Electromagnetic waves or electromagnetic radiation (EMR) is a form of energy that has both electric and magnetic field components. Electromagnetic waves can have many different frequencies.
Modern telecommunication systems manipulate electromagnetic waves in the electromagnetic spectrum in order to provide wireless communications to subscribers of the telecommunication systems. In particular, modern telecommunication systems manipulate those waves having a frequency categorizing them as Radio Frequency (RF) waves. In order to utilize RF waves, telecommunication systems utilize certain essential hardware components, such as filters, mixers, amplifiers, and antennas.
The technology described herein relates to a radio frequency (RF) conductive medium for improving the conductive efficiency of an RF device. The RF conductive medium improves the conductive efficiency of the RF device by including one or more conductive pathways in a transverse electromagnetic axis that is free from the loss inducing impact of skin effect at the radio frequencies of interest.
One embodiment is a radio frequency (RF) conductive medium that includes a diversity of conductive media forming a plurality of continuous conductive pathways in a transverse electromagnetic axis. The RF conductive medium also includes a suspension dielectric periodically surrounding each of the plurality of continuous conductive pathways in the transverse electromagnetic axis. The suspension dielectric is configured to periodically insulate each of the plurality of conductive pathways from propagating RF energy in an axis perpendicular to the transverse electromagnetic axis. The suspension dielectric is further configured to provide mechanical support for each of the plurality of continuous conductive pathways.
In an embodiment, each of the plurality of continuous conductive pathways may be a conductive layer in a plurality of conductive layers of conductive pathways. Each of the plurality of conductive layers may be structured and have uniform position or arrangement with respect to other layers of the plurality of conductive layers. In another embodiment, each of the plurality of conductive layers may be unstructured and have a mesh arrangement with respect to other layers of the plurality of conductive layers.
In some embodiments, the transverse electromagnetic axis is an axis parallel to a surface upon which the RF conductive medium is applied. In other embodiments the transverse electromagnetic axis is an axis that is coplanar to a surface upon which the RF conductive medium is applied.
The RF conductive medium may also include a solvent configured to maintain the RF conductive medium in a viscous state during application of the RF conductive medium onto a dielectric surface. The solvent is configured to evaporate in response to being stimulated by a heat source.
Each medium of the diversity of conductive media may be made of a nanomaterial composed of an element that is at least one of: silver, copper, aluminum, and gold. Also, each medium of the diversity of conductive media may have a structure that is at least one of: wire, ribbon, tube, and flake.
In addition, each of the plurality of continuous conductive pathways may have a conductive cross-sectional area no greater than skin depth at a desired frequency of operation. In an embodiment, the skin depth “δ” may be calculated by:
where u0 is the permeability of a vacuum, ur is the relative permeability of a nanomaterial of the conductive media, p is the resistivity of the nanomaterial of the conductive media, and f is the desired frequency of operation.
The desired frequency of operation may correspond to at least one of: a desired resonant frequency of a cavity filter, a desired resonant frequency of an antenna, a cutoff frequency of a waveguide, a desired operational frequency range of a coaxial cable, and combined operational frequency ranges of an integrated structure including a cavity filter and an antenna.
Each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 50 nm-4000 nm. In other examples, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1000 nm-3000 nm. In yet another example, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1500 nm-2500 nm.
The RF conductive medium may also include a protective layer covering the plurality of layers of continuous conductive pathways, where the protective layer includes a material that is non-conductive and minimally absorptive to RF energy at a desired frequency of operation. The material may be at least one of: a polymer coating and fiberglass coating.
Another embodiment is a radio frequency (RF) conductive medium that includes a diversity of conductive media forming a plurality of continuous conductive pathways. Each medium of the conductive media is made of a material that is conductive in a transverse electromagnetic axis and weakly conductive in an axis perpendicular to the transverse electromagnetic axis. The RF conductive medium also includes a layer of RF inert material surrounding the diversity of conductive media.
The RF inert material is non-conductive and minimally absorptive to RF energy at a desired frequency of operation. Also, the layer of RF inert material is configured to secure the diversity of conductive media onto a dielectric surface. The RF inert material may be at least one of: a polymer coating and fiberglass coating.
