Optimal cut for SAW devices on langatate

Abstract

A lanthanum gallium tantalate single crystal substrate, referred to as langatate, has a prescribed range of Euler angles for substrate and crystal orientation for improving signal processing for a surface acoustic wave (SAW) device. When a voltage is applied to an input interdigital transducer (IDT) of the SAW device, a surface acoustic wave is generated in the langatate piezoelectric substrate. The surface acoustic wave propagates in a direction generally perpendicular to electrodes of the IDT. The langatate crystal cut and wave propagation directions are defined which reduce insertion loss and frequency response distortion due to SAW transduction, diffraction, and beam steering, while achieving improved temperature stability SAW device as compared to other commonly used crystal substrates. A low power flow angle and reduced level of diffraction is also achieved.

Description

FIELD OF THE INVENTION

The invention relates to a surface acoustic wave (SAW) device and, more particularly, to a device having a langatate crystal substrate with a predetermined crystalline orientation for causing a surface acoustic wave to propagate along a predetermined crystalline axis of the substrate.

BACKGROUND OF THE INVENTION

This invention relates to an optimal surface acoustic wave orientation on single crystal lanthanum gallium tantalate or La.sub.3 Ga.sub.5.5 Ta.sub.0.5 O.sub.14, commonly known as langatate (LGT). SAW devices are currently used as bandpass filters, resonators, delay lines, convolvers, etc. in a broad range of RF and IF applications such as wireless, cellular communication and cable TV. Three commonly used substrates are lithium niobate, quartz, and lithium tantalate. There are several material properties that determine the usefulness of any particular crystal and, in particular, orientation of a particular crystal. These properties include: 1) SAW velocity, Vs; 2) the SAW piezoelectric coupling coefficient, k.sup.2 ; 3) the power flow angle, PFA; 4) the diffraction or beam spreading coefficient, y (gamma); and 5) the temperature coefficient of frequency, TCF. It has not been possible to find an orientation in any existing substrate which optimizes these properties at the same time; so the choice of substrate and orientation depends upon what is important for the application, and almost always involves a compromise between the SAW material properties. A high velocity is desirable for high frequency devices, because the device geometry patterns are larger and, therefore, the devices are easier to fabricate. At low frequencies, a low velocity is usually desirable because the device size is smaller, resulting in lower device and packaging costs. Thus, there is no universally optimum velocity. For moderate to wide bandwidth devices, a high value of k.sup.2 is desirable because it allows lower insertion loss. From the point of view of k.sup.2, lithium niobate is best, quartz is worst, and lithium tantalate is in between. For most devices, and in particular narrow band devices, TCF should be as low as possible and ideally zero. From this point of view, ST-Quartz is best, lithium niobate is worst, and lithium tantalate is in between (just the opposite ranking as for k.sup.2). The optimum value of y is -1, which results in minimum beam spreading. From this point of view, YZ lithium niobate is now ideal, ST-Quartz is worst, and lithium tantalate is in between. The PFA should be zero, and this is the case for most of the commonly used SAW substrates, with an exception being 112.degree. lithium tantalate, which has a PFA of 1.55.degree.. For the most narrow band applications, quartz is a quite acceptable choice; and for the very wide band applications where temperature stability is not so important, lithium niobate is usually quite acceptable. What is needed is a substrate orientation that offers the temperature stability of ST-Quartz but with higher k.sup.2 and at the same time low or zero beam steering (PFA) and diffraction (y=-1). It is an object of the present invention to disclose a substrate called langatate that meets these conditions.

SUMMARY OF THE INVENTION

It is the object of the present invention to provide a langatate crystal having a substantially planar surface defined by the Euler angles, such that SAW propagation within this range of angles on langatate is characterized by piezoelectric coupling about five to eight times stronger than typically found with ST-Quartz, by way of example, near zero PFA, near zero TCF, and near minimum beam spreading. While the latter three conditions may not all be met exactly for any orientation, the performance as measured just by these three conditions together is significantly better than any known cut of Li Nb O.sub.3, Li Ta O.sub.3, or quartz, and choices within this range can be chosen to favor one or two at the slight expense of the third.

