Wavelength shifting and optical switching

Abstract
A method produces a wavelength shift into an optical signal. The method includes producing a coherent temporal array of optical signals (CTAS) from an incoming optical signal and broadening the signals of the CTAS to produce a interference pattern. The broadening results from transmitting the CTAS or the incoming optical signal through a dispersive medium. The method also includes selectively transmitting a peak of the interference pattern. The transmitted peak has a selected wavelength shift with respect to the incoming optical signal.
Description




BACKGROUND OF THE INVENTION




This invention relates to optical devices and networks.




Future networks for broadband communications will need higher bandwidths for data transmission. One avenue to obtaining higher bandwidth entails using wavelength division multiplexed (WDM) optical networks. A WDM optical network can simultaneously transmit several optical signals in a single optical fiber. The simultaneously transmitted optical signals have different wavelengths, and WDM receivers selectively accept signals based on their wavelength.




Some optical networks are also dynamically reconfigurable so that transmission routes can be rapidly chanced. Dynamic reconfigurability can be achieved using programmable optical add/drop multiplexers (OADM's) and optical cross connects (OXC's). OADM's add optical signals to and drop optical signals from trunk optical fibers. OXC's switch optical signals between different trunk fibers. Contemporary OXC's and OADM's can switch optical signals transparently. OXC's and OADM's using thermal control signals can transparently switch routes of optical signal at frequencies of about 2 kilo Hertz (Khz).




Herein, a transparent process is defined to be a process that chances a property or routing of an optical signal without an intermediate conversion of the optical signal into an electrical signal.




Other features and advantages of the invention will be apparent from the following description and claims.




SUMMARY OF THE INVENTION




In one aspect, the invention features a method of producing a wavelength shift into an optical signal. The method includes transparently producing a coherent temporal array of signals (CTAS) from the incoming optical signal and broadening the signals of the CTAS to produce an interference pattern by transmitting the CTAS through a dispersive medium. The method also includes selectively transmitting a peak of the interference pattern to an output terminal. A wavelength of a center of the transmitted peak has a selected wavelength shift with respect to a wavelength of the incoming optical signal.




In a second aspect, the invention features a method of producing a wavelength shift into an optical signal. The method includes transparently producing a coherent temporal array of signals (CTAS) from the incoming optical signal and Broadening the signals of the CTAS to produce an interference pattern by transmitting the incoming optical signal through a dispersive medium. The method also includes selectively transmitting a peak of the interference pattern to an output terminal. A wavelength of a center of the transmitted peak has a selected wavelength shift with respect to a wavelength of the incoming optical signal.




In a third aspect, the invention features a method of switching optical signals in an optical network. The method includes receiving an optical signal from a first optical conduit of the network and transparently shifting a wavelength of the received optical signal. The method also includes transmitting the optical signal with the shifted wavelength to a second optical conduit of the network.




In a fourth aspect, the invention features an apparatus for routing optical pulses. The apparatus includes a variable temporal splitter (VTS) and a dispersive medium connected serially to the VTS. The VTS is capable of transparently producing a coherent temporal array of pulses (CTAP) from a received optical pulse. The dispersive medium is capable of broadening the pulses of the CTAP to form an interference pattern with a plurality of peaks. The apparatus includes a 1×M wavelength division multiplexer (WDM) coupled to receive one of the peaks.




In a fifth aspect, the invention features an optical switch. The optical switch includes a variable wavelength shifter (VWS) and a wavelength division multiplexer (WDM) coupled to receive optical pulses with shifted wavelengths from the VWS. The VWS transparently shifts a wavelength of a received optical pulse.




Various embodiments provide transparent optical multiplexers and switches with switching frequencies of between a few tens of giga Hertz to a few hundreds of giga Hertz. The optical switches can provide high speed programmable OXC and OADM's for use in reconfigurable optical networks.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

shows one embodiment of a variable wavelength shifter (VWS);





FIG. 2

is a flow chart for a method of shifting a wavelength of an optical signal with the VWS of

FIG. 1

;





FIG. 3

shows an alternate embodiment of a variable wavelength shifter (VWS);





FIG. 4

shows an embodiment of a variable temporal splitter (VTS), which may be used in the VWS's of

FIGS. 1 and 3

;





FIG. 5

shows an electrically controlled variable path element, which may be used in the VTS of

FIG. 4

;





FIG. 6

shows an optically controlled variable path element, which may be used in the VTS of

FIG. 4

;





FIG. 7

shows an optical multiplexer that uses a wavelength shifting to multiplex optical signals;





FIG. 8

shows one embodiment of a wavelength division multiplexer (WDM);





FIG. 9

shows a unidirectional switch that uses wavelength shifting to route optical signals;





FIG. 10

shows a bi-directional switch that uses wavelength shifting to route optical signals; and





FIG. 11

shows an optical cross connect that uses wavelength shifting to transmit optical signals between different optical networks.











