Acoustic resonator performance enhancement using alternating frame structure

Abstract
Disclosed is an acoustic resonator that includes a substrate, a first electrode, a layer of piezoelectric material, a second electrode, and an alternating frame region. The first electrode is adjacent the substrate, and the first electrode has an outer perimeter. The piezoelectric layer is adjacent the first electrode. The second electrode is adjacent the piezoelectric layer and the second electrode has an outer perimeter. The alternating frame region is on one of the first and second electrodes.
Description
BACKGROUND

The need to reduce the cost and size of electronic equipment has created a need for smaller single filtering elements. Thin-Film Bulk Acoustic Resonators (FBARs) and Stacked Thin-Film Bulk Wave Acoustic Resonators (SBARs) represent one class of filter elements with potential for meeting these needs. These filters can collectively be referred to as FBARs. An FBAR is an acoustic resonator that uses bulk longitudinal acoustic waves in thin-film piezoelectric (PZ) material. Typically, an FBAR includes a layer of PZ material sandwiched between two metal electrodes. The combination PZ material and electrodes are suspended in air by supporting the combination around its perimeter or are placed over an acoustic mirror.


When an electrical field is created between the two electrodes, the PZ material converts some of the electrical energy into mechanical energy in the form of acoustic waves. The acoustic waves propagate generally in the same direction as the electric field and reflect off the electrode-air or electrode-acoustic mirror interface at some frequency, including at a resonance frequency. At the resonance frequency, the device can be used as an electronic resonator. Multiple FBARs can be combined such that each is an element in RF filters.


Ideally, the resonant energy in the filter elements is entirely “trapped” in the resonator. In practice, however, dispersive modes exist. These modes can result in a decreased quality factor (Q) for the filter.


For these and other reasons, a need exists for the present invention.


SUMMARY

One aspect of the present invention provides an acoustic resonator that includes a substrate, a first electrode, a layer of piezoelectric material, a second electrode, and an alternating frame region. The first electrode is adjacent the substrate, and the first electrode has an outer perimeter. The piezoelectric layer is adjacent the first electrode. The second electrode is adjacent the piezoelectric layer and the second electrode has an outer perimeter. The alternating frame region is on one of the first and second electrodes.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 illustrates a top plan view of an FBAR.



FIG. 2 illustrates a cross-sectional view of an FBAR.



FIG. 3 illustrates a cross-sectional view of an FBAR with an alternating frame region according to one embodiment of the present invention.



FIG. 4 illustrates a top plan view of one embodiment of the FBAR illustrated in FIG. 3.



FIG. 5 illustrates a cross-sectional view of an FBAR with an alternating frame region according to one embodiment of the present invention.



FIG. 6 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIG. 7 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIG. 8 illustrates a cross-sectional view of an FBAR with an alternating frame region according to one embodiment of the present invention.



FIG. 9 illustrates a cross-sectional view of an FBAR with an alternating frame region according to one embodiment of the present invention.



FIG. 10 illustrates Q circles for two exemplary FBARs plotted on a Smith chart.



FIG. 11 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIG. 12 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIG. 13 illustrates a cross-sectional view of an FBAR with an alternating frame region according to one embodiment of the present invention.



FIG. 14 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIG. 15 illustrates a cross-sectional view of an FBAR with an alternating frame region according to another embodiment of the present invention.



FIGS. 16A-16C are cross-sectional views illustrating various stages of fabrication of an FBAR with an alternating frame region according to one embodiment of the present invention.





DETAILED DESCRIPTION

In the following Detailed Description, reference is made to the accompanying drawings, which form a part hereof, and in which is shown by way of illustration specific embodiments in which the invention may be practiced. In this regard, directional terminology, such as “top,” “bottom,” “front,” “back,” “leading,” “trailing,” etc., is used with reference to the orientation of the Figure(s) being described. Because components of embodiments of the present invention can be positioned in a number of different orientations, the directional terminology is used for purposes of illustration and is in no way limiting. It is to be understood that other embodiments may be utilized and structural or logical changes may be made without departing from the scope of the present invention. The following detailed description, therefore, is not to be taken in a limiting sense, and the scope of the present invention is defined by the appended claims.



FIGS. 1 and 2 illustrate top and cross-sectional views, respectively, of FBAR 10. FBAR 10 includes substrate 12, depression 14, first electrode 16, piezoelectric (PZ) layer 18, and second electrode 20. In FIG. 1, PZ layer 18 and depression 14 are hidden from view. Second electrode 20 has a perimeter that is illustrated in FIG. 1 as pentagon-shaped, having edges 20a, 20b, 20c, 20d and 20e. Two edges, 20b and 20e, are illustrated in the cross-sectional view of FIG. 2. Typically, contacts (not illustrated) are coupled to first electrode 16 and to second electrode 20 and a passivation layer (not illustrated) may cover top electrode 20. The contacts facilitate connecting the first and second electrodes 16 and 20 to a source of voltage.


First electrode 16, PZ layer 18, and second electrode 20 collectively form an FBAR membrane. The FBAR membrane is adjacent substrate 12 and suspended over depression 14 to provide an electrode-air interface. In one embodiment, depression 14 is created by etching away a portion of substrate 12. Depression 14 is deep enough so that sufficient electrode-air interface is created under the FBAR membrane.


In an alternative embodiment, the FBAR membrane may be placed adjacent an acoustic mirror (not illustrated in FIGS. 1 and 2) formed within substrate 12. In this way, an electrode-acoustic mirror interface is formed. The resonator thus formed is a Solid Mounted Resonator (SMR).


In one embodiment, substrate 12 is made of silicon (Si) and PZ layer 18 is made from aluminum nitride (AlN). Alternatively, other piezoelectric materials may be used for PZ layer 18. In one embodiment, first and second electrode 16 and 20 may be made of molybdenum (Mo). Alternatively, other materials may be used for the electrodes. In one embodiment, the contacts may be made of gold (Au). Alternatively, other materials may be used for the contacts.