The RF conductive medium may also include a binding agent to bind the RF conductive medium to the surface. The RF conductive medium may further include a solvent configured to maintain the RF conductive medium in a viscous state during application of the RF conductive medium onto the dielectric surface. The solvent further is configured to evaporate in response to being stimulated by a heat source.
Each medium of the diversity of conductive media may be made of a nanomaterial composed of an element that is at least one of: carbon and graphene. Also, each conductive medium in the diversity of conductive media may be at least one of: single walled carbon nanotubes (SWCNTs), multi-walled carbon nanotubes (MWCNTs), and graphene.
In addition, each of the plurality of continuous conductive pathways may have a conductive cross-sectional area no greater than skin depth at a desired frequency of operation. In an embodiment, the skin depth “δ” may be calculated by:
where u0 is the permeability of a vacuum, ur is the relative permeability of a nanomaterial of the conductive media, p is the resistivity of the nanomaterial of the conductive media, and f is the desired frequency of operation.
The desired frequency of operation may correspond to at least one of: a desired resonant frequency of a cavity filter, a desired resonant frequency of an antenna, a cutoff frequency of a waveguide, a desired operational frequency range of a coaxial cable, and combined operational frequency ranges of an integrated structure including a cavity filter and an antenna.
Each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 50 nm-4000 nm. In other examples, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1000 nm-3000 nm. In yet another example, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1500 nm-2500 nm.
A further embodiment is a radio frequency (RF) conductive medium. The RF conductive medium includes a bundle of discrete electrically conductive nanostructures. In addition, the RF conductive medium includes a bonding agent enabling the bundle of discrete conductive nanostructures to be applied to a dielectric surface. The bundle of discrete conductive nanostructures form a continuous conductive layer having a uniform lattice structure and uniform conductive cross-sectional area in response to being sintered by a heat source. The heat source may apply a stimulation of heat based on an atomic structure and thickness of nanomaterial of each discrete conductive nanostructure of the bundle of discrete conductive nanostructures.
Each of the nanostructures may be made of a nanomaterial that is composed of an element that is at least one of: carbon, silver, copper, aluminum, and gold. Also, each of the discrete conductive nanostructures may be a conductive structure that is at least one of: wire, ribbon, tube, and flake.
The continuous conductive layer may have a uniform conductive cross-sectional area that is no greater than a skin depth at a desired frequency of operation. In an embodiment, the skin depth “δ” may be calculated by:
where μ0 is the permeability of a vacuum, μr is the relative permeability of a nanomaterial of the nanostructure, p is the resistivity of the nanomaterial of the nanostructure, and f is a desired frequency of operation.
The desired frequency of operation may correspond to at least one of: a desired resonant frequency of a cavity filter, a desired resonant frequency of an antenna, a cutoff frequency of a waveguide, a desired operational frequency range of a coaxial cable, and combined operational frequency ranges of an integrated structure including a cavity filter and an antenna.
The continuous conductive layer may have a uniform conductive cross-sectional area having a skin depth of 50 nm-4000 nm. In other examples, the continuous conductive layer may have a uniform conductive cross-sectional area having a skin depth of 1000 nm-3000 nm. In yet another example, the continuous conductive layer may have a uniform conductive cross-sectional area having a skin depth of 1500 nm-2500 nm.
The dielectric surface may have a surface smoothness free from irregularities greater than a skin depth in size. In an embodiment, the dielectric surface may have a surface smoothness with irregularities having a depth no greater than a depth “δ” that is calculated by:
where u0 is the permeability of a vacuum, ur is the relative permeability of a nanomaterial of the nanostructure, p is the resistivity of the nanomaterial of the nanostructure, and f is a frequency (in Hz) of interest.
The RF conductive medium also includes a protective layer covering the continuous conductive layer. The protective layer includes a material that is non-conductive and minimally absorptive to RF energy at a desired frequency of operation. The material may be at least one of: a polymer coating and a fiberglass coating.
The dielectric surface may be an inner surface of a cavity having an internal geometry corresponding to a desired frequency response characteristic of the cavity. In another embodiment, the bundle of discrete nanostructures may be applied to an outer surface of a first dielectric surface and to a concentric inner surface of a second dielectric surface. The first dielectric surface is an inner conductor and the second dielectric surface is an outer conductor of a coaxial cable. Also, the bundle of discrete conductive nanostructures may be applied to a dielectric structure, where the geometry of the dielectric structure and conductive properties of the bundle of discrete conductive nanostructures define a resonant frequency response and radiation pattern of an antenna.
