Filter network combining non-superconducting and superconducting filters

Information

  • Patent Grant
  • 6686811
  • Patent Number
    6,686,811
  • Date Filed
    Monday, March 26, 2001
    23 years ago
  • Date Issued
    Tuesday, February 3, 2004
    20 years ago
Abstract
A filter network designed for providing high frequency selectivity with a high degree of reliability and availability. The filter network comprises a superconducting filter and a non-superconducting filter, or a combination thereof to form multiplexers. A receive side of the non-superconducting filter pre-filters received RF signals before inputting them to the superconducting filter. The non-superconducting filter is constructed and arranged to pass RF signals having a frequency within a first pass band to the superconducting filter. The superconducting device is constructed and arranged to exhibit a high-degree of frequency selectivity in further narrowing the received RF signals. Other aspects are directed to the arrangement, construction, and uses of the same structures to accomplish different but similar goals. In a multiplexed configuration, various combinations of transmit filters are used to enable the use of a common antenna with the receive side electronics, which may be located at the top of the antenna tower or in the base station.
Description




FIELD OF THE INVENTION




The present invention relates generally to structures and techniques for filtering radio waves and more particularly to the implementation of a filter network using a combination of superconducting filters and non-superconducting filters.




BACKGROUND OF THE INVENTION




Radio frequency (RF) equipment have used a variety of approaches and structures for receiving and transmitting radio waves in selected frequency bands. The type of filtering structure used often depends upon the intended use and the specifications for the radio equipment. For example, dielectric filters may be used for filtering electromagnetic energy in the ultra-high frequency (UHF) band, such as those used for cellular communications in the 800+ MHz frequency range. Typically, such filter structures are implemented by coupling a number of dielectric resonator structures together. One can also use metal coaxial resonators in such filters are coupled together via capacitors, inductors, or by apertures in walls separating the resonator structures. The number of resonator structures used for any particular application also depends upon the system specifications and, typically, added performance is realized by increasing the number of intercoupled resonator structures.




However, because of an increase in the number of users utilizing a limited bandwidth, demand has increased for greater frequency selectivity than can be provided by normal or non-superconducting resonator filters, especially for RF signals in the ultra-high frequency bands used for cellular communications. High frequency selectivity has previously been accomplished using High Temperature Superconducting (HTS) filters, usually as front-end filters for cellular base station receivers. However, HTS front-end filters may be susceptible to failure, or degradation in performance, induced by lightning surges or other high power signals. In addition, the non-linearity of HTS filters produces in-band intermodulation spurious signals from out-of-band interferers.




For cellular or similar base stations, typical lightning protectors have only one resonator and do not provide sufficient protection from high power co-located radio frequency signals originating from the transmit side of the base stations. These co-located transmission signals are especially troublesome because they are relatively closely spaced to the operating frequency of the base station receivers. Accordingly, there is a need for a filter that overcomes the above-mentioned and other disadvantages associated with the prior art.




SUMMARY OF THE INVENTION




The present invention is directed toward a filter network that provides high frequency selectivity to a receiver. The filter network of the present invention comprises a non-superconducting filter and a superconducting filter. The output of the non-superconducting filter is coupled to the input of a superconducting filter. The non-superconducting filter pre-filters received RF signals by passing RF signals having a frequency within a first pass band to the superconducting filter. The superconducting filter further filters the RF signals to provide a high degree of frequency selectivity at its output.




The filter network of the present invention is able to provide high frequency selectivity while overcoming many of the disadvantages associated with superconducting filters. This is achieved by pre-filtering the RF signals with the non-superconducting filter before inputting them to the superconducting filter. The non-superconducting filter protects the superconducting filter from lightning surges or other high power signals. In addition, the non-superconducting filter filters out interferers that produce in-band intermodulation spurious signals at the superconducting filter output. In a multiplexed configuration, the non-superconducting filter protects the superconducting filter directly from transmit signal energy.