FBAR 10 illustrated in FIGS. 1 and 2 is configured to use longitudinal or shear acoustic waves propagating in PZ layer 18. An electric field is created between first and second electrodes 16 and 20 via an impressed voltage. The piezoelectric material of PZ layer 18 then converts some of the electrical energy into mechanical energy in the form of acoustic waves. So configured, FBAR 10 exhibits dispersive modes resulting in a quality factor (Q) loss for FBAR 10.



FIG. 3 illustrates a cross-sectional view of FBAR 40 in accordance with one embodiment of the present invention. FBAR 40 includes substrate 42, depression 44, first electrode 46, piezoelectric (PZ) layer 48, second electrode 50 first frame 60 and second frame 62. Typically, contacts (not illustrated in FIG. 3) are coupled to first and second electrodes 46 and 50, and a passivation layer typically covers the second electrode (also not illustrated in FIG. 3). The contacts facilitate connecting first and second electrodes 46 and 50 to a voltage source. First electrode 46, PZ layer 48, and second electrode 50 collectively form an FBAR membrane, which may be placed over a depression 44 or over an acoustic mirror as discussed above. The FBAR membrane is illustrated adjacent substrate 42 and suspended over depression 44 to provide an electrode-air interface. As with previous embodiments, an electrode-acoustic mirror interface is also obtainable using an SMR design in accordance with the present invention.


Second electrode 50 and the other layers of the FBAR membrane have a perimeter that can be of various configurations. For example, the perimeters of each can be pentagon-shaped, similar to FBAR 10 above. They could also be any of various polygonal shapes, circular, or various irregular shapes. The cross-sectional view illustrated in FIG. 3 illustrates two locations along the perimeter of second electrode 50, edges 50b and 50e. In one embodiment, an edge of PZ layer 48 is generally aligned with edges 50b and 50e of second electrode 50 in the vertical direction in FBAR 40 as illustrated in FIG. 3.


In FBAR 40 illustrated in FIG. 3, second electrode 50 includes first frame 60 and second frame 62 added around the perimeter of the electrode and shown adjacent edges 50b and 50e of second electrode 50. In one embodiment, first and second frames 60 and 62 are located just outside the perimeter of depression 44. In this way, when the perimeter or outside diameter of depression 44 is extended in the vertical direction (as oriented in the illustration of FIG. 3), first and second frames 60 and 62 are just “outside” the perimeter of depression 44. In other embodiments, first and second frames 60 and 62 overlap the perimeter of depression 44 such that portions of first and second frames 60 and 62 are “inside” and portions are “outside” the perimeter of depression 44. In other embodiments, first and second frames 60 and 62 are located just inside the perimeter of depression 44. In this way, when the perimeter or outside diameter of depression 44 is extended in the vertical direction (as oriented in the illustration of FIG. 3), first and second frames 60 and 62 are just “inside” the perimeter of depression 44.


First and second frames 60 and 62 form an alternating frame region. In the alternating frame region, first and second frames 60 and 62 are spaced apart in order to achieve a multiple periodic pattern consisting of the frames having spaces between them. In this way, a material having a first acoustic impedance (first frame 60) is followed by a region with different acoustic impedance (illustrated as air in FIG. 3). Second frame 62 spaced apart from first frame 60 adds another element to the periodic pattern with another interface of differing acoustic impedance. By building alternating regions of different impedances with the alternating frame region, certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to provide improved Q.


In one embodiment, this alternating frame region of first and second frames 60 and 62 further forms a distributed Bragg reflector (DBR) structure. In this way, the width (left to right in the illustration) of each of first and second frames 60 and 62 within the alternating frame region, as well as the widths of the areas of space between them, is roughly one-quarter wavelength of at least one of the lateral acoustic modes. In another embodiment, the width of each component of the periodic pattern is a multiple of one-quarter wavelength of at least one of the lateral acoustic modes. In one case, the width of each component of the periodic pattern is one-quarter wavelength of the dominant lateral mode. In this way, FBAR 40 with the alternating frame region structure performs as a high efficiency mirror.


In addition to the alternating frame region trapping certain modes, in some embodiments either first frame 60 or second frame 62 may also provide a thicker region at the outer edge of FBAR 40 (around the perimeter of the electrode and shown adjacent second electrode edges 50b and 50e) thereby providing more stiffness at that boundary. In this way, additional energy trapping occurs due to the effect of having a thicker frame at the edge.


In some embodiments, first frame 60 and/or second frame 62 is a material selected from the croup comprising dielectrics, metals, metal alloys. piezoelectrics, Mo, Pt, Al, Cu, W, Au, Ag, polyimide, benzocyclobutene (BCB), SiO2, Si3N4, ZnO, LiNbO3, PZT, LiTaO3, and AI203.



FIG. 4 illustrates a plan view of FBAR 40 of FIG. 3 in accordance with an embodiment of the present invention. As illustrated in FIG. 4, FBAR 40 includes substrate 42, first electrode 46, and second electrode 50. In FIG. 4, piezoelectric (PZ) layer 48 and depression 44 are hidden from view. Typically, contacts (not illustrated in the Figures) are coupled to first and second electrodes 46 and 50, and a passivation layer (also not illustrated in the Figures) covers second electrode 50.


In FIG. 4, first and second frames 60 and 62 are illustrated extending adjacent the perimeter of second electrode 50. In FIG. 4, the perimeter of second electrode 50 is generally pentagon-shaped having five relatively straight edges (50a, 50b, 50c, 50d, and 50e), but in alternative embodiments can be essentially any polygonal shape, circular in shape, or have any other smooth or irregular shape.


