The disclosures of the above applications are hereby incorporated by reference as part of the specification of this application.
This document relates to Composite Right/Left Handed (CRLH) Metamaterial (MTM) antenna apparatus.
The propagation of electromagnetic waves in most materials obeys the right-hand rule for the (E,H,β) vector fields, which denotes the electrical field E, the magnetic field H, and the wave vector β (or propagation constant). The phase velocity direction is the same as the direction of the signal energy propagation (group velocity) and the refractive index is a positive number. Such materials are Right-Handed (RH) materials. Most natural materials are RH materials; artificial materials can also be RH materials.
A metamaterial is an artificial structure. When designed with a structural average unit cell size ρ much smaller than the wavelength of the electromagnetic energy guided by the metamaterial, the metamaterial behaves like a homogeneous medium to the guided electromagnetic energy. Unlike RH materials, a metamaterial may exhibit a negative refractive index, wherein the phase velocity direction is opposite to the direction of the signal energy propagation where the relative directions of the (E,H,β) vector fields follow a Left-Hand (LH) rule. Metamaterials that support only a negative index of refraction while at the same time having negative permittivity ∈ and negative permeability μ are referred to as pure LH metamaterials.
Many metamaterials are mixtures of LH metamaterials and RH materials and thus are CRLH metamaterials. A CRLH MTM can behave like an LH metamaterial at low frequencies and an RH material at high frequencies. Implementations and properties of various CRLH MTMs are described in, for example, Caloz and Itoh, “Electromagnetic Metamaterials: Transmission Line Theory and Microwave Applications,” John Wiley & Sons (2006). CRLH MTMs and their applications in antennas are described by Tatsuo Itoh in “Invited paper: Prospects for Metamaterials,” Electronics Letters, Vol. 40, No. 16 (August, 2004).
CRLH MTMs can be structured and engineered to exhibit electromagnetic properties that are tailored for specific applications and can be used in applications where it may be difficult, impractical or infeasible to use other materials. In addition, CRLH MTMs may be used to develop new applications and to construct new devices that may not be possible with RH materials.
This application describes, among others, techniques, apparatus and systems that use composite left and right handed (CRLH) metamaterial structures to combine and divide electromagnetic signals and multiple pole multiple throw switch devices that are based on these structures.
A pure LH material follows the left hand rule for the vector trio (E,H,β) and the phase velocity direction is opposite to the signal energy propagation. Both the permittivity and permeability of the LH material are negative. A CRLH Metamaterial can exhibit both left hand and right hand electromagnetic modes of propagation depending on the regime or frequency of operation. Under certain circumstances, a CRLH metamaterial can exhibit a non-zero group velocity when the wavevector of a signal is zero. This situation occurs when both left hand and right hand modes are balanced. In an unbalanced mode, there is a bandgap in which electromagnetic wave propagation is forbidden. In the balanced case, the dispersion curve does not show any discontinuity at the transition point of the propagation constant β(ωo)=0 between the Left and Right handed modes, where the guided wavelength is infinite λg=2π/|β|→∞ while the group velocity is positive:
This state corresponds to the Zeroth Order mode m=0 in a Transmission Line (TL) implementation in the LH handed region. The CRHL structure supports a fine spectrum of low frequencies with a dispersion relation that follows the negative β parabolic region which allows a physically small device to be built that is electromagnetically large with unique capabilities in manipulating and controlling near-field radiation patterns. When this TL is used as a Zeroth Order Resonator (ZOR), it allows a constant amplitude and phase resonance across the entire resonator. The ZOR mode can be used to build MTM-based power combiners and splitters or dividers, directional couplers, matching networks, and leaky wave antennas. Examples of MTM-based power combiners and dividers are described below.
