US20030169964A1 - Power splitter/combiner with parameter tolerance and design process therefor - Google Patents
Power splitter/combiner with parameter tolerance and design process therefor Download PDFInfo
- Publication number
- US20030169964A1 US20030169964A1 US10/093,663 US9366302A US2003169964A1 US 20030169964 A1 US20030169964 A1 US 20030169964A1 US 9366302 A US9366302 A US 9366302A US 2003169964 A1 US2003169964 A1 US 2003169964A1
- Authority
- US
- United States
- Prior art keywords
- splitter
- combiner
- phase shifts
- couplers
- output signal
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
Images
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29346—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by wave or beam interference
- G02B6/2935—Mach-Zehnder configuration, i.e. comprising separate splitting and combining means
- G02B6/29352—Mach-Zehnder configuration, i.e. comprising separate splitting and combining means in a light guide
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2821—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers using lateral coupling between contiguous fibres to split or combine optical signals
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29379—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
- G02B6/29395—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device configurable, e.g. tunable or reconfigurable
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/313—Digital deflection, i.e. optical switching in an optical waveguide structure
- G02F1/3136—Digital deflection, i.e. optical switching in an optical waveguide structure of interferometric switch type
Definitions
- Power splitters/combiners are essential components in optical systems, and especially integrated, planar waveguide systems. They are important where coherent signal splitting, signal combining, or both signal splitting and combining are required. Splitters are typically used to split a single optical signal into two signals. Combiners are typically used to combine two signals into a single signal. Splitter/combiner pairs are often used to control power flow through optical elements. Splitters and combiners can also be configured as multifunctional splitter/combiners, where the operation performed depends upon the direction of the input signals and the number of inputs provided.
- a frequently used splitter/combiner is composed of two waveguides that are side-coupled to each other, forming a directional coupler. Light traveling in one waveguide couples to the other waveguide so that splitting or combining can occur.
- the power splitting ratio is defined as the ratio of the percentage of power at the output of the first waveguide to the percentage of power at the output of the second waveguide.
- the power splitting ratio, P is related to the coupling value, ⁇ , as
- ⁇ is the product of the coupling coefficient, ⁇ , and the coupling length, L, of the device.
- the coupling value for the coupler has to be exact. For example, if the coupling value of the coupler in a 50/50 splitter is smaller than the ideal value by 10%, the power splitting ratio becomes 57.8/42.2; and if the coupling value is smaller by 20%, the power splitting ratio becomes 65.5/34.5.
- the performance of directional couplers is inherently sensitive to fabrication errors.
- the coupling value is a function of physical parameters, such as waveguide cross-section, effective index, and waveguide-to-waveguide separation. Fabrication errors can also lead to undesired dependencies between the coupling value and the frequency and polarizations of the input optical signals, on otherwise nominally spectrally flat, polarization insensitive designs.
- splitters/combiners have been proposed that include cascaded splitters and phase shifters. These systems are typically optimized for wavelength insensitivity, and sometimes robustness against uniform fabrication errors.
- each splitter/combiner is comprised of two or more directional couplers serially connected to two or more phase shifts in an alternating order (e.g., directional coupler, phase shift, directional coupler, phase shift, directional coupler).
- the invention addresses the problem of parameter deviations in splitter/combiners by selecting specific coupling and phase values for the directional couplers and phase shifts to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants, for example.
- Parameter deviations such as coupling value deviations and phase value deviations from the nominal design due to fabrication errors, for example, typically give rise to frequency dependency, polarization dependency in the output signal and are specifically addressed in the invention by designing the system so that the sensitivity of the output signal to these changes is minimized.
- the invention can be applied to address the specific problem of matched deviations in coupling values and phase values in a splitter/combiner system.
- the invention also addresses the problem of differential deviations in the phase values of the phase shifts by providing tunable phase shifts, employing controlled effects, such as electro-optic or thermo-optic refractive index changes.
- two splitter/combiners are coupled to an external system and engineered for desired reflection and transmission spectra.
- the splitter/combiner is designed for maximal flatness of the spectrum with respect to the deviations in the parameters in one example. Other methods, such as designing for equal-ripple of the spectrum for the desired ranges of the values for the parameters, can also be implemented.
- two splitter/combiners are coupled to two external systems that have nominally identical reflection and transmission spectra.
- the splitter/combiner system of the invention can also be designed for a wide range of ratios for splitting and/or combining signals.
- the invention can be used for both mono-directional or bi-directional splitting and combining.
- the invention features a splitter/combiner system that comprises a serial connection of at least two couplers and at least two phase shifts.
- the coupling coefficients of the couplers and propagation constants of the phase shifts are selected to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants.
- the invention can be characterized as a design process for a splitter/combiner system, in which a serial connection of at least two couplers and at least two phase shifts are provisioned to connect an input waveguide to an external system. Coupling coefficients of the couplers and propagation constants of the phase shifts are proscribed to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants.
- FIG. 1 is a block diagram of a splitter/combiner coupled to an external system having a reflection and transmission spectrum, in accordance with the invention
- FIG. 2 is a plan view of the generalized configuration of the directional couplers and phase shifts in accordance with the invention
- FIG. 3 is a plan view of a splitter/combiner system coupled to a transmissive external optical system, according to a first embodiment of the invention
- FIG. 4 is a plan view illustrating the layout of the waveguides in the first embodiment splitter/combiner system
- FIG. 5 is a plot of the power of output signal C as a function of the coupling coefficient, showing a region in which changes in the coupling coefficient yields only small changes in the output signal;
- FIG. 6 is a plan view of a splitter/combiner coupled to a reflective external optical system in accordance with a second embodiment of the invention.
- FIG. 7 is a plan view of two exemplary splitter/combiners coupled an external system, in accordance with a third embodiment of the invention.
- FIG. 8 is a block diagram of a splitter/combiner system coupled to two external optical systems (sub-elements) having the same reflection and transmission spectra, in accordance with a fourth embodiment of the invention.
- FIGS. 9A and 9B are schematic block diagrams illustrating the design process for the fourth embodiment in view of the reflection and transmission characteristics of the external system
- FIG. 10 is a plan view of a simplified splitter/combiner configuration for reflection/transmission spectra in accordance with the invention.
- FIG. 11 is a plan view of an alternate splitter/combiner configuration for reflection and transmission spectra in accordance with the invention.
- FIG. 12 is a plan view illustrating the layout of the waveguides in still another embodiment of the splitter/combiner system.
- This invention describes a splitter/combiner system that, when coupled to an external system having a reflection and/or transmission response, has a high level of tolerance to parameter deviations for the desired spectra of the output signal.
- FIG. 1 illustrates the typical application for the invention.
- FIG. 1 is a block diagram of one or more of splitter/combiners 100 are coupled to an external system 10 that has reflection (R( ⁇ )) and transmission (T( ⁇ )) spectra.
- the splitter/combiners 100 are monolithically fabricated from planar waveguides in a high index contrast material system in the current implementation. That is, the material system provides an index contrast between the refractive indices of the waveguides and the cladding that is greater than 1%, or preferably a higher contrast of greater than 2%.