In FIG. 4, first and second frames 60 and 62 are illustrated extending adjacent the perimeter of second electrode 50 along four of the five edges of the pentagon-shaped electrode, that is, adjacent edges 50b, 50c, 50d, and 50e. In one embodiment, a contact is attached to the fifth edge 50a of second electrode 50, so first and second frames 60 and 62 do not extend along that edge in that embodiment. In alternative embodiments, however, first and second frames 60 and 62 extend adjacent the perimeter of second electrode 50 along all of the five edges of the pentagon-shaped electrode, for example, adjacent edges 50a, 50b, 50c, 50d, and 50e.


As one skilled in the art will understand, any number of alternative first and second frames 60 and 62 can be provided adjacent the edges of second electrode 50 to form the alternating frame region consistent with the present invention. First and second frames 60 and 62 can be continuously extended along some or all of the edges of second electrode 50 as illustrated, first and second frames 60 and 62 can have smaller segments that are not continuous along the edge, and other shapes and configurations of first and second frames 60 and 62 can be used, especially where second electrode 50 is a shape other than a pentagon.


In addition to the alternating frame region having first and second frames 60 and 62 illustrated in FIGS. 3 and 4, multiple alternating frame structures may be employed. In some embodiments, each alternating frame structure forms a DBR structure having regions with widths that correspond to quarter wavelengths or multiples of quarter wavelengths of different lateral modes. These alternative embodiments can also be configured such that the reflected wavelengths interfere constructively to trap the primary and/or other lateral modes to produce an improved performing FBAR. In addition, they may be configured to provide stiffening at the edges of the FBAR providing further mode trapping thereby enhancing FBAR performance. In some embodiments, the alternating frame region has areas of thicknesses that extend above the electrode surface, followed by regions that have the same thickness as the electrode (see FIG. 3). In other embodiments, the alternating regions of the alternating frame structure have thicknesses that extend above the electrode surface, followed by regions that have thickness that is thinner than the electrode.



FIG. 5 illustrates a cross-sectional view of FBAR 70 in accordance with an alternative embodiment of the present invention. FBAR 70 is similar to that illustrated in FIG. 3, and includes substrate 72, depression 74, first electrode 76, piezoelectric (PZ) layer 78, second electrode 80 and first and second frames 90 and 92.


In one embodiment, the performance of FBAR 70 as illustrated in FIG. 5 is similar to that described above for FBAR 40 as depicted in FIG. 3. In this way, first and second frames 90 and 92 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region, certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. In one embodiment, all of the reflected wavelengths interfere to improve Q. In one embodiment, the alternating frame region of FBAR 70 is constructed as a DBR structure such that the width of each component of the alternating pattern is a multiple of one-quarter wavelength of at least one of the lateral acoustic modes.


In addition, first frame 90 is wider than second frame 92 in FBAR 70. Consequently, this wider region of first frame 90 provides more stiffness at the edge of FBAR 70 such that it acts like a hard boundary, thereby providing good energy trapping. This further improves the performance of FBAR 70.



FIG. 6 illustrates a cross-sectional view of an alternative FBAR 100 in accordance with one embodiment of the present invention. FBAR 100 is similar to those illustrated above, and includes substrate 102, depression 104, first electrode 106, piezoelectric (PZ) layer 108, second electrode 110 and first and second frames 120 and 122.


In one embodiment, the performance of FBAR 100 as illustrated in FIG. 6 is similar to those illustrated above, in that first and second frames 120 and 122 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 120 and 122 separated by air in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region, in one embodiment, is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 100, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 100 is constructed as a DBR structure.


In addition, first frame 120 and second frame 122 are separated by a region of second electrode 110 that is thinner than are the remaining portions of second electrode 110. Furthermore, frame 120 provides stiffness at the edge of FBAR 100 providing additional energy trapping, which further improves its performance.



FIG. 7 illustrates a cross-sectional view of an alternative FBAR 130 in accordance with one embodiment of the present invention. FBAR 130 is similar to those illustrated above, and includes substrate 132, depression 134, first electrode 136, piezoelectric (PZ) layer 138, second electrode 140 and first and second frames 150 and 152.


In one embodiment, the performance of FBAR 130 as illustrated in FIG. 7 is similar to those illustrated above, in that first and second frames 150 and 152 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 150 and 152 separated by air in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 130, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 130 is constructed as a DBR structure.


In addition, first frame 150 and second frame 152 are separated by a region of second electrode 140 that is thicker than are the remaining portions of second electrode 140. Furthermore, frame 150 and the raised region (that is, raised relative to the surface of second electrode 140) between frames 150 and 152 provide stiffness at the edge of FBAR 130 providing additional energy trapping, which further improves its performance.



FIG. 8 illustrates a cross-sectional view of an alternative FBAR 160 in accordance with one embodiment of the present invention. FBAR 160 is similar to those illustrated above, and includes substrate 162, depression 164, first electrode 166, piezoelectric (PZ) layer 168, second electrode 170 and frame 172.


In one embodiment, the performance of FBAR 160 as illustrated in FIG. 8 is similar to those illustrated above, in that frame 172, combined with adjacent recessed region on either side, forms an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frame 172 and recessed regions immediately adjacent frame 172 on either side in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change with some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 160 and improving its performance. In one embodiment, the alternating frame region of FBAR 160 is constructed as a DBR structure.


In addition, frame 172 is the same thickness as the remaining portions of second electrode 170, while the recessed regions immediately adjacent frame 172 are thinner than the remaining portions of second electrode 170. Furthermore, frame 172 provides stiffness at the edge of FBAR 160 providing additional energy trapping, which further improves its performance.



FIG. 9 illustrates a cross-sectional view of an alternative FBAR 175 in accordance with one embodiment of the present invention. FBAR 175 is similar to those illustrated above, and includes substrate 176, depression 177, first electrode 178, piezoelectric (PZ) layer 179, second electrode 180 and frame 182.