The foregoing will be apparent from the following more particular description of example embodiments of the disclosure, as illustrated in the accompanying drawings in which like reference characters refer to the same parts throughout the different views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating embodiments of the present disclosure.
A description of example embodiments of the disclosure follows.
Modern telecommunication systems manipulate electromagnetic waves having a range of wavelengths in the electromagnetic spectrum that categorize them as Radio Frequency (RF) waves. In order to utilize RF waves, telecommunication systems employ certain essential RF hardware components such as filters, mixers, amplifiers, and antennas.
The RF hardware components interact with the RF waves via RF conductive elements. The RF conductive elements are generally composed of an RF conductive medium, such as, aluminum, copper, silver, and gold. However, the structures of conventional RF conductive media suffer from effective electrical resistance that impedes the conduction of RF energy, introducing undesirable insertion loss into all RF hardware components and lowering the Q factor of specific RF hardware components like resonant cavity filters.
The principal physical mechanism for undesirable loss in the conduction of RF energy through RF hardware components is skin effect. Skin effect occurs due to counter-electromotive force in a conductor, which is a consequence of the alternating electron currents in the conductive medium induced by applied RF energy. As its name suggests, skin effect causes the majority of electron current to flow at the surface of the conductor, a region defined as the “skin depth.” Skin effect reduces the effective cross sectional area of a conductor, often to a small fraction of its physical cross section. The effective skin depth of a conductor is a frequency dependent quality, which is inversely proportional to wavelength. This means that the higher the frequency, the more shallow the skin depth and, by extension, the greater the effective RF conduction loss.
The technology described herein relates to a radio frequency (RF) conductive medium (hereinafter, “technology”) for reducing the RF conduction loss of an RF hardware component. The RF conductive medium created by this technology reduces the RF conduction loss of the RF device by frustrating the formation of counter-electromotive force in the conductor.
For context and without limitation, the technology herein is described in the context of an RF cavity resonator. However, it should be noted that the technology can be applied to any RF component requiring an RF conductive medium configured to interact with RF waves. For example, the RF component can be an antenna, waveguide, coaxial cable, and an integrated structure including a cavity filter and an antenna.
The Q factor of any resonant circuit or structure (e.g., cavity filter 101) measures the degree to which the resonant circuit or structure damps energy applied to it. Thus, Q factor may be expressed as a ratio of energy stored in the resonant circuit or structure to energy dissipated in the resonant circuit or structure per oscillation cycle. The less energy dissipated per cycle, the higher the Q factor. For example, the Q factor “Q” can be defined by:
where fr is resonant frequency of the circuit or structure.
The Q factor of the cavity filter 101 is influenced by two factors: (a) power losses in a dielectric medium 115 of the cavity filter 101 and (b) power losses in the walls 110a-n of the cavity filter 101. In practical applications of cavity resonator based filters such as cavity filter 101, the dielectric medium 115 is often air. Losses induced by air can be considered miniscule at the frequencies in the lower microwave spectrum commonly used for mobile broadband communications. Thus, conductor losses in the walls 110a-n of the cavity filter 101 contribute most to lower effective Q factor and higher insertion loss of the cavity filter 101.
For instance, the Q factor “Q” of the cavity filter 101 can be defined by:
where Qc is the Q factor of the cavity walls and Qd is the Q factor of the dielectric medium.
As stated above, the RF conduction losses of the dielectric medium (e.g., air) 115 is negligible because RF energy in the lower microwave spectrum is weakly interactive with air and other common cavity dielectrics. Thus, the RF conductivity of the walls 110a-n “Qc” of the cavity filter 101 contributes most to the quality factor “Q” of the cavity filter 101. The quality factor contribution of the RF conductivity of the walls 110a-n “Qc” can be defined by:
where k=wavenumber; n=dielectric impedance, Rs=surface resistivity of the cavity walls 110a-n, and a/b/d are physical dimensions of the cavity filter 101. Thus, an increasing value of surface resistivity “Rs” of the cavity walls 110a-n decreases the value of Qc, thereby, reducing the Q factor of the cavity filter 101.