In RH TL resonators, the resonance frequency corresponds to electrical lengths θm=βml=mπ (m=1, 2, 3, . . . ), where l is the length of the TL. The TL length should be long to reach low and wider spectrum of resonant frequencies. The operating frequencies of a pure LH material are at low frequencies. A CRLH metamaterial structure is very different from RH and LH materials and can be used to reach both high and low spectral regions of the RF spectral ranges of RH and LH materials. In the CRLH case θm=βml=mπ, where l is the length of the CRLH TL and the parameter m=0, ±1, ±2, ±3, . . . , ±∞.
Referring back to
At ωse and ωsh the group velocity (vg=dω/dβ) is zero and the phase velocity (vp=ω/β) is infinite. When the series and shunt resonances are equal: LRCL=LLCR the structure is said to be balanced, and the resonant frequencies coincide:
ωse=ωsh=ω0.
For the balanced case, the phase response can be approximated by:
where N is the number of unit cells. The slope of the phase is given by:
The characteristic impedance is given by:
The inductance and capacitance values can be selected and controlled to create a desired slope for a chosen frequency. In addition, the phase can be set to have a positive phase offset at DC. These two factors are used to provide the designs of multi-band and other MTM power combining and dividing structures presented in this specification.
The following sections provide examples of determining MTM parameters of dual-band mode MTM structures and similar techniques can be used to determine MTM parameters with three or more bands.
In a dual-band MTM structure, the signal frequencies f1, f2 for the two bands are first selected for two different phase values: φ1 at f1 and φ2 at f2. Let N be the number of unit cells in the CRLH TL and Zt, the characteristic impedance. The values for parameters LR, CR, LL and CL can be calculated:
In the unbalanced case, the propagation constant is given by:
For the balanced case:
A CRLH TL has a physical length of d with N unit cells each having a length of p: d=N.p. The signal phase value is φ=−βd. Therefore,
It is possible to select two different phases φ1 and φ2 at two different frequencies f1 and f2, respectively:
In comparison, a conventional RH microstrip transmission line exhibits the following dispersion relationship:
See, for example, the description on page 370 in Pozar, Microwave Engineering, 3rd Edition and page 623 in Collin, Field Theory of Guided Waves, Wiley-IEEE Press; 2 Edition (Dec. 1, 1990).
Dual- and multi-band CRLH TL devices can be designed based on a matrix approach described in U.S. patent application Ser. No. 11/844,982 entitled “Antennas Based on Metamaterial Structures” and filed on Aug. 24, 2007, which is incorporated by reference as part of the specification of this application. Under this matrix approach, each 1D CRLH transmission line includes N identical cells with shunt (LL, CR) and series (LR, CL) parameters. These five parameters determine the N resonant frequencies and phase curves, corresponding bandwidth, and input/output TL impedance variations around these resonances.
The frequency bands are determined from the dispersion equation derived by letting the N CRLH cell structure resonates with nπ propagation phase length, where n=0, ±1, . . . ±(N−1). That means, a zero and 2π phase resonances can be accomplished with N=3 CRLH cells. Furthermore, a tri-band power combiner and splitter can be designed using N=5 CRLH cells where zero, 2π, and 4π cells are used to define resonances.
The n=0 mode resonates at ω0=ωSH and higher frequencies are given by the following equation for the different values of M specified in Table 1:
Table 1 provides M values for N=1, 2, 3, and 4.
Hence, CRLH power combiners and dividers can be designed for combining and dividing signals at two or more different frequencies under impedance matched conditions to achieve compact devices that are smaller than conventional combiners and dividers. Referring back to
Each unit cell can be in a “mushroom” structure which includes a top conductive patch formed on the top surface of a dielectric substrate, a conductive via connector formed in the substrate 201 to connect the top conductive patch to the ground conductive patch. Various dielectric substrates can be used to design these structures, with a high or a low dielectric constant and varying heights. It is also possible to reduce the footprint of this structure by using a “vertical” technology, i.e., by way of example a multilayer structure or on Low Temperature Co-fired Ceramic (LTCC).