According to one embodiment of the present invention, the non-superconducting resonator filter comprises a housing enclosing three resonators. The resonators are coupled to each other through apertures in the housing. The effect of using this coupling with the three resonators is to produce a filter response with a pass band and a finite frequency transmission zero located outside the pass band.











BRIEF DESCRIPTION OF THE DRAWINGS




Other aspects and advantages of the invention will become apparent upon reading the following detailed description and upon reference to the drawings in which:





FIG. 1

shows a communications system incorporating a filter network according to one embodiment of the invention.





FIG. 2A

shows a top view of a non-superconducting filter according to one embodiment of the present invention.





FIG. 2B

shows a cross-sectional side view of the non-superconducting filter according to one embodiment of the present invention.





FIG. 3

shows a plot of the filter response of the non-superconducting filter according to one embodiment of the present invention.





FIG. 4

shows a multiplexer according to one embodiment of the present invention.





FIG. 5

shows a double-duplexer according to one embodiment of the present invention.





FIG. 6

shows a double-duplexer according to another embodiment of the present invention.











DETAILED DESCRIPTION OF THE PREFFERED EMBODIMENT




The present invention is believed to be applicable to a variety of radio frequency (RF) applications in which achieving low insertion loss in the pass band with high attenuation in the stop band, and an extremely high degree of selectivity in the pass band are necessary. The present invention is particularly applicable and beneficial for cellular-communication base stations, and other communication applications. While the present invention is not so limited, an appreciation of the present invention is best presented by way of a particular example application, in this instance, in the context of such a communication system.




Now turning to the drawings,

FIG. 1

shows a front-end receiver system


10


of a base station, according to a particular application and embodiment of the present invention. The front-end receiver system


10


includes an antenna


12


for receiving RF signals


15


, a filter network


100


for filtering the received RF signals, and a receiver


16


. The filter network


100


is used to selectively pass received RF signals within a designated pass band to the receiver


16


, while filtering out interferers. The interferers are interfering signals located outside the operating frequency of the receiver


16


, and include RF signals transmitted by other cellular service providers. The interferers also include co-located transmission signals transmitted by the transmitter side of the same base station.




The filter network


100


comprises a non-superconducting filter


20


and a superconducting filter


30


, preferable a High Temperature Superconducting (HTS) filter. The input of the non-superconducting filter


20


receives RF signals


15


from the antenna


12


. The output of the non-superconducting filter


20


is coupled to the input of the superconducting filter


30


, and the output of the superconducting filter is coupled to the receiver


16


. The non-superconducting filter


20


pre-filters the received RF signals


15


before they are filtered by the superconducting filter


30


.




The non-superconducting filter


20


is a bandpass filter tuned to pass the received RF signals having a frequency within a first pass band to the superconducting filter


30


. Preferably, the first pass band encompasses a receiving frequency range of the base station. For base stations using the Advanced Mobile Phone Service (AMPS) standard, for example, the total receiving frequency range is approximately 824 MHz to 849 MHz. The superconducting filter


30


is a bandpass filter tuned to pass the pre-filtered RF signals having a frequency within a second pass band to the receiver


16


. The second pass band is a narrow pass band located inside the first pass band for providing high frequency selectivity to the receiver


16


.




The non-superconducting filter


20


protects the superconducting filter


30


from high power out-of-band signals that can cause catastrophic failure of the superconducting filter


30


. The high power signals include electrical surges caused by lightning strikes. In addition, the non-superconducting


20


filter filters out interferers located outside the first pass band before they are inputted to the superconducting filter


30


. This is done because these interferers produce in-band intermodulation spurious signals in the superconducting filter


30


. By filtering out these interferers before they are inputted to the superconducting filter


30


, the non-superconducting filter


20


dramatically reduces the in-band intermodulation spurious signals.




The superconducting filter


30


provides high frequency selectivity to the receiver


16


for rejecting undesirable signals that are closely spaced in frequency to desirable signals. The advantage of using a superconducting filter is its ability to provide a precise narrow pass band around the desired signals with low insertion loss due to its low resistance. This allows the superconducting filter


30


to provide high frequency selectivity without adversely affecting the signal sensitivity of the receiver


16


.




