Patent Application
20180007454
The present invention generally relates to an optical switch and its applications in optical communication. In optical communication, an optical switch enables optical signals to be selectively switched from one optical fiber/optical circuit to another optical fiber/optical circuit. An optical switch can operate by mechanical, electro-optic or magneto-optic effects.
LiNbO3-LN or (Pb,La)(Zr,Ti)O3—PLZT or waveguide based optical switch is commercially available. LN/PLZT waveguide based optical switch is a modified balance bridge type 1×2 switch, which is composed of (a) a Mach-Zehnder (MZ) device integrated with top electrodes and (b) input-output 3-dB couplers.
The switching speed of a LN waveguide based optical switch is approximately 100 nanoseconds. Furthermore, it suffers from (a) high voltage requirement, (b) polarization dependence problem and (c) DC drift.
The switching speed of a PLZT waveguide based optical switch is approximately 10 nanoseconds.
The switching speed of a semiconductor optical amplifier (SOA) waveguide based optical switch is about 1 to 2 nanoseconds. However, the semiconductor optical amplifier waveguide based optical switch suffers from (a) noise, (b) polarization dependence problem, (c) wavelength dependence problem and (d) high electrical power consumption.
In view of the foregoing, three objectives of the present invention are:
Applications for such an optical switch with a switching speed of less than 10 nanoseconds are:
Optical Communication
Computing
Vanadium dioxide is broadly related to phase transition/change materials. Vanadium dioxide exhibits rapid (less than 10 nanoseconds) insulator-to-metal phase transition, upon temperature increase. Vanadium dioxide shows an abrupt decrease of resistance when applied current or voltage exceeds certain a threshold value. This is an electric field-induced rapid phase transition/change.
The rapid (less than 10 nanoseconds) insulator-to-metal phase transition can be utilized in conjunction with a coupled waveguide configuration (e.g., a directional coupler/multi mode interference (MMI) coupler or Mach-Zehnder (MZ) configuration) to fabricate/construct a fast optical switch.
The operational principle of a directional coupler is evanescent wave coupling in a configuration, where two single-mode waveguides come close to each other along a coupling length.
The dimension of the coupling length can depend on other parameters (e.g., overall dimension and switching speed of the optical switch). Furthermore, extinction ratio/power transfer ratio can depend on the index mismatch and the coupling parameters and the state of 120—the vanadium dioxide ultra thin-film.
100A—the fast optical switch (in the directional coupler configuration) can be fabricated/constructed on a silicon-on-insulator (SOI) substrate.
But other suitable substrate (e.g., a silicon-on-sapphire (SOS) substrate) can also be utilized.
An electrical pulse can be a current pulse or a voltage pulse. 120—the vanadium dioxide ultra thin-film is receiving a voltage pulse or a current pulse via two electrodes just to induce insulator-to-metal phase in the vanadium dioxide ultra thin-film. For example, a square wave shaped voltage pulse with a rise time of approximately 10 nanoseconds and a fall time of approximately 10 nanoseconds with a pulse duration of 500 nanoseconds can be utilized.
In
The thickness of 120—the vanadium dioxide ultra thin-film is less than 0.1 microns.
120—the vanadium dioxide ultra thin-film is approximately in the range of 0.01 microns2 to 2 microns2 in area on 140A—the left region.
120—the vanadium dioxide ultra thin-film is approximately in the range of 0.01 microns2 to 2 microns2 in area on 140B—the right region.
It should be noted by nanoscaling the area of 120—the vanadium dioxide ultra thin-film in the range of approximately 0.01 microns2, an ultrafast (approximately 0.1 nanoseconds) optical switch (activated by an electrical pulse) can be realized.
The ridge width and ridge depth of 200—the optical waveguide in 140A—the left region are approximately in the range of 2 microns to 5 microns and 0.1 microns to 1 micron respectively. Furthermore, both ends of 200—the optical waveguide in 140A—the left region can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
The ridge width and ridge depth of 200—the optical waveguide in 140B—the right region are approximately in the range of 2 microns to 5 microns and 0.1 microns to 1 micron respectively. Furthermore, both ends of 200—the optical waveguide in 140B—the right region can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
The distance between 140A—the left region and 140B—the right region is at or less than 5 microns.
100A—the fast optical switch is a 2×2 fast optical switch with two inputs and two outputs.
The fabrication process of 100A—the fast optical switch (in a directional coupler configuration) is outlined below, when 120—the vanadium dioxide is an ultra thin-film.