DESCRIPTION OF THE PREFERRED EMBODIMENTS





FIG. 1

shows a variable wavelength shifter (VWS)


8


, which receives an incoming optical signal


10


from optical fiber


12


. The optical signal


10


has a peak whose center wavelength is λ and wavelength spread is δλ. From incoming optical signal


10


, VWS


8


transparently produces an outgoing optical signal


14


having a shifted peak (e.g., at outgoing center wavelength λ+ε) on optical fiber


13


. The size of wavelength shift ε produced by VWS


8


is determined by a control signal applied to control terminal


16


. Control signals can change wavelength shift ε at high frequencies, e.g., tens to hundreds of giga Hertz.




The VWS


8


shifts the wavelength of incoming optical signal


10


according to a method


40


shown in FIG.


2


. Each incoming optical signal


10


passes through a bandwidth enhancer


18


that spectrally enhances the incoming signal


10


(step


42


). Bandwidth enhancer


18


improves the spectral form of received signals by filling in spectral absorption regions. Such absorption regions occur in incoming optical signal


10


because of prior processing by network elements (not shown) that absorb light in certain frequency ranges.




After enhancement, enhanced optical signal


20


enters a variable temporal splitter (VTS)


22


. VTS


22


produces a coherent temporal array of signals (CTAS)


24


from optical signal


20


transparently (step


44


). CTAS


22


is a temporal series of individual optical signals


25


-


28


, which are mutually coherent. If incoming optical signal


10


is a narrow pulse, CTAS


22


is a coherent temporal array of pulses (CTAP) in which signals


25


-


28


are non-overlapping pulses. To form CTAS


24


, VTS


22


amplitude splits the received optical signal


20


into separate optical signals, delays each separate optical signal differently, and recombines the delayed optical signals to produce CTAS


24


. The delays between the signals


25


-


28


of the CTAS


24


are responsive to control signals applied to control terminal


16


.




From VTS


22


, CTAS


24


travels through a dispersive medium


30


, e.g., a roll of dispersive optical fiber. Dispersive medium


30


broadens each optical signal


25


-


28


of CTAS


24


so that the broadened optical signals strongly spatially overlap (step


46


). Due to the spatial overlap, the separate optical signals of the CTAS


24


interfere and produce an interference pattern


32


.




Interference pattern


32


has an envelope


33


and a number of spatially separated peaks


34


-


37


. Envelop


33


is the signal that dispersion would produce if enhanced optical signal


20


passed directly into dispersive medium


30


without undergoing intermediate production of CTAS


24


. Dispersion produces a broader range of wavelengths in envelop


33


than the range of wavelengths in enhanced signal


20


. Different spatial portions of envelope


33


correspond to different wavelengths. Since different peaks


34


-


37


are in different spatial portions of envelop


33


, these peaks


34


-


37


have different wavelengths. In particular, the center of largest amplitude peak


35


has a wavelength shift ε with respect to wavelength λ of incoming signal


10


, i.e., the wavelength of the center of envelop


33


. Due to dispersion broadening, the shift ε of largest amplitude peak


35


may be significantly greater than the spread Δλ in enhanced optical signal


20


.




Interference pattern


32


enters a nonlinear optical loop mirror (NOLM)


38


, i.e., an optical amplitude discriminator. NOLM


38


selectively transmits largest amplitude peak


35


and attenuates or removes remaining peaks


34


,


36


, and


37


to produce outgoing optical signal


14


on optical fiber


13


(step


48


). Since largest peak


35


has a wavelength λ+ε, VWS


8


has shifted the wavelength λ of incoming signal


10


by ε.




The wavelength λ+ε of outgoing optical signal


14


is determined by the temporal spacings between signals


25


-


28


of CTAS


24


. The temporal spacings between signals


25


-


28


are controlled by control signals applied to control terminal


16


. The signals at control terminal


16


are selected to produce a desired value for wavelength shift ε.