Therefore, the filter network


100


according to the present invention exhibits high frequency selectively and low insertion loss without many of the disadvantages associated with a superconducting filter. This is achieved by pre-filtering the RF signals with the non-superconducting filter


20


before inputting the RF signals to the superconducting filter


30


. That way, catastrophic failure due to high power out-of-band signals and performance degradation due to in-band intermodulation spurious signals are dramatically reduced.





FIG. 2A

of a non-superconducting filter


200


according to one embodiment of the present invention. The non-superconducting filter


200


comprises a housing


210


enclosing three round-rod resonators


215


,


220


and


225


. Alternatively, the resonators


215


,


220


and


225


can be waveguide resonators, cavity resonators, dielectric resonators, stripline resonators, or other resonators known in the art. The housing


210


and resonators


215


,


220


and


225


may be machined from aluminum and silver plated to minimize insertion loss. The resonators


215


,


220


and


225


are placed in three cavities


230


,


235


, and


240


, respectively, formed inside the housing


210


, creating coaxially resonant structures. The input


275


and the output


285


of the non-superconducting


200


filter are directly coupled


290


and


295


to resonators


215


and


225


, respectively. Alternatively, the input


275


and the output


285


may be coupled to the resonators


215


and


225


, respectively, using capacitors, inductors or any other coupling technique used by those skilled in the art.





FIG. 2B

shows a cross-sectional view of the non-superconducting filter


200


taken along line


2


B in FIG.


2


A.

FIG. 2B

shows a top plate


310


placed over the housing


210


of the non-superconducting filter


200


. In addition, tuning screws


320


are inserted into each resonator


215


,


220


and


225


though the top plate


310


. The tuning screws


320


are secured to the top plate


310


by nuts


330


. The functionality of the tuning screws


320


will be discussed later.




Each resonator


215


,


220


and


225


is electro-magnetically coupled to each one of the other two resonators


215


,


220


and


225


through apertures in the housing


210


. The aperture coupling resonators


215


and


220


is shown in

FIG. 2A

as the opening between cavities


230


and


235


. The aperture coupling resonators


220


and


225


is shown in

FIG. 2A

as the opening between cavities


235


and


240


. The aperture coupling resonators


215


and


225


is best shown in

FIG. 2B

as an opening


270


in a housing wall


275


positioned between resonators


215


and


225


. Alternatively, the resonators can be coupled to each other using transformers or capacitors.




The turning screws


320


are used to adjust the capacitance of the resonators


215


,


220


and


225


. Turning the tuning screws


320


inwardly increases the capacitance of the resonators


215


,


220


and


225


, which lowers the resonance frequency of the resonators


215


,


220


and


225


. Turning the tuning screws


320


outwardly decreases the capacitance of the resonators, which increases the resonance frequency of the resonators


215


,


220


and


225


.




The non-superconducting filter


200


of

FIGS. 2A and 2B

produces a first pass band and a finite frequency transmission zero positioned at a frequency outside the first pass band. The finite frequency transmission zero provides enhanced rejection of signals located in its vicinity. The position of the finite frequency transmission zero can be controlled by adjusting the dimensions of the aperture coupling resonators


215


and


225


. Preferably, the finite frequency transmission zero is positioned at a frequency within a frequency range containing powerful interferers to provide enhanced rejection of these interferers. For example, the co-located transmission signals transmitted by the transmitter side of the base station can be powerful due to the proximity between the transmitter and receiver side of the base station. In this example, the finite frequency transmission zero can be positioned at a frequency inside the transmitting frequency range of the base station to enhance rejection of the co-located transmission signals. For base stations using the AMPS standard, for example, the transmitting frequency range is approximately 869 MHz to 894 MHz, which is located near the receiving frequency range of 824 MHz to 849 MHz. The finite frequency transmission zero can be positioned at a frequency either above or below the first pass band, depending on the location of powerful interferers.




