BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1
a illustrates a first configuration for a tunable laser;
FIG. 1
b illustrates a second configuration for a tunable laser;
FIG. 2 is a schematic of shows a directly modulated tunable laser with an RF switch;
FIG. 3 is a schematic a directly modulated tunable laser with a MEMS RF switch;
FIG. 4 is a semi-schematic/semi-block diagram of a further embodiment of a directly modulated tunable laser with a MEMS RF switch;
FIG. 5 illustrates a laser chip flip chip mounted on a MEMS switch chip, and
FIGS. 6
a-c illustrate an embodiment of a MEMS RF switch.
DETAILED DESCRIPTION
FIGS. 1
a and 1b show two configurations for tunable lasers using a DFB laser array. In some embodiments lasers in the array are other than DFB lasers. For example, in some embodiments, the lasers are DBR lasers or other lasers, and in some embodiments the lasers are VCSELs.
FIG. 1
a shows a first configuration for a tunable laser using an array of lasers. In the first configuration a moveable mirror 40 switches light from a selected laser of an array of lasers 10 into a fiber 60. Generally, the movable mirror tilts to couple the correct beam into the fiber. As shown in FIG. 1a the lasers are on a common substrate 20, with a beam emitted by the laser collimated by a first lens 30 between the lasers and the mirror and focused into the fiber by a second lens 50 between the mirror and the fiber.
FIG. 1
b shows a second configuration for a tunable laser using an array of lasers. In the second configuration an integrated combiner 42 is used to provide light from lasers in an array of lasers 10 to a fiber 60. The integrated combiner is lithographically defined on the laser chip in most embodiments. As in the configuration of FIG. 1a, the lasers are on a common substrate 20 and light from the lasers is collimated by a first lens 30 and focused into the fiber by a second lens 50. Generally only a single laser of the array is activated at a given time, and accordingly light collimated and focused by the lenses and received by the fiber is light from only the activated laser. In addition, in various embodiments different combinations of lenses may be used, or even a single lens in some embodiments.
In most embodiments of the configurations of FIGS. 1a and 1b each individual laser in the array of lasers emits light at a different wavelength than other lasers in the array of lasers. In addition, in FIGS. 1a and 1b only three elements of the DFB laser array are shown. Typically the number is about 12, and the devices are temperature tuned in order to achieve any of about 80 wavelengths in a main communication band.
For a directly modulated application, when using an array of lasers, an RF modulation signal generally is switched to a selected laser as well as a DC bias signal. As shown in FIG. 2, a DC current source 110 provides a current that is switched with a low frequency switch 120 through bypass inductors 130 to a laser array 10, with the laser array on a common substrate 20. The switch 120 provides the current to a selected laser of the laser array, with the selected laser dependent on the state of the switch. An RF source provides a data or modulation signal that is switched by an RF switch 160 through bypass capacitors 150 and matching resistors 140 to the selected laser, so the selected laser receives both the bias current and the modulation signal. The inductors generally decouple the RF from the DC parts of the circuit and prevent the RF from being lost into the DC source.
This configuration is relatively complex with a DC current switch, an RF switch, an array of capacitors, an array of inductors, and an array of matching resistors. Moreover, a typical RF switch for this application, such as the Hittite Microwave Corporation GaAs based MESFET switch, has an insertion loss of up to 3 dB at 10 Gb/s.
FIG. 3 shows a circuit configuration using a MEMS RF switch 200. A laser array 10 on a common substrate 20 receives an RF signal from an RF signal source 20 and a DC bias signal from a DC signal source 110, with as illustrated the DC source coupled to laser anodes and the RF signal source coupled to laser cathodes. The DC signal source provides a DC bias signal, a DC current, to the laser array with the laser receiving the DC current dependent on the state of the MEMS RF switch. The RF signal source provides a data or modulation signal to the laser array.
A bypass capacitor 240 couples a signal line between the DC source and the MEMS RF switch to ground. The bypass capacitor also serves as the return pathway for the high speed RF signal. Accordingly, the laser effectively receiving the RF signal is also dependent on the state of the switch, with the switch selectively coupling the DC bias signal and the RF modulation signal to a selected laser (with the other lasers open circuited). In addition, as the MEMS RF switch can conduct DC as well as RF, no other additional integrated circuit may be required to perform switching functions. In addition, as illustrated a matching resistor 210 and a coupling capacitor 240 couple the RF signal source to the laser array, and an inductor 230 DC couples the laser cathodes to ground. In most embodiments, unlike the previously described configuration, only a single element of each type is used rather than an array of each type of element.