In one embodiment, the performance of FBAR 175 as illustrated in FIG. 9 is similar to those illustrated above, in that frame 182, combined with adjacent recessed region on either side, forms an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frame 182 and recessed regions immediately adjacent frame 182 on either side in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change with some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 175 and improving its performance. In one embodiment, the alternating frame region of FBAR 175 is constructed as a DBR structure.


In addition, frame 182 is the thicker than the remaining portions of second electrode 180, while the recessed regions immediately adjacent frame 182 are thinner than the remaining portions of second electrode 180. Furthermore, frame 182 adjacent the recessed region provides stiffness at the edge of FBAR 175 providing additional energy trapping, which further improves its performance.



FIG. 10 illustrates Q circles for two exemplary FBARs plotted on a Smith chart, and illustrates improvement in Rp and therefore Q in one of the FBARs. As is known in the art, a Smith Chart is a polar plot of a complex impedance (used in FIG. 10 to illustrate measures of s11 and s22 scattering parameters). These s11 and s22 scattering parameters represent a ratio of complex amplitudes of backward and forward waves. The Smith Chart aids in translating the reflection coefficients into impedance and it maps part of the impedance placed into a unit circle.


The improved performance of FBAR 175 is demonstrated by the Q circles illustrated in FIG. 10. FIG. 10 illustrates the S-parameter measurements of an exemplary FBAR device, such as FBAR 175 with an alternating frame region. As illustrated, the alternating frame region of FBAR 175 (solid line labeled s11) has a much improved Rp versus that of a control device, such as that illustrated in FIG. 2 (dashed line labeled s22) in the upper half of the chart.


Generally, the horizontal axis passing through the unit circle represents real impedance, the area above the axis represents inductive reactance and the area below represents capacitive reactance. The left-hand portion of the chart at zero reactance represents series resonance frequency (fs) and occurs where the Q circle crosses the real axes on the left side of the Smith Chart. The left-hand portion of the chart also demonstrates the parameter of resistance Rs. The right-hand portion of the chart at zero reactance represents parallel resonant frequency (fp) and occurs where the Q circle crosses the real axes on the right side of the Smith Chart. The right-hand portion of the chart also demonstrates the parameter of resistance Rp. The closer that a plot of FBAR filter characteristics on a Smith Chart is to the perimeter of the Smith Chart, the higher the Q will be for that FBAR. Also, the more smooth that the curve is, the lower the noise is in the FBAR.


In FIG. 10, the performance of FBAR 175 as a filter is illustrated by the solid line Q circle s11 and the performance of a prior art FBAR without an alternating frame region on the electrode is illustrated by the dashed line Q circle s22. As evident, FBAR 175 improves the quality of the filter near the frequency fp. FBAR 175, illustrated by Q circle s11, more closely approximates a unit circle in the upper half of the unit circle and is representative of a less lossy device in that area, which improves the performance of FBAR 175 when used in a filter.


Furthermore, there is also improvement in the lower half of the unit circle for FBAR 175 due to the recessed region inside the frame 182. Thus, FBAR 175 exhibits combined improvement (“closeness” of the Q-circle to the edge of the Smith Chart) at both an 8 o'clock position of the chart and at a 2 o'clock position of the chart.



FIG. 11 illustrates a cross-sectional view of an alternative FBAR 190 in accordance with one embodiment of the present invention. FBAR 190 is similar to those illustrated above, and includes substrate 192, depression 194, first electrode 196, piezoelectric (PZ) layer 198, second electrode 200 and first and second frames 210 and 212.


In one embodiment, the performance of FBAR 190 as illustrated in FIG. 11 is similar to those illustrated above, in that first and second frames 210 and 212 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 210 and 212 separated by air in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 190, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 190 is constructed as a DBR structure.


In addition, first frame 210 and second frame 212 are separated by a region of second electrode 200 that is thinner than are the remaining portions of second electrode 200. An additional thinner recessed region is provided adjacent second frame 212 toward the center of FBAR 190. Furthermore, frame 210 provides stiffness at the edge of FBAR 190 providing additional energy trapping, which further improves its performance.



FIG. 12 illustrates a cross-sectional view of an alternative FBAR 220 in accordance with one embodiment of the present invention. FBAR 220 is similar to those illustrated above, and includes substrate 222, depression 224, first electrode 226, piezoelectric (PZ) layer 228, second electrode 230 and first and second frames 240 and 242.


In one embodiment, the performance of FBAR 220 as illustrated in FIG. 12 is similar to those illustrated above, in that first and second frames 240 and 242 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 240 and 242 separated by air in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 220, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 220 is constructed as a DBR structure.


In addition, first frame 240 and second frame 242 are separated by a region of second electrode 230 that is thicker than are the remaining portions of second electrode 230. An additional thinner recessed region is provided adjacent second frame 242 toward the center of FBAR 220. Furthermore, frame 240 provides stiffness at the edge of FBAR 220 providing additional energy trapping, which further improves its performance.


For each of the above-illustrated cross-sectional views of the various FBAR embodiments, various alternating frame regions are illustrated. One skilled in the art will understand that other combinations of relative thicknesses of the portions within the alternating frame regions are possible. For example, an alternating frame region can have a single recessed region followed by thicker frame, or several recessed and thicker frames may be alternated in the alternating frame region. In addition, each of the above-illustrated FBAR embodiments has alternating frame regions consisting of the same material as the second electrode. Other materials can also be used, however, as will be discussed below.



FIG. 13 illustrates a cross-sectional view of an alternative FBAR 250 in accordance with one embodiment of the present invention. FBAR 250 is similar to those illustrated above, and includes substrate 252, depression 254, first electrode 256, piezoelectric (PZ) layer 258, second electrode 260 and first and second frames 270 and 272.


In one embodiment, the performance of FBAR 250 as illustrated in FIG. 13 is similar to those illustrated above, in that first and second frames 270 and 272 form an alternating frame region. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 270 and 272 separated by air in the illustration), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 250, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 250 is constructed as a DBR structure.