An alternate embodiment of a VWS


8


′ is shown in FIG.


3


. In VWS


8


′, dispersive medium


30


is located earlier on the optical path of incoming signal


10


than VTS


22


. Dispersion medium


30


broadens signal


20


to produce signal


39


prior to production of a CTAS by VTS


22


. Since the signal


39


is spatially broad, the separate optical signals of the CTAS are broad and interfere at production of the CTAS to produce interference pattern


32


. Again, sending interference pattern


32


through NOLM


38


produces outgoing optical signal


14


with shifted wavelength λ+ε.




One embodiment of a VTS


50


capable of producing CTAS's, e.g., CTAS


22


of

FIGS. 1 and 3

, from incoming optical signal


20


is shown in FIG.


4


. VTS


50


receives incoming optical signal


20


from optical fiber


52


, which connects to an input terminal of a 1×N optical fiber coupler


54


. Optical fiber coupler


54


amplitude splits received optical signal


20


into N mutually coherent optical signals and directs each signal into a different optical conduit


56


to


58


. The optical conduits


56


to


58


may be single mode optical fibers. Each optical conduit


56


to


58


includes a variable path element


60


to


62


, which serially connects Lo the fiber. The variable path elements


60


to


62


have optical path lengths that depend on values of signals received at control terminals


64


to


66


. The individual control terminals connect to control terminal


16


of

FIGS. 1 and 3

. The variable path elements


60


to


62


also connect to an N×1 optical coupler


68


via optical conduits


70


to


72


, e.g., single mode optical fibers. Optical coupler


68


combines delayed optical signals received from the optical conduits


70


to


72


to produce CTAS


74


on outgoing optical fiber


76


.




The variable path elements


60


to


62


of

FIG. 4

are either electrically or optically controlled.




Variable path elements


60


to


62


may be implemented as electrically controlled path element


80


shown in FIG.


5


. In path element


80


, an optical conduit


84


connects incoming and outgoing optical fibers


56


and


70


. A portion of a top surface of optical conduit


84


is covered by a metal layer


82


, which connects electrically to control terminal


16


. Optical conduit


84


rests on a conductive layer


85


located in a portion of a substrate


86


. Metal layer


82


and conductive layer


85


form a capacitive device.




The optical conduit


84


is constructed of a material, e.g., lithium niobate, whose index of refraction depends on the voltage applied across the conduit


84


. During operation, a control voltage is applied to the metal layer


82


via control terminal


16


, and conductive layer


85


is grounded. The size of the applied voltage determines the index of refraction of optical conduit


84


. Thus, optical conduit


84


delays an optical signal from optical fiber


56


to optical fiber


70


by a time characterized by the voltage applied to control terminal


16


.




The speed at which the index of refraction of optical conduit


84


responds to applied voltages determines the maximum switching frequency for a VWS, e.g., VWS


8


or


8


′, using variable path element


80


. The maximum switching frequency is about 50 giga Hertz if the optical conduit


84


is constructed with lithium niobate.




The variable path elements


60


to


62


of

FIG. 4

may also be implemented as an optically controlled element


90


shown in FIG.


6


. Element


90


includes a nonlinear optical media


92


having an index of refraction that depends on the total light intensity in the media


92


. Nonlinear media


92


transmits optical signals from optical fiber


56


to a 1×2 optical fiber coupler


94


. Coupler


94


transmits optical signals received from nonlinear medium


92


to outgoing optical fiber


70


. The optical signal on outgoing optical fiber


70


has a delay, which is determined by the index of refraction of nonlinear medium


92


.




The index of refraction of nonlinear material


92


is chanced by control optical signals introduced into media


92


through an optical fiber


96


, i.e., control terminal


16


of FIG.


4


. Optical coupler


94


transmits the control optical signals from fiber


96


into nonlinear media


92


without substantially contaminating outgoing optical fiber


70


. Fiber


70


is not contaminated by control optical signals, because control and incoming optical signals propagate in opposite directions in the nonlinear mater


92


. Control optical signals adjust the total light intensity in nonlinear material


92


producing an index of refraction therein that provides desired delays for optical signals traveling from fiber


56


to fiber


70


.




Other embodiments for VTS's will be known to persons of ordinary skill in the art in light of the above-disclosure and U.S. application Ser. No. 09/362,349, titled “Fast Variable Optical Delay”, filed Jul. 27, 1999 by Katherine L. Hall et al, which is incorporated by reference, and U.S. application Ser. No. 09/282,880.