Deposition of 120—the vanadium dioxide ultra thin-film of less than 0.1 microns in thickness by radio frequency (RF) magnetron sputtering from vanadium dioxide target under argon gas flow (approximately 100 sccm) and oxygen gas flow (approximately 10 sccm) at approximately in the range of 300 degrees centigrade to 550 degrees centigrade on a silicon-on-insulator substrate, having silicon layer thickness of about in the range of 0.1 microns to 0.5 microns, having insulator (silicon dioxide) layer thickness of about in the range of 0.25 micron to 3 microns, having substrate thickness of about in the range of 350 microns to 675 microns.
Alternatively, direct current (DC) magnetron sputtering from vanadium target under suitable argon gas flow and oxygen gas flow at approximately in the range of 300 degrees centigrade to 550 degrees centigrade can be utilized to deposit 120—the vanadium dioxide ultra thin-film.
Alternatively, electron beam evaporation or laser assisted electron beam evaporation from high purity form of divanadium tetroxide (V2O4) powder can be utilized to deposit 120—the vanadium dioxide ultra thin-film.
Alternatively, a low-temperature atomic layer epitaxial (ALE) process can be utilized to deposit 120—the vanadium dioxide ultra thin-film.
Alternatively, a low-temperature molecular beam epitaxy (MBE) process can be utilized to deposit 120—the vanadium dioxide ultra thin-film.
Additionally, thermal annealing/rapid thermal annealing (RTA) process under suitable argon gas flow and oxygen gas flow can be utilized to enhance grain size and correct any oxygen deficiency of 120—the vanadium dioxide ultra thin-film.
Additionally, an ultra thin-film aluminum oxide in the range of 0.010 microns to 0.015 microns in thickness, as a buffer layer prior to any deposition of 120—the vanadium dioxide ultra thin-film can lead to improved crystallinity and textures in 120—the vanadium dioxide ultra thin-film.
Furthermore, deposition of an ultra thin-film aluminum oxide in the range of 0.010 microns to 0.015 microns in thickness as a protective layer on 120—the vanadium dioxide ultra thin-film can be beneficial for future fabrication/processing steps.
Reactive ion or ion etching of 120—the vanadium dioxide ultra thin-film and the silicon layer (of the silicon-on-insulator substrate) to approximately in the range of 2 microns to 5 microns in width and approximately in the range of 0.1 microns to 1 micron in depth to form 200—an optical waveguide in 140A—the left region and its continued curved structure. Furthermore, the both ends of 200—the optical waveguide can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
Similarly, reactive ion or ion etching of 120—the vanadium dioxide ultra thin-film and the silicon layer (of the silicon-on-insulator substrate) to approximately in the range of 2 microns to 5 microns in width and approximately in the range of 0.1 microns to 1 micron in depth to form 200—an optical waveguide in 140B—the right region and its continued curved structure. Furthermore, the both ends of 200—the optical waveguide can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
Electron beam lithography and lift off of:
The thickness of the first metal layer of titanium/chromium is approximately in the range of 0.010 microns to 0.02 microns.
The thickness of the second metal layer of gold is approximately in the range of 0.25 microns to 0.35 microns. It should be noted that thickness of the second metal layer of gold can be optimized to reduce stress on 120—the vanadium dioxide ultra thin-film in mitigating stability/reliability issues with 120—the vanadium dioxide ultra thin-film.
Furthermore, a high dielectric constant insulator (e.g., hafnium silicate, zirconium silicate, hafnium dioxide and zirconium dioxide) of approximate thickness of 0.005 microns can be fabricated/constructed to electrically insulate two electrodes on 140A—the left region and two electrodes on 140B—the right region from 120—the vanadium dioxide ultra thin-film.
Alternatively, a parallel plate capacitor with an air gap can be utilized instead of a high dielectric constant insulator. When a voltage pulse is applied across electrodes on a parallel plate capacitor, an electric field due to the voltage pulse is established across the air gap and a smaller electric field due to the voltage pulse is then coupled with 120—the vanadium dioxide ultra thin-film.
It should be noted that the above fabrication steps can be modified in a number of ways (e.g., self alignment and/or planarization) for not heating adjacent silicon, as heating adjacent silicon can undesirably slow the switching speed of 100A—the optical switch.
Dicing, testing and single-mode optical fiber pigtailing of 100A—the fast optical switch chips.