- a silicon oxy-nitride system is used in which the refractive index of the waveguides is 1.60 and the refractive index of the cladding layers is about 1.44.
- ⁇ n/n cladding is greater than about 10%.
- the external system 10 is usually comprised of one or more devices, such as, but not limited to, waveguides, filters, and amplifiers.
- the splitter/combiner system can include one or more splitter/combiners 100 that are coupled to the external system 10 . As a result of increasing the tolerance of the splitter/combiner systems 100 , the performance and/or yield of the entire system is improved.
- FIG. 2 is a plan view of the generalized configuration of the directional couplers and phase shifts in accordance with the invention.
- FIG. 2 shows the general design of the splitter/combiners 100 of FIG. 1.
- Each splitter/combiner 100 is preferably comprised of two or more directional couplers 110 and two or more phase shifts 112 .
- Various mathematical criteria are used in designing a high parameter tolerance for the spectra of interest, such as designing for maximal flatness of the spectrum with respect to the changes in the parameters and designing for equal-ripple of the spectrum for the desired ranges of the values for the parameters.
- designing for maximal flatness the derivatives of the signal of interest with respect to the parameters of interest are engineered to be preferably negligible.
- designing for equal ripple the deviation of the spectrum of interest, from the ideal spectrum, is engineered to be within the desired tolerance for the desired parameter range.
- Combinations of spectra of interest such as the reflection spectrum, the transmission spectrum, or simultaneously both the reflection and transmission spectra, can be designed for high parameter tolerance.
- FIG. 3 is a plan view of a splitter/combiner system coupled to a transmissive external optical system in accordance with a first exemplary embodiment of the invention.
- the splitter/combiner system includes one splitter/combiner 100 providing a high parameter tolerance transmission spectrum at a desired power splitting ratio.
- the exemplary splitter/combiner 100 includes three directional couplers 110 and two phase shifts 112 , which are serially connected to each other in alternating order.
- the splitter/combiner system is coupled to an external system 10 , which, in this embodiment, is comprised of two waveguides that have no reflection and unity transmission over the frequency range of interest, in this specific example.
- FIG. 4 is a plan view illustrating the layout of the waveguides in the first embodiment splitter/combiner system 100 of FIG. 3.
- each of the directional couplers 110 comprises a region in which the waveguides AC and BD are in close physical proximity to each other. This enables the coherent combination and cross-coupling of energy between the waveguides.
- Each of the phase shifts 112 comprises segments of the waveguides AC and BD that have different lengths with respect to each other. This introduces a relative phase shift between signals propagating in the waveguides.
- the spectra of the splitter/combiner system are expressed as a function of parameters, such as the coupling values of the directional couplers 110 and the phase values of the phase shifts 112 .
- ⁇ 1 and ⁇ 2 are the phase values of the phase shifts and ⁇ 1 , ⁇ 2 , and ⁇ 3 are the coupling values of the directional couplers.
- an input A is preferably equally split between outputs C and D. Therefore, for an input signal A with a normalized power of 1 and an input signal B with negligible power, the outputs C and D have normalized powers of 1 ⁇ 2.
- the output signal C is given by,
- the output signal D can be described by a similar equation.
- the splitter/combiner 100 in this embodiment has five designable parameters: 1) the coupling value of the first directional coupler, ⁇ 1 ; 2) the phase value of the first phase shift, ⁇ 1 ; 3) the coupling value of the second directional coupler, ⁇ 2 ; 4) the phase value of the second phase shift, ⁇ 2 ; and 5) the coupling value of the third directional coupler, ⁇ 3 .
- the coupling values of the directional couplers 110 are affected by the respective coupling coefficients and the coupling lengths of the directional couplers.
- the phase values of the phase shifts 112 are affected by the respective propagation constants and the propagation lengths of the phase shifts.
- Deviations in the coupling coefficients, the coupling lengths, the propagation constants, and the propagation lengths away from the nominal design will, therefore, affect the output signals C, D. Additionally, the deviations may be matched for similar devices. These effects are common to monolithic fabrication of planar waveguide systems due to the fabrication errors in layer thickness, doping to control refractive indices, and waveguide etching, for example.
- the coupling coefficients, of the directional couplers 110 are assumed to deviate by the same amount and the propagation constants p of both phase shifts 112 deviate by the same amount, which is typical for deviations resulting from common fabrication errors that can give rise to undesired frequency dependencies and polarization dependencies.
- the high tolerances for the output signals C, D are achieved by engineering the output signals C, D relative to the deviations in the coupling coefficients and the propagation constants, and specifically to matched deviations in the coupling coefficients and propagation constants, in this example.
- the coupling coefficients of the directional couplers 110 are assumed to be susceptible to a matched deviation, ⁇ , and the propagation constants of the phase shifts 112 are assumed to be susceptible to a matched deviation, ⁇ .
- the derivatives of the output signal C, with respect to ⁇ and ⁇ are preferably negligible so that the spectrum is maximally flat.
- the output signal C has preferably a normalized power of 1 ⁇ 2.
- the deviations of the parameter, ⁇ preferably do not change the normalized power of output C by greater than a desired amount, ⁇ , over the desired range of the parameter, ⁇ , as shown in FIG. 5.
- the method described above can be used to obtain other exemplary embodiments of the invention.
- the number of directional couplers and phase shifts may be extended to any desired number or other splitting ratios can be obtained.
- FIG. 6 is a plan view of a splitter/combiner 100 coupled to a reflective external optical system 10 in accordance with a second embodiment of the invention.
- a high parameter tolerance reflection spectrum is obtained by engineering a splitter/combiner 100 that is coupled to an external system 10 with a desired reflection spectrum in the frequency range of interest.
- a single splitter/combiner 100 preferably contains two directional couplers 110 and two phase shifts 112 , which are serially connected to each other in alternating order.
- the reflection spectrum, R( ⁇ ), of the external system 10 is preferably [ 1 0 0 1 ] ⁇ r ⁇ ( ⁇ )
- the input signals, A in and B in are directed in ports A and B, and the reflected output signals, A R and B R , are also produced at ports A and B.
- the reflected output signal A R is preferably negligible so that the entire input signal A in is directed to reflected output signal B R .
- the input signal A in preferably has a normalized power of 1 and the input signal B in is preferably negligible.
- the reflected output signal A R is given by,
- a R e 2i ⁇ 2 [e i ⁇ 1 cos( ⁇ 1 )cos( ⁇ 2 ) ⁇ sin( ⁇ 1 )sin( ⁇ 2 )] 2 ⁇ [e i ⁇ 1 cos( ⁇ 1 )sin( ⁇ 2 )+sin( ⁇ 1 )cos( ⁇ 2 )] 2 (13)
- the coupling coefficients of the directional couplers 110 are engineered for a matched deviation, ⁇ , and the propagation constants of the phase shifts 112 are engineered for a matched deviation, ⁇ .
- the reflected output signal A R and the derivatives of A R are preferably negligible. The resulting equations are:
- n, m are non-negative integers, 2n+1 ⁇ 4m+2 and q is any integer.
- n is a non-negative integer and m is a positive integer, 2n+1 ⁇ 4m and q is
- the first directional coupler is preferably a 50% coupler and the second directional coupler is preferably a 100% coupler.