One preferred embodiment of the present invention includes a device which contains a langatate substrate on the surface of which input and output IDT's are placed. The surface of the langatate substrate is perpendicular to axis Z', and electrodes of IDT's are nominally perpendicular to axis X' and parallel to axis Y'. Axes X', Y', Z' are defined by Euler angles with respect to crystal axes X, Y, Z of langatate. Angle .phi. is in the range -5.degree. to +5.degree.; angle .theta. in the range of 130.degree. to 150.degree.; and angle .psi. in the range of 15.degree. to 35.degree.. A SAW device includes devices which consist of piezoelectric substrate having a planar SAW propagation surface on the surface of which any number of transduction, reflection, waveguiding, energy trapping, or other acoustic elements have been placed in desired configurations. Such elements include, but are not limited to, transducers which are ordinary, tapered, apodized, otherwise weighted, unweighted, single phase unidirectional, other unidirectional, IIDT, etc.; reflective elements of various kinds, multistrip couplers; and may include metal, groove, or dielectric structures. Additional preferred embodiments of the present invention utilize langatate as the piezoelectric substrate.

Another aspect of the present invention includes a langatate substrate comprising a planar SAW propagation surface, wherein a surface wave direction of propagation is defined to be along an X' axis, the substrate further having a Z' axis normal to the surface, and a Y' axis along the surface and perpendicular to the X' axis, and a crystal orientation defined by crystal axes X, Y, and Z, wherein the relative orientation of the X', Y', and Z' axes is defined by Euler angles .phi. and .THETA., and .phi. has a value ranging from -5.degree. to 5.degree., and .theta. has a value ranging from 130.degree. to 150.degree..

A method aspect of the present invention includes forming a surface acoustic wave device comprising the steps of providing a lanthanum gallium tantalate (langatate) single crystal, orientating the crystal for cutting a planar surface with a defined direction of propagate, the crystal orientating defined by Euler angles .phi., .theta., and .psi., cutting the crystal for forming the planar surface, the cut defined by the Euler angles, wherein .phi. has a value ranging from approximately -5.degree. to approximately 5.degree., and .theta. has a value ranging from approximately 130.degree. to approximately 150.degree., and affixing an interdigitized transducer on the surface for propagating and detecting surface acoustic waves propagating in a direction generally along an axis of propagation defined relative to the crystal orientation angle .psi., where .psi. has a value ranging from approximately 15.degree. to approximately 35.degree..

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a perspective view of a SAW device illustrating interdigital transducers located on a langatate substrate surface, and a power flow angle .phi.;

FIG. 2 diagrammatically illustrates substrate axes X', Y', and Z' and crystal axes X, Y, and Z along with Euler angles .phi., .theta., .psi. describing relative orientation of X, Y, and Z to X', Y', and Z', wherein X' is defined as a direction of SAW propagation;

FIG. 3 illustrates SAW Velocity versus propagation angle .psi. for selected values of .theta. for a positive stiffness constant;

FIG. 4 illustrates SAW Power Flow Angle versus propagation angle .psi. for selected values of .theta. for a positive stiffness constant;

FIG. 5 illustrates SAW Anisotropy Parameter versus propagation angle .psi. for selected values of .theta. for a positive stiffness constant;

FIG. 6 illustrates SAW Electromechanical Coupling Coefficient, versus propagation angle .psi. for selected values of .theta. for a positive stiffness constant;

FIG. 7 illustrates SAW Velocity versus propagation angle .psi. for selected values of .theta. for a negative stiffness constant;

FIG. 8 illustrates SAW Power Flow Angle versus propagation angle .psi. for selected values of .theta. for a negative stiffness constant;

FIG. 9 illustrates SAW Anisotropy Parameter versus propagation angle .psi. for selected values of .theta. for a negative stiffness constant; and

FIG. 10 illustrates SAW Electromechanical Coupling Coefficient, versus propagation angle .psi. for selected values of .theta. for a negative stiffness constant.

DESCRIPTION OF THE PREFERRED EMBODIMENT

As illustrated, by way of example with reference to FIG. 1, one preferred embodiment of the present invention includes a SAW device 10 which contains a langatate substrate 12 on the surface 14 of which an input interdigital transducer and an output interdigital transducer (IDT) are placed.

