Optical devices that perform optical filtering and can be tuned to select one or more narrow band of wavelengths from a wider wavelength spectrum are known as tunable optical filters. They are used in a variety of optical systems, e.g., wavelength division multiplexed (WDM) systems. In WDM systems that operate typically over wavelength bands of tens of nanometers, tunable optical filters are used for optical performance monitoring (OPM) to ensure that signal power, signal wavelength, and/or signal to noise ratios (OSNR) are within specified limits. Other applications for tunable optical filters include optical noise filtering, noise suppression, wavelength division demultiplexing, and optical routing.
Complex state-of-the-art dense wavelength division multiplexed (DWDM) systems have many channels operating across a wide optical spectrum. Monitoring these channels is a challenge because many measurements are required. A monitoring equipment that reduces the time and complexity of performing these measurements can significantly increase overall system performance and reduce system costs.
One or more embodiments of the present invention provide a reconfigurable optical device, e.g., a reconfigurable optical add/drop multiplexer (ROADM), that has a high degree of flexibility such that any wavelength channel from any optical signal introduced through add ports may be added to any of the optical signals transmitted through output ports, and any wavelength channel from any optical signal received through inputs ports may be dropped through any of drop ports. The add/drop functionality provided by a ROADM according to one or more embodiments of the present invention can be characterized as colorless, directionless, and contentionless.
An optical device, according to an embodiment of the invention, includes a plurality of drop ports, a plurality of optical filter switches, each coupled to one of the drop ports, and a plurality of splitters, each splitter coupled to the optical filter switches to supply a WDM signal that is received at an input thereof to each of the optical filter switches. In this embodiment, the optical filter switches are configurable to allow any wavelength channel of a WDM signal supplied from any one of the splitters to be directed to any one of the drop ports.
An optical device, according to another embodiment of the invention, includes a plurality of add ports, a plurality of optical filter switches, each coupled to one of the add ports, and a plurality of combiners, each combiner coupled to the optical filter switches to receive a WDM signal therefrom and generate a combined WDM signal. In this embodiment, the optical filter switches are configurable to allow any wavelength channel of an optical signal supplied through any one of the add ports to be directed to any one of the combiners.
A method of adding or dropping wavelength channels to and from optical signals passing through a reconfigurable optical device having an array of filter switches each of which includes a mirror that is rotatable about first and second axes, according to an embodiment of the invention, includes the step of rotating a mirror of one of the filter switches about a first axis to select one of the optical signals and about a second axis to select a wavelength channel in the selected optical signal to be output through a drop port.
A method of adding or dropping wavelength channels to and from optical signals passing through a reconfigurable optical device having an array of filter switches each of which includes a mirror that is rotatable about first and second axes, according to another embodiment of the invention, includes the step of rotating a mirror of one of the filter switches about a first axis to select a wavelength channel corresponding to an optical signal supplied through an add port and about a second axis to select an output port to which the wavelength channel corresponding to the optical signal supplied through the add port is to be directed.
So that the manner in which the above recited features of the present invention can be understood in detail, a more particular description of the invention, briefly summarized above, may be had by reference to embodiments, some of which are illustrated in the appended drawings. It is to be noted, however, that the appended drawings illustrate only typical embodiments of this invention and are therefore not to be considered limiting of its scope, for the invention may admit to other equally effective embodiments.
For clarity, identical reference numbers have been used, where applicable, to designate identical elements that are common between figures. It is contemplated that features of one embodiment may be incorporated in other embodiments without further recitation.
The embodiments shown are described in the context of OPM applications. However, it should be understood that the basic devices described herein are also useful as wavelength selective devices for routing selected WDM channels.
The specific optics as represented by ray optics, for the embodiment of
The optical fibers are shown only schematically in the figures. Typically they will be standard single mode fibers with a cladding diameter of 125 microns and a core diameter of 10 microns or less. In the portion of the array shown, i.e., the portion addressed by the wavelength selection elements, the optical fibers are stripped of the usual polymer coating. This allows greater precision in the array, producing, in many cases, a predictable spacing between cores of the fibers. Recognizing that a variety of options in the format of the array may be desirable, as will be discussed in greater detail below, optical fibers with sizes other than the conventional 125 microns may be useful. For example, cladding diameters of 50, 62.5, 250, may be used to advantage to vary the overall aperture (size) of the array. It is expected that small aperture arrays may be most cost effective.
Mirror 16 is rotatable about the x-axis into one of many positions. In the example shown in
When mirror 16 is rotated about the x-axis, another beam component (wavelength channel) will be normal to the mirror 16 and will be selectively reflected back through output fiber 13 and its properties measured. In this manner, the wavelength spectrum of the input beam to optical fiber 12 may be scanned and the properties of all of its beam components can be measured.