- the first and second phase shifts are preferably both + 2 ⁇ ⁇ 3 ⁇ ⁇ or ⁇ ⁇ both ⁇ - 2 ⁇ ⁇ 3 .
- FIG. 7 is a plan view of two exemplary splitter/combiners 100 coupled an external system 10 , in accordance with a third embodiment of the invention.
- the splitter/combiner system is designed for a high parameter tolerance transmission spectrum.
- two splitter/combiners 100 are coupled to an external system 10 with a transmission spectrum.
- the splitter/combiners 100 in this embodiment preferably include two directional couplers 110 and two phase shifts 112 that are serially connected to each other in alternating order.
- the external system 10 is comprised of waveguides coupling the first splitter/combiner to the second splitter/combiner.
- the transmission spectrum of the waveguides, T( ⁇ ) is [ 1 0 0 1 ] ⁇ t ⁇ ( ⁇ )
- the waveguides are preferably completely transmissive at the frequency or frequencies of interest, so that t( ⁇ ) is preferably 1.
- the input is preferably directed in port A and the output is directed out ports C and D.
- the response of the output signal C T is preferably negligible and the derivatives for signal C T are preferably negligible.
- This embodiment can be used as a waveguide cross.
- a splitter/combiner system is designed for high parameter tolerance reflection and transmission spectra. Two splitter/combiners are coupled to an external system, such as a directional-coupler assisted add/drop filter having reflection and transmission spectra, as described, for example, in U.S. Pat. Appl. No. Unknown, entitled “Directional-coupler Assisted Add/Drop Filter With IQ Induced On/Off Switching and Modulation” filed Mar. 7, 2002 by common assignee, which is incorporated herein by reference in its entirety.
- FIG. 8 is a block diagram of a splitter/combiner system coupled to two external optical systems (sub-elements) having the same reflection and transmission spectra, in accordance with a fourth embodiment of the invention.
- the DCA filter resonator-system is reflective at particular frequencies and transmissive at others.
- the splitter/combiners 100 have 50/50 power splitting ratios and couple to the two DCA filter resonator sub-elements 10 - 1 , 10 - 2 .
- FIGS. 9A and 9B are schematic block diagrams illustrating the design process for the fourth embodiment in view of the reflection and transmission characteristics of the external system.
- Splitter/combiners 100 are preferably designed separately for the reflection and the transmission spectra.
- the first splitter/combiner 100 - 1 is designed using the parameter tolerance requirements for the reflection spectrum, similar to the second embodiment, as illustrated in FIG. 9A.
- the second splitter/combiner 100 - 2 is designed to satisfy the parameter tolerance requirements on the transmission spectrum as illustrated in FIG. 9B.
- the desired values of output signal C T and output signal A R are simultaneously negligible, so that there is no crosstalk and no leakage.
- the derivatives of signal C T and signal A R with respect to these parameters are preferably negligible.
- FIG. 10 is a plan view of a simplified splitter/combiner configuration for reflection/transmission spectra in accordance with the invention.
- the design is made for a splitter/combiner for reflection and then the design is mirrored for transmission.
- the splitter/combiner described in the second embodiment, for reflection can also be used for transmission, as shown in FIG. 10.
- the output signal A R and output signal C T are preferably negligible.
- the input signal A in preferably has a normalized power of 1.
- the input signal B in preferably has negligible power.
- the reflection signal A R is:
- FIG. 11 is a plan view of an alternate splitter/combiner configuration for reflection and transmission spectra in accordance with the invention.
- phase values of the phase shifts in the splitter/combiner systems are controlled by an effect, such as electro-optic or thermo-optic refractive index changes.
- an effect such as electro-optic or thermo-optic refractive index changes.
- yields may not be high enough.
- This embodiment enables the phase values to vary by different amounts, addressing a differential error, for example.
- the differential error is corrected by tuning the phase values using a refractive effect, typically in a post-fabrication tuning step. The tolerance of the phase value, and the splitter/combiner, is thereby increased.
- FIG. 12 shows one such implementation.
- FIG. 12 is a plan view illustrating the layout of the waveguides in still another embodiment of the splitter/combiner system.
- a post fabrication tuning mechanism is provided. Specifically, heaters 210 are integrated with the waveguides, and specifically on the phase shifts to enable post fabrication control over the refractive indices of waveguide A. This allows tuning of the propagation constants of the phase shifts 112 .
- the operation of the splitter/combiner 100 is tested post fabrication.
- the refractive indices of the waveguides are temperature tuned to optimize the splitter/combiner's performance.
- the heaters 210 maintain the waveguides at these calibrated temperatures in a steady state.
- Other techniques are used to fine-tune the operation of the splitter/combiner 100 in other implementations. For example, instead of temperature tuning the refractive indices, ultraviolet exposure is used to modify the waveguides in a post fabrication calibration operation.
- each port can be used as an input port, an output port, or both an input and an output port.
- the methods described above may be extended to any number of directional couplers and phase shifts.
- the methods may also be extended to any desired power splitting ratio and a wide range of parameter deviations.
- the designs are not limited to any specific tolerance values or any specific set of parameters.
Abstract
Description
- Power splitters/combiners are essential components in optical systems, and especially integrated, planar waveguide systems. They are important where coherent signal splitting, signal combining, or both signal splitting and combining are required. Splitters are typically used to split a single optical signal into two signals. Combiners are typically used to combine two signals into a single signal. Splitter/combiner pairs are often used to control power flow through optical elements. Splitters and combiners can also be configured as multifunctional splitter/combiners, where the operation performed depends upon the direction of the input signals and the number of inputs provided.
- A frequently used splitter/combiner is composed of two waveguides that are side-coupled to each other, forming a directional coupler. Light traveling in one waveguide couples to the other waveguide so that splitting or combining can occur. For an input signal directed into a first waveguide of the directional coupler, the power splitting ratio is defined as the ratio of the percentage of power at the output of the first waveguide to the percentage of power at the output of the second waveguide. The power splitting ratio, P, is related to the coupling value, φ, as
- P=cos2 (φ)/sin2(φ) (1)
- where φ is the product of the coupling coefficient, μ, and the coupling length, L, of the device.
- To achieve a desired power splitting ratio, the coupling value for the coupler has to be exact. For example, if the coupling value of the coupler in a 50/50 splitter is smaller than the ideal value by 10%, the power splitting ratio becomes 57.8/42.2; and if the coupling value is smaller by 20%, the power splitting ratio becomes 65.5/34.5.
- The performance of directional couplers is inherently sensitive to fabrication errors. The coupling value is a function of physical parameters, such as waveguide cross-section, effective index, and waveguide-to-waveguide separation. Fabrication errors can also lead to undesired dependencies between the coupling value and the frequency and polarizations of the input optical signals, on otherwise nominally spectrally flat, polarization insensitive designs.
- In order to improve performance, splitters/combiners have been proposed that include cascaded splitters and phase shifters. These systems are typically optimized for wavelength insensitivity, and sometimes robustness against uniform fabrication errors.
