The present invention is directed to resonators for oscillator circuits and more specifically to resonators for use in low radiation oscillators.
Zero intermediate frequency (ZIF) or very low intermediate frequency (IF) architecture is taking the place of heterodyne conversion architecture in many wireless applications. ZIF architecture provides low part count, simple frequency plan, and immunity to system noise (such as digital switching noise or spurious noise).
However, ZIF architecture has a major disadvantage, both in receive and transmit chains because the local oscillator (LO) frequency is very close to that of the signal on the antenna (both received and transmitted). Leakage of the LO in the receive case generates a direct current (DC) level in the receiver output. This DC level is not static, and requires increased dynamic range of an analog to digital converter or sophisticated cancellation techniques in some standards (such as Global System for Mobile Communications (GSM)). In the transmit case, the LO leakage may override the signal transmitted to the antenna (such as in wireless code division multiple access (W-CDMA) systems where transmit levels may reach down to −40 decibels (dBm)). In any transmit case, there may be a problem of LO pulling by the transmitted signal, due to radiation coupling.
While certain techniques are used to reduce these phenomena, certain drawbacks exist. Frequency division or multiplication is the most common technique, however this results in a higher current drain and circuit area and a limited noise floor. Other techniques utilize polar feedback to cope with transmitter effects, and cause the same current/area (and therefore cost) penalty.
Thus there is a need for a local oscillator with lower radiation to prevent leakage and pulling.
In various embodiments of the present invention, an electroacoustic resonator may be used in a local oscillator. In certain embodiments, such an electroacoustic resonator may avoid antenna-to-antenna coupling caused by using an electromagnetic resonator in the LO. The cause for such coupling between the antenna (or the devices that are attached to it such as the antenna switch or the transmit filter) and the LO is that the electromagnetic resonator is an LC (i.e., an inductor-capacitor) circuit. The inductor in such an electromagnetic resonator is actually a miniature antenna, and thus may couple to the antenna.
In certain embodiments, an electroacoustic resonator may be made from quartz, ceramic, or a surface acoustic wave (SAW) resonator, for example. In certain embodiments using such resonators, the resonator may be located off of a substrate supporting the LO.
In other embodiments, a thin film bulk acoustic resonator (F-BAR) may be used in a local oscillator. Such an F-BAR resonator may be made using conventional microelectromechanical systems (MEMS) manufacturing techniques. Further, in certain embodiments an F-BAR resonator may be incorporated in a wireless chip. For example, the F-BAR resonator may be mounted to the substrate of the LO and be housed within the same package as the LO (i.e., in the wireless chip). In other embodiments, the F-BAR resonator may be outside a wireless chip housing the LO.
Referring now to
Following the receive signal path, antenna 20 may be coupled through duplexer 25 to a filter 30 and an amplifier 35, in one embodiment. After such filtering and amplification, the incoming signal may be mixed via a complex (IQ) mixer 45 with outputs of a local oscillator 50. As shown in the embodiment of
In certain embodiments, local oscillator 50 may be operated at a frequency substantially identical to the frequency of incoming signals. In such manner, complex mixer 45 may convert incoming signals to zero intermediate frequency signals. In the embodiment of
While wireless device 10 shown in
In embodiments of the present invention, it may be desirable to avoid antenna coupling between antenna 20 and local oscillator 50. As discussed above, an LC circuit used in local oscillator 50 may cause such antenna to antenna coupling to occur. Thus in embodiments of the present invention, an electroacoustic resonator may be used in local oscillator 50 in place of an LC circuit.
Referring now to
As shown in
As discussed above, in various embodiments electroacoustic resonator 110 may be a quartz, ceramic, SAW, or F-BAR resonator. Also coupled in parallel may be a varactor network having first varactor D1 and a second varactor D2. The node connecting the varactors may be coupled to a resistor R3, which may have values between 10 and 100 kiloOhm (kOhm), in certain embodiments. A voltage Vtune may tune local oscillator 100 to a desired frequency, in certain embodiments.
In certain embodiments, local oscillator 100 may operate such that it oscillates at a frequency substantially identical to a frequency of an antenna to which it is coupled. As such, local oscillator 100 may appropriately be mixed with RF signals received from the antenna to obtain zero or near zero intermediate frequency signals for processing. Similarly, local oscillator 100 may be mixed with baseband signals to upconvert them to a desired radio frequency for transmission.
Referring now to
A resistor R1 may be coupled to a node coupling varactors D1 and D2, and in certain embodiments may be a 10 to 100 kOhm resistor. Voltage Vtune may tune oscillator 200 to a desired frequency, in certain embodiments. As discussed above regarding the local oscillator of
While the present invention has been described with respect to a limited number of embodiments, those skilled in the art will appreciate numerous modifications and variations therefrom. It is intended that the appended claims cover all such modifications and variations as fall within the true spirit and scope of this present invention.
Number | Name | Date | Kind |
---|---|---|---|
5355524 | Higgins, Jr. | Oct 1994 | A |
5903820 | Hagstrom | May 1999 | A |
6204737 | Ella | Mar 2001 | B1 |
6307440 | Shimanuki | Oct 2001 | B1 |
6479921 | Ma et al. | Nov 2002 | B2 |
6724804 | Kegasa et al. | Apr 2004 | B1 |
6744829 | Mohindra | Jun 2004 | B1 |
7035341 | Mohindra | Apr 2006 | B2 |
20040137870 | Kivekas et al. | Jul 2004 | A1 |
20040227578 | Hamalainen | Nov 2004 | A1 |
Number | Date | Country | |
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20040180640 A1 | Sep 2004 | US |