In order to increase the Q factor of the cavity filter 101 and other RF device, embodiments of the present invention provide a RF conductive medium that reduces the surface resistivity “Rs” of RF conductive elements of RF devices such as the cavity filter 101.
The structural dielectric 210 is composed of a material with a low relative permittivity. Also, the material of the structural dielectric 210 has a high conformality potential. For instance, the material of the structure dielectric 210 enables the structural dielectric 210 to conform to complex and smoothly transitioning geometries. The material of the structural dielectric 210 also has high dimensional stability under thermal stress. For example, the material prevents the structural dielectric 210 from deforming under thermal stresses the cavity resonator may experience in typical operational environments. In another embodiment, the material of the structural dielectric 210 has high dimensional stability under mechanical stress such that the material prevents the structural dielectric 210 from denting, flexing, or otherwise mechanically deforming under mechanical stresses experienced in typical operational applications.
In addition, the structural dielectric 210 has an internal surface 211 with a high surface smoothness. In particular, the internal surface 211 is substantially free from surface irregularities. In an embodiment, the dielectric surface 211 may a surface smoothness with irregularities having a depth no greater than a depth “δ” at a desired frequency of operation of the radio frequency (RF) cavity resonator 200.
The cavity resonator 200 also includes an RF input port 230a and RF output port 230b. In an example, the RF input port 230a and RF output port 230b can be a SubMiniature version A (SMA) connector. The RF input port 230a and RF output port 230b can be made of an RF conductive material such as copper, gold, nickel, and silver.
The RF input port 230a is electrically coupled to a coupling loop 235a. The RF input port 230a receives an oscillating RF electromagnetic signal from an RF transmission medium such as a coaxial cable (not shown). In response to receiving the oscillating RF electromagnetic signal, the RF input port 230a via the coupling loop 235a radiates an oscillating electric and magnetic field (i.e., RF electromagnetic wave) corresponding to the received RF electromagnetic signal.
As stated herein, the cavity 216 has an internal geometry corresponding to a desired frequency response characteristic of the cavity resonator 200. In particular, the internal geometry reinforces a range of radio frequencies corresponding to the desired frequency response characteristic of the cavity resonator 200 and attenuates undesired radio frequencies. In addition, the cavity resonator 200 also includes a resonator element 220. The resonator element 220, in this example, is formed by the structural dielectric 210. However, it should be noted that the resonator element 220 can be a separate and distinct structure within the cavity resonator 200. The resonator element 220 has a resonant dimension and overall structural geometry that further reinforces desired radio frequencies and attenuates undesired radio frequencies.
The electromagnetic wave corresponding to the received RF electromagnetic signal induces a resonant mode or modes in the cavity 216. In doing so, the electromagnetic wave interacts with the RF conductive medium 205. In particular, the electromagnetic wave induces an alternating current (AC) in the RF conductive medium 205. As described herein, embodiments of the present disclosure provide an RF conductive medium 205 that has a structure and composition giving the RF conductive medium 205 a low effective surface conductive resistivity “Rs”. The low surface conductive resistivity “Rs” allows the RF conductive medium 205 to support resonant modes in the cavity 216 with a high level of efficiency, thereby increasing the quality factor “Q” of the cavity resonator 200.
The reinforced frequency of interest induces an AC signal in the coupling loop 235b. The AC signal is output from the cavity resonator 200 via the RF output 230b. The RF output 230b is electrically coupled to a transmission medium (not shown), which passes the AC signal to an RF hardware component such as an antenna or receiver.
The RF conductive medium 205 can also include a protective layer (e.g., layer 306 of
The RF conductive medium 305 includes a bundle of discrete electrically conductive nanostructures. Each of the nanostructures may be made of a nanomaterial that is composed of an element that is at least one of: carbon, silver, copper, aluminum, and gold. Also, each of the discrete conductive nanostructures may be a conductive structure that is at least one of: wire, ribbon, tube, and flake. The nanomaterial may have a sintering temperature that is a small fraction of a melting temperature of the material on a macro scale. For example, Silver (Ag) melts at 961° C., while nano Silver (Ag) may sinter well below 300° C.