Thus the device achieves wavelength selection and provides an optical filter. The wavelength of the filter is tuned by the rotational orientation of mirror 16.
It should be noted that a similar result can be obtained if the axis of the dispersive element is rotated by 90 degrees and the mirror is tilted in the same axis that the beam is dispersed. In this configuration the light beam from the grating is dispersed into the wavelength components of the signal beam along the same axis of the fiber array, and there is some likelihood that the spectra from a fiber port will overlap with an adjacent or non-adjacent fiber port. The wavelength components which are diffracted from the dispersion element can be distinguished by increasing the separation of the fiber ports, although this will require a large optical aperture. To obtain satisfactory performance fiber port separation would be increased to three or more times larger than the separation required when the axis of the dispersive element is orthogonal to the fiber array.
It should be understood that a function of the rotating mirror 16 is to select a wavelength component of the incident beam and return it to a fixed position, in the case of the arrangement of
It should be recognized that the optical paths in the x-axis cross section of
The orientation of the mirror may be changed by an actuator or several actuators. The mirror may comprise a micro electro-mechanical system (MEMS), or comprise a discrete mirror driven by motors or any other types or actuators. The tilt of the mirror may be changed in one axis, or more than one axis.
Another WDM channel may be input as an input beam to optical fiber 18. The output of the beam components from this channel are directed through output optical fiber 19 and measured by the associated photodetector as shown in the top portion of
It should be appreciated by those skilled in the art that, while the array of input optical fibers, e.g., 12 and 18, and the array of output fibers 13 and 19 are shown closely packed and precisely aligned, the device input optical fibers and the device output optical fibers may have any length and be routed in any suitable fashion to other components/couplers in the system. For example, the photodetectors 21 are shown as an array of elements receiving light beams directly from the closely packed array of output optical fibers. However, the optical fiber 13 may route an optical signal to a photodiode non-aligned with respect to the output array of optical fibers.
The detection device may take any of a variety of forms, and measure a variety of optical beam properties. The arrangement shown is simple and useful for illustration. If the input beams are suitably time division multiplexed, a single detection device may be used. Alternatively a single spectrum analyzer may be used as the detection device.
In this description the optical elements are shown as separate elements. These represent functional elements. The physical elements providing these functions may, in some cases, be combined as a single module. For example, a grating may have a reflective surface or an attached or integral lens.
In the embodiments of
The fiber array may have other formats, one of which is illustrated in FIGS. A and 4B.
In the systems described it is not required that the ports be tuned simultaneously.
If the mirror orientation can be controlled by rotating it about 2 different axes, i.e., both the x-axis and the y-axis, then the ports can be read in series, i.e., there will be one input fiber and a number of output fibers. In
It should be evident that the number of optical fibers in a multiport optical filter according to the invention may vary widely. In embodiments like
The light waveguides described above are optical fibers. However, other waveguide arrays may be substituted. For example, the arrays of optical waveguides may comprise optical integrated circuits (OIGs) where parallel waveguides are formed in a common substrate such as lithium niobate, doped glass, or indium phosphide. The term “waveguide” used herein is intended to include any suitable light guiding element.
The placement of the optical fibers, both for the input side and the output side may vary significantly. In the embodiments of
As mentioned earlier, the devices described above may be used as wavelength selective devices in any application requiring that function. The embodiment shown in
The device of
A wide variety of applications exist for wavelength selective devices. For example, channel selectors in DWDM transmission and display require a single channel to be selected among a large number of channel options. Recognizing that the reflector element can itself provide added functionality, optical systems may be employed in which the reflector is tilted to transmit a predetermined sequence of wavelengths. These may be used in coding devices.
In the embodiments described above, the reflector is tilted with respect to the dispersive element to achieve wavelength selectivity. However, devices may be designed in which the dispersive element is moved and the reflector is fixed. Likewise other optical elements, for example, lenses, may be used to achieve the same effect. All arrangements in which some controlled predetermined movement of a dispersive element with respect to a reflector or refractive element to achieve the purpose of the invention should be considered equivalent.
As mentioned earlier, the beam steering element is preferably a light reflecting element or a light refracting element. In both cases the element is typically operated as a moving element, e.g., a MEMS mirror or the like. Optionally, the beam steering function may be provided by a non-moving element, for example, an electro-optic device. In one embodiment using an electro-optic device the beam steering element relies on changes in refractive index of an electro-optic medium. The changes in refractive index may be used to change the direction of diffraction of a light beam being analyzed or switched.
