The present disclosure relates to a resistor, and more particularly to a resistor used for a Radio Frequency (RF) switch.
Radio Frequency (RF) multi-throw switches are critical components in today's mobile devices. They are used to connect a common port of the switch to one of two or more selectable output/input ports. The connection path must exhibit very low loss so as not to degrade system efficiency, while at the same time, the two connected ports must have high isolation from the remaining ports. At the antenna of an RF front-end, for example, the high isolation is very important for protecting the sensitive receiver input from high RF transmit power.
Semiconductor Field-Effect Transistors (FETs) on materials such as GaAs, Silicon-On-Insulator (SOI), etc. are widely used for implementing RF switches. However, in order to achieve the high levels of isolation required, multiple devices must be stacked in series in the through and shunt paths. To change the state of these switches, a Direct Current (DC) control voltage must be selectively applied to the gates of the appropriate FETs. To prevent RF energy from being lost into the control circuit, the control voltages are typically applied through a network of resistors. These resistors impede the flow of the RF energy into the control circuit. To achieve the very low insertion losses required, these resistors are typically tens or hundreds of kilohms (kΩ) in value. While the isolated FETs could be switched from conducting to isolated states extremely rapidly, an RF switch implemented in the manner described exhibits relatively long switching times. This is attributable to the high value of the resistors, through which the control voltage is applied, which, along with internal capacitances inherent in the FET switches, lead to very large RC time constants for the device.
Accordingly, resistors and switches are needed for reducing the switching time of RF switches while maintaining high isolation.
A frequency-dependent resistor and circuitry employing the same are provided. In some embodiments, a resistor includes a substrate, an input port, an output port, and a conductive trace on the substrate between the input port and the output port. A resistance between the input port and the output port for a low frequency signal is at least five times lower than the resistance between the input port and the output port for an RF signal, and the ratio of the frequencies of the RF signal to the low frequency signal is at least fifty.
In some embodiments, circuitry includes at least one transistor with an input coupled to a source of the at least one transistor and an output coupled to a drain of the at least one transistor. The at least one transistor is adapted to selectively couple the input to the output in response to a control signal provided via at least one resistor. The at least one resistor has resistance for a low frequency signal at least five times lower than the resistance for an RF signal. This circuitry will have a reduced switching time while still isolating the RF signal.
Those skilled in the art will appreciate the scope of the present disclosure and realize additional aspects thereof after reading the following detailed description of the preferred embodiments in association with the accompanying drawing figures.
The accompanying drawing figures incorporated in and forming a part of this specification illustrate several aspects of the disclosure, and together with the description serve to explain the principles of the disclosure.
A Radio Frequency (RF) switch with reduced switching time using skin-effect resistors is provided. In some embodiments, a resistor includes a substrate, an input port, an output port, and a conductive trace on the substrate between the input port and the output port. A resistance between the input port and the output port for a low frequency signal is at least five times lower than the resistance between the input port and the output port for an RF signal.
The embodiments set forth below represent the necessary information to enable those skilled in the art to practice the embodiments and illustrate the best mode of practicing the embodiments. Upon reading the following description in light of the accompanying drawing figures, those skilled in the art will understand the concepts of the disclosure and will recognize applications of these concepts not particularly addressed herein. It should be understood that these concepts and applications fall within the scope of the disclosure and the accompanying claims.
This difference in the resistivity of the resistor R is due to the use of materials that exhibit a frequency-dependent resistance. According to some embodiments, this is achieved by using a material with both high resistivity and a high magnetic permeability. Magnetic permeability (μ) is measured in Henries/meter (H/m). For instance, the magnetic permeability of a vacuum is 4π×10−7 H/m and is referred to as μ0. The relative magnetic permeability of a substance is given by its magnetic permeability divided by μ0. In some embodiments, the conductive trace 14 has a relative magnetic permeability of at least 100, meaning that its magnetic permeability is at least 100 times larger than that of a vacuum. In other embodiments, the conductive trace has a relative magnetic permeability of at least 1000. In some embodiments, the conductive trace 14 includes at least one of Iron, Cobalt, Nickel, or a combination of one of these.