- Previously proposed power splitter/combiner systems with phase shifts are not adequately robust against errors for many fabrication processes. This is especially true for planar waveguide fabrication in high index contrast material systems. Lithographic patterning and material deposition processes used to control waveguide cross-sections, effective indices, waveguide lengths, and waveguide-to-waveguide separations, for example, do not always provide enough control to fabricate commercially relevant systems with adequate yields.
- The invention is directed to a splitter/combiner that is tolerant of parameter deviations. It is specifically applicable to integration into the transmission and/or reflection light paths of external systems. In this power splitter/combiner system, each splitter/combiner is comprised of two or more directional couplers serially connected to two or more phase shifts in an alternating order (e.g., directional coupler, phase shift, directional coupler, phase shift, directional coupler).
- The invention addresses the problem of parameter deviations in splitter/combiners by selecting specific coupling and phase values for the directional couplers and phase shifts to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants, for example. Parameter deviations, such as coupling value deviations and phase value deviations from the nominal design due to fabrication errors, for example, typically give rise to frequency dependency, polarization dependency in the output signal and are specifically addressed in the invention by designing the system so that the sensitivity of the output signal to these changes is minimized.
- Additionally, the invention can be applied to address the specific problem of matched deviations in coupling values and phase values in a splitter/combiner system. The invention also addresses the problem of differential deviations in the phase values of the phase shifts by providing tunable phase shifts, employing controlled effects, such as electro-optic or thermo-optic refractive index changes.
- In an exemplary embodiment of the invention, two splitter/combiners are coupled to an external system and engineered for desired reflection and transmission spectra. The splitter/combiner is designed for maximal flatness of the spectrum with respect to the deviations in the parameters in one example. Other methods, such as designing for equal-ripple of the spectrum for the desired ranges of the values for the parameters, can also be implemented. In another exemplary embodiment, two splitter/combiners are coupled to two external systems that have nominally identical reflection and transmission spectra.
- The splitter/combiner system of the invention can also be designed for a wide range of ratios for splitting and/or combining signals. The invention can be used for both mono-directional or bi-directional splitting and combining.
- In general, according to one aspect, the invention features a splitter/combiner system that comprises a serial connection of at least two couplers and at least two phase shifts. The coupling coefficients of the couplers and propagation constants of the phase shifts are selected to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants.
- In general, according to another aspect, the invention can be characterized as a design process for a splitter/combiner system, in which a serial connection of at least two couplers and at least two phase shifts are provisioned to connect an input waveguide to an external system. Coupling coefficients of the couplers and propagation constants of the phase shifts are proscribed to minimize changes in an output signal in response to changes in the coupling coefficients and the propagation constants.
- The above and other features of the invention including various novel details of construction and combinations of parts, and other advantages, will now be more particularly described with reference to the accompanying drawings and pointed out in the claims. It will be understood that the particular method and device embodying the invention are shown by way of illustration and not as a limitation of the invention. The principles and features of this invention may be employed in various and numerous embodiments without departing from the scope of the invention.
- In the accompanying drawings, reference characters refer to the same parts throughout the different views. The drawings are not necessarily to scale; emphasis has instead been placed upon illustrating the principles of the invention.
- FIG. 1 is a block diagram of a splitter/combiner coupled to an external system having a reflection and transmission spectrum, in accordance with the invention;
- FIG. 2 is a plan view of the generalized configuration of the directional couplers and phase shifts in accordance with the invention;
- FIG. 3 is a plan view of a splitter/combiner system coupled to a transmissive external optical system, according to a first embodiment of the invention;
- FIG. 4 is a plan view illustrating the layout of the waveguides in the first embodiment splitter/combiner system;
- FIG. 5 is a plot of the power of output signal C as a function of the coupling coefficient, showing a region in which changes in the coupling coefficient yields only small changes in the output signal;
- FIG. 6 is a plan view of a splitter/combiner coupled to a reflective external optical system in accordance with a second embodiment of the invention;
- FIG. 7 is a plan view of two exemplary splitter/combiners coupled an external system, in accordance with a third embodiment of the invention;
- FIG. 8 is a block diagram of a splitter/combiner system coupled to two external optical systems (sub-elements) having the same reflection and transmission spectra, in accordance with a fourth embodiment of the invention;
- FIGS. 9A and 9B are schematic block diagrams illustrating the design process for the fourth embodiment in view of the reflection and transmission characteristics of the external system;
- FIG. 10 is a plan view of a simplified splitter/combiner configuration for reflection/transmission spectra in accordance with the invention;
- FIG. 11 is a plan view of an alternate splitter/combiner configuration for reflection and transmission spectra in accordance with the invention; and
- FIG. 12 is a plan view illustrating the layout of the waveguides in still another embodiment of the splitter/combiner system.
- This invention describes a splitter/combiner system that, when coupled to an external system having a reflection and/or transmission response, has a high level of tolerance to parameter deviations for the desired spectra of the output signal.
- FIG. 1 illustrates the typical application for the invention. FIG. 1 is a block diagram of one or more of splitter/
combiners 100 are coupled to anexternal system 10 that has reflection (R(ω)) and transmission (T(ω)) spectra. - The splitter/
combiners 100 are monolithically fabricated from planar waveguides in a high index contrast material system in the current implementation. That is, the material system provides an index contrast between the refractive indices of the waveguides and the cladding that is greater than 1%, or preferably a higher contrast of greater than 2%. Presently, a silicon oxy-nitride system is used in which the refractive index of the waveguides is 1.60 and the refractive index of the cladding layers is about 1.44. Thus, Δn/ncladding is greater than about 10%. - The
external system 10 is usually comprised of one or more devices, such as, but not limited to, waveguides, filters, and amplifiers. The splitter/combiner system can include one or more splitter/combiners 100 that are coupled to theexternal system 10. As a result of increasing the tolerance of the splitter/combiner systems 100, the performance and/or yield of the entire system is improved. - FIG. 2 is a plan view of the generalized configuration of the directional couplers and phase shifts in accordance with the invention. FIG. 2 shows the general design of the splitter/
combiners 100 of FIG. 1. Each splitter/combiner 100 is preferably comprised of two or moredirectional couplers 110 and two or more phase shifts 112. - Arbitrarily combining directional couplers and phase shifts in a sequential manner will generally not improve tolerance, however. Instead, the coupling value, φ, of each
directional coupler 110 and the phase value, θ, of eachphase shift 112 must be chosen carefully so that the output signals of interest have a desired power splitting ratio and a high tolerance to a particular type, or types, of parameter deviation. - Various mathematical criteria are used in designing a high parameter tolerance for the spectra of interest, such as designing for maximal flatness of the spectrum with respect to the changes in the parameters and designing for equal-ripple of the spectrum for the desired ranges of the values for the parameters. In designing for maximal flatness, the derivatives of the signal of interest with respect to the parameters of interest are engineered to be preferably negligible. In designing for equal ripple, the deviation of the spectrum of interest, from the ideal spectrum, is engineered to be within the desired tolerance for the desired parameter range. Combinations of spectra of interest, such as the reflection spectrum, the transmission spectrum, or simultaneously both the reflection and transmission spectra, can be designed for high parameter tolerance.