VWS


8


can be used to construct a 1×N optical multiplexer


100


shown in FIG.


7


. Optical multiplexer


100


receives incoming optical signals from an optical fiber


102


that connects to an input terminal of VWS


8


. VWS


8


shifts the wavelength of the incoming optical signal and transmits the optical signal with a shifted wavelength to an optical fiber


104


. Optical fiber


104


carries the optical signal with a shifted wavelength to a WDM


106


that routes the optical signal to an output optical fiber


108


to


110


. Each output fiber


108


to


110


may include a second VWS, as show for fiber


110


by the VWS


111


, to shift wavelengths of outgoing optical signals to desired values.




One embodiment of the WDM


106


uses an optical grating


112


shown in FIG.


8


. Optical grating


112


receives optical signals from fiber


102


, which is oriented along direction N, and reflects the received optical signals into fibers


108


to


110


oriented along different directions. The reflection directions depend on the wavelength of the received optical signals. By properly shifting the wavelength of optical signals received from fiber


102


, VWS


8


of

FIG. 7

controls the reflection direction produced by grating


112


and thus, the route selection between fibers


108


to


110


.




VWS


8


can also be used to construct a M×N switch


120


shown in FIG.


9


. M×N switch


120


receives incoming optical signals from optical fibers


122


to


124


via an M×1 optical fiber coupler


126


. The optical output terminal of M×1 fiber coupler


126


connects to optical fiber


102


of the 1×N optical multiplexer


100


shown in FIG.


7


.




M×N switch


120


again transparently routes incoming optical signals to selected outgoing optical fibers


108


-


110


by appropriately shifting the wavelengths of the incoming optical signals. The wavelength shifts are performed by VWS


8


under the control of signals received from control terminal


16


. The size of wavelength shifts depends both on the wavelength of the incoming optical signal and the final routing desired. A programmable controller


128


determines the size of wavelength shifts and generates the appropriate control signal for each incoming optical signal received from fibers


122


-


124


.




Using two VWS's


129


and


129


′, a bi-directional optical switch


130


may be constructed as shown in FIG.


10


. In the bi-directional optical switch


130


, the two VWS's


129


and


129


′ separately route optical signals received from optical fibers


108


′-


110


′ and from optical fibers


108


-


110


. To separately route signals received from the two sets of optical fibers


108


′-


110


′ and fibers


108


-


110


, the switch


130


employs two optical circulators


132


and


132


′.




Optical circulators


132


and


132


′ route optical signal received at any terminal to the nearest clockwise adjacent terminal of the same circulator


132


and


132


′. Thus, first circulator


132


routes optical signals received from optical fibers


108


-


110


via WDM


106


to second VWS


129


′. Similarly, second circulator


132


′ routes optical signals received from optical fibers


108


′-


110


′ via WDM


106


′ to first VWS


129


. VWS's


129


and


129


′ transparently shift the wavelength of received optical signals and transmit the signals with shifted wavelengths to WDM


106


′ and


106


, respectively, via one of the circulators


132


′ or


132


.




Using a multiple terminal optical switch, e.g., switch


120


of

FIG. 9

, an optical cross connect (OXC)


140


can be constructed for connecting optical networks A and B as shown in FIG.


11


. OXC


140


has at least two input and two output terminals and functions by wavelength shifting as described in relation to

FIGS. 3-9

. Switch


140


responds to control signals received from a control terminal


144


. If networks A and B carry signals of predetermined wavelength, the control signals have values for connecting A⇄A, B⇄B, A⇄B, and B⇄A, e.g., four different digital control signals.




The bi-directional optical switch


130


of

FIG. 10

can also be used to make OXC


140


bi-directional by techniques that would be evident to persons of skill in the art in light of the above disclosure.




The optical switch


140


can also be used to construct optical add/drop multiplexers (OADM) having the form shown in FIG.


11


. For an OADM, fibers


124


and


109


are optical conduits for transparently adding and dropping optical signals, respectively, from trunk optical fiber


122


and


108


.




Other embodiments are within the scope of the following claims.