With reference to
Alternatively, the device shown in
In another alternative embodiment the parallel readout implementation of the embodiment of
These embodiments illustrate the very large versatility of devices operating according to the invention that operate with a wavelength selective mirror (for example) that may be tilted around more than one axis. In the arrangement shown, the rotation about the y-axis selects the beam position, i.e., the output port, while the rotation about the x-axis selects the wavelength. The biaxial rotation allows a selected wavelength component of an input beam to be directed as an output beam to any point in the x-y plane. This gives rise to another level of versatility in the design of devices operating according to the principles of the invention. This will be described in conjunction with the illustrations in
The view in
While five wavelengths are illustrated in
The output array in
In
It should be noted that the precision of the fiber array spacing in either x or y axes does not affect the performance provided the rotation of the mirror in the x or y axes can be optimized to minimize loss. This can be facilitated through a calibration process which stores a look up table with the location of the fibers stored, or using an optimization algorithm such as a hill-climbing algorithm that seeks to minimize the loss in any optical light path.
To identify or monitor the positions of the output optical fibers in an organized or random array it may be useful to employ a monitor that periodically locates the position of the members of the array. One suitable device for doing this is a CCD or CMOS imaging device which, when the output optical fibers are illuminated, can record the spatial position of each member in the array. A CCD imaging device is also useful as a light output detector in the normal operation of any of the devices or systems described earlier. If the CCD image plane is made as large as the aperture of the device it can serve as an output detector without regard to the precise locations of the individual members in the array.
As will be understood by those skilled in the art, arrays similar to those shown in
ROADM 1100 includes K inputs ports (I) 1101, K output ports (O) 1102, splitters (SPL) 1103 (also referred to herein as “primary splitters”), L×1 wavelength selective switches (WSS) 1104, an optical add section 1120, an optical drop section 1140, and a control module 1150. Optical add section 1120 includes M add ports 1122, M filter switches 1124, and N combiners 1121 (only one of which is shown). Optical drop section 1140 includes M drop ports 1142, M filter switches 1134, and N splitters 1141 (only one of which is shown and also referred to herein as “secondary splitters”). In the embodiment illustrated in
Control module 1150 is further illustrated in
During operation, ROADM 1100 receives optical signals, which may contain one or more wavelength channels, through its input ports 1101, and directs optical signals through its output ports 1102 and drop ports 1142. The composition of optical signals transmitted through output ports 1102 and drop ports 1142 is determined according to the configuration parameters for ROADM 1100. ROADM 1100 provides a high degree of flexibility such that any wavelength channel from any optical signal introduced through add ports 1122 may be added to any of the optical signals transmitted through output ports 1102, and any wavelength channel from any optical signal received through inputs ports 1101 may be dropped through any of drop ports 1142. Indeed, the add/drop functionality provided by ROADM 1100 can be characterized as:
The configurable parameters of ROADM 1100 include two control settings for each of filter switches 1124, indicated as λ and OUT in
When an optical signal is received at an input port, it is first split into split optical signals by a primary splitter coupled to the input port. The split optical signals are distributed to each of output ports 1102 other than the complementary output port. That is, as shown in
Wavelength channels are added by introducing them through add ports 1122. Filter switches 1124 each have control settings that define the wavelength channel appearing at a corresponding add port and the output port at which the wavelength channel to be added is to appear. For example, if a wavelength channel to be added is to appear at the fifth output port, e.g., output port 1102-5, the filter switch 1124 that receives this wavelength channel should be configured to receive this particular wavelength channel and direct it to combiner 1121. Combiner 1121 then outputs the wavelength channel of interest to the wavelength selective switch corresponding to output port 1102-5. This optical path is illustrated in
As further illustrated in
Initially, filter switch 1124-5 is configured to receive the λ2 wavelength channel from a corresponding add port in accordance with the control setting for that tunable filter defined in control module 1150. As shown in
In a similar manner, filter switch 1124-6 is configured to receive the λ3 wavelength channel from a corresponding add port in accordance with the control setting for that tunable filter defined in control module 1150. As shown in
The second control setting for the filter switches determines the output port to which the received wavelength channel is to be directed. As shown in
Initially, the splitter coupled to the input port 1101-3 generates split optical signals, one of which is transmitted to splitter 1141-3 for further splitting, and the splitter coupled to the input port 1101-7 generates split optical signals, one of which is transmitted to splitter 1141-7 for further splitting. Each of filter switches 1134 subsequently receives the further split signals that contain the two λ3 wavelength channels to be dropped at its third and seventh input ports, respectively. Control settings for these filter switches define the drop port through which the two λ3 wavelength channels are to be dropped.