In one specific example of the non-superconducting filter


200


in

FIGS. 2A and 2B

, the non-superconducting filter


200


structure has the dimensions given below. The housing


210


has a height H


1


of 2.30 inches. Chamber


235


has a width W


1


of 3.50 inches and a length L


1


of 2.75 inches, and chambers


230


and


240


each have a width W


2


of 2.55 inches and a length L


2


of 2.55 inches. Each one of the resonators


215


,


220


and


225


has a diameter d of 0.75 inches and a height H


2


of 2.15 inches. The center of resonator


220


is positioned in chamber


235


a length L


5


of 1.275 inches from one side of the housing


210


and width W


4


of 1.75 from another side of the housing


210


. The center of resonator


225


is position in chamber


240


a length L


6


of 1.275 inches from one side of the housing


210


and a width W


5


of 1.275 from another side of the housing


210


. The center of resonator


215


is in the same relative position in chamber


230


as the center of resonator


235


is in chamber


240


. The housing wall


275


separating resonators


215


and


225


has a width W


3


of 0.20 inches and a length L


3


of 2.75 inches. Finally, the aperture


270


coupling resonators


215


and


225


has a height H


3


of 0.70 inches and a length L


4


of 1.70 inches.





FIG. 3

shows a plot


345


of the frequency response of a non-superconducting filter


200


made from silver-plated aluminum and having the above dimensions. Specifically, the plot


345


shows an insertion loss


350


measured in decibels (dB) between the input


275


and the output


285


of the non-superconducting filter


200


versus frequency in the range of 750 MHz to 950 MHz. The filter


200


passes frequencies at which the insertion loss


350


is low and rejects frequencies at which the insertion loss


350


is high. In

FIG. 3

, the insertion loss


350


is low within a receiving frequency range of about 824 MHz to 849 MHz, which is bounded by lines


355


and


360


. In contrast, the insertion loss is high within a transmitting frequency range of 869 MHz to 894 MHz, which is bounded by lines


365


and


370


. Thus, the non-superconducting filter


200


measured in plot


345


passes signals within the receiving frequency range of 824 MHz to 849 MHz, while rejecting signals within the transmitting frequency range of 869 MHz to 894 MHz. These frequency ranges correspond to the receiving and transmitting frequency ranges used by cellular base stations in the AMPS standard.




In this specific example, the effect of the cross coupling between the resonators


215


,


220


and


225


produces a finite frequency transmission zero, which can been seen as a deep spike


375


in the insertion loss


350


in the plot


345


. This transmission zero is located inside the base station transmitting frequency range of 869 MHz to 894 MHz and provides enhanced rejection of frequencies within this frequency range.





FIG. 4

shows a multiplexer


410


according to one embodiment of the present invention. The multiplexer


410


comprises at least one transmit filter


420


-n and at least one receive filter network


425


-n. The receive filter network


425


-n further comprises a non-superconducting filter


430


-n, and a superconducting filter and receive electronics


440


-n. The output of the transmit filter


420


-n and the input of the receive filter network


425


-n are coupled to a common antenna port


450


-n. The transmit filter


420


-n and the receive filter network


425


-n may be coupled to the common antenna port


450


-n by an interconnecting phasing network (not shown), the construction of which is well known in the art. The common antenna port


450


-n is coupled to an antenna


460


, for example, through a cable. The multiplexer


410


may be located in close proximity to the antenna


460


. For example, the multiplexer


410


and the antenna


460


may be mounted to the same antenna tower. Alternatively, the multiplexer


410


may be located away from the antenna


460


, such as in a base station.




The transmit filter


420


-n filters incoming transmit signals


422


-n from the transmitter side of a base station (not shown). The transmit filter


420


-n is a bandpass filter constructed to pass signals within a transmitting frequency range of the base station, for example, approximately 869 MHz to 984 for the AMPS standard. The transmit filter


420


-n may include one or more finite frequency transmission zeros for providing enhanced rejection of signals located outside of the transmitting frequency range, such as the receive signals on the common antenna port


450


-n. The non-superconducting filter


430


-n of the receive filter network


425


-n pre-filters receive signals from the antenna


460


. The non-superconducting filter


430


-n is a bandpass filter constructed to pass signals within a receiving frequency range of the base station, for example, 824 MHz to 849 MHz for the AMPS standard. The non-superconducting filter