The surface 14 of the langatate substrate 12 is perpendicular to axis Z', electrodes 20, 22 of IDT's 16, 18 respectively, are perpendicular to axis X' and are parallel to axis Y'. As illustrated with reference to FIG. 2, axes X', Y' and Z' are defined by Euler angles with respect to crystal axes X, Y and Z of the langatate substrate 12. For the preferred embodiment of the present invention, angle .phi. is in the range -5.degree. to 5.degree.; angle .theta. in the range of 130.degree. to 150.degree.; and angle .psi. in the range of 15.degree. to 35.degree..

The crystal cut of langatate with Euler angles .phi.=0.+-.5.degree., .theta.=140.degree..+-.10.degree., and .psi.=25.degree..+-.10.degree., provide improved performance for SAW devices. Specifically, the crystal cut provides a near simultaneous optimization of three critical SAW propagation parameters and a favorable value of a fourth parameter. This fourth parameter is the coupling constant k.sup.2, which varies between 0.6% and 0.9% as compared to 0.12% for ST-Quartz crystal. The three SAW propagation parameters are the PFA, .gamma. and TCF, which, as earlier described, are the power flow angle, the diffraction coefficient, and the temperature coefficient of frequency, respectively. PFA is also known as .phi., the beam steering angle, and is the angle between the SAW wave vector, which is normal to the tap electrodes, and the direction of the power flow, as illustrated again with reference to FIG. 1. Ideally, the PFA would be zero. .gamma. is a measure of the diffraction or beam spreading. Normally, as a SAW propagates on a substrate, the beam profile will change and broaden. This beam spread causes diffraction loss and distortion to the filter response. For isotropic materials, the value of .gamma. is zero, and diffraction is a moderately serious problem. Diffraction is minimized when .gamma.=-1, and this is nearly the case for YZ Li Nb O.sub.3 and a special MDC (minimum diffraction cut) of Li Ta O.sub.3. For ST-Quartz, .gamma.=+0.38, and diffraction is worse than the isotropic case. There is a range of angles within the designated range of this disclosure for which .gamma.=-1, which is ideal. Likewise there is a range of angles for which the TCF is zero. (TCF is the relative change in frequency per degree centigrade.) The desired parameter values are obtained for each parameter within the restricted range of angles of this disclosure; but since the angles associated with the values form a locus of points in a two-dimensional angle space (over .theta. and .psi.), it is very difficult to find a point at which the three loci intersect. That means it is possible to achieve a desired performance in two of the three parameters and nearly ideal performances for all three parameters. Therefore, within this range, the optimal choice of angles would still be dependent upon the application, and in fact are intermediate points that minimize the problem of all three parameters. This is the reason for the spread of angles disclosed herein.

The Euler angle convention used is as described by Slobodnik et al. in "Microwave Acoustic Handbook," Vol. 1, Surface Wave Velocities, AFCRL-70-0164, March 1970, Physical Sciences Research Papers, No. 414, Office of Aerospace Research, USAF.

By way of further example with regard to an orientation procedure for defining a substrate (also referred to as a wafer) using Euler angles, begin with axes X, Y, Z as the crystal axes (also referred to as a boule axes) coincident with the substrate axes X', Y', Z'. The relationship between X, Y, Z and X', Y', Z' is independent of the overall orientation of its combined system in space. In preparation for cutting the crystal, and as viewed from the positive Z' axis (now coincident with the positive Z axis), first rotate the substrate .phi..degree. counterclockwise around its axis Z'. Second, as viewed from the positive X' axis, rotate the substrate counterclockwise by .theta..degree. about the substrate axis X'. Next, as viewed from the positive Z' substrate axis, rotate the substrate counterclockwise by .psi..degree. about the substrate axis Z'. The crystal is now prepared for a cut normal to the substrate axis Z', and a flat defining the direction of propagation is placed normal to the wafer axis X' along a substrate edge in the positive X' direction.