In addition, the RF conductive medium 305 includes a bonding agent (not shown) enabling the bundle of discrete conductive nanostructures to be applied to a surface 345 of the structural dielectric 310. The bundle of discrete conductive nanostructures forms the continuous conductive layer 340 in response to being sintered by a heat source. The size of each of the discrete electrically conductive nanostructures may be chosen such that the continuous conductive layer 340 has a uniform conductive cross-sectional area that is no greater than a skin depth “δ” at a desired frequency of operation of the cavity resonator 200. The continuous conductive layer 340 has a uniform lattice structure and uniform conductive cross-sectional area. The heat source may apply a stimulation of heat based on an atomic structure and thickness of nanomaterial of each discrete conductive nanostructure of the bundle of discrete conductive nanostructures. For example, the temperature of heat applied by the heat source and the length of time the heat is applied is a function of the atomic structure and thickness of nanomaterial of each discrete conductive nanostructure of the bundle of discrete conductive nanostructures. Any heat source known or yet to be known in the art may be used.
As stated above, an RF electromagnetic wave induces an alternating current (AC) in the RF conductive medium 305. For AC, an influence of the structure's cross sectional area on AC resistance is radically different than for direct current (DC) resistance. For example, a direct current may propagate throughout an entire volume of a conductor; an alternating current (such as that produced by an RF electromagnetic wave) propagates only within a bounded area very close to a surface of the conductive medium. This tendency of alternating currents to propagate near the surface of a conductor is known as “skin effect.” In an RF device, such as the cavity resonator 200, skin effect reduces the usable conductive cross sectional area to an extremely thin layer at the surface of the cavity's inner structure. Thus, skin effect is at least one significant mechanism for RF conduction loss in a resonant cavity, reducing the cavity's Q factor.
Thus, the continuous conductive layer 340 may have a uniform conductive cross-sectional area that is no greater than a skin depth “δ” at a desired frequency of operation of a cavity resonator (e.g., the cavity resonator 200 of
where μ0 is the permeability of a vacuum, μr is the relative permeability of a nanomaterial of the nanostructure, p is the resistivity of the nanomaterial of the nanostructure, and f is the desired frequency of operation. Table 1 below illustrates an example application of EQN. 4 with respect to a set of radio frequencies. However, it should be noted that any other known or yet to be known method of determining skin depth “δ” can used in place of EQN. 4.
In an embodiment, the continuous conductive layer 340 may have a uniform conductive cross-sectional area having a skin depth of 50 nm-4000 nm. In another embodiment, the continuous conductive layer 340 may have a uniform conductive cross-sectional area having a skin depth of 1000 nm-3000 nm. In yet another example, the continuous conductive layer 340 may have a uniform conductive cross-sectional area having a skin depth of 1500 nm-2500 nm.
Each medium of the diversity of RF conductive media 470 is made of a nanomaterial composed of an element that is at least one of: silver, copper, aluminum, carbon, and graphene. In an example where the element is at least one of: silver, copper, and aluminum, each medium of the diversity of conductive media 470 has a structure that is at least one of wire, ribbon, tube, and flake. In an example where the element is at least one of: carbon and graphene, each conductive medium in the diversity of conductive media 470 is at least one of: single walled carbon nanotubes (SWCNTs), multi-walled nanotubes (MWCNTs), and graphene.
Also, each of the plurality of continuous conductive pathways 490a-n may have a conductive cross-sectional area no greater than skin depth at a desired frequency of operation of, for example, a cavity resonator (e.g., the cavity resonator 200 of
In an embodiment, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 50 nm-4000 nm. In other examples, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1000 nm-3000 nm. In yet another example, each of the plurality of continuous conductive pathways may have a uniform conductive cross-sectional area having a skin depth of 1500 nm-2500 nm.
It should be noted that the desired frequency of operation “f” may also correspond to at least one of: a desired resonant frequency of an antenna, a cutoff frequency of a waveguide, a desired operational frequency range of a coaxial cable, and combined operational frequency ranges of an integrated structure including a cavity filter and an antenna.
A suspension dielectric 460 periodically surrounds each of the plurality of the plurality of conductive pathways 490a-n in the transverse electromagnetic axis. In particular, the suspension dielectric 460 periodically insulates each of the plurality of conductive pathways 490a-n from propagating RF energy in the axis 475 (i.e., the axis perpendicular to the transverse electromagnetic axis 480). The suspension dielectric 460 can also be configured to provide mechanical support for each of the plurality of conductive pathways 490a-n.