- FIG. 3 is a plan view of a splitter/combiner system coupled to a transmissive external optical system in accordance with a first exemplary embodiment of the invention. The splitter/combiner system includes one splitter/
combiner 100 providing a high parameter tolerance transmission spectrum at a desired power splitting ratio. - The exemplary splitter/
combiner 100 includes threedirectional couplers 110 and twophase shifts 112, which are serially connected to each other in alternating order. The splitter/combiner system is coupled to anexternal system 10, which, in this embodiment, is comprised of two waveguides that have no reflection and unity transmission over the frequency range of interest, in this specific example. - FIG. 4 is a plan view illustrating the layout of the waveguides in the first embodiment splitter/
combiner system 100 of FIG. 3. Specifically, each of thedirectional couplers 110 comprises a region in which the waveguides AC and BD are in close physical proximity to each other. This enables the coherent combination and cross-coupling of energy between the waveguides. Each of the phase shifts 112 comprises segments of the waveguides AC and BD that have different lengths with respect to each other. This introduces a relative phase shift between signals propagating in the waveguides. - Using a transfer matrix method, the spectra of the splitter/combiner system are expressed as a function of parameters, such as the coupling values of the
directional couplers 110 and the phase values of the phase shifts 112. The output signals C and D for the splitter/combiner system are related to the input signals A and B as follows: - where θ1 and θ2 are the phase values of the phase shifts and φ1, φ2, and φ3 are the coupling values of the directional couplers. In this embodiment, an input A is preferably equally split between outputs C and D. Therefore, for an input signal A with a normalized power of 1 and an input signal B with negligible power, the outputs C and D have normalized powers of ½. The output signal C is given by,
- C=cos(φ1)cos(φ2)cos(φ3)e iθ 1 +iθ 2 −sin(φ1)sin(φ2)cos(φ3)e iθ 2 −cos(φ1)sin(φ2)sin(φ3)e iθ 1 −sin(φ1)cos(φ2)sin(φ3) (3)
- The output signal D can be described by a similar equation.
- The splitter/
combiner 100 in this embodiment has five designable parameters: 1) the coupling value of the first directional coupler, θ1; 2) the phase value of the first phase shift, φ1; 3) the coupling value of the second directional coupler, φ2; 4) the phase value of the second phase shift, θ2; and 5) the coupling value of the third directional coupler, φ3. The coupling values of thedirectional couplers 110 are affected by the respective coupling coefficients and the coupling lengths of the directional couplers. The phase values of the phase shifts 112 are affected by the respective propagation constants and the propagation lengths of the phase shifts. Deviations in the coupling coefficients, the coupling lengths, the propagation constants, and the propagation lengths away from the nominal design will, therefore, affect the output signals C, D. Additionally, the deviations may be matched for similar devices. These effects are common to monolithic fabrication of planar waveguide systems due to the fabrication errors in layer thickness, doping to control refractive indices, and waveguide etching, for example. - In this first embodiment, the coupling coefficients, of the
directional couplers 110 are assumed to deviate by the same amount and the propagation constants p of bothphase shifts 112 deviate by the same amount, which is typical for deviations resulting from common fabrication errors that can give rise to undesired frequency dependencies and polarization dependencies. - According to the invention, the high tolerances for the output signals C, D are achieved by engineering the output signals C, D relative to the deviations in the coupling coefficients and the propagation constants, and specifically to matched deviations in the coupling coefficients and propagation constants, in this example.
- In this embodiment, the coupling coefficients of the
directional couplers 110 are assumed to be susceptible to a matched deviation, δμ, and the propagation constants of the phase shifts 112 are assumed to be susceptible to a matched deviation, δβ. To achieve a desired insensitivity to the matched deviations in this embodiment, the derivatives of the output signal C, with respect to μ and β, are preferably negligible so that the spectrum is maximally flat. The output signal C has preferably a normalized power of ½. - As a result of this design, the deviations of the parameter, μ, preferably do not change the normalized power of output C by greater than a desired amount, ε, over the desired range of the parameter, Δμ, as shown in FIG. 5. FIG. 5 is a plot of the power of output signal C as a function of the coupling coefficient, showing a region in which changes in the coupling coefficient yields only small changes in the output signal. The resulting equations are,
-
- φ3=φ1 (9)
-
- The method described above can be used to obtain other exemplary embodiments of the invention. For example, the number of directional couplers and phase shifts may be extended to any desired number or other splitting ratios can be obtained.
- FIG. 6 is a plan view of a splitter/
combiner 100 coupled to a reflective externaloptical system 10 in accordance with a second embodiment of the invention. A high parameter tolerance reflection spectrum is obtained by engineering a splitter/combiner 100 that is coupled to anexternal system 10 with a desired reflection spectrum in the frequency range of interest. In this embodiment, a single splitter/combiner 100 preferably contains twodirectional couplers 110 and twophase shifts 112, which are serially connected to each other in alternating order. -
-
- —the external system is preferably completely reflective, r(ω)=1, over the frequency range of interest. The input signals, Ain and Bin, are directed in ports A and B, and the reflected output signals, AR and BR, are also produced at ports A and B. In this embodiment, the reflected output signal AR is preferably negligible so that the entire input signal Ain is directed to reflected output signal BR. The input signal Ain preferably has a normalized power of 1 and the input signal Bin is preferably negligible. The reflected output signal AR is given by,
- A R =e 2iθ 2 [e iθ 1 cos(φ1)cos(φ2)−sin(φ1)sin(φ2)]2 −[e iθ 1 cos(φ1)sin(φ2)+sin(φ1)cos(φ2)]2 (13)
- In this embodiment, the coupling coefficients of the
directional couplers 110 are engineered for a matched deviation, δμ, and the propagation constants of the phase shifts 112 are engineered for a matched deviation, δβ. To achieve the desired insensitivity to the matched deviations in this embodiment, the reflected output signal AR and the derivatives of AR, with respect to μ and β, are preferably negligible. The resulting equations are: - These equations result in the following two sets of definitions for the coupling ratios and the phase shifts in this embodiment:
-
- where n, m are non-negative integers, 2n+1<4m+2 and q is any integer.
-
- where n is a non-negative integer and m is a positive integer, 2n+1<4m and q is
-
- FIG. 7 is a plan view of two exemplary splitter/
combiners 100 coupled anexternal system 10, in accordance with a third embodiment of the invention. The splitter/combiner system is designed for a high parameter tolerance transmission spectrum. In this embodiment, two splitter/combiners 100 are coupled to anexternal system 10 with a transmission spectrum. The splitter/combiners 100 in this embodiment preferably include twodirectional couplers 110 and twophase shifts 112 that are serially connected to each other in alternating order. -
-
- —the waveguides are preferably completely transmissive at the frequency or frequencies of interest, so that t(ω) is preferably 1. The input is preferably directed in port A and the output is directed out ports C and D. Similar to the previous embodiment, the response of the output signal CT is preferably negligible and the derivatives for signal CT are preferably negligible. This embodiment can be used as a waveguide cross. In a fourth exemplary embodiment of the invention, a splitter/combiner system is designed for high parameter tolerance reflection and transmission spectra. Two splitter/combiners are coupled to an external system, such as a directional-coupler assisted add/drop filter having reflection and transmission spectra, as described, for example, in U.S. Pat. Appl. No. Unknown, entitled “Directional-coupler Assisted Add/Drop Filter With IQ Induced On/Off Switching and Modulation” filed Mar. 7, 2002 by common assignee, which is incorporated herein by reference in its entirety.