A high relative magnetic permeability leads to an increase in the Skin-Effect. This usually undesirable effect is caused due to the rapidly fluctuating magnetic field in the conductive trace 14 when an alternating current (AC) signal is applied. The higher the frequency of the signal, the more rapidly the magnetic field changes. This causes charge carriers to be limited to the skin of the conductive trace 14. The higher the frequency of the signal, the shallower the skin depth of the charge carriers becomes in the conductive trace 14. The shallower skin depth creates a reduced cross-sectional area of the conductive trace 14 that is available for charge carriers. This leads to a higher resistance of the conductive trace 14.
In one embodiment of the resistor R, the resistance between the input port 16 and the output port 18 for a signal at or below 10 MHz is at most 10 kilohms (kΩ), and the resistance between the input port and the output port for a signal at or above 1 GHz is at least 100 kΩ.
By applying the control voltages SW1 and SW2 through the resistors R which have resistance for a low frequency signal at least five times lower than the resistance for an RF signal, the RF switch 24 has a reduced switching time for the same level of RF isolation. This is because the control voltages SW1 and SW2 are DC signals, which have a frequency of zero. In practice, when the RF switch 24 is being switched from the RF1 port to the RF2 port rapidly, the control signals SW1 and SW2 essentially behave as low frequency signals. Since the resistance exerted on these control signals by the one or more resistors R is lower for a low frequency signal, the RC time constant for switching is reduced. However, the resistance exerted on the RF signals as they attempt to leak out into the control circuits is at least at least five times higher. This provides increased isolation of the RF signals and reduces the amount of energy lost into the control circuits. In some embodiments, an RC time constant of the at least one FET 22 and the at least one resistor R is less than or equal to 10 microseconds (μs) while still providing a high level of isolation.
The previous embodiments can be implemented with any resistor wherein a resistance between the input port and the output port for a low frequency signal is at least five times lower than the resistance between the input port and the output port for a RF signal. As discussed above, one way of accomplishing this is to use a resistor with a conductive trace that has a high relative magnetic permeability.
In contrast, the magnetic permeability of Nickel (Ni) is between 1.26×10−4-7.54×10−4 H/m or a relative magnetic permeability of approximately 100-600. As such, the plot of the trace resistance ratio of Ni in
By using a material with a high magnetic permeability to create a resistor, the resistor may have a resistance between the input port and the output port for a low frequency signal that is at least five times lower than the resistance between the input port and the output port for an RF signal. By using a resistor with this frequency-dependent resistance, an RF switch can be made with a reduced switching time while maintaining a high isolation. Such a switch can be used in several places in an RF transmitter to increase the performance of the RF transmitter.
When receiving, the RF front end circuitry 26 performs a similar process but in reverse. Although, where the transmitted signal passed through one or more of the plurality of power amplifiers 30A-30N, where it was amplified and delivered through the duplexer circuitry 34 to the antenna switching circuitry 36, the received signal is delivered through the duplexer circuitry 34 to pass through one or more of a plurality of low-noise amplifiers 32A-32N.
A resistor R of
Those skilled in the art will recognize improvements and modifications to the preferred embodiments of the present disclosure. All such improvements and modifications are considered within the scope of the concepts disclosed herein and the claims that follow.
This application claims the benefit of provisional patent application Ser. No. 62/186,775, filed Jun. 30, 2015, the disclosure of which is hereby incorporated herein by reference in its entirety.
Number | Name | Date | Kind |
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20030107465 | Hiraoka | Jun 2003 | A1 |
20100245030 | Ikeda | Sep 2010 | A1 |
20130113575 | Easter | May 2013 | A1 |
Entry |
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M. Rezaei, “A New Frequency Dependent Resistor for Modeling Skin Effect of Wire and Echo Cancellation by PSO”, Apr. 2010, IEEE. |
Number | Date | Country | |
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20170004909 A1 | Jan 2017 | US |
Number | Date | Country | |
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62186775 | Jun 2015 | US |