The values of LL, CL, CR and LR at two different frequencies, for example, f1=2.44 GHz and f2=5.85 GHz, with a phase of (0+2πn) at f1 and −2π(n+1) at f2, with n= . . . , −1, 0, 1, 2, . . . . In these examples, lumped elements are used to model the left-handed capacitors and the left-handed inductors can be realized by, e.g., using shorted stubs to minimize the loss. The RH part is modeled by using a conventional RH microstrip with an electrical length determined by CR and LR. The number of unit cells is defined by N(=l/d), where d is the length of the unit cell and l is the length of the CRLH transmission line. For example, a unit cell can be designed by with a phase of zero degree at f1 and a phase of −360 degree at f2. A two-cell CRLH cell can use the following calculated values LL=2.0560 nH, CL=0.82238 pF, CR=2.0694 pF and LR=5.1735 nH. It can be noticed that LRCL=CRLL and
which is the balanced case, ωse=ωsh. Such a CRLH TL can be implemented by using an FR4 substrate with the values of H=31 mil (0.787 mm) and ∈r=4.4.
by way of example N=2 for this structure, as a result Z0=70.7Ω.
The above and other dual-band and multi-band CRLH structures can be used to construct N-port dual-band and multi-band CRLH TL serial power combiners and dividers
The two signal frequencies f1 has f2 do not have a harmonic frequency relationship with each other. This feature can be used to comply with frequencies used in various standards such as the 2.4 GHz band and the 5.8 GHz in the Wi-Fi applications. In this configuration, the port position and the port number along the dual-band CRLH TL 1110 can be selected as desired because of the zero degree spacing at f1 and 360° at f2 between each port. For example, the unit cells described in
The above described multi-band CRLH TL power dividers or combiners can be used to construct multi-band CRLH TL power dividers or combiners in resonator configurations.
A power combiner or divider can be structured in a radial configuration.
The main feedline can be a conventional RH feedline or a CRLH feedline. The conventional feedline is optimal when a power combiner is used in a switch configuration, where one branch line is connected to the main feedline and the rest of plural branches are disconnected. The main CRLH feedline is optimal when the branch CRLH lines are simultaneously connected.
We simulated, fabricated and measured performance parameters of CRLH TL zero degree compact single band radial power combiners and dividers based on the above design. All single band radial power combiners/dividers presented are using the same feeding line length of 20 mm in order to compare the device performance. The length of the feeding line can be selected based on the specific need in each application.
The above single-band radial CRLH devices can be configured as dual-band and multi-band devices by replacing a single-band CRLH TL component with a respective dual-band or multi-band CRLH TL component.
Microstrip/Strip-Line RF Switch Device
As previously indicated, CRLH TLs can be used in power combiner/divider devices, providing advantages such as size reduction and performance enhancements. The electrical length can be made to be a multiple of 180° (including zero degree) based on the CRLH properties under impedance matched conditions for multi-band operations. The use of CRLH TLs in power combiner/divider devices offers other advantages such as low RF return loss and multi-band capability which are not harmonically related as in the case of RH TLs. For example,
In
Multiple Pole Multiple Throw (MPMT) RF Switch Device
A Multiple Pole Multiple Throw (MPMT) switch device disclosed in this document is a multiple terminal device that includes multiple branches and multiple switch mechanisms on each branch for providing one or more connections between the multiple terminals. According to one implementation, an MPMT switch device based on RF switches and CRLH TLs includes a power combiner/divider device formed using a plurality of CRLH TLs, multiple RF switches coupled to each CRLH TL, and multiple branches and a feed line having CRLH TLs. The branches and the feed line are configured to be equivalent without particular directionality with respect to a signal transmission in this device. These equivalently configured branches and the feed line are together called “branches” hereinafter in this document. An RF switch is placed on each branch and is controlled by a controller to direct the signal from any arbitrary branch or combination of branches to any other arbitrary branch or combination of branches. The MPMT RF switch devices that are compact in size may be constructed based on the CRLH TL principles and techniques described above. Examples of such devices are described next.
