RF and microwave switches have widespread applications in microwave systems. They typically may use semiconductor active devices as the switching element. Semiconductor switches, however, cannot be used for applications that require high power handling as they will generate unwanted harmonics and distortions in the signal due to intermodulation effects. Although there are semiconductor RF switches that can handle up to several watts, they usually suffer from high insertion loss. An alternative may be to use mechanical switches with very high power handling, but those switches are bulky, heavy and consume a lot of power.
Therefore, there is a need for small, low loss, and linear RF switches that may be used in a wide range of RF and microwave frequencies, with high power handling capability.
An embodiment of the present invention provides an apparatus, comprising a radio frequency switch capable of using tunable dielectric capacitors as the switching element. The apparatus may further comprise a cross connector a plurality of ports and wherein at least one of the tunable dielectric capacitors may be placed between the cross connector and at least one port, thereby enabling impedance variations between the cross connector and the ports. Further, an embodiment of the present invention may provide at least one Tee connector between the cross connector and at least one of the plurality of ports, wherein at least one tunable dielectric capacitor may be associated with the Tee connector to vary the impedance in at least one node of the Tee connector.
Another embodiment of the present invention provides an apparatus, comprising an On-Off switch including a first port and a second port separated by a stop band filter, wherein at least one tunable dielectric capacitor may be integrated between the first port and the stop band filter and between the second port and the stop band filter. This embodiment may further comprise at least one additional port separated by the first and second ports by the stop band filter and at least one additional tunable dielectric capacitor between the at least one additional port and the stop band filter. A voltage source may facilitate the tunability of the tunable dielectric capacitors.
In yet another embodiment of the present invention is provided a method of switching radio frequency RF signals, comprising using tunable dielectric capacitors as the switching element for an RF switch. This method may further comprise connecting a plurality of ports with a cross connector in the RF switch and enabling impedance variations between the cross connector and the ports by at least one of the tunable dielectric capacitors placed between the cross connector at and least one port. The method may further comprise placing at least one T connector between the cross connector and at least one of the plurality of ports, wherein at least one tunable dielectric capacitor is associated with the T connector to vary the impedance in at least one node of the T connector.
The present invention is described with reference to the accompanying drawings. In the drawings, like reference numbers indicate identical or functionally similar elements. Additionally, the left-most digit(s) of a reference number identifies the drawing in which the reference number first appears.
An embodiment of the present invention provides a switch topology that may be based on Parascan® tunable material. Parascan® is a family of tunable dielectric material with excellent RF and microwave properties, such as, high Q, fast tuning, and high IP3. Further, the term Parascan® as used herein is a trademarked word indicating a tunable dielectric material developed by the assignee of the present invention. Parascan® tunable dielectric materials have been described in several patents. Barium strontium titanate (BaTiO3—SrTiO3), also referred to as BSTO, is used for its high dielectric constant (200-6,000) and large change in dielectric constant with applied voltage (25-75 percent with a field of 2 Volts micron). Tunable dielectric materials including barium strontium titanate are disclosed in U.S. Pat. No. 5,312,790 to Sengupta, et al. entitled “Ceramic Ferroelectric Material”; U.S. Pat. No. 5,427,988 by Sengupta, et al. entitled “Ceramic Ferroelectric Composite Material-BSTO-MgO”; U.S. Pat. No. 5,486,491 to Sengupta, et al. entitled “Ceramic Ferroelectric Composite Material-BSTO-ZrO2”; U.S. Pat. No. 5,635,434 by Sengupta, et al. entitled “Ceramic Ferroelectric Composite Material-BSTO-Magnesium Based Compound”; U.S. Pat. No. 5,830,591 by Sengupta, et al. entitled “Multilayered Ferroelectric Composite Waveguides”; U.S. Pat. No. 5,846,893 by Sengupta, et al. entitled “Thin Film Ferroelectric Composites and Method of Making”; U.S. Pat. No. 5,766,697 by Sengupta, et al. entitled “Method of Making Thin Film Composites”; U.S. Pat. No. 5,693,429 by Sengupta, et al. entitled “Electronically Graded Multilayer Ferroelectric Composites”; U.S. Pat. No. 5,635,433 by Sengupta entitled “Ceramic Ferroelectric Composite Material BSTO-ZnO”; U.S. Pat. No. 6,074,971 by Chiu et al. entitled “Ceramic Ferroelectric Composite Materials with Enhanced Electronic Properties BSTO-Mg Based Compound-Rare Earth Oxide”. These patents are incorporated herein by reference. The materials shown in these patents, especially BSTO-MgO composites, show low dielectric loss and high tunability. Tunability is defined as the fractional change in the dielectric constant with applied voltage.