In an example embodiment where each medium of the diversity of RF conductive media 470 is made of a nanomaterial composed of an element that is at least one of: silver, copper, and aluminum, the suspension dielectric 460 is composed of a structurally rigid and thermally stable material that is weakly interactive with RF energy at the desired frequency of operation.
In another example embodiment where each medium of the diversity of RF conductive media 470 is made of a nanomaterial composed of an element that is at least one of: carbon and graphene, the suspension dielectric 460 is air. In such a case, the suspension dielectric 460 can be composed of air because, for example, single walled carbon nanotubes (SWCNTs), multi-walled nanotubes (MWCNTs), and graphene are materials that are inherently conductive in the transverse electromagnetic axis 480 and weakly conductive in the axis 475.
In this example, the RF conductive medium 405 includes an RF transparent protective layer 450. The RF transparent protective layer 450 covers the plurality of continuous conductive pathways 490a-n. The protective layer 405 includes a material that is non-conductive and minimally absorptive to RF energy at a desired frequency of operation of, for example, a cavity resonator (e.g., the cavity resonator 200 of
The RF conductive medium 405 may also include a binding agent (not shown). The binding agent is configured to bind the RF conductive medium 405 to the surface 445 of the structural dielectric 410. In addition, the RF conductive medium 405 may also include a solvent (not shown). The solvent is configured to maintain the RF conductive medium 405 in a viscous state during application of the RF conductive medium 405 onto the surface 445. The solvent is further configured to evaporate in response to being stimulated by a heat source. The heat source, in an example, can be an ambient temperature of air surrounding the RF conductive medium 405.
In order for the alternating current to only predominately travel in the transverse electromagnetic axis 480 along each of the pathways 490a-n, the suspension dielectric 460 periodically surrounds each of the plurality of conductive pathways 490a-n. In particular, the suspension dielectric periodically insulates each of the plurality of conductive pathways 490a-n from propagating RF energy (e.g., alternating current), in the axis 475. At certain points, for example point 495, the suspension dielectric 460 provides avenues for the RF energy to pass from one pathway (e.g., pathway 409b) to another pathway (e.g., pathway 490n).
In embodiments where each of the continuous conductive pathways 490a-n, as described above, has a conductive cross-sectional area no greater than a skin depth “δ” at a desired frequency of operation of an RF device (e.g., the cavity resonator 200 of
A diversity of conductive media is structured and periodically arranged to form a structured arrangement of the plurality of continuous conductive pathways 590. Each of the plurality of continuous conductive pathways 590 is periodically insulated from a neighboring continuous conductive pathway by a dielectric medium 560 (e.g., a suspension dielectric 460 of
In embodiments where each of the continuous conductive pathways 590, as described above, has a conductive cross-sectional area no greater than a skin depth “δ” at a desired frequency of operation of an RF device (e.g., the cavity resonator 200 of
The teachings of all patents, published applications and references cited herein are incorporated by reference in their entirety.
While this disclosure has been particularly shown and described with references to example embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the scope of the disclosure encompassed by the appended claims.
This application is continuation of U.S. application Ser. No. 15/016,632, filed on Feb. 5, 2016, which is continuation of U.S. application Ser. No. 14/706,707, now U.S. Pat. No. 9,893,404, filed on May 7, 2015, which is a divisional of U.S. application Ser. No. 13/872,679, now U.S. Pat. No. 9,166,268, filed on Apr. 29, 2013, which in turn claims the benefit of both U.S. Provisional Application No. 61/782,629, filed on Mar. 14, 2013, and U.S. Provisional Application No. 61/640,784, filed on May 1, 2012. The entire teachings of the above applications are incorporated herein by reference.
Number | Date | Country | |
---|---|---|---|
61782629 | Mar 2013 | US | |
61640784 | May 2012 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 16253395 | Jan 2019 | US |
Child | 17119013 | US | |
Parent | 13872679 | Apr 2013 | US |
Child | 14706707 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 15986044 | May 2018 | US |
Child | 16253395 | US | |
Parent | 15016632 | Feb 2016 | US |
Child | 15986044 | US | |
Parent | 14706707 | May 2015 | US |
Child | 15016632 | US |