- FIG. 8 is a block diagram of a splitter/combiner system coupled to two external optical systems (sub-elements) having the same reflection and transmission spectra, in accordance with a fourth embodiment of the invention. The DCA filter resonator-system is reflective at particular frequencies and transmissive at others. The splitter/
combiners 100 have 50/50 power splitting ratios and couple to the two DCA filter resonator sub-elements 10-1, 10-2. - FIGS. 9A and 9B are schematic block diagrams illustrating the design process for the fourth embodiment in view of the reflection and transmission characteristics of the external system. Splitter/
combiners 100 are preferably designed separately for the reflection and the transmission spectra. Specifically, the first splitter/combiner 100-1 is designed using the parameter tolerance requirements for the reflection spectrum, similar to the second embodiment, as illustrated in FIG. 9A. Once the first splitter/combiner 100-1 is designed based on the reflection spectrum, the second splitter/combiner 100-2 is designed to satisfy the parameter tolerance requirements on the transmission spectrum as illustrated in FIG. 9B. - In this embodiment, the desired values of output signal CT and output signal AR are simultaneously negligible, so that there is no crosstalk and no leakage. To achieve high tolerance to common deviations in the coupling coefficients and the propagation constants, the derivatives of signal CT and signal AR with respect to these parameters are preferably negligible. These requirements result in definitions for the coupling values and phase values.
- FIG. 10 is a plan view of a simplified splitter/combiner configuration for reflection/transmission spectra in accordance with the invention. The design is made for a splitter/combiner for reflection and then the design is mirrored for transmission. For example, the splitter/combiner described in the second embodiment, for reflection, can also be used for transmission, as shown in FIG. 10. In this embodiment, the output signal AR and output signal CT are preferably negligible. The input signal Ain preferably has a normalized power of 1. The input signal Bin preferably has negligible power. The reflection signal AR is:
- A R ={e 2iθ 2 [e iθ 1 cos(φ1)cos(φ2)−sin(φ1)sin(φ2)]2 −[e iθ 1 cos(φ1)sin(φ2)+sin(φ1)cos(φ2)]2 }r(ω)=0 (26)
- and the transmission signal CT is:
- C T ={e 2iθ 2 [e iθ 1 cos(φ1)cos(φ2)−sin(φ1)sin(φ2)]2 −[e iθ 1 cos(φ1)sin(φ2)+sin(φ1)cos(φ2)]2 }t(ω)=0 (27)
- Since the two signals have the same form, it is clear that a solution to one equation is also a solution to the other equation. A further alternate embodiment using this method is shown in FIG. 11. FIG. 11 is a plan view of an alternate splitter/combiner configuration for reflection and transmission spectra in accordance with the invention.
- In another exemplary embodiment of the invention, the phase values of the phase shifts in the splitter/combiner systems are controlled by an effect, such as electro-optic or thermo-optic refractive index changes. Specifically, even with the foregoing parameter tolerant designs, in high index contrast planar waveguide systems, yields may not be high enough. This embodiment enables the phase values to vary by different amounts, addressing a differential error, for example. The differential error is corrected by tuning the phase values using a refractive effect, typically in a post-fabrication tuning step. The tolerance of the phase value, and the splitter/combiner, is thereby increased.
- FIG. 12 shows one such implementation. FIG. 12 is a plan view illustrating the layout of the waveguides in still another embodiment of the splitter/combiner system. A post fabrication tuning mechanism is provided. Specifically,
heaters 210 are integrated with the waveguides, and specifically on the phase shifts to enable post fabrication control over the refractive indices of waveguide A. This allows tuning of the propagation constants of the phase shifts 112. - In the typical application, the operation of the splitter/
combiner 100 is tested post fabrication. In the calibration sequence, the refractive indices of the waveguides are temperature tuned to optimize the splitter/combiner's performance. During normal operation, theheaters 210 maintain the waveguides at these calibrated temperatures in a steady state. Other techniques are used to fine-tune the operation of the splitter/combiner 100 in other implementations. For example, instead of temperature tuning the refractive indices, ultraviolet exposure is used to modify the waveguides in a post fabrication calibration operation. - It should be appreciated that this post fabrication fine-tuning technique is applicable to any of the previously described embodiments to improve performance of the final system.
- Further, in all of the above-described embodiments, the splitter/combiner systems can be used for signal propagation in either direction. As well, each port can be used as an input port, an output port, or both an input and an output port.
- The methods described above may be extended to any number of directional couplers and phase shifts. The methods may also be extended to any desired power splitting ratio and a wide range of parameter deviations. As well, the designs are not limited to any specific tolerance values or any specific set of parameters.
- Although the present invention has been shown and described with respect to several preferred embodiments thereof, various changes, omissions and additions to the form and detail thereof, may be made therein, without departing from the spirit and scope of the invention.