In addition, first frame 270 and second frame 272 are made of a different material than is second electrode 260. In this embodiment, the alternating thinner and thicker areas of the alternating frame region can be used to capture different frequency modes in the FBAR 250 in order to improve its performance, and the different material of frames 270 and 272 and second electrode 260 can be selected to achieve further performance enhancement.


In one embodiment, both the regions of the alternating frame region and of the second electrode are molybdenum (Mo). In other embodiments the alternating frame region can consist of other materials, such as metals (for example, W, Pt, Au), dielectrics (for example, Si3N4, SiO2), and piezoelectrics (for example, AlN), or combinations thereof. In yet other embodiments, the second electrode can be made of a conductive material, such as Mo or Pt, and the alternating frame regions can be made of any other material with different acoustic impedance, such as metals (for example, W, Pt, Au), dielectrics (for example, Si3N4, SiO2), and piezoelectrics (for example, AlN), or combinations thereof.



FIG. 14 illustrates a cross-sectional view of an alternative FBAR 280 in accordance with one embodiment of the present invention. FBAR 280 is similar to those illustrated above, and includes substrate 282, depression 284, first electrode 286, piezoelectric (PZ) layer 288, second electrode 290 and first and second frames 300 and 302.


In one embodiment, the performance of FBAR 280 as illustrated in FIG. 14 is similar to those illustrated above, in that first and second frames 300 and 302 form an alternating frame region. In this embodiment, however, the alternating frame region is formed on a top surface of first electrode 286. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 300 and 302 separated by regions of first electrode 286), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q in FBAR 280, thereby improving its performance. In one embodiment, the alternating frame region of FBAR 280 is constructed as a DBR structure.



FIG. 15 illustrates a cross-sectional view of an alternative FBAR 310 in accordance with one embodiment of the present invention. FBAR 310 is similar to those illustrated above, and includes substrate 312, depression 314, first electrode 316, piezoelectric (PZ) layer 318, second electrode 320 and first and second frames 330 and 332.


In one embodiment, the performance of FBAR 310 as illustrated in FIG. 15 is similar to those illustrated above, in that first and second frames 330 and 332 form an alternating frame region. In this embodiment, however, the alternating frame region is formed on a bottom surface of first electrode 316. By building alternating regions of different acoustic impedance with the alternating frame region (that is, frames 330 and 332 separated by regions of first electrode 316), certain wavelengths of signals within the FBAR membrane will reflect such that there is a phase change on some of the reflection. The alternating frame region is constructed such that all of the reflected wavelengths interfere to improve Q of FBAR 310, thereby improving its performance. In addition, frames 330 and 332 are made of a different material than first electrode 316 and selected to further improve performance. In one embodiment, the alternating frame region of FBAR 310 is constructed as a DBR structure.


Alternative alternating frame regions may be integrated with either surface of the first and second electrodes for all the above-illustrated FBARs. In addition, each can use the same or different materials for the frames and corresponding electrodes. Alternatively, the alternating frame region can even be integrated in the piezoelectric layer.


For each of the above-illustrated cross-sectional views of the various FBAR embodiments, contacts are not illustrated in the Figures, but are typically added to each of the first and second electrodes. Also, an optional passivation layer is not illustrated in the Figures, but is typically used to cover each of the second electrodes. In addition, each of the first electrodes, PZ layers, and second electrodes collectively form an FBAR membrane, which is illustrated in each case placed over a depression. In each case, the FBAR membrane can also be placed over an electrode-acoustic mirror interface using an SMR design in accordance with the present invention.


Each of the above-illustrated FBARs can be fabricated in a variety of ways consistent with the present invention. FIGS. 16A-16C are cross-sectional views illustrating various intermediate stages of fabrication of an FBAR 340 according to one embodiment of the present invention. Analogous steps can be applied to manufacture each of the above-described FBARs.


FBAR 340 is similar to those illustrated above, and includes substrate 342, depression 344, first electrode 346, piezoelectric (PZ) layer 348, and second electrode 350, which collectively form an FBAR membrane. FIG. 16A illustrates FBAR 340 prior to formation of any frame, alternating frame region, or DBR structure.



FIG. 16B illustrates FBAR 340 with a photo mask 352 deposited over the FBAR membrane. Photo mask 352 is used to pattern mask regions 352a and 352b using a lift-off process. Mask regions 352a and 352b are effectively recessed in the photo mask 352 such that they are then used in the formation of frames in the fabrication of the alternating frame structure in subsequent steps.



FIG. 16C illustrates FBAR 340 after additional electrode material metal 354 is deposited, but before the lift-off process. In this step, first and second frames 360 and 362 are illustrated formed in mask regions 352a and 352b. A lift off process then removes photo mask 352 and all metal 354 that is on photo mask 352. After the lift-off process, where photo mask 352 is removed and the structure cleaned, an FBAR such as FBAR 40 illustrate in FIG. 3, is left behind. Contacts are then added to the electrodes and, in some embodiments, the FBAR may additionally utilize at least one passivation layer.


An alternating frame region on the bottom electrode may be constructed similarly. In addition, rather than using additional electrode material metal 354 in FIG. 16C, a different material can be used in that step so that the electrode and alternating frame structure are made of different materials.


Although specific embodiments have been illustrated and described herein, it will be appreciated by those of ordinary skill in the art that a variety of alternate and/or equivalent implementations may be substituted for the specific embodiments shown and described without departing from the scope of the present invention. This application is intended to cover any adaptations or variations of the specific embodiments discussed herein. Therefore, it is intended that this invention be limited only by the claims and the equivalents thereof.

