standards committee ANSI has provided a draft document, “ANSI T1.105-1988”, dated Mar. 10, 1988, which sets forth specifications for rate and format of signals which are to be used in optical interfaces. The provided specifications detail the Synchronous Optical Network (SONET) standard. SONET defines a hierarchy of multiplexing levels and standard protocols which allow efficient use of the wide bandwidth of fiber optic cable, while providing a means to merge lower level DS
0
and DS
1
signals into a common medium. In essence, SONET established a uniform standardization transmission and signaling scheme, which provided a synchronous transmission format that is compatible with all current and anticipated signal hierarchies. Because of the nature of fiber optics, expansion of bandwidth is easily accomplished.
Currently this expansion of bandwidth is being accomplished by what is known as “wavelength division multiplexing” (WDM), in which separate subscriber/data sessions may be handled concurrently on a single optic fiber by means of modulation of each of those subscriber datastreams on different portions of the light spectrum. Therefore, WDM is the optical equivalent of frequency division multiplexing (FDM). Current International Telecommunications Union (ITU) specifications call for channel separations of approximately 0.4 nm, i.e., 50 GigaHertz. At this separation, as many as 128 channels may be carried by a single fiber in a bandwidth range within the same capacity of an erbium doped fiber amplifier (EDFA). Each subscriber datastream is optically modulated onto the output beam of a corresponding semiconductor laser. The modulated information from each of the semiconductor lasers is combined onto a single optic fiber for transmission.
The lasers presently deployed are distributed-feedback (DFB) diode lasers. The wavelength grid is defined by the transmission peaks of a Fabry-Perot reference etalon. The technology for fabricating these etalons from glass or fused silica in large quantities at reasonable cost is well developed. Present transmitters use a combination of a DFB laser and a reference etalon in a feedback control loop. DFB lasers suffer from the drawback that they have small tuning ranges of ~3 nm (See, e.g., J. Carroll, J. Whiteaway, & D. Plumb,
Distributed feedback semiconductor lasers
, SPIE Press, 1998). A DFB laser's characteristics can only be approximately determined by design. In practice the center wavelengths are distributed across the grid span due to statistical variations in the manufacturing process. Thus each DFB laser transmitter must be individually sorted and is usable for only one channel or a small number of adjacent channels. As a result, DFB laser transmitters cannot be assigned to arbitrary channels.
On the other hand, WDM networks are evolving towards re-configurable architectures in which each transmitter's wavelength must be re-selectable by remote command. Re-configurable networks offer significant capacity, reliability, and management advantages over static systems (See, e.g., R. Ramaswami and K. Sivarajan,
Optical Networks, A Practical Perspective
, Morgan Kaufmann Publishers, 1998).
Thus there exists a need for laser transmitters that can be arbitrarily switched to desired channel wavelengths within the wavelength grid of a WDM network.
SUMMARY OF THE INVENTION
The present invention provides a tunable external cavity laser (ECL) with a compact form factor and precise tuning to any selected center wavelength of a predetermined wavelength grid. The ECL may thus be utilized in telecom applications to generate the center wavelengths for any channel on the ITU or other optical grid. The ECL does not require a closed loop feedback. A novel tuning mechanism is disclosed which provides for electrical or mechanical tuning to a known position or electrical parameter, e.g., voltage, current, capacitance, with the required precision in the selected center wavelength arising as a result of a novel arrangement of a grid generator and a channel selector. The grid generator exhibits first pass bands which correspond to the individual channels of a selected wavelength grid and a finesse which suppresses side modes of the laser. The channel selector exhibits second pass bands that are wider than the first pass bands. In an embodiment of the invention the second pass bands have a periodicity that at least substantially corresponds with the separation between the shortest wavelength channel and the longest wavelength channel of the selected wavelength grid and a finesse which suppresses channels adjacent to the selected channel. The broad second pass bands of the channel selector reduce the sensitivity of the ECL to tuning variations of the channel selector about the selected channel, thus avoiding the requirement of a closed loop feedback system of for example wavelength to control the channel selector.
In an embodiment of the invention a tunable external cavity laser tunable to each selected center wavelength of a plurality of channels each centered on a corresponding gridline of a selected wavelength grid is disclosed. The tunable external cavity laser includes a gain medium, a grid generator and a channel selector. The gain medium to emit a beam. The grid generator is located in an optical path of the beam, and the grid generator of a first selected optical path length determinative of a first free spectral range substantially corresponding to a spacing between adjacent gridlines of the selected wavelength grid. The channel selector is located in the optical path of the beam and the channel selector with a second free spectral range broader than the first free spectral range and a selected order of the channel selector tunable within the selected wavelength grid to tune the beam to a selected one of the plurality of channels of the wavelength grid.
In an alternate embodiment of the invention the tunable external cavity laser includes the gain medium, a first filter and a tunable filter. The gain medium to emit a beam. The first filter is located in an optical path of the beam. The first filter exhibits first pass bands substantially corresponding to the channels of the selected wavelength grid. The tunable filter is located in the optical path of the beam. The tunable filter exhibits second pass bands broader than the first pass bands. A selected order of the tunable filter is tunable within the wavelength grid to tune the beam to a selected one of the plurality of channels of the wavelength grid.
In an alternate embodiment of the invention a method for tuning a beam emitted by a gain medium to a corresponding center wavelength for each of a plurality of channels of a selected wavelength grid is disclosed. The method for tuning comprising the acts of:
filtering the beam to provide feedback to the gain medium of a first periodic set of wavelengths substantially corresponding with the center wavelengths for each of the plurality of channels; and
tuning the beam to provide feedback to the gain medium of a selected one of the center wavelengths of the first periodic set of wavelengths to tune the beam to the selected one of the plurality of channel
Chapman William B.
Green Evan D. H.
Jenq Michael Y.
Zorabedian Paul
Bozicevic Field & Francis LLP
Cannon Alan W.
Jr. Leon Scott
New Focus Inc.
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