430


-n may include one or more finite frequency transmission zeros for providing enhanced rejection of signals located outside of the receiving frequency range, such as the transmit signals on the common antenna port


450


-n. The superconducting filter


440


-n is a sharp bandpass filter for providing high frequency selectivity of the receive signals. The receive electronics


440


-n further processes the receive signals. The receive electronics


440


-n may include a Low Noise Amplifier (LNA), which may or may not be cryogenically cooled, for amplifying the receive signals. The receive electronics


440


-n may also include protection circuits for protecting the superconducting filter


440


-n and/or base station (not shown) from electrical surges. The protection circuits may include gas discharge tube voltage arrestors, quarter wavelength stubs, and any other protection circuits that are well known in the art. The receive signals are outputted


445


-n by the receive filter network


425


-n to the receiver side of a base station (not shown).




The multiplexer


410


according to the present invention enables the same antenna


460


to both transmit and receive signals, thereby reducing costs. This is achieved by coupling the transmit filter


420


-n and the receive filter network


425


-n to the common antenna port


450


-n of the multiplexer


410


, and coupling the common antenna port


450


-n to the antenna


460


.





FIG. 5

shows a double duplexer


510


according to another embodiment of the present invention. The double duplexer


510


includes a transmit filter


515


and a receive filter network


520


. The receive filter network


520


further includes a first non-superconducting filter


530


, a second non-superconducting filter


550


, and a superconducting filter and receive electronics


540


coupled between the first and second non-superconducting filter


530


,


550


. The output of the transmit filter


515


and the input of the receive filter network


520


are coupled to a common antenna port


560


. The common antenna port


560


is coupled to an antenna


565


, for example, through a cable. The input of the transmit filter


515


and the output of the receive filter network


520


are coupled to a common port


570


. The common port


570


is coupled to a base station (not shown) through a cable


575


.




The transmit filter


515


filters incoming transmit signals from the base station (not shown) in a manner similar to the transmit filter


420


-n of the multiplexer


410


. The first non-superconducting filter


530


pre-filters receive signals from the antenna


565


in a manner similar to the non-superconducting filter


430


of the multiplexer


410


. The superconducting filter


540


is a sharp bandpass filter for providing high frequency selectivity of the receive signals. The receive electronics


540


further processes the receive signal in a manner similar to the receive electronics


440


-n of the multiplexer


410


. The second non-superconducting filter


550


is a bandpass filter that passes the receive signals to the common port


570


while blocking the transmit signals on the common port


570


from the entering the receive electronics


540


. The second non-superconducting filter


550


may be the identical to the first non-superconducting filter


530


.




The double-duplexer


510


according to the present invention enables the same antenna


565


to both transmit and receive signals, thereby reducing costs. In addition, the double-duplexer


510


enables the transmit signals and the receive signals to flow between the double-duplexer


510


and the base station (not shown) through the common port


570


. As a result, a single cable


575


can be used to coupled the double-duplexer


510


to the base station. Because the base station uses a single cable


575


to both transmit signals to and receive signals from the double-duplexer


510


, additional filters may be needed to split the transmit and receive signals at the base station. This may be accomplished by providing a transmit filter


580


between the transmitter side of the base station (not shown) and the cable


575


, and a receive filter


585


between the receiver side of the base station (not shown) and the cable


575


.




Although, the double-duplexer


510


was described as including one transmit filter


515


and one receive filter network


520


, those skilled in the art will appreciate that any number of transmit filters and receive filter network may be added to the double-duplexer to realize a double-multiplexer.





FIG. 6

shows a double-duplexer


610


according to another embodiment of the present invention. In this embodiment, the receive filter network


620


includes a first superconducting filter


630


, a second superconducting filter


650


, and receive electronics


640


coupled between the first and second superconducting filter


630


,


650


. The first superconducting filter


630


is a sharp bandpass filter for providing high frequency selectivity of the receive signals from the antenna


565


. The receive electronics


630


further processes the receive signals and may include an LNA and protection circuits. The second superconducting filter


650


is a bandpass filter that passes the receive signals to the common port


570


while blocking transmit signals on the common port


570


from entering the receive electronics


640


. Alternatively, the second superconducting filter


650


may be replaced by a non-superconducting filter.