Claims
  • 1. An acoustic resonator comprising: a first electrode;a layer of piezoelectric material adjacent the first electrode;a second electrode adjacent the layer of piezoelectric material, the second electrode having an outer perimeter; andan alternating frame region configured on the second electrode adjacent the outer perimeter;wherein the alternating frame region further comprises a first region having a first acoustic impedance and a second region having a second acoustic impedance, the first and second acoustic impedances being different such that certain wavelengths of signals within the acoustic resonator reflect and interfere to improve Q.
  • 2. The acoustic resonator of claim 1, wherein the alternating frame region comprises at least a first raised frame and a second raised frame on the second electrode, the first and second raised frames being spaced apart from each other.
  • 3. The acoustic resonator of claim 2, wherein the alternating frame region is a distributed Bragg reflector.
  • 4. The acoustic resonator of claim 2, wherein the first and second spaced apart raised frames are the same width.
  • 5. The acoustic resonator of claim 2, wherein the first frame is wider than the second frame.
  • 6. The acoustic resonator of claim 2, wherein the first frame is thicker than the second electrode.
  • 7. The acoustic resonator of claim 2, further including a recessed region inside the first and second raised frames.
  • 8. An acoustic resonator comprising: a substrate;a first electrode adjacent the substrate, wherein the first electrode has an outer perimeter;a piezoelectric layer adjacent the first electrode;a second electrode adjacent the piezoelectric layer, wherein the second electrode has an outer perimeter; andan alternating frame region on one of the first and second electrodes;wherein the alternating frame region includes at least one raised frame adjacent at least one relatively recessed region;wherein the alternating frame region is a distributed Bragg reflector.
  • 9. An acoustic resonator comprising: a substrate;a first electrode adjacent the substrate, wherein the first electrode has an outer perimeter;a piezoelectric layer adjacent the first electrode;a second electrode adjacent the piezoelectric layer, wherein the second electrode has an outer perimeter; andan alternating frame region on one of the first and second electrodes;wherein a depression is formed in the substrate and wherein the depression has a depression perimeter;wherein the alternating frame region is outside the depression perimeter adjacent the outer perimeter of the second electrode.
  • 10. An acoustic resonator comprising: a substrate;a first electrode adjacent the substrate, wherein the first electrode has an outer perimeter;a piezoelectric layer adjacent the first electrode;a second electrode adjacent the piezoelectric layer; wherein the second electrode has an outer perimeter; andan alternating frame region on one of the first and second electrodes;wherein a depression is formed in the substrate and wherein the depression has a depression perimeter;wherein the alternating frame region overlaps the depression perimeter.
  • 11. An acoustic resonator comprising: a substrate;a first electrode adjacent the substrate, wherein the first electrode has an outer perimeter;a piezoelectric layer adjacent the first electrode;a second electrode adjacent the piezoelectric layer; wherein the second electrode has an outer perimeter; andan alternating frame region on one of the first and second electrodes;wherein a depression is formed in the substrate and wherein the depression has a depression perimeter;wherein the alternating frame region is inside the depression perimeter.
  • 12. An acoustic resonator comprising: a substrate;a first electrode adjacent the substrate;a layer of piezoelectric material adjacent the first electrode;a second electrode adjacent the layer of piezoelectric material, wherein the first electrode, the layer of piezoelectric material and the second electrode together form an acoustic membrane having an outer edge and a center; andan alternating frame region adjacent the outer edge of the acoustic membrane, which includes a plurality of raised frames on the second electrode, each of the plurality of raised frames being spaced apart, wherein the alternating frame region traps lateral modes within the acoustic membrane.
  • 13. The acoustic resonator of claim 12, wherein the alternating frame region further comprises a first region having a first acoustic impedance and a second having a second acoustic impedance, the first and second acoustic impedances being different such that certain wavelengths of signals within the acoustic resonator reflect and interfere to improve Q.
  • 14. The acoustic resonator of claim 12, wherein at least one of the raised frames on the second electrode stiffens the edge of the acoustic membrane thereby trapping modes within the resonator.
CROSS-REFERENCE TO RELATED APPLICATIONS

This Patent Application is related to U.S. Pat. No. 7,161,448, filed on Jun. 14, 2004, entitled “ACOUSTIC RESONATOR PERFORMANCE ENHANCEMENT USING SELECTIVE METAL ETCH;” to Utility Patent Application Ser. No. 11/100,311, filed on Apr. 6, 2005, entitled “ACOUSTIC RESONATOR PERFORMANCE ENHANCEMENT USING FILLED RECESSED REGION;” to Provisional Patent Application Ser. No. 60/615,255, filed on Oct. 1, 2004, entitled “A THIN FILM BULK ACOUSTIC RESONATOR WITH A MASS LOADED PERIMETER; and to Utility Patent Application Ser. No. 10/990,201, filed on Nov. 15, 2004, entitled A THIN FILM BULK ACOUSTIC RESONATOR WITH A MASSED PERIMETER, and is commonly assigned to the same assignee as the present invention.