Claims (38)
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10/093,663 US20030169964A1 (en) | 2002-03-08 | 2002-03-08 | Power splitter/combiner with parameter tolerance and design process therefor |
US10/290,875 US7027686B1 (en) | 2002-03-08 | 2002-11-08 | Parameter tolerant splitter/combiner with subdivided couplers |
PCT/US2003/006474 WO2003076987A2 (en) | 2002-03-08 | 2003-03-03 | Optical power splitter/combiner with parameter tolerance and design process therefor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10/093,663 US20030169964A1 (en) | 2002-03-08 | 2002-03-08 | Power splitter/combiner with parameter tolerance and design process therefor |
Related Child Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US10/290,875 Continuation-In-Part US7027686B1 (en) | 2002-03-08 | 2002-11-08 | Parameter tolerant splitter/combiner with subdivided couplers |
Publications (1)
Publication Number | Publication Date |
---|---|
US20030169964A1 true US20030169964A1 (en) | 2003-09-11 |
Family
ID=27788006
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US10/093,663 Abandoned US20030169964A1 (en) | 2002-03-08 | 2002-03-08 | Power splitter/combiner with parameter tolerance and design process therefor |
US10/290,875 Expired - Fee Related US7027686B1 (en) | 2002-03-08 | 2002-11-08 | Parameter tolerant splitter/combiner with subdivided couplers |
Family Applications After (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US10/290,875 Expired - Fee Related US7027686B1 (en) | 2002-03-08 | 2002-11-08 | Parameter tolerant splitter/combiner with subdivided couplers |
Country Status (2)
Country | Link |
---|---|
US (2) | US20030169964A1 (en) |
WO (1) | WO2003076987A2 (en) |
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040042722A1 (en) * | 2002-08-29 | 2004-03-04 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20040057687A1 (en) * | 2002-08-29 | 2004-03-25 | Micron Technology, Inc. | Resonator for thermo optic device |
US6768843B1 (en) * | 2002-08-16 | 2004-07-27 | Wavesplitter Technologies, Inc. | Cascaded fourier filter interleaver having enhanced performance |
US20050031284A1 (en) * | 2002-08-29 | 2005-02-10 | Micron Technology, Inc., Clarendon Photonics | Waveguide for thermo optic device |
EP1987382A2 (en) * | 2006-02-24 | 2008-11-05 | Lightwave Microsystems Corporation | Broadband 2x2 optical splitter |
WO2015176311A1 (en) * | 2014-05-23 | 2015-11-26 | 华为技术有限公司 | Polarization control device and polarization control method |
JP2017037215A (en) * | 2015-08-11 | 2017-02-16 | 国立研究開発法人産業技術総合研究所 | Optical switch |
WO2019143571A1 (en) * | 2018-01-16 | 2019-07-25 | Cisco Technology, Inc. | Complementary optical phase shifting arrangement |
JP2020519973A (en) * | 2017-08-14 | 2020-07-02 | 河南仕佳光子科技股▲分▼有限公司 | Tunable broad-spectrum wavelength-insensitive directional coupler |
CN113568098A (en) * | 2021-07-05 | 2021-10-29 | 烽火通信科技股份有限公司 | Optical splitter, design method and reconstruction method of optical splitter |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5169536B2 (en) * | 2008-02-08 | 2013-03-27 | 沖電気工業株式会社 | Optical multiplexing / demultiplexing device |
US10338309B2 (en) * | 2012-12-13 | 2019-07-02 | Luxtera, Inc. | Method and system for stabilized directional couplers |
US20140293393A1 (en) * | 2013-03-28 | 2014-10-02 | Barthelemy Fondeur | Flat-top tunable filter |
Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5044715A (en) * | 1989-02-07 | 1991-09-03 | Nippon Telegraph And Telephone Corporation | Guided-wave optical branching components and optical switches |
US5119453A (en) * | 1991-04-05 | 1992-06-02 | Ecole Polytechnique | Wavelength-flattened 2x2 splitter for single-mode optical waveguides and method of making same |
US5162869A (en) * | 1989-12-23 | 1992-11-10 | Johannes Heidenhain Gmbh | Apparatus and method having at least one waveguide coupler to create at least two signals having a mutual phase shift not equal to 180 degrees |
US5943457A (en) * | 1998-03-24 | 1999-08-24 | Telecommunications Research Laboratories | Generalized resonant coupler filters |
US6208780B1 (en) * | 1999-01-19 | 2001-03-27 | Lucent Technologies Inc. | System and method for optical monitoring |
US6285810B1 (en) * | 1996-07-26 | 2001-09-04 | Italtel Spa | Tunable add/drop optical device |
US6400870B1 (en) * | 1999-11-11 | 2002-06-04 | Her Majesty The Queen In Right Of Canada As Represented By The Secretary Of State For Industry | Symmetric interferometers unbalanced by using light exposure to tailor the spectral behavior |
US20030002797A1 (en) * | 2001-06-29 | 2003-01-02 | Tzu-Yih Chu | All optical logic using cross-phase modulation amplifiers and mach-zehnder interferometers with phase-shift devices |
US20030063834A1 (en) * | 2001-09-28 | 2003-04-03 | Nicolas Godbout | Optical phase shifting, splitting and combining device |
US6633698B2 (en) * | 2000-04-26 | 2003-10-14 | Sumitomo Electric Industries, Ltd. | Optical filter |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5596661A (en) * | 1994-12-28 | 1997-01-21 | Lucent Technologies Inc. | Monolithic optical waveguide filters based on Fourier expansion |
US6212315B1 (en) * | 1998-07-07 | 2001-04-03 | Lucent Technologies Inc. | Channel power equalizer for a wavelength division multiplexed system |
JP2003021814A (en) * | 2001-07-09 | 2003-01-24 | Communication Research Laboratory | Optical delay multiple circuit |
US6832011B2 (en) * | 2002-09-13 | 2004-12-14 | Lucent Technologies Inc. | Push-pull thermooptic switch having single control signal |
-
2002
- 2002-03-08 US US10/093,663 patent/US20030169964A1/en not_active Abandoned
- 2002-11-08 US US10/290,875 patent/US7027686B1/en not_active Expired - Fee Related
-
2003
- 2003-03-03 WO PCT/US2003/006474 patent/WO2003076987A2/en active Application Filing
Patent Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5044715A (en) * | 1989-02-07 | 1991-09-03 | Nippon Telegraph And Telephone Corporation | Guided-wave optical branching components and optical switches |
US5162869A (en) * | 1989-12-23 | 1992-11-10 | Johannes Heidenhain Gmbh | Apparatus and method having at least one waveguide coupler to create at least two signals having a mutual phase shift not equal to 180 degrees |
US5119453A (en) * | 1991-04-05 | 1992-06-02 | Ecole Polytechnique | Wavelength-flattened 2x2 splitter for single-mode optical waveguides and method of making same |
US6285810B1 (en) * | 1996-07-26 | 2001-09-04 | Italtel Spa | Tunable add/drop optical device |
US5943457A (en) * | 1998-03-24 | 1999-08-24 | Telecommunications Research Laboratories | Generalized resonant coupler filters |
US6208780B1 (en) * | 1999-01-19 | 2001-03-27 | Lucent Technologies Inc. | System and method for optical monitoring |
US6400870B1 (en) * | 1999-11-11 | 2002-06-04 | Her Majesty The Queen In Right Of Canada As Represented By The Secretary Of State For Industry | Symmetric interferometers unbalanced by using light exposure to tailor the spectral behavior |
US6633698B2 (en) * | 2000-04-26 | 2003-10-14 | Sumitomo Electric Industries, Ltd. | Optical filter |
US20030002797A1 (en) * | 2001-06-29 | 2003-01-02 | Tzu-Yih Chu | All optical logic using cross-phase modulation amplifiers and mach-zehnder interferometers with phase-shift devices |
US20030063834A1 (en) * | 2001-09-28 | 2003-04-03 | Nicolas Godbout | Optical phase shifting, splitting and combining device |