Thus, in the embodiment of FIG. 3, the RF signal goes through the matching (termination) resistor through the laser array and down to ground through the MEMS RF switch, while the DC first goes through the MEMS RF switch, through the array and then to ground through the inductor. This greatly simplifies the circuit compared to the layout of for example FIG. 2.
FIG. 4 shows portions of another implementation of directly modulated laser array, for example for 10 Gbps systems. In the embodiment of FIG. 4 a laser array 411 is configured to receive a modulation signal from an RF source 413 and a bias signal from a DC source (not shown). The RF source is coupled, as illustrated, to laser cathodes of the laser array, with a bias T circuit 415 between the RF source and the laser cathodes and the RF source AC coupled to the lasers by the bias T circuit. Anodes of the lasers of the laser array are selectively coupled to a further bias T circuit 417 by a MEMS RF switch 419. In most embodiments the DC source is coupled to a DC port of the further bias T circuit 417. The AC port of the further bias T circuit is coupled to ground, to complete the RF portion of the circuit.
The embodiment of FIG. 4 also has a matching (termination) resistance approximate the end of the transmission line following the laser and RF switch. Often the inductance in the RF pathway increases as the physical distance between the matching (termination) resistor and ground is increased, degrading bandwidth and return loss of the RF pathway, and the RF signal integrity may be degraded. The size of the RF MEMS switch, which is in the RF pathway, hence affects the signal integrity of the optical signal. The embodiment of FIG. 4, therefore is believed to allow for larger MEMS chip size for high data frequency applications. The RF MEMS switch may be designed to offer a characteristic impedance of 50 Ohms or 25 Ohms depending the RF driver used in the application, and the termination resistance may be a 45 Ohm resistor. This configuration for the modulated laser to appear electrically as a matched transmission line yielding high bandwidth and low return loss.
The laser diode appears as a capacitor for high frequency RF signals even when it is not turned on. As a result, in the architectures shown in FIGS. 3 and 4, the laser stripes that are not turned on appear as short stubs in the RF signal pathway. The total length of this parasitic stub is the sum of the length of the wire bond and the length of the trace on the MEM's chip to the switch element. The presence of stubs can cause parasitic resonances that will impact the RF signal integrity and necessitates the use of extremely short wire bonds between the laser chip and MEM's chip.
FIG. 5 shows a laser chip 511 mounted in flip chip fashion on a MEMS chip 513 directly. In this case, the MEMS chip makes contact with the individual lasers from the bottom side. This design is believed to further reduce parasitic inductive discontinuity in the RF signal path.
The RF MEMS switch is in many embodiments a moveable cantilever based component, available from a number of sources, although other structures may be used in various embodiments. A characteristic that is believed desirable is a low off state capacitance and the ability to conduct DC as well as AC. FIGS. 6a-c show an implementation of such a simple two port RF switch, such as discussed in “Mechanics-based solutions to RF MEMS switch stiction problem”, Mercado, L. L.; Kuo, S.-M.; Lee, T.-Y. T.; Lianjun Liu; IEEE Transactions on Components and Packaging Technologies, Volume 27, Issue 3, September 2004 p. 560-567, incorporated by reference herein. A cantilever 711 is free to move in a y-direction. The cantilever is electrostatically actuated to move towards a substrate 713 by application of a high voltage to a pad 715 under the cantilever. As the cantilever moves down towards the pad, the cantilever shorts two contacts 717a,b and makes an electrical connection. To release the cantilever, the high voltage is removed from the pad and the restoring force of the cantilever lifts the cantilever, acting as a shorting bar, off the contacts. In one implementation the switch comprises an array of corresponding cantilevers, pads, and contacts, with high voltage applied to a particular pad to select one element of the laser array.
There are advantages of a MEMS-based cantilever switch for the tunable laser application. When the device is off and the cantilever is raised, there is very little capacitance between the two sides of the switch. The device also conducts DC as well as RF, and the distance between the pads can be made very small. Any parasitic capacitance between the cantilever and ground, such from the electrostatic pad under the cantilever is largely inconsequential as the switch grounds the lasers anyway.
There are also particular advantages to this implementation. RF MEMS switches typically have lifetime issues when cycled more than a billion times. Since the tunable laser is not expected to switch more than a few thousand times, we do not expect any reliability issues. Furthermore, it is possible to turn off the RF and DC sources prior to switching and therefore “hot switching” is not required. This significantly reduces any chance of a discharge between the contacts in the RF switch that could degrade the performance.
Accordingly, the invention provides for directly modulated tunable lasers. Although the invention has been described with respect to certain embodiments, it should be recognized that the invention may be practiced other than as specifically discussed, for example through the use of insubstantial variations of aspects of embodiments of the invention.
Patent Application
20080025359