Claims
  • 1. A method of switching optical signals in a network, comprising:receiving an optical signal from a first optical conduit of the network; transparently shifting a wavelength of the received optical signal; and transmitting the optical signal with the shifted wavelength to a second optical conduit of the network, wherein the act of transparently shifting a wavelength comprises: producing a coherent temporal array of optical signals (CTAS) from a received optical signal; broadening the signals of the CTAS to produce a interference pattern by transmitting the CTAS through a dispersive medium; and selectively transmitting a peak of the interference pattern, the transmitted peak having the shifted wavelength.
  • 2. The method of claim 1, further comprising:transmitting the optical signal having the shifted wavelength to a wavelength division multiplexer coupled to the second optical conduit.
  • 3. The method of claim 1, wherein the act of producing comprises:splitting the received signal into signals directed into separate optical conduits; and changing an index of refraction of a portion of one of the optical conduits.
  • 4. The method of claim 1, wherein the act of receiving includes transmitting the received optical signal through a many port to one port optical coupler prior to the act of transparently shifting.
  • 5. A method of switching optical signals in a network, comprising:receiving an optical signal from a first optical conduit of the network; transparently shifting a wavelength of the received optical signal; and transmitting the optical signal with the shifted wavelength to a second optical conduit of the network, wherein the act of transparently shifting a wavelength comprises: producing a coherent temporal array of optical signals (CTAS) from a received optical signal; broadening the signals of the CTAS to produce a interference pattern by transmitting the received optical signal through a dispersive medium; and selectively transmitting a peak of the interference pattern, the transmitted peak having the shifted wavelength.
  • 6. The method of claim 5, further comprising:transmitting the optical signal having the shifted wavelength to a wavelength division multiplexer coupled to the second optical conduit.
  • 7. The method of claim 5, wherein the act of producing comprises:splitting the received signal into signals directed into separate optical conduits; and changing an index of refraction of a portion of one of the optical conduits.
  • 8. The method of claim 5, wherein the act of receiving includes transmitting the received optical signal through a many port to one Port optical coupler prior to the act of transparently shifting.
  • 9. An apparatus for routing optical pulses, comprising:a variable temporal splitter (VTS) capable of transparently producing a coherent temporal array of pulses (CTAP) from an incoming optical pulse; a dispersive medium coupled serially to the VTS and capable of broadening the pulses of the CTAP to overlap and form an interference pattern with a plurality of peaks; and a 1×M wavelength division multiplexer (WDM) coupled to receive one of the peaks.
  • 10. The apparatus of claim 9, wherein the dispersive medium is coupled to the input terminal of the VTS.
  • 11. The apparatus of claim 9, further comprising:an intensity discriminator coupled to receive the interference pattern and to transmit one of the peaks to the WDM.
  • 12. The apparatus of claim 11, further comprising:an optical bandwidth enhancer coupled to an input terminal of the VTS.
  • 13. The apparatus of claim 11, wherein the VTS comprises:an amplitude splitter coupled to receive the incoming optical pulse; and a plurality of optical conduits, each conduit coupled to receive a portion of the incoming optical pulse from the amplitude splitter, one of the optical conduits having a serial element with a variable index of refraction.
  • 14. The apparatus of claim 13, wherein the serial element further comprises:a segment of optical conduit having an index of refraction that depends on a value of an applied voltage.
  • 15. The apparatus of claim 13, wherein the serial element further comprises:a segment of optical conduit comprising a nonlinear optical material having index of refraction that depends on a light intensity in the segment.
  • 16. An optical switch, comprising:a variable wavelength shifter (VWS) to transparently shift a wavelength of a received optical pulse; and a wavelength division multiplexer (WDM) coupled to receive optical pulses with shifted wavelengths from the VWS, wherein the VWS comprises: a variable temporal splitter (VTS); and a dispersive medium serially connected to the VTS, the dispersive medium capable of causing interference between pulses of coherent temporal arrays of pulses produced by the VTS.
  • 17. The optical switch of claim 16, further comprising:an N×1 optical coupler to transmit received optical pulses to the VWS.
  • 18. The optical switch of claim 17,wherein the N×1 optical coupler includes a second WDM.
  • 19. The optical switch of claim 18, wherein the optical switch is a bi-directional switch.
  • 20. The optical switch of claim 18, further comprising:a second VWS coupled between the two WDM's with an inversed orientation with respect to the first VWS.
Parent Case Info

This application is a divisional of application Ser. No. 09/405,262, filed Sep. 23, 1999 now U.S. Pat. No. 6,427,039, which is a continuation-in-part of application Ser. No. 09/282,880, filed Mar. 31, 1999 now U.S. Pat. No. 6,563,620, which claims the benefit of U.S. Provisional Application No. 60/117,146, filed Jan. 25, 1999. This application claims the benefit of U.S. Provisional Application No. 60/126,730, filed Mar. 29, 1999, and U.S. Provisional Application No. 60/143,010, filed Jul. 9, 1999.