Connecting the tested/pigtailed good 100A—the fast optical switch chips onto a printed electronics circuit board.
In
However, the input wavelength at 180A—the first input port can exit via 220B—an output exit, when 140A—the left region comprising 120—the vanadium dioxide ultra thin-film is electrically activated by an electrical pulse on both 160A1—the left metal electrode and 160A2—the right metal electrode on 120—the vanadium dioxide ultra thin-film (on 140A—the left region) just to induce insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
Similarly, the input wavelength at 180B—the second input port can exit via 200A—an output exit, when 140B—the right region comprising 120—the vanadium dioxide ultra thin-film is electrically activated by an electrical pulse on both 160B1—the left metal electrode and 160B2—the right metal electrode on 120—the vanadium dioxide ultra thin-film (on 140B—the right region) just to induce insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
120—the vanadium dioxide ultra thin-film is receiving an electrical pulse just to induce insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
Other coupler configurations (e.g., multimode interference configuration) can be realized by an electrical pulse for just inducing insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
It should be noted that a cluster of vanadium dioxide particles (less than 0.5 microns in diameter) embedded in an ultra thin-film of a polymeric material or in a mesh of metal nanowires can be utilized, instead of 120—the vanadium dioxide ultra thin-film in fabricating/constructing 100A—the fast optical switch, activated by an electrical pulse. The polymeric material can be either conducting, semiconducting or non-conducting. Thus, vanadium dioxide particles (less than 0.5 microns in diameter) embedded in an ultra thin-film of a polymeric material or in a mesh of metal nanowires can receive an electrical pulse just to induce insulator-to-metal phase transition in the cluster of vanadium dioxide particles (less than 0.5 microns in diameter).
Furthermore, 120—the vanadium dioxide ultra thin-film can be replaced by a monolayer(s) of a two-dimensional (2-D) material (e.g., germanene, graphene, phosphorene, silicene and stanene) first, then followed by the vanadium dioxide ultra thin-film last (option 1) or the vanadium dioxide ultra thin-film first, then followed by a monolayer(s) of a two-dimensional material last (option 2) or a monolayer(s) of a two-dimensional material first, then followed by the vanadium dioxide ultra thin-film in middle, then followed by a monolayer(s) of a two-dimensional material last (option 3). Integration of a monolayer(s) of a two-dimensional material can enable at least faster heat dissipation and/or electronic properties of the entire stacked materials for faster off switching time. The total thickness of vanadium dioxide ultra thin-film and a monolayer(s) of a two-dimensional (2-D) material is less than 0.15 microns. It should be noted that the two-dimensional material and/or vanadium dioxide can be in the form a quantum dot(s). It should be noted that vanadium dioxide can be also doped (e.g., tungsten metal).
Furthermore, the silicon layer of the silicon-on-insulator substrate can be reactive ion or ion etched up to the silica layer of the silicon-on-insulator substrate.
In
300A—the electronic subsystem integrates 240, 260 and 280A. 300A—the electronic subsystem is to drive 100A—the fast optical switch.
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array.
In
Thus, 400A—the fast optical switch processor A can switch a wavelength from any input fiber to any output fiber in less than 10 nanoseconds.
In
The thickness of 120—the vanadium dioxide ultra thin-film is less than 0.1 microns.
120—the vanadium dioxide ultra thin-film is approximately in the range of 0.01 microns2 to 2 microns2 in area on 140A—the left region.
120—the vanadium dioxide ultra thin-film is approximately in the range of 0.01 microns2 to 2 microns2 in area on 140B—the right region.
It should be noted by nanoscaling the area of 120—the vanadium dioxide ultra thin-film in the range of approximately 0.01 microns2, an ultrafast (approximately 0.1 nanoseconds) optical switch (activated by a light pulse) can be realized.
The ridge width and ridge depth of 200—the optical waveguide in 140A—the left region are approximately in the range of 2 microns to 5 microns and 0.1 microns to 1 micron respectively. Furthermore, both ends of 200—the optical waveguide in 140A—the left region can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
The ridge width and ridge depth of 200—the optical waveguide in 140B—the right region are approximately in the range of 2 microns to 5 microns and 0.1 microns to 1 micron respectively. Furthermore, both ends of 200—the optical waveguide in 140B—the right region can be tapered out gradually for optical mode matching for higher % single-mode optical fiber coupling.
The distance between 140A—the left region and 140B—the right region is at or less than 5 microns.