US Referenced Citations (225)
Number Name Date Kind
3174122 Fowler et al. Mar 1965 A
3189851 Fowler Jun 1965 A
3321648 Kolm May 1967 A
3422371 Poirier et al. Jan 1969 A
3568108 Poirier et al. Mar 1971 A
3582839 Pim et al. Jun 1971 A
3590287 Berlincourt et el. Jun 1971 A
3610969 Clawson et al. Oct 1971 A
3826931 Hammond Jul 1974 A
3845402 Nupp Oct 1974 A
4084217 Brandis et al. Apr 1978 A
4172277 Pinson Oct 1979 A
4272742 Lewis Jun 1981 A
4281299 Newbold Jul 1981 A
4320365 Black et al. Mar 1982 A
4355408 Scarrott Oct 1982 A
4456850 Inoue et al. Jun 1984 A
4529904 Hattersley Jul 1985 A
4625138 Ballato Nov 1986 A
4719383 Wang et al. Jan 1988 A
4798990 Henoch Jan 1989 A
4836882 Ballato Jun 1989 A
4841429 Mcclanahan et al. Jun 1989 A
4906840 Zdeblick et al. Mar 1990 A
5048036 Scifres et al. Sep 1991 A
5048038 Brennan et al. Sep 1991 A
5118982 Inoue et al. Jun 1992 A
5129132 Zdeblick et al. Jul 1992 A
5162691 Mariani et al. Nov 1992 A
5241209 Sasaki Aug 1993 A
5241456 Marcinkiewicz et al. Aug 1993 A
5294898 Dworsky et al. Mar 1994 A
5382930 Stokes et al. Jan 1995 A
5384808 Van Brunt et al. Jan 1995 A
5448014 Kong et al. Sep 1995 A
5465725 Seyed-Boloforosh Nov 1995 A
5587620 Ruby et al. Dec 1996 A
5589858 Kadowaki et al. Dec 1996 A
5594705 Connor et al. Jan 1997 A
5671242 Takiguchi et al. Sep 1997 A
5692279 Mang et al. Dec 1997 A
5714917 Ella Feb 1998 A
5853601 Krishaswamy et al. Dec 1998 A
5864261 Weber Jan 1999 A
5872493 Ella Feb 1999 A
5873153 Ruby et al. Feb 1999 A
5873154 Ylilammi et al. Feb 1999 A
5894647 Lakin Apr 1999 A
5910756 Ella Jun 1999 A
5936150 Kobrin et al. Aug 1999 A
5953479 Zhou et al. Sep 1999 A
5982297 Welle Nov 1999 A
6040962 Kanazawa Mar 2000 A
6060818 Ruby et al. May 2000 A
6087198 Panasik Jul 2000 A
6107721 Lakin Aug 2000 A
6111480 Iyama et al. Aug 2000 A
6124756 Yaklin et al. Sep 2000 A
6150703 Cushman et al. Nov 2000 A
6187513 Katakura Feb 2001 B1
6215375 Larson, III et al. Apr 2001 B1
6228675 Ruby et al. May 2001 B1
6229247 Bishop May 2001 B1
6252229 Hays et al. Jun 2001 B1
6262600 Haigh et al. Jul 2001 B1
6262637 Bradley et al. Jul 2001 B1
6265246 Ruby et al. Jul 2001 B1
6278342 Ella Aug 2001 B1
6292336 Cheng Sep 2001 B1
6307447 Barber et al. Oct 2001 B1
6307761 Nakagawa Oct 2001 B1
6376280 Ruby et al. Apr 2002 B1
6377137 Ruby Apr 2002 B1
6384697 Ruby May 2002 B1
6407649 Tikka et al. Jun 2002 B1
6414569 Nakafuku Jul 2002 B1
6420820 Larson, III Jul 2002 B1
6424237 Ruby et al. Jul 2002 B1
6429511 Ruby et al. Aug 2002 B2
6434030 Rehm et al. Aug 2002 B1
6437482 Akihiko Aug 2002 B1
6441539 Kitamura et al. Aug 2002 B1
6462631 Bradley et al. Oct 2002 B2
6466105 Lobl et al. Oct 2002 B1
6466418 Horng Oct 2002 B1
6469597 Ruby et al. Oct 2002 B2
6472954 Ruby et al. Oct 2002 B1
6476536 Pensala Nov 2002 B1
6479320 Gooch Nov 2002 B1
6483229 Ylilammi et al. Nov 2002 B2
6486751 Barber et al. Nov 2002 B1
6489688 Baumann et al. Dec 2002 B1
6492883 Liang et al. Dec 2002 B2
6507983 Ruby et al. Jan 2003 B1
6515558 Ylilammi Feb 2003 B1
6518860 Ella et al. Feb 2003 B2
6525996 Miyazawa Feb 2003 B1
6530515 Glenn et al. Mar 2003 B1
6534900 Aigner et al. Mar 2003 B2
6542055 Frank et al. Apr 2003 B1
6548942 Panaski Apr 2003 B1
6550664 Bradley et al. Apr 2003 B2
6564448 Oura et al. May 2003 B1
6566979 Larson et al. May 2003 B2
6583374 Knieser et al. Jun 2003 B2
6583688 Klee et al. Jun 2003 B2
6593870 Dummermuth et al. Jul 2003 B2
6600390 Frank Jul 2003 B2
6601276 Barber Aug 2003 B2
6617249 Ruby et al. Sep 2003 B2
6617750 Dummermuth et al. Sep 2003 B2
6630753 Malik et al. Oct 2003 B2
6635509 Ouellet Oct 2003 B1
6639872 Rein Oct 2003 B1
6651488 Larson et al. Nov 2003 B2
6657363 Aigner Dec 2003 B1
6668618 Larson et al. Dec 2003 B2
6670866 Ella et al. Dec 2003 B2
6693500 Yang et al. Feb 2004 B2
6710508 Ruby et al. Mar 2004 B2
6710681 Figueredo et al. Mar 2004 B2
6714102 Ruby et al. Mar 2004 B2
6720844 Lakin Apr 2004 B1
6720846 Iwashita et al. Apr 2004 B2
6724266 Plazza et al. Apr 2004 B2
6774746 Whatmore et al. Aug 2004 B2
6777263 Gan et al. Aug 2004 B1
6787048 Bradley et al. Sep 2004 B2
6788170 Kaitila et al. Sep 2004 B1
6803835 Frank Oct 2004 B2
6812619 Kaitila et al. Nov 2004 B1
6828713 Bradley et al. Dec 2004 B2
6842088 Yamada et al. Jan 2005 B2