Additionally, to alleviate catastrophic failure of the receive side of the systems shown in

FIGS. 4 and 5

, a switched bypass (not shown) may be used. In the event of an electrical surge in a receive path of the systems, the switched bypass directs the receive signals around the superconducting filters shown in the receive electronics


440


-n and


540


. Also included in this bypass function may be one or more low noise amplifiers, which may or may not be cooled, along with any other circuitry in the path of the receive signals that may be considered prone to failure.




Other aspects and embodiments of the present invention will be apparent to those skilled in the art from consideration of the specification and practice of the invention disclosed herein. For example, the non-superconducting filter illustrated in

FIGS. 2A and 2B

may be implemented in a variety of ways to achieve similar results according to the design and specifications. In addition, those skilled in the art will appreciate that the invention is not restricted to frequency bands used in the AMPS standard, and may, in principle, operate in other frequency bands used in other mobile phone standards. It is intended that the specification and illustrated embodiments be considered as exemplary only, with a true scope and spirit of the invention being indicated by the following claims.



Claims
  • 1. A multiplexer, comprising:at least one transmit filter, said transmit filter having an output; at least one receive filter network, said receive filter network comprising a non-superconducting bandpass filter, said non-superconducting filter having an input, an output, and a first pass band; and a superconducting filter, said superconducting filter having an input coupled to the output of the non-superconducting filter; and a common port coupled to the output of the transmit filter and the input of the non-superconducting filter of the receive filter network; wherein the transmit filter or the non-superconducting filter has a finite frequency transmission zero positioned at a frequency outside of the first pass band.
  • 2. A multiplexer, comprising:at least one transmit filter, said transmit filter having an output; at least one receive filter network, said receive filter network comprising a non-superconducting bandpass filter, said non-superconducting filter having an input, an output, and a first pass band; and a superconducting bandpass filter, said superconducting filter having an input coupled to the output of the non-superconducting filter, and a second pass band located inside the first pass band of the non-superconducting bandpass filter; and a common port coupled to the output of the transmit filter and the input of the non-superconducting filter of the receive filter network.
  • 3. The multiplexer of claim 2, further comprising a Low Noise Amplifier (LNA) for amplifying signals sent through the receive network filter.
  • 4. The multiplexer of claim 3, wherein the LNA is cryogenically cooled.
  • 5. The multiplexer of claim 3, wherein the LNA is not cryogenically cooled.
  • 6. A double-multiplexer, comprising:at least one transmit filter, said transmit filter having an input and an output; at least one receive filter network, said received filter network comprising a first non-superconducting filter, said first non-superconducting filter having an input and an output; a superconducting filter, said superconducting filter having an input coupled to the output of the first non-superconducting filter and an output; and a second non-superconducting filter, said second non-superconducting filter having an input coupled to the output of the superconducting filter and an output; a first common port coupled to the output of the transmit filter and the input of the first non-superconducting filter of the receive filter network; and a second common port coupled to the transmit filter and the output of the second non-superconducting filter of the receive filter network.
  • 7. The double-multiplexer of claim 6, wherein the first common port is coupled to an antenna.
  • 8. The double-multiplexer of claim 6, wherein the second common port is coupled to a base station.
  • 9. The double-multiplexer of claim 6, wherein the first non-superconducting filter is a bandpass filter having a first pass band.
  • 10. The double-multiplexer of claim 9, wherein the transmit filter or the first non-superconducting filter has a finite frequency transmission zero positioned at a frequency outside of the first pass band.
  • 11. The double-multiplexer of claim 9, wherein the transmit filter or the first non-superconducting filter has none or more than one finite frequency transmission zero positioned at frequencies outside of the first pass band.
  • 12. The double-multiplexer of claim 9, wherein the superconducting filter is a bandpass filter having a second pass band located inside the first pass band.
  • 13. The multiplexer of claim 6, further comprising a Low Noise Amplifier (LNA) for amplifying signals sent through the receive network filter.