5-Branch MPMT RF Switch Device Based on CRLH TLs
As illustrated in
Referring again to
In this example, the RF switch 2815 may be placed on each branch and controlled by a control signal 2817 to direct the RF signal from any five branches or combination of branches to any other arbitrary branch or combination of branches. The operation of the RF switch device shown in
Multi-Branch MPMT RF Switch Device
In another embodiment, the CRLH MPMT RF switch device presented in this document may have various configurations and numbers of branches connected to various combinations of terminals to direct one or more RF signals. For example, the 5-Branch switch device described above can be generalized to a multi-branch MPMT RF switch device having m-number of branches coupled to m-number of terminals, n-number of branches coupled to n-number of terminals, and p-number of branches coupled to p-number terminals, where m, n, and p are greater than or equal to 1. In this example, the m, n, and p-number of terminals may be respectively coupled to m-number of TX ports, n-number of RX ports, and p-number of Antenna ports.
According to an example of this embodiment, a control switch 2945 may be placed on each branch and may be controlled by a control signal to direct an RF signal from any number of branches or combination of branches to any other arbitrary branch or combination of branches. The control switch 2945, such as an RF switch, may be placed on each branch and controlled externally. Examples of the RF switch are a PIN diode, Field Effect Transistor (FET), Single Pole Single Throw (SPST) switch, or Single Pole Dual Throw (SPDT) switch. In one implementation, digital control signals are provided to control the ON/OFF of the RF switches. For example, logic 1 can cause the RF switch to turn on, and logic 0 can cause the RF switch to turn off. These signals can be General Purpose Input/Output (GPIO) from a system controller. This device in
The operation of the control switch 2945 shown in
TX Branch MPMT RF Switch Device (m=2, n=0, p=4)
In another embodiment, the number of RX or TX ports may be zero. For example, the multi-branch MPMT device 3000 shown in
A truth table for the multi-branch MPMT device 3000 shown in
Implementation of MPMT RF Switch in Single Pole, Double Throw (SPDT) and Single Pole Triple Throw (SP3T) Switch Topologies
The SPDT/SP3T switch topology 3100 shown in
Furthermore, the CRLH MPMT RF switch device as shown
Therefore, the MPMT RF switch device based on CRLH materials described in this document can provide flexibility in choosing signal transmission directions and paths depending on target applications while achieving compactness for single as well as multi-band operations.
While this specification contains many specifics, these should not be construed as limitations on the scope of an invention or of what may be claimed, but rather as descriptions of features specific to particular embodiments of the invention. Certain features that are described in this specification in the context of separate embodiments can also be implemented in combination in a single embodiment. Conversely, various features that are described in the context of a single embodiment can also be implemented in multiple embodiments separately or in any suitable subcombination. Moreover, although features may be described above as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can in some cases be excised from the combination, and the claimed combination may be directed to a subcombination or a variation of a subcombination.
Only a few implementations are disclosed. However, it is understood that variations and enhancements may be made.
This application is a continuation-in-part of U.S. patent application Ser. No. 11/963,710, now issued as U.S. Pat. No. 7,839,236, entitled “POWER COMBINERS AND DIVIDERS BASED ON COMPOSITE RIGHT AND LEFT HANDED METAMATERIAL STRUCTURES,” and filed on Dec. 21, 2007, and this application claims priority to U.S. Provisional Patent Application Ser. No. 61/138,054, entitled “MULTIPLE POLE MULTIPLE THROW RF SWITCH DEVICE BASED ON COMPOSITE RIGHT AND LEFT HANDED METAMATERIAL STRUCTURES,” and filed on Dec. 16, 2008, the benefit of priority of each of which is claimed hereby, and each of which are incorporated by reference herein in its entirety.
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Parent | 11963710 | Dec 2007 | US |
Child | 12639831 | US |