100B—the fast optical switch is a 2×2 fast optical switch with two inputs and two outputs.
In
However, the input wavelength at 180A—the first input port can exit via 220B—the output exit, when 140A—the left region comprising 120—the vanadium dioxide ultra thin-film is optically activated by a light pulse (e.g., a light pulse from a mode locked semiconductor laser) on 120—the vanadium dioxide ultra thin-film on 140A—the left region just to induce insulator-to-metal phase transition on 120—the vanadium dioxide ultra thin-film.
Similarly, the input wavelength at 180B—the second input port can exit via 200A—the output exit, when 140B—the right region comprising 120—the vanadium dioxide ultra thin-film is optically activated by a light pulse (e.g., a light pulse from a mode locked semiconductor laser) on 120—the vanadium dioxide ultra thin-film on 140B—the right region just to induce insulator-to-metal phase transition on 120—the vanadium dioxide ultra thin-film.
The intensity (optical power per unit area) of the light pulse is approximately in the range of 0.1 mJ/cm2 to 50 mJ/cm2. The pulse width of the light pulse is approximately in the range of 0.001 nanoseconds to 0.1 nanoseconds.
120—the vanadium dioxide ultra thin-film is receiving a light pulse just to induce insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
The light pulse can propagate through 460—a waveguide and focused by 480—a lens 480 onto 120—the vanadium dioxide ultra thin-film.
However, either a focusing up configuration or a focusing down configuration is possible
460—the waveguide is fabricated/constructed on 440—a buffer layer, wherein 440—the buffer layer is fabricated/constructed on 420—a suitable substrate (e.g., a silicon-on-insulator substrate).
One pulsed light source is required for 140A—the left region, comprising 120—the vanadium dioxide ultra thin-film and another pulsed light source is required for 140B—the right region, comprising 120—the vanadium dioxide ultra thin-film.
Furthermore, 480—a metamaterial based lens can be utilized for focusing of the light pulse below the diffraction limit.
Other coupler configurations (e.g., multimode interference configuration) can be realized by a light pulse for just inducing insulator-to-metal phase transition in 120—the vanadium dioxide ultra thin-film.
It should be noted that a cluster of vanadium dioxide particles (less than 0.5 microns in diameter) embedded in an ultra thin-film of a polymeric material or in a mesh of metal nanowires can be utilized, instead of 120—the vanadium dioxide ultra thin-film in fabricating/constructing 100A—the fast optical switch, activated by a light pulse. The polymeric material can be either conducting, semiconducting or non-conducting. Thus, vanadium dioxide particles (less than 0.5 microns in diameter) embedded in an ultra thin-film of a polymeric material or in a mesh of metal nanowires can receive a light pulse just to induce insulator-to-metal phase transition in the cluster of vanadium dioxide particles (less than 0.5 microns in diameter).
Furthermore, 120—the vanadium dioxide ultra thin-film can be replaced by a monolayer(s) of a two-dimensional (2-D) material (e.g., germanene, graphene, phosphorene, silicene and stanene) first, then followed by the vanadium dioxide ultra thin-film last (option 1) or the vanadium dioxide ultra thin-film first, then followed by a monolayer(s) of a two-dimensional material last (option 2) or a monolayer(s) of a two-dimensional material first, then followed by the vanadium dioxide ultra thin-film in middle, then followed by a monolayer(s) of a two-dimensional material last (option 3). Integration of a monolayer(s) of a two-dimensional material can enable at least faster heat dissipation and/or electronic properties of the entire stacked materials for faster off switching time. The total thickness of vanadium dioxide ultra thin-film and a monolayer(s) of a two-dimensional (2-D) material is less than 0.15 microns.
In
300B—the electronic subsystem integrates 240, 260 and 280B 300B—the electronic subsystem is to drive 100B—the fast optical switch (based on 120—the vanadium ultra thin-film dioxide, activated by a light pulse).
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array.
In
Thus, 400B—the fast optical switch processor B can switch a wavelength from any input fiber to any output fiber in less than 10 nanoseconds.
In
It should be noted that a semiconductor optical amplifier can be utilized instead of 500—the erbium doped waveguide amplifier integrated with a 980-nm pump laser 500.
It should be noted that arrayed waveguide gratings (AWG) based wavelength multiplexer/demultiplexer can also be utilized.
560A denotes a fixed (wavelength) demultiplexer, 560B denotes a (wavelength) tunable demultiplexer and 560C denotes a (wavelength) tunable one-dimensional (1-D) photonic crystal based demultiplexer.
