Mobile phones and other wireless devices may generate spurious emissions due to nonlinear response characteristics of their component parts. For example,
Referring to
Filters 115 (or alternatively, duplexers or multiplexers) may be implemented by acoustic resonators, such as Surface Acoustic Wave (SAW) resonators, Bulk Acoustic Wave (BAW) resonators, Film Bulk Acoustic Wave Resonators (FBARs). These acoustic resonators typically generate spurious output signals at second or third harmonics of a transmit carrier frequency due to nonlinearity of a piezoelectric material contained therein. In general, it is desirable to reduce these and other spurious emissions to improve the quality of communication and to avoid interfering with other communications.
One conventional method for canceling the second harmonic power (H2) generated by an acoustic resonator device is to cross connect two parallel, equal area resonators, called a splitbar. Another conventional method, called a powerbar, uses two equal area resonators in series, where each resonator has twice the area of the original device, and the resonators are connected to with opposing piezoelectric orientations. The powerbar method is effective but increases the total area of the filter, increasing the cost.
In view of the above shortcomings of conventional technologies, there is a general need for improved filter and multiplexer circuits in which H2 generation is reduced without an increase in the area of acoustic resonator devices in each filter or the size of a multiplexer module.
The example embodiments are best understood from the following detailed description when read with the accompanying drawing figures. It is emphasized that the various features are not necessarily drawn to scale. In fact, the dimensions may be arbitrarily increased or decreased for clarity of discussion. Wherever applicable and practical, like reference numerals refer to like elements.
In the following detailed description, for purposes of explanation and not limitation, example embodiments disclosing specific details are set forth in order to provide a thorough understanding of the present teachings. However, it will be apparent to one having ordinary skill in the art having the benefit of the present disclosure that other embodiments according to the present teachings that depart from the specific details disclosed herein remain within the scope of the appended claims. Moreover, descriptions of well-known apparatuses and methods may be omitted so as to not obscure the description of the example embodiments. Such methods and apparatuses are clearly within the scope of the present teachings.
The terminology used herein is for purposes of describing particular embodiments only, and is not intended to be limiting. The defined terms are in addition to the technical, scientific, or ordinary meanings of the defined terms as commonly understood and accepted in the relevant context.
The terms ‘a’, ‘an’ and ‘the’ include both singular and plural referents, unless the context clearly dictates otherwise. Thus, for example, ‘a device’ includes one device and plural devices. The terms ‘substantial’ or ‘substantially’ mean to within acceptable limits or degree. The term ‘approximately’ means to within an acceptable limit or amount to one of ordinary skill in the art. Relative terms, such as “above,” “below,” “top,” “bottom,” “upper” and “lower” may be used to describe the various elements' relationships to one another, as illustrated in the accompanying drawings. These relative terms are intended to encompass different orientations of the device and/or elements in addition to the orientation depicted in the drawings. For example, if the device were inverted with respect to the view in the drawings, an element described as “above” another element, for example, would now be below that element. Other relative terms may also be used to indicate the relative location of certain features along a path such as a signal path. For instance, a second feature may be deemed to “follow” a first feature along a signal path if a signal transmitted along the path reaches the second feature before the second feature.
The described embodiments relate generally to multiplexers comprising acoustic resonator based filters in which second or higher order harmonic generation is suppressed at an antenna port (or some other common node) by tuning an output impedance of each filter to a series resonance at or near to a second harmonic frequency of one or more other filters. For example, in certain embodiments a diplexer (i.e., a 1:2 multiplexer) comprises a first filter and a second filter, wherein an impedance of the first filter is tuned to resonate at a second harmonic frequency of the second filter, and an impedance of the second filter is tuned to resonate at a second harmonic frequency of the first filter. A series resonant or harmonic trap for each filter circuit can be implemented using an antenna side series input inductance (LTx), a capacitance of a first series FBAR resonator on the antenna side (Cs1), a capacitance of a first shunt FBAR resonator on the antenna side (Ch1), and PCB inductance from a first shunt FBAR on the antenna side to a module ground (L1). The series combination of LTX, Cs1, Ch1, and L1 forms a series resonant circuit. The PCB inductance to ground L1 can be adjusted during a design process to achieve a desired resonant frequency at the second harmonic of an opposing filter.
The combination of multiple tuned output impedances can potentially reduce H2 emissions to power levels lower than for a single harmonic trap, and without increasing the size, cost, or adding external components to the multiplexer module.
Referring to
The harmonic trap circuit may be tuned to a series resonance (low impedance) at the second harmonic of a filter operating band, for example. The trap may present a low impedance at the second harmonic, which results in a mismatch to the load of the filter, and therefore reduced harmonic power at the antenna or load.