Barium strontium titanate of the formula BaxSr2-xTiO3 is a preferred electronically tunable dielectric material due to its favorable tuning characteristics, low Curie temperatures and low microwave loss properties. In the formula BaxSr1-xTiO3 x can be any value from 0 to 1, preferably from about 0.15 to about 0.6. More preferably, x is from 0.3 to 0.6.
Other electronically tunable dielectric materials may be used partially or entirely in place of barium strontium titanate. An example is BaxCa1-xTiO3, where x is in a range from about 0.2 to about 0.8, preferably from about 0.4 to about 0.6. Additional electronically tunable ferroelectrics include PbxZr1-xTiO3 (PZT) where x ranges from about 0.0 to about 1.0, PbxZr1-xSrTiO3 where x ranges from about 0.05 to about 0.4, KTaxNb1-xO3 where x ranges from about 0.0 to about 1.0, lead lanthanum zirconium titanate (PLZT), PbTiO3, BaCaZrTiO3, NaNO3, KNbO3, LiNbO3, LiTaO3, PbNb2O6, PbTa2O6, KSr(NbO3) and NaBa2(NbO3)5KH2PO4, and mixtures and compositions thereof. Also, these materials can be combined with low loss dielectric materials, such as magnesium oxide (MgO), aluminum oxide (Al2O3), and zirconium oxide (ZrO2), and/or with additional doping elements, such as manganese (MN), iron (Fe), and tungsten (W), or with other alkali earth metal oxides (i.e. calcium oxide, etc.), transition metal oxides, silicates, niobates, tantalates, aluminates, zirconnates, and titanates to further reduce the dielectric loss.
In addition, the following U.S. Patent Applications, assigned to the assignee of this application, disclose additional examples of tunable dielectric materials: U.S. application Ser. No. 09/594,837 filed Jun. 15, 2000, entitled “Electronically Tunable Ceramic Materials Including Tunable Dielectric and Metal Silicate Phases”; U.S. application Ser. No. 09/768,690 filed Jan. 24, 2001, entitled “Electronically Tunable, Low-Loss Ceramic Materials Including a Tunable Dielectric Phase and Multiple Metal Oxide Phases”; U.S. application Ser. No. 09/882,605 filed Jun. 15, 2001, entitled “Electronically Tunable Dielectric Composite Thick Films And Methods Of Making Same”; U.S. application Ser. No. 09 834,327 filed Apr. 13, 2001, entitled “Strain-Relieved Tunable Dielectric Thin Films”; and U.S. Provisional Application Ser. No. 60 295,046 filed Jun. 1, 2001 entitled “Tunable Dielectric Compositions Including Low Loss Glass Frits”. These patent applications are incorporated herein by reference.
The tunable dielectric materials can also be combined with one or more non-tunable dielectric materials. The non-tunable phase(s) may include MgO, MgAl2O4, MgTiO3, Mg2SiO4, CaSiO3, MgSrZrTiO6, CaTiO3, Al2O3, SiO2 and/or other metal silicates such as BaSiO3 and SrSiO3. The non-tunable dielectric phases may be any combination of the above, e.g., MgO combined with MgTiO3, MgO combined with MgSrZrTiO6, MgO combined with Mg2SiO4, MgO combined with Mg2SiO4, Mg2SiO4 combined with CaTiO3 and the like.