  • 14. The multiplexer of claim 13, wherein the LNA is cryogenically cooled.
  • 15. The multiplexer of claim 13, wherein the LNA is not cryogenically cooled.
  • 16. The double-multiplexer of claim 6, wherein the first common port of the double-multiplexer is coupled to an antenna through a cable, and the double-multiplexer and the antenna are located on a common antenna tower within substantially close proximity to each other in order to minimize cable losses between the double-multiplexer and the antenna.
  • 17. The double-multiplexer of claim 6, further comprising a switched bypass for providing a bypass path around the superconducting filter in the event of an electrical surge in a receive path of the double-multiplexer.
  • 18. A double-multiplexer, comprising:at least one transmit filter, said transmit filter having an input and an output; at least one receive filter network, said receive filter network comprising a first superconducting filter, said first superconducting filter having an input and an output; receive electronics, said receive electronics having an input coupled to the output of the first superconducting filter and an output; and a second superconducting filter, said second superconducting filter having an input coupled to the output of the receive electronics and an output; a first common port coupled to the output of the transmit filter and the input of the first superconducting filter of the receive filter network; and a second common port coupled to the input of the transmit filter and the output of the second superconducting filter of the receive filter network.
  • 19. The double-multiplexer of claim 18, wherein the first common port is coupled to an antenna.
  • 20. The double-multiplexer of claim 18, wherein the second common port is coupled to a base station.
  • 21. The multiplexer of claim 18, wherein the receive electronics comprising a Low Noise Amplifier (LNA).
  • 22. The multiplexer of claim 21, wherein the LNA is cryogenically cooled.
  • 23. The multiplexer of claim 21, wherein the LNA is not cryogenically cooled.
  • 24. The double-multiplexer of claim 18, wherein the first common port of the double-multiplexer is coupled to an antenna through a cable, and the double-multiplexer and the antenna are located on a common antenna tower within substantially close proximity to each other in order to minimize cable losses between the double-multiplexer and the antenna.
  • 25. The double-multiplexer of claim 18, further comprising a switched bypass for providing a bypass path around the first and second superconducting filter in the event of an electrical surge in a receive path of the double-multiplexer.
  • 26. A multiplexer, comprising:at least one transmit filter, said transmit filter having an output; at least one receive filter network, said receive filter network comprising a non-superconducting filter, said non-superconducting filter having an input and an output; and a superconducting filter, said superconducting filter having an input coupled to the output of the non-superconducting filter; and a common port coupled to the output of the transmit filter and the input of the non-superconducting filter of the receive filter network; wherein the multiplexer is located in a base station that is remote from the location of an antenna, and the common port of the multiplexer is coupled to the antenna through a length of cable.
  • 27. A multiplexer, comprising:at least one transmit filter, said transmit filter having an output; at least one receive filter network, said receive filter network comprising a non-superconducting filter, said non-superconducting filter having an input and an output; and a superconducting filter, said superconducting filter having an input coupled to the output of the non-superconducting filter; and a common port coupled to the output of the transmit filter and the input of the non-superconducting filter of the receive filter network; wherein the common port of the multiplexer is coupled to an antenna through a cable, and the multiplexer and the antenna are both located on a common antenna tower within substantially close proximity to each other in order to minimize cable losses between the multiplexer and the antenna.
  • 28. A multiplexer, comprising:at least one transmit filter, said transmit filter having an output; at least one receive filter network, said receive filter network comprising a non-superconducting filter, said non-superconducting filter having an input and an output; and a superconducting filter, said superconducting filter having an input coupled to the output of the non-superconducting filter; and a switched bypass for providing a bypass path around the superconducting filter in the event of an electrical surge in a receive path of the multiplexer; and a common port coupled to the output of the transmit filter and the input of the non-superconducting filter of the receive filter network.
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