Ladder filter 205 is typically implemented in a module that is mounted on a printed circuit board (PCB), and the external harmonic trap is typically implemented by surface mount components placed on the PCB or integrated into layers of the PCB. Examples of such implementations are illustrated in
Referring to
The high power signals from TX filter 305A generate harmonics at a TX filter output due to nonlinearity of devices in TX filter 305A, including acoustic resonators. To suppress the harmonics generated by TX filter 305A, an output impedance of RX filter 310A is tuned to create a short circuit at the second (or third) harmonic of the TX band. This, in turn, reduces the harmonic power delivered to the antenna port.
Referring to
One significant difference between the harmonic trap of
Referring to
The silicon die, in combination with the inductor traces and via inductances, can be used to implement a duplexer module with harmonic traps, as illustrated in
Referring to
Capacitances Cseries and Cshunt, in combination with input inductance LTXinput and shunt inductance Lshunt, are used to implement a harmonic trap, or LC series resonance, at the second harmonic of an adjacent filter in a multiplexer. At frequencies far removed from a piezoelectric resonance frequency of the FBAR devices, the FBAR devices are electrically equivalent to capacitors, which the capacitance approximately equal to the plate capacitance of the device.
The following analysis describes the function of RX filter 310A based on the equivalent circuits shown in
The input impedance of the RX filter has a series resonance at frequency fres described by the following equation (1).
At the series resonance frequency fres, assuming that the losses of the resonant circuit are dominated by the equivalent series resistances Rtx and Rshunt of inductors LTXinput and Lshunt, the input impedance of the filter at fres is described by the following equation (2).
R
res
=R
tx
+R
shunt (2)
For the purpose of simplifying the analysis of the harmonic trap circuit, it is assumed that the output impedance of the TX filter at frequency fres is a real impedance Rout, and that the antenna port impedance at frequency fres is a real impedance Rant. The simplified circuit is shown in
In the absence of the harmonic trap, the power at the antenna port depends on the ratio of the filter output impedance Rtxout to the antenna impedance Rant, assuming the RX filter with no harmonic trap is an effective open circuit at frequency fres, as indicated approximately by the following equation (3).
On the other hand, with the harmonic trap circuit, most of the harmonic power is shorted to ground, and the harmonic power at the antenna port is described by the following equation (4).
The parallel resistance of the series resonance and the antenna impedance is described by the following equation (5).
Assuming the series resistance of the harmonic trap Rres is much less than the antenna impedance Rant, the harmonic power is described by the following equation (6).
For example, assuming that at the second harmonic frequency, the equivalent series resistance of the harmonic trap is 3 Ohms, the antenna impedance is 50 Ohms, and the TX filter output impedance is 15 Ohms. Then by implementing the harmonic trap, the second harmonic power at the antenna is reduced by approximately 13 dB.
Referring to
Each of first and second filters 505 and 510 has substantially the same structure as RX filter 310A of
During typical operation, both first filter 505 and second filter 510 may be used to transmit RF power to the antenna, and second harmonic generation of each transmit filter is suppressed by the harmonic trap implemented at the antenna side of the adjacent filter. The inclusion of the harmonic trap in each filter will typically have little or no impact on the size of a module including the diplexer. The tuned inductors Lseries and Lshunt in first and second filters 505 and 510 can be implemented as integrated components on a PCB board of the module, similar to the implementation of module 300C shown in
In an illustrative example, suppose first filter 505 has an operating frequency of f1 and a second harmonic at 2f1. The harmonic trap of second filter 510 may then be tuned to have low impedance at 2f1 to remove the second harmonic of first filter 505. Similarly, suppose second filter 510 has an operating frequency of f2 and a second harmonic at 2f2. The harmonic trap of first filter 505 may then be tuned to have low impedance at 2f2 to remove the second harmonic of second filter 510.
Referring to
First filter 605 is a TX filter connected between a first PA port (“PA Port 1”) and antenna matching network 615, second filter 610 is a TX filter connected between a second PA port (“PA Port 2”) and antenna matching network 615, and N-th filter 620 is a TX filter connected between an N-th PA port (“PA Port N”) and antenna matching network 615. For explanation purposes, it will be assumed that the first through N-th filters operate as transmit filters, although they could additionally or alternatively operate as receive filters. For example in a typical multiplexer, a single filter may be used to filter both transmitted and received signals over a particular frequency band.
The filters in multiplexer 600 may be similar to those of diplexer 500. In addition, the operation of multiplexer 600 may be similar to that of diplexer 500, except that the harmonic trap in each filter may be tuned according to an operating frequency of any of the other filters, not necessarily the one directly adjacent. For instance, in a quadplexer (i.e., N=4), the harmonic trap of first filter 605 could be tuned according to an operating frequency of a third or fourth filter, and vice versa.
The data shown in
Referring to
Referring to
While example embodiments are disclosed herein, one of ordinary skill in the art appreciates that many variations that are in accordance with the present teachings are possible and remain within the scope of the appended claims. The embodiments therefore are not to be restricted except within the scope of the appended claims.