Additional minor additives in amounts of from about 0.1 to about 5 weight percent can be added to the composites to additionally improve the electronic properties of the films. These minor additives include oxides such as zirconnates, tannates, rare earths, niobates and tantalates. For example, the minor additives may include CaZrO3, BaZrO3, SrZrO3, BaSnO3, CaSnO3, MgSnO3, Bi2O32SnO2, Nd2O3, Pr—Ot1, Yb2O3, Ho2O3, La2O3, MgNb2O6, SrNb2O6, BaNb2O6, MgTa2O6, BaTa2O6 and Ta2O3.
Thick films of tunable dielectric composites can comprise Ba1-xSrxTiO3, where x is from 0.3 to 0.7 in combination with at least one non-tunable dielectric phase selected from MgO, MgTiO3, MgZrO3, MgSrZrTiO6, Mg2SiO4, CaSiO3, MgAl2O4, CaTiO3, Al2O3, SiO2, BaSiO3 and SrSiO3. These compositions can be BSTO and one of these components, or two or more of these components in quantities from 0.25 weight percent to 80 weight percent with BSTO weight ratios of 99.75 weight percent to 20 weight percent.
The electronically tunable materials can also include at least one metal silicate phase. The metal silicates may include metals from Group 2A of the Periodic Table, i.e., Be, Mg, Ca, Sr, Ba and Ra, preferably Mg, Ca, Sr and Ba. Preferred metal silicates include Mg2SiO4, CaSiO3, BaSiO3 and SrSiO3. In addition to Group 2A metals, the present metal silicates may include metals from Group 1A, i.e., Li, Na, K, Rb, Cs and Fr, preferably Li, Na and K. For example, such metal silicates may include sodium silicates such as Na2SiO3 and NaSiO3—5H2O, and lithium-containing silicates such as LiAlSiO4, Li2SiO3 and Li4SiO4. Metals from Groups 3A, 4A and some transition metals of the Periodic Table may also be suitable constituents of the metal silicate phase. Additional metal silicates may include Al2Si2O7, ZrSiO4, KalSi3O8, NaAlSi3O8, CaAl2Si2O8, CaMgSi2O6, BaTiSi3O9 and Zn2SiO4. The above tunable materials can be tuned at room temperature by controlling an electric field that is applied across the materials.
In addition to the electronically tunable dielectric phase, the electronically tunable materials can include at least two additional metal oxide phases. The additional metal oxides may include metals from Group 2A of the Periodic Table, i.e., Mg, Ca, Sr, Ba, Be and Ra, preferably Mg, Ca, Sr and Ba. The additional metal oxides may also include metals from Group 1A, i.e., Li, Na, K, Rb, Cs and Fr, preferably Li, Na and K. Metals from other Groups of the Periodic Table may also be suitable constituents of the metal oxide phases. For example, refractory metals such as Ti, V, Cr, Mn, Zr, Nb, Mo, Hf, Ta and W may be used. Furthermore, metals such as Al, Si, Sn, Pb and Bi may be used. In addition, the metal oxide phases may comprise rare earth metals such as Sc, Y, La, Ce, Pr, Nd and the like.
The additional metal oxides may include, for example, zirconnates, silicates, titanates, aluminates, stannates, niobates, tantalates and rare earth oxides. Preferred additional metal oxides include Mg2SiO4, MgO, CaTiO3, MgZrSrTiO6, MgTiO3, MgAl2O4, WO3, SnTiO4, ZrTiO4, CaSiO3, CaSnO3, CaWO4, CaZrO3, MgTa2O6, MgZrO3, MnO2, PbO, Bi2O3 and La2O3. Particularly preferred additional metal oxides include Mg2SiO4, MgO, CaTiO3, MgZrSrTiO6, MgTiO3, MgAl2O4, MgTa2O6 and MgZrO3.
The additional metal oxide phases are typically present in total amounts of from about 1 to about 80 weight percent of the material, preferably from about 3 to about 65 weight percent, and more preferably from about 5 to about 60 weight percent. In one preferred embodiment, the additional metal oxides comprise from about 10 to about 50 total weight percent of the material. The individual amount of each additional metal oxide may be adjusted to provide the desired properties. Where two additional metal oxides are used, their weight ratios may vary, for example, from about 1:100 to about 100:1, typically from about 1:10 to about 10:1 or from about 1:5 to about 5:1. Although metal oxides in total amounts of from 1 to 80 weight percent are typically used, smaller additive amounts of from 0.01 to 1 weight percent may be used for some applications.
