Coherent light generators – Particular beam control device – Tuning
Reexamination Certificate
2001-01-02
2004-02-10
Scott, Jr., Leon (Department: 2828)
Coherent light generators
Particular beam control device
Tuning
C372S092000, C372S094000, C372S032000
Reexamination Certificate
active
06690687
ABSTRACT:
BACKGROUND OF THE INVENTION
I. Field of the Invention
The invention generally relates to tunable lasers and in particular to tunable lasers for use in a dense wavelength division multiplexers (DWDM).
II. Description of the Related Art
A DWDM is a device for simultaneously transmitting a set of discrete information channels over a single fiber optic transmission line. A conventional fiber optic transmission line is capable of reliably transmitting signals within a bandwidth of 1280 to 1625 nanometers (nm), the “low loss” region for silica fiber. Within that overall bandwidth, the International Telecommunications Union (ITU) has defined various transmission bands and specified certain transmission channel protocols for use within each transmission band. One example of a transmission band is the ITU “C” band, which extends 40 nm from 1525 nm to 1565 nm. Within the C band, specific transmission channel protocols of 40, 80, or 160 discrete channels are defined and, for each protocol, the ITU has defined a grid of transmission wavelengths, with each line corresponding to an acceptable transmission wavelength. For the 40 channel protocol, the corresponding ITU grid has 40 lines with channel spacing of 0.8 nm; for the 80 channel protocol, the corresponding ITU grid has 80 lines with channel spacing of 0.4 nM; and so forth. The protocols have been defined to ensure that all DWDM transmission and reception equipment is fabricated to operate at the same wavelengths. Other exemplary ITU transmission bands are the S- and L-bands.
To simultaneously transmit the set of channels on a fiber optic cable, the DWDM employs a set of the individual lasers, with one laser per channel.
FIG. 1
illustrates a DWDM
100
having forty individual lasers
102
for transmitting optical signals via a single optic fiber
104
. An optical multiplexer
106
couples signals received from the individual lasers via a set of intermediate optic fibers
107
into output optic fiber
104
. Each laser transmits at a different wavelength of the forty channel ITU C band. This enables forty separate channels of information to be transmitted via the single optical fiber
104
to a de-multiplexer (not shown) provided at the far end of the optical fiber.
To permit the DWDM to transmit forty separate channels simultaneously, each individual laser must be tuned to a single ITU transmission channel wavelength. Preferably, widely tunable lasers (WTLs) are employed as the transmission lasers to permit any of the individual lasers to be tuned to any of the ITU channels. The wide tunability is achieved by choosing the amplifying medium with a wide gain curve (typically a semiconductor structure) and configuring the WTL in such a way that low cavity loss is only achieved at a narrow wavelength region. The WTL is tuned by changing the aforementioned peak in the spectral response of the cavity to operate at a particular resonant wavelength aligned with a selected one of the ITU channel wavelengths. The desire to achieve low bit error rate leads to requirements for high spectral purity of the emitted light which is usually stated in terms of the side mode suppression, i.e. the ratio of the light intensity emitted by the WTL at the side band wavelength to the intensity of the main mode. While the requirements may differ from system to system, typically for reliable operation of a DWDM transmitting ITU channels, the side mode suppression should be 30 decibels (dB) or better. Such requirements often are not easily reconciled with the wide tunability, particularly with relatively inexpensive WTLs. Furthermore, while monolithic semiconductor WTLs, currently the state of the art devices, provide the necessary degree of miniaturization and ruggedness, tuning of such devices involves a complicated tuning pattern. That is, tuning currents are applied to multiple sections of the laser and their influence on the emitted wavelength and spectral purity is not independent.
Accordingly, it would be desirable to provide an improved WTL capable of being more easily, precisely and reliably tuned to a selected wavelength and in particular to provide an improved WTL capable of meeting the aforementioned 30 dB sideband requirement for use within DWDMs transmitting at ITU channel wavelengths. It is to these ends that the invention is primarily directed.
SUMMARY OF THE INVENTION
In accordance with a one aspect of the invention, a semiconductor laser is provided having a cavity comprising gain chip, an interferometric wide tuning port, and a ring resonator mirror. The gain chip provides radiant energy and amplification for resonance within the cavity. The ring resonator mirror limits resonance within the cavity to a set of sharp resonance peaks. The interferometric wide tuning port, which may be a Mach-Zehnder interferometer, selects one resonance peak out of the aforementioned set of peaks based on a wide tuning profile having a broad peak. The wide tuning port is configured to align a wavelength of the broad peak of the wide tuning profile near a selected wavelength. The ring resonator mirror is configured to align a wavelength of one of the sharp peaks also near the selected wavelength. In this manner, the laser cavity resonates primarily at the selected emission wavelength. Other sharp resonant peaks permitted by the ring resonator are filtered by the wide tuning port so as to substantially limit the amplitudes thereof. Hence, transmission sidebands of the laser are substantially reduced. With appropriate selection of components, the side bands may be limited to amplitudes 30 dB below the selected transmission wavelength.
In an exemplary embodiment, the gain chip is formed of III/IV material. The Mach-Zehnder wide tuning port and the ring resonator mirror are formed on a silicon tuning chip utilizing rib-loaded planar wave guides with silicon oxynitride core and silicon dioxide claddings. An output optical channel of the gain chip is coupled to an input optical channel of the Mach-Zehnder wide tuning port. The Mach-Zehnder wide tuning port includes a splitter for splitting the input channel into a pair of channels of differing lengths and a combining section for combining the pair of optical channels into a single output channel. The single output channel of the Mach-Zehnder wide tuning port is coupled to an input channel of the ring resonator mirror. The ring resonator mirror also includes a splitter for splitting the input optical channel into a pair of parallel channels. A ring-shaped channel is formed between the pair of parallel channels with portions of the ring-shaped optical channel sufficiently close to the pair of parallel channels to permit evanescent coupling.
With this configuration, optical signals generated by the gain chip propagate through the Mach-Zehnder wide tuning port and into the ring resonator. Optical signals of certain wavelengths are reflected back into the Mach-Zehnder wide tuning port and ultimately are reflected again by the gain chip, thereby permitting resonance at those wavelengths and limiting resonance at other wavelengths, resulting in the aforementioned sharp resonance peaks. The wavelengths reflected by the ring resonator depend upon the length of the ring. The ring resonator is heated, or otherwise controlled, to vary the dimensions and the refractive index of the ring so as to maintain one of the sharp peaks at a selected transmission wavelength, such as at a particular ITU channel wavelength. As the optical signals reflected between the ring resonator and the gain chip propagate back and forth through the Mach-Zehnder wide tuning port, the signals are split between the two channels of differing lengths in the wide tuning port resulting in optical interference. The optical interference limits the ability of the laser cavity to resonate at wavelengths wherein destructive interference occurs. As a result, resonance is substantially limited to within a broad peak determined by the relative lengths of the two channels. The Mach-Zehnder wide tuning port is heated, or otherwise controlled, to vary the relative lengths a
Ksendzov Alexander
May Randy Dean
Jr. Leon Scott
Kukkonen, III Carl A.
SpectraSensors, Inc.
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