An array of rapidly wavelength tunable lasers can provide a set of new wavelengths to add ports. The output (wavelengths) of 560A/560B/560C—the second wavelength demultiplexer 2 and these newly added wavelengths can be switched by an array of 100As—the fast optical switches.
Switched wavelengths from 100As—the fast optical switches can be modulated by 580s—optical modulators (e.g., silicon traveling-waveguide/graphene-on-silicon optical modulators).
The optical power output of 580—the optical modulator can be controlled by 500—the erbium doped waveguide amplifier integrated with a 980-nm pump laser, 600—a variable optical attenuator (VOA) (e.g., PLZT based variable optical attenuator) and 620—a photodiode.
The modulated wavelengths (or modulated optical signals) can be independently controlled at a specified optical power and then multiplexed by 640A/640B/640C—a multiplexer. Thus, an independent control of each wavelength can enable an approximately flat optical power curve for all output wavelengths at 380—an output optical fiber.
640A denotes a fixed (wavelength) multiplexer, 640B denotes a (wavelength) tunable multiplexer and 640C denotes a (wavelength) tunable one-dimensional photonic crystal based multiplexer.
A wavelength tunable multiplexer/demultiplexer includes a control circuit and one or more controls such as, heaters thermally coupled and/or refractive index changing electrical paths electrically coupled to waveguides of the multiplexer/demultiplexer.
The control circuit is in signal communication with the one or more controls and also includes a microprocessor/field programmable gate array coupled with an electronic memory component. The control circuit is to receive an identification signal and adjust the control in response to the identification signal and based on parameter values stored in the electronic memory component.
Alternatively, a voltage tunable multiplexer/demultiplexer can be realized when the material composition of the multiplexer/demultiplexer is a crystalline semiconductor (e.g., indium phosphide) rather than silica. Furthermore, the transmission characteristics of the tunable multiplexer/demultiplexer can be varied depending on external control input(s).
In
300C—the electronic subsystem integrates 240, 260 and 280C. 300C—the electronic subsystem is to drive 660A.
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array.
In
Thus, 680A—the optical network processor system A, demultiplex, multiplex and switch a wavelength from any input fiber to any output fiber.
In
An array of rapidly wavelength tunable lasers can provide a set of new wavelengths to the add ports. The output (wavelengths) of 560A/560B/560C—the second wavelength demultiplexer 2 and these newly added wavelengths can be switched by an array of 100Bs-the fast optical switches.
Switched wavelengths from 100Bs—the fast optical switches can be modulated by an array of 580s—the optical modulators.
The optical power output of 580—the optical modulator can be controlled by 500—the erbium doped waveguide amplifier integrated with a 980-nm pump laser, 600—the variable optical attenuator and 620—the photodiode.
The modulated wavelengths (or modulated optical signals) can be independently controlled at a specified optical power and then multiplexed by 640A/640B/640C—the multiplexer. Thus, an independent control of each wavelength can enable an approximately flat optical power curve for all output wavelengths at 380—the output optical fiber.
In
300D—the electronic subsystem integrates 240, 260 and 280D. 300D—the electronic subsystem is to drive 660B.
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array.
In
Thus, 680B—the optical network processor system B, demultiplex, multiplex and switch a wavelength from any input fiber to any output fiber.
Alternatively, a wavelength converter can be fabricated/constructed, utilizing a semiconductor optical amplifier or a quantum dot based semiconductor optical amplifier (QD-SOA).
In
An array of rapidly wavelength tunable lasers can provide a set of new wavelengths to the add ports. The output (wavelengths) of 560A/560B/560C—the second wavelength demultiplexer 2 can converted in wavelength by an array of 820A/B/Cs—the wavelength converters. Thus, the converted wavelengths from the array 820A/B/Cs—the wavelength converters and these newly added wavelengths can be switched by an array of 100As—the fast optical switches.
Switched wavelengths from 100As—the fast optical switches can be modulated by an array of 580s—the optical modulators.
The optical power output of 580—the optical modulator can be controlled by 500—the erbium doped waveguide amplifier integrated with a 980-nm pump laser, 600—the variable optical attenuator and 620—the photodiode
The modulated wavelengths (or modulated optical signals) can be independently controlled at a specified optical power and then multiplexed by 640A/640B/640C—the multiplexer. Thus, an independent control of each wavelength can enable approximately flat optical power curve for all output wavelengths at 380—the output optical fiber.