Cited By (38)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6768843B1 (en) * | 2002-08-16 | 2004-07-27 | Wavesplitter Technologies, Inc. | Cascaded fourier filter interleaver having enhanced performance |
US7509005B2 (en) | 2002-08-29 | 2009-03-24 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US7359607B2 (en) | 2002-08-29 | 2008-04-15 | Micron Technology, Inc. | Waveguide for thermo optic device |
US20050025424A1 (en) * | 2002-08-29 | 2005-02-03 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US7565039B2 (en) | 2002-08-29 | 2009-07-21 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20050031284A1 (en) * | 2002-08-29 | 2005-02-10 | Micron Technology, Inc., Clarendon Photonics | Waveguide for thermo optic device |
US7006746B2 (en) | 2002-08-29 | 2006-02-28 | Micron Technology, Inc. | Waveguide for thermo optic device |
US7020365B2 (en) * | 2002-08-29 | 2006-03-28 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20060098911A1 (en) * | 2002-08-29 | 2006-05-11 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US7120336B2 (en) | 2002-08-29 | 2006-10-10 | Micron Technology, Inc. | Resonator for thermo optic device |
US20060228084A1 (en) * | 2002-08-29 | 2006-10-12 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20060263027A1 (en) * | 2002-08-29 | 2006-11-23 | Micron Technology, Inc. | Resonator for thermo optic device |
US7215838B2 (en) | 2002-08-29 | 2007-05-08 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US7323353B2 (en) | 2002-08-29 | 2008-01-29 | Micron Technology, Inc. | Resonator for thermo optic device |
US8111965B2 (en) | 2002-08-29 | 2012-02-07 | Micron Technology, Inc. | Waveguide for thermo optic device |
US20080089647A1 (en) * | 2002-08-29 | 2008-04-17 | Micron Technology, Inc | Resonator for thermo optic device |
US20080226247A1 (en) * | 2002-08-29 | 2008-09-18 | Micron Technology, Inc. | Waveguide for thermo optic device |
US9042697B2 (en) | 2002-08-29 | 2015-05-26 | Micron Technology, Inc. | Resonator for thermo optic device |
US20040042722A1 (en) * | 2002-08-29 | 2004-03-04 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20050031263A1 (en) * | 2002-08-29 | 2005-02-10 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US20040057687A1 (en) * | 2002-08-29 | 2004-03-25 | Micron Technology, Inc. | Resonator for thermo optic device |
US7720341B2 (en) | 2002-08-29 | 2010-05-18 | Micron Technology, Inc. | Waveguide for thermo optic device |
US7706647B2 (en) | 2002-08-29 | 2010-04-27 | Micron Technology, Inc. | Resistive heater for thermo optic device |
US8195020B2 (en) | 2002-08-29 | 2012-06-05 | Micron Technology, Inc. | Resonator for thermo optic device |
US20100220958A1 (en) * | 2002-08-29 | 2010-09-02 | Blalock Guy T | Waveguide for thermo optic device |
US7936955B2 (en) | 2002-08-29 | 2011-05-03 | Micron Technology, Inc. | Waveguide for thermo optic device |
US20110206332A1 (en) * | 2002-08-29 | 2011-08-25 | Blalock Guy T | Waveguide for thermo optic device |
US8442369B2 (en) | 2006-02-24 | 2013-05-14 | Neophotonics Corporation | Distributing optical power with a power balance ratio substantially constant over a broadband of wavelengths |
EP1987382A4 (en) * | 2006-02-24 | 2010-07-21 | Lightwave Microsystems Corp | Broadband 2x2 optical splitter |
EP1987382A2 (en) * | 2006-02-24 | 2008-11-05 | Lightwave Microsystems Corporation | Broadband 2x2 optical splitter |
US20100040328A1 (en) * | 2006-02-24 | 2010-02-18 | Lightwave Microsystems Corporation | Distributing optical power with a power balance ratio substantially constant over a broadband of wavelengths |
WO2015176311A1 (en) * | 2014-05-23 | 2015-11-26 | 华为技术有限公司 | Polarization control device and polarization control method |
JP2017037215A (en) * | 2015-08-11 | 2017-02-16 | 国立研究開発法人産業技術総合研究所 | Optical switch |
US10908359B2 (en) * | 2017-08-14 | 2021-02-02 | Henan Shijia Photons Technology Co., Ltd. | Adjustable wide-spectrum wavelength-insensitive directional coupler |
JP2020519973A (en) * | 2017-08-14 | 2020-07-02 | 河南仕佳光子科技股▲分▼有限公司 | Tunable broad-spectrum wavelength-insensitive directional coupler |
WO2019143571A1 (en) * | 2018-01-16 | 2019-07-25 | Cisco Technology, Inc. | Complementary optical phase shifting arrangement |
US10649305B2 (en) | 2018-01-16 | 2020-05-12 | Cisco Technology, Inc. | Complementary optical phase shifting arrangement |
CN113568098A (en) * | 2021-07-05 | 2021-10-29 | 烽火通信科技股份有限公司 | Optical splitter, design method and reconstruction method of optical splitter |
Also Published As
Publication number | Publication date |
---|---|
WO2003076987A3 (en) | 2004-08-19 |
US7027686B1 (en) | 2006-04-11 |
WO2003076987A2 (en) | 2003-09-18 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US10088628B1 (en) | Optical waveguide element and receiving circuit | |
EP1426800B1 (en) | Optical multi/demultiplexing circuit equipped with phase generating device | |
US7492983B2 (en) | Optical circuit device | |
US7356206B2 (en) | Integrated optics polarization beam splitter using form birefringence | |
JP4102792B2 (en) | Waveguide type optical interferometer | |
EP1643302A1 (en) | Interferometer optical switch and variable optical attenuator | |
EP2439566A1 (en) | Broadband interferometer type polarized light combiner and splitter | |
US20030081873A1 (en) | Polarization beam splitter | |
US20050058386A1 (en) | Integrated optics polarization beam splitter using form birefringence | |
US5889899A (en) | Article comprising a Bragg reflective Mach-Zehnder filter of reduced coupled dependence | |
US20030169964A1 (en) | Power splitter/combiner with parameter tolerance and design process therefor | |
US20180299620A1 (en) | Delay line interferometer with polarization compensation at selective frequency | |
US20180167146A1 (en) | Temperature insensitive delay line interferometer | |
Guan et al. | Passive silicon ring-assisted Mach–Zehnder interleavers operating in the broadband spectral range | |
CA2333436C (en) | Optical multiplexer/ demultiplexer | |
JPH112735A (en) | Spectral camera type multiplexer and demultiplexer optical component with waveguide array | |
JP3695273B2 (en) | Optical multiplexer / demultiplexer | |
US20030128926A1 (en) | Compact wavelength routing device having substantially flat passband | |
US20230228944A1 (en) | Wavelength division multiplexer and demultiplexer | |
US5526439A (en) | Optical filter using electro-optic material | |
US20030030870A1 (en) | Tunable chromatic dispersion compensation | |
JP4934625B2 (en) | PLC type variable dispersion compensator | |
TW200405048A (en) | Polarization-insensitive planar lightwave circuits and method for fabricating the same | |
Moreira | Integrated optical delay line circuits on a ultra-low loss planar waveguide platform | |
JP3420501B2 (en) | Optical branch coupler |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
AS | Assignment |
Owner name: CLARENDON PHOTONICS, INC., MASSACHUSETTS Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:WANG, TAIRAN;FORESI, JAMES S.;REEL/FRAME:012694/0290 Effective date: 20020307 |
|
AS | Assignment |
Owner name: PENTECH FINANCIAL SERVICES, INC., CALIFORNIA Free format text: SECURITY AGREEMENT;ASSIGNOR:CLARENDON PHOTONICS, INC.;REEL/FRAME:012839/0474 Effective date: 20020312 |
|
AS | Assignment |
Owner name: CAMBRIUS, INC., MASSACHUSETTS Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:CLARENDON PHOTONICS, INC.;REEL/FRAME:016096/0682 Effective date: 20040611 |
|
STCB | Information on status: application discontinuation |
Free format text: ABANDONED -- FAILURE TO RESPOND TO AN OFFICE ACTION |