The additional metal oxide phases can include at least two Mg-containing compounds. In addition to the multiple Mg-containing compounds, the material may optionally include Mg-free compounds, for example, oxides of metals selected from Si, Ca, Zr, Ti, Al and or rare earths.
Turning to
The RF short at n3145 of the tee 140 is achieved by the combination of the transmission lines shown in
Turning now to
Turning now to
In another embodiment of the present invention as shown in
Turning now to
In an embodiment of the present invention, in the “On” condition, the capacitors may be tuned to different values by changing the bias voltage, and the stop band filter may no longer work as such. Although not limited in this respect, this condition may be achieved typically by a 2:1 capacitance tuning.
While certain features of the invention have been illustrated and described herein, many modifications, substitutions, changes, and equivalents will now occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true spirit of the invention.
This application is a continuation of U.S. patent application 11 045,957, filed Jan. 28, 2005 now U.S. Pat. No. 7,268,643, entitled APPARATUS, SYSTEM AND METHOD CAPABLE OF RADIO FREQUENCY SWITCHING USING TUNABLE DIELECTRIC CAPACITORS, to Hersey et al. which claimed the benefit of priority under 35 U.S.C. Section 119 from U.S. Provisional Application Ser. No. 60/539,771, filed Jan. 28, 2004, entitled “RF Switch Using Tunable Dielectric Capacitors” by Hersey et al.
Number | Name | Date | Kind |
---|---|---|---|
5061941 | Lizzi et al. | Oct 1991 | A |
5312790 | Sengupta et al. | May 1994 | A |
5427988 | Sengupta et al. | Jun 1995 | A |
5486491 | Sengupta et al. | Jan 1996 | A |
5593495 | Masuda et al. | Jan 1997 | A |
5635433 | Sengupta | Jun 1997 | A |
5635434 | Sengupta | Jun 1997 | A |
5640042 | Koscica et al. | Jun 1997 | A |
5693429 | Sengupta et al. | Dec 1997 | A |
5694134 | Barnes | Dec 1997 | A |
5766697 | Sengupta et al. | Jun 1998 | A |
5830591 | Sengupta et al. | Nov 1998 | A |
5846893 | Sengupta et al. | Dec 1998 | A |
5886867 | Chivukula et al. | Mar 1999 | A |
5990766 | Zhang et al. | Nov 1999 | A |
6074971 | Chiu et al. | Jun 2000 | A |
6377142 | Chiu et al. | Apr 2002 | B1 |
6377217 | Zhu et al. | Apr 2002 | B1 |
6377440 | Zhu et al. | Apr 2002 | B1 |
6404614 | Zhu et al. | Jun 2002 | B1 |
6454914 | Nakamura | Sep 2002 | B1 |
6492883 | Liang et al. | Dec 2002 | B2 |
6514895 | Chiu et al. | Feb 2003 | B1 |
6525630 | Zhu et al. | Feb 2003 | B1 |
6531936 | Chiu et al. | Mar 2003 | B1 |
6535076 | Partridge et al. | Mar 2003 | B2 |
6538603 | Chen et al. | Mar 2003 | B1 |
6556102 | Sengupta et al. | Apr 2003 | B1 |
6590468 | du Toit et al. | Jul 2003 | B2 |
6597265 | Liang et al. | Jul 2003 | B2 |
6646522 | Kozyrev et al. | Nov 2003 | B1 |
6741207 | Allison et al. | May 2004 | B1 |
6855992 | Emrick et al. | Feb 2005 | B2 |
7030463 | Subramanyam et al. | Apr 2006 | B1 |
7268643 | Hersey et al. | Sep 2007 | B2 |
Number | Date | Country |
---|---|---|
WO 2005043669 | May 2005 | WO |
Number | Date | Country | |
---|---|---|---|
20070013466 A1 | Jan 2007 | US |
Number | Date | Country | |
---|---|---|---|
60539771 | Jan 2004 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 11045957 | Jan 2005 | US |
Child | 11494066 | US |