In
300E—the electronic subsystem integrates 240, 260 and 280E. 300E—the electronic subsystem is to drive 840A.
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array
In
Thus, 860A—the advanced optical network processor system C can demultiplex, multiplex, convert and switch a wavelength from any input fiber to any output fiber.
In
An array of rapidly wavelength tunable lasers can provide a set of new wavelengths to the add ports. The output (wavelengths) of 560A/560B/560C—the second wavelength demultiplexer 2 can converted in wavelength by an array of 820A/B/Cs—the wavelength converters. Thus, the converted wavelengths from the array 820A/B/Cs—the wavelength converters and these newly added wavelengths can be switched by an array of 100Bs—the fast optical switches.
Switched wavelengths from 100Bs—the fast optical switches can be modulated by an array of 580s—the optical modulators.
The optical power output of 580—the optical modulator can be controlled by 500—the erbium doped waveguide amplifier integrated with a 980-nm pump laser, 600—the variable optical attenuator and 620—the photodiode
The modulated wavelengths (or modulated optical signals) can be independently controlled at a specified optical power and then multiplexed by 640A/640B/640C—the multiplexer. Thus, an independent control of each wavelength can enable an approximately flat optical power curve for all output the wavelengths at 380—the output optical fiber.
In
300F—the electronic subsystem integrates 240, 260 and 280F. 300F—the electronic subsystem is to drive 840B.
240—the external controller can communicate serially with 260—the microprocessor/field programmable gate array
In
Thus, 860B—the advanced optical network processor system D can demultiplex, multiplex, convert and switch a wavelength from any input fiber to any output fiber.
100A/100B can be integrated with a semiconductor laser/widely tunable semiconductor laser/widely tunable fast switching semiconductor laser at 180A—the input waveguide and/or at 180B—the input waveguide for higher functionality. Such integration can include coupling from a waveguide to waveguide via a collimating lens, wherein the collimating lens can be suitably positioned by a microelectro-mechanical system (MEMS)/nanoelectro-mechanical system (NEMS) based actuator.
100A/100B can be integrated with an array of semiconductor laser/widely tunable semiconductor laser/widely tunable fast switching semiconductor laser at 180A—the input waveguide and/or at 180B—the input waveguide for higher functionality. Such integration can include coupling of the array of semiconductor laser/widely tunable semiconductor laser/widely tunable fast switching semiconductor laser to 180A—the input waveguide and/or at 180B—the input waveguide via a microelectromechanical system/nanoelectromechanical system based tilt mirror.
400A, 400B, 680A, 680B, 860A and 860B can be integrated with microring resonator filters and/or wavelength tunable optical dispersion compensators.
Furthermore, 400A, 400B, 680A, 680B, 860A and 860B can be integrated with biplexer filters and/or triplexer filters.
400A or 400B can be integrated with log2N demultiplexer for an optical packet switched optical networks, where the switching delay is critical for high performance. A log2N demultiplexer can consist of rectangular shaped periodic frequency filters connected in series, wherein the rectangular shaped periodic frequency filters can be formed in one dimensional photonic crystal structure on a ridge waveguide.
Flip-chip bonding was developed as an alternative to wirebonding. In flip-chip bonding, components are flipped upside-down and placed on an array of solder bumps that form the connection between a device and circuit. 400A, 400B, 680A, 680B, 860A and 860B can be packaged, utilizing flip-chip bonding onto a precise silicon-on-insulator substrate.
Single-mode optical fibers can be aligned passively with precise metal alignment pins seated into v-grooves on the precise substrate. The precise metal alignment pins can be utilized top mate with a pluggable optical fiber connector integrated with a molded plastic lens. Alternatively, an array of multi-mode optical fibers can be used instead of an array of single-mode optical fibers for short distance (e.g., LAN) applications.
In the above disclosed specifications “/” has been used to indicate an “or” and real-time means near real-time in practice.
Any example in the above disclosed specifications is by way of an example only and nut by way of any limitation.