6873065 Haigh et al. Mar 2005 B2
6873529 Ikuta Mar 2005 B2
6874211 Bradley et al. Apr 2005 B2
6874212 Larson, III Apr 2005 B2
6888424 Takeuchi et al. May 2005 B2
6900705 Nakamura et al. May 2005 B2
6903452 Ma et al. Jun 2005 B2
6906451 Yamada Jun 2005 B2
6911708 Park Jun 2005 B2
6917261 Unterberger Jul 2005 B2
6924583 Lin et al. Aug 2005 B2
6924717 Ginsburg et al. Aug 2005 B2
6927651 Larson, III et al. Aug 2005 B2
6936928 Hedler et al. Aug 2005 B2
6936954 Peczalski Aug 2005 B2
6946928 Larson et al. Sep 2005 B2
6954121 Bradley et al. Oct 2005 B2
6963257 Ella et al. Nov 2005 B2
6975183 Aigner et al. Dec 2005 B2
6977563 Komuro et al. Dec 2005 B2
6985052 Tikka Jan 2006 B2
6987433 Larson et al. Jan 2006 B2
6989723 Komuro et al. Jan 2006 B2
6998940 Metzger Feb 2006 B2
7019604 Gotoh et al. Mar 2006 B2
7019605 Larson et al. Mar 2006 B2
7057476 Hwu Jun 2006 B2
7084553 Ludwiczak Aug 2006 B2
7091649 Larson Aug 2006 B2
7098758 Wang et al. Aug 2006 B2
7170215 Namba et al. Jan 2007 B2
7173504 Larson Feb 2007 B2
7187254 Su et al. Mar 2007 B2
7230509 Stoemmer Jun 2007 B2
20020000646 Gooch et al. Jan 2002 A1
20020030424 Iwata Mar 2002 A1
20020121944 Larson, III et al. Sep 2002 A1
20020121945 Ruby et al. Sep 2002 A1
20020152803 Larson, III et al. Oct 2002 A1
20020190814 Yamada et al. Dec 2002 A1
20030001251 Cheever et al. Jan 2003 A1
20030006502 Karpman Jan 2003 A1
20030087469 Ma May 2003 A1
20030102776 Takeda et al. Jun 2003 A1
20030111439 Fetter et al. Jun 2003 A1
20030128081 Ella et al. Jul 2003 A1
20030132493 Kang et al. Jul 2003 A1
20030141946 Ruby et al. Jul 2003 A1
20030179053 Aigner et al. Sep 2003 A1
20040092234 Pohjonen May 2004 A1
20040124952 Tikka Jul 2004 A1
20040150293 Unterberger Aug 2004 A1
20040150296 Park et al. Aug 2004 A1
20040195937 Matsubara et al. Oct 2004 A1
20040257172 Schmidhammer et al. Dec 2004 A1
20040263287 Ginsburg et al. Dec 2004 A1
20050012570 Korden et al. Jan 2005 A1
20050023931 Bouche et al. Feb 2005 A1
20050030126 Inoue et al. Feb 2005 A1
20050036604 Scott et al. Feb 2005 A1
20050057117 Nakatsuka et al. Mar 2005 A1
20050057324 Onishi et al. Mar 2005 A1
20050068124 Stoemmer Mar 2005 A1
20050093396 Larson et al. May 2005 A1
20050093653 Larson, III May 2005 A1
20050093654 Larson et al. May 2005 A1
20050093655 Larson et al. May 2005 A1
20050093657 Larson et al. May 2005 A1
20050093658 Larson et al. May 2005 A1
20050093659 Larson et al. May 2005 A1
20050104690 Larson May 2005 A1
20050110598 Larson, III May 2005 A1
20050128030 Larson et al. Jun 2005 A1
20050140466 Larson, III et al. Jun 2005 A1
20050167795 Higashi Aug 2005 A1
20050193507 Ludwiczak Sep 2005 A1
20050206271 Higuchi et al. Sep 2005 A1
20050218488 Matsuo Oct 2005 A1
20060087199 Larson et al. Apr 2006 A1
20060103492 Feng et al. May 2006 A1
20060132262 Fazzio et al. Jun 2006 A1
20060164183 Tikka Jul 2006 A1
20060185139 Larson, III et al. Aug 2006 A1
20070084964 John et al. Apr 2007 A1
20070085447 Larson Apr 2007 A1
20070085631 Larson et al. Apr 2007 A1
20070085632 Larson et al. Apr 2007 A1
20070086080 Larson et al. Apr 2007 A1
20070086274 Nishimura et al. Apr 2007 A1
20070090892 Larson Apr 2007 A1
20070170815 Unkrich Jul 2007 A1
20070171002 Unkrich Jul 2007 A1
Foreign Referenced Citations (36)
Number Date Country
10160617 Jun 2003 DE
0865157 Sep 1998 EP
0880227 Nov 1998 EP
0 973 256 Jan 2000 EP
1047189 Oct 2000 EP
1100196 Nov 2000 EP
1 096 259 May 2001 EP
1 180 494 Jul 2001 EP
1 249 932 Oct 2002 EP
1 258 989 Nov 2002 EP
1 258 990 Nov 2002 EP
1542362 Jun 2003 EP
1 517 443 Mar 2005 EP
1517444 Mar 2005 EP
1528674 May 2005 EP
1528675 May 2005 EP
1528677 May 2005 EP
1557945 Jul 2005 EP
1 575 165 Sep 2005 EP
1207974 Oct 1970 GB
2411239 Aug 2005 GB
2 418 791 Apr 2006 GB
2002217676 Aug 2002 JP
WO-9816957 Apr 1998 WO
WO-2005043752 May 2000 WO
WO 0106647 Jan 2001 WO
WO 0199276 Dec 2001 WO
WO 02103900 Dec 2002 WO
WO-03030358 Apr 2003 WO
WO 03043188 May 2003 WO
WO-03050950 Jun 2003 WO
WO-03058809 Jul 2003 WO
WO-2004034579 Apr 2004 WO
WO 2004051744 Jun 2004 WO
WO-2005043753 May 2005 WO
WO-2005043756 May 2005 WO
Related Publications (1)
Number Date Country
20060071736 A1 Apr 2006 US
Provisional Applications (1)
Number Date Country
60615255 Oct 2004 US