Government Interests

The U.S. Government has non-exclusive rights in this invention pursuant to contract number F19628-95-C-0002 awarded by DARPA and AF.

US Referenced Citations (4)
Number Name Date Kind
5982963 Feng et al. Nov 1999 A
6025915 Michal et al. Feb 2000 A
6215927 Singh Apr 2001 B1
6427039 Hakimi et al. Jul 2002 B1
Non-Patent Literature Citations (18)
Entry
“Interferometric All-optical switches for Ulrafast signal processing” by Patel et al, APplied Optics, vol. No. 14, May 10, 1998, pp2831-2842.*
“Dense Wavelength Division Multiplexer,” Lucent Technologies company brochure/performance specifications, Bell Labs Innovations, Copyright 1997, 2 pages.
“New 3-Port/4-Port Optical Circulator,” Jay Van Delden, Photonics Spectra, Jan. 1992, Laurin Publishing Co., Inc., 2 pages.
“Nonlinear Loop Mirror Devices and Applications,” K.J. Blow et al., BT Technol J, vol. 11, No. 2, Apr. 1993, p 99-107.
“Interferometric All-Optical Switches for Ultrafast Signal Processing,” Naimish S. Patel et al., Applied Optics, vol. 37, No. 14, May 10, 1998, p 2831-2842.
“Devices for Wavelength-Division Multiplexing (WDM),” Fiber Optics Handbook, p 3.63-3.79.
“Recent Progress in Silica-Based Planar Lightwave Circuits on Silicon,” M. Kawachi, IEE Proc.—Optoelectron, vol. 143, No. 5, Oct. 1996, 257-262.
“Waveguide Array Wavelength Router Design to Improve Insertion Loss Uniformity,” Hideaki Okayama et al. Optical Review, vol. 4, No. 5, 1997, p 543-545.
“Applications of the Integrated Waveguide Grating Router,” B. Glance, Journal of Lightwave Technology, vol. 12, No. 6, Jun. 1994, 957-962.
“Space-Switching 2.5 Gbit/s Signals Using Wavelength Conversion and Phased Array Routing,” L.H. Spiekman et al., Electronics Letters, vol. 32, No. 4, Feb. 15, 1996, p 377-379.
“Fibre Dispersion or Pulse Spectrum Measurement Using a Sampling Oscilloscope,” Y.C. Tong et al., Electronics Letters, vol. 33, No. 11, May 22, 1997, p 983-985.
“Real-Time Fourier Transformation In Dispersive Optical Fibers,” Tomasz Jannson, Optics Letters, vol. 8, No. 4, Apr. 1983, p 232-234.
“Space-Switching 2.5 Gbit/s Signals Using Wavelength Conversion and Phased Array Routing,” A.A.M. Staring et al., Electronics Letters, vol. 32, No. 4, Feb. 15, 1996, pp 377-379.
“Recent Progress in Silica-Based Planar Lightwave Circuits on Silicon,” M. Kawachi, IEE Proc. Optoelectron, vol. 143, No. 5, Oct. 1996, pp 257-261.
“Devices for Wavelength-Division Multiplexing (WDM),” Pierangelo Morra et al., Fiber Optics Handbook for Engineers and Scientists, Frederick C. Allard, Ed., Ch. 3, pp 3.63-3.78.
“New 3-Port/4-Port Optical Circulator,” Jay Van Delden, Photonics Spectra, Jan. 1992, 2 pages.
“Dense Wavelength Division Multiplexer,” 1X16 and 1Z32 DWDM's with Integral Thermal Management System, Lucent Technologies Advertisement (1997), 2 pages.
“Dense Wavelength Division Multiplexing Networks: Principles and Applications,” C. A. Bracket, IEEE Journal on Selected Areas in Communications, vol. 8, No. 6, Aug. 1990, pp 948-964.
Provisional Applications (3)
Number Date Country
60/143010 Jul 1999 US
60/126730 Mar 1999 US
60/117146 Jan 1999 US
Continuation in Parts (1)
Number Date Country
Parent 09/282880 Mar 1999 US
Child 09/405262 US