The best mode requirement “requires an inventor(s) to disclose the best mode contemplated by him/her, as of the time he/she executes the application, of carrying out the invention.” “ . . . [T]he existence of a best mode is a purely subjective matter depending upon what the inventor(s) actually believed at the time the application was filed.” See Bayer AG v. Schein Pharmaceuticals, Inc. The best mode requirement still exists under the America Invents Act (AIA). At the time of the invention, the inventor(s) described preferred best mode embodiments of the present invention. The sole purpose of the best mode requirement is to restrain the inventor(s) from applying for a patent, while at the same time concealing from the public preferred embodiments of their inventions, which they have in fact conceived. The best mode inquiry focuses on the inventor(s)' state of mind at the time he/she filed the patent application, raising a subjective factual question. The specificity of disclosure required to comply with the best mode requirement must be determined by the knowledge of facts within the possession of the inventor(s) at the time of filing the patent application. See Glaxo, Inc. v. Novopharm LTD., 52 F.3d 1043, 1050 (Fed. Cir. 1995).
The above disclosed specifications are the preferred best mode embodiments of the present invention. However, they are not intended to be limited only to the preferred best mode embodiments of the present invention. Numerous variations and/or modifications are possible within the scope of the present invention. Accordingly, the disclosed preferred best mode embodiments are to be construed as illustrative only. Those who are skilled in the art can make various variations and/or modifications (e.g., a light emitting diode instead of a laser, or electrically/wirelessly coupled instead of electrically/wirelessly connected, or a cloud based storage unit instead of a cloud based server, whenever it is applicable) without departing from the scope and spirit of this invention. It should be apparent that features of one embodiment can be combined with one or more features of another embodiment to form a plurality of embodiments. The inventor(s) of the present invention is not required to describe each and every conceivable and possible future embodiment in the preferred best mode embodiments of the present invention. See SRI Int'l v. Matsushita Elec. Corp. of America, 775F.2d 1107, 1121, 227 U.S.P.Q. (BNA) 577, 585 (Fed. Cir. 1985) (enbanc). The scope and spirit of this invention shall be defined by the claims and the equivalents of the claims only. The exclusive use of all variations and/or modifications within the scope of the claims is reserved. The general presumption is that claim terms should be interpreted using their plain and ordinary meaning. See Oxford Immunotec Ltd. v. Qiagen, Inc. et al., Action No. 15-cv-13124-NMG. Unless a claim term is specifically defined in the preferred best mode embodiments, then a claim term has an ordinary meaning, as understood by a person with an ordinary skill in the art, at the time of the present invention. As noted long ago: “Specifications teach. Claims claim”. See Rexnord Corp. v. Laitram Corp., 274 F.3d 1336, 1344 (Fed. Cir. 2001). The rights of claims (and rights of the equivalents of the claims under the Doctrine of Equivalents-meeting the “Triple Identity Test” (a) performing substantially the same function, (b) in substantially the same way and (c) yielding substantially the same result. See Crown Packaging Tech., Inc. v. Rexam Beverage Can Co., 559 F.3d 1308, 1312 (Fed. Cir. 2009)) of the present invention are not narrowed or limited by the selective imports of the specifications (of the preferred embodiments of the present invention) into the claims. The term “means” was not used nor intended nor implied in the disclosed preferred best mode embodiments of the present invention. Thus, the inventor(s) has not limited the scope of the claims as mean plus function. Additionally, “apparatus claims are not necessarily indefinite for using functional language . . . [f]unctional language may also be employed to limit the claims without using the means-plus-function format.” See Microprocessor Enhancement Corp. v. Texas Instruments Inc.
This application claims the benefit of priority from U.S. Provisional Patent Application No. 62/498,246 (“the '246 provisional patent application”) entitled, “FAST OPTICAL SWITCH AND ITS APPLICATIONS IN OPTICAL COMMUNICATION” filed on Dec. 20, 2016. The present application is a continuation-in-part (CIP) of (a) U.S. Non-Provisional patent application Ser. No. 14/756,096 entitled, “FAST OPTICAL SWITCH AND ITS APPLICATIONS IN OPTICAL COMMUNICATION” filed on Aug. 1, 2015, which (a) claims the benefit of priority from U.S. Provisional Patent Application No. 61/999,601 (“the '601 provisional patent application”) entitled, “FAST OPTICAL SWITCH” filed on Aug. 1, 2014. The entire contents of all Non-Provisional Patent Applications and Provisional Patent Applications as listed in the previous paragraph and the filed Application Data Sheet (ADS) are hereby incorporated by reference.
| Number | Date | Country | |
|---|---|---|---|
| 62498246 | Dec 2016 | US | |
| 61999601 | Aug 2014 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 14756096 | Aug 2015 | US |
| Child | 15731683 | US |