As shown in
Similarly, as shown in
While the foregoing is directed to embodiments of the present invention, other and further embodiments of the invention may be devised without departing from the basic scope thereof, and the scope thereof is determined by the claims that follow. In particular, further embodiments of the present invention provide a reconfigurable optical device that includes only the optical add section of ROADM 1100 or only the optical drop section of ROADM 1100. In addition, such reconfigurable optical devices may be further simplified by removing the wavelength selective switches and primary splitters. A reconfigurable optical device without wavelength selective switches and primary splitters and having only the optical add section may be used to add channels in a reconfigurable manner to a WDM signal transmitted between two nodes in an optical communication system. Similarly, a reconfigurable optical device without wavelength selective switches and primary splitters and having only the optical drop section may be used to drop channels in a reconfigurable manner from a WDM signal transmitted between two nodes in an optical communication system.
This application is a continuation-in-part of U.S. patent application Ser. No. 12/927,066, filed Nov. 5, 2010, now U.S. Pat. No. 8,755,651 which is a continuation-in-part of U.S. patent application Ser. No. 12/804,627, filed Jul. 26, 2010 now U.S. Pat. No. 8,577,192. The entire contents of both of these applications are incorporated by reference herein.
Number | Name | Date | Kind |
---|---|---|---|
4923270 | Carter | May 1990 | A |
6654157 | Islam et al. | Nov 2003 | B2 |
6704487 | Parhami et al. | Mar 2004 | B2 |
6798551 | Gu | Sep 2004 | B2 |
6891676 | Ford et al. | May 2005 | B2 |
6992777 | Han et al. | Jan 2006 | B2 |
7016098 | Giles et al. | Mar 2006 | B2 |
7236660 | Ducellier et al. | Jun 2007 | B2 |
7340128 | Shibata et al. | Mar 2008 | B2 |
7362930 | Davis et al. | Apr 2008 | B2 |
7440648 | Oikawa et al. | Oct 2008 | B2 |
7672585 | Sone et al. | Mar 2010 | B2 |
7720329 | Presley et al. | May 2010 | B2 |
20010038730 | Sorin et al. | Nov 2001 | A1 |
20020005970 | Lang | Jan 2002 | A1 |
20040156581 | Golub et al. | Aug 2004 | A1 |
20060228070 | Davis et al. | Oct 2006 | A1 |
20060257091 | Tabuchi et al. | Nov 2006 | A1 |
20090103861 | Presley et al. | Apr 2009 | A1 |
20090304328 | Presley et al. | Dec 2009 | A1 |
20100150563 | Nakajima | Jun 2010 | A1 |
20120020617 | Wu | Jan 2012 | A1 |
Number | Date | Country |
---|---|---|
1656721 | Aug 2005 | CN |
1831574 | Sep 2006 | CN |
1996075 | Jul 2007 | CN |
101384933 | Mar 2009 | CN |
202339423 | Jul 2012 | CN |
WO 2007078415 | Jul 2007 | WO |
Entry |
---|
United States Patent and Trademark Office, Non-Final Rejection, U.S. Appl. No. 12/927,066, Jun. 10, 2013, 18 Pages. |
United States Patent and Trademark Office, Non-Final Rejection, U.S. Appl. No. 13/226,275, Jun. 11, 2013, 23 Pages. |
The State Intellectual Property Office of the People's Republic of China, Second Office Action, Chinese Patent Application No. 201110210059.X, Mar. 21, 2013, 15 pages. |
Patent Cooperation Treaty, Written Opinion of the International Search Authority, International Patent Application No. PCT/US2010/002449, mailed Nov. 2, 2010, 6 pages. |
Patent Cooperation Treaty, International Search Report, International Patent Application No. PCT/US2010/002449, mailed Nov. 2, 2010, 2 pages. |
Patent Cooperation Treaty, Written Opinion of the International Search Authority, International Patent Application No. PCT/US2011/045424, mailed Dec. 5, 2011, 9 pages. |
Patent Cooperation Treaty, International Search Report, International Patent Application No. PCT/US2011/045424, mailed Dec. 5, 2011, 2 pages. |
Patent Cooperation Treaty, Written Opinion of the International Search Authority, International Patent Application No. PCT/US2011/059448, mailed Apr. 4, 2012, 4 pages. |
Patent Cooperation Treaty, International Search Report, International Patent Application No. PCT/US2011/059448, mailed Apr. 4, 2012, 2 pages. |
The State Intellectual Property Office of the People's Republic of China, First Office Action, Chinese Patent Application No. 201110210059.X, mailed Aug. 17, 2012, 17 pages. |
The United States Patent and Trademark Office, Final Rejection, United States Patent Application No. 12/804,627, mailed Jan. 31, 2013, 16 pages. |
The United States Patent and Trademark Office, Non-Final Rejection, U.S. Appl. No. 12/804,627, mailed May 11, 2012, 20 pages. |
Number | Date | Country | |
---|---|---|---|
20120163825 A1 | Jun 2012 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12927066 | Nov 2010 | US |
Child | 13411487 | US | |
Parent | 12804627 | Jul 2010 | US |
Child | 12927066 | US |