Consider a wafer outline on a surface normal to the axis Z'. Now construct a flat plane along one edge of the wafer which is normal to the axis X'. The direction of SAW propagation is parallel to axis X'. Now assume that the crystal axes X, Y, Z are coincident with the wafer outline axes X', Y', Z', respectively. With no rotation, the wafer is considered a Z cut (the wafer is cut with the polished surface normal to Z) and X propagating (the SAW propagates in a direction parallel to the X axis). With any subsequent rotation, the wafer axes X', Y', Z' are rotated, and the crystal axes X, Y, Z are assumed to be fixed. Now, by way of example, consider the Euler angles (.phi., .theta., .psi.)=(0.degree., 140.degree., 25.degree.), which is a case near the middle of the designated range. The first rotation would rotate around Z' (X' toward Y') by .phi.. Since .phi.=0.degree., there is no rotation for this case. The next rotation is around the "new" X' (the "new" axes are always tied to the wafer so that any rotation is around a wafer axis that includes all previous rotations) by .theta. (which is 140.degree.) (Y' toward Z' for a positive angle rotation). Finally, rotate around Z' (X' toward Y') by .psi., which for the case herein described is 25.degree..

Studies are being conducted to determine the value of the stiffness constant (C.sub.14). If C.sub.14 is positive, the propagation characteristics are as described by FIGS. 3-6 in which case the optimal range of Euler angles are .phi.=0.degree. (.+-.5.degree.), 130.degree..ltoreq..theta..ltoreq.150.degree., and 20.degree..ltoreq..psi..ltoreq.40.degree..

If C.sub.14 is negative the propagation characteristics are described by FIGS. 7-10, in which case the range at the preferred Euler angles are .phi.=0.degree. (.+-.5.degree.), 30.degree..ltoreq..theta..ltoreq.50.degree., and 20.degree..ltoreq..psi..ltoreq.40.degree..

FIGS. 3-6 illustrate SAW velocity, PFA .phi., anisotropy parameter y, and electromechanical coupling k.sub.s.sup.2 versus Euler angle .psi. for selected values, by way of example, of angle .theta. and for .phi.=0.degree. and C.sub.14 positive.

Again with reference to FIG. 1, and by way of example, one preferred embodiment of the present invention includes the SAW device 10 containing the langatate substrate 12, and IDT's 16, 18. As earlier described, the axis Z' is normal to the substrate surface 14, the axis X' is normal to electrodes 20, 22, and the Y' axis is parallel to the electrodes 20, 22. These axes X', Y' and Z' are defined with respect to crystal axes as follows: .phi.=-5.degree. to 5.degree.; .theta.=130.degree. to 150.degree., .psi.=15.degree. to 35.degree., where .phi., .theta., .psi. are the Euler angles.

With reference again to FIG. 2, .phi. is the angle between crystal axis X and auxiliary axis X", which is the axis of rotation of the plane XY (up to required orientation of the substrate surface).

.theta. is the angle between axis Z and the normal Z' to the substrate surface 14.

.psi. is the angle between axis X" and axis X', X' is perpendicular to electrodes of IDT's 20, 22.

With reference again to FIGS. 3-6 and 7-10, it is shown that in the present invention, the PFA, .phi. is less than 5.degree. and the electromechanical coupling coefficient is more than 0.6% with the maximum value 0.9%. Consequently for the orientations of the present invention, the electromechanical coupling coefficient k.sup.2 is more than five, and for some cases up to eight times, that of earlier devices on ST-Quartz. There are several selections of orientations for which the PFA is substantially zero and the diffraction parameter .gamma. is near the optimal value of -1. Additionally, the TCF in this range of orientations is lower than for most other SAW substrate materials.

While specific embodiments of the invention have been described in detail herein above, it is to be understood that various modifications may be made from the specific details described herein without departing from the spirit and scope of the invention as set forth in the appended claims.

Having now described the invention, the construction, the operation and use of preferred embodiments thereof, and the advantageous new and useful results obtained thereby, the new and useful constructions, methods of use and reasonable mechanical equivalents thereof obvious to those skilled in the art, are set forth in the appended claims.

Claims

1. A surface acoustic wave (SAW) device comprising:

a lanthanum gallium tantalate (langatate) substrate having a planar SAW propagation surface; and

input and output interdigital transducers having electrodes on the surface for launching and detecting surface acoustic waves, wherein a surface wave direction of propagation is along an X' axis, the substrate further having a Z' axis normal to the surface, and a Y' axis along the surface and perpendicular to the X' axis, the langatate substrate further having a crystal orientation defined by crystal axes X, Y, and Z, the relative orientation of device axes X', Y', and Z' being defined by Euler angles .phi., .THETA., and .psi., wherein .phi.has a value ranging from -5.degree. to 5.degree., .theta. has a value ranging from 130.degree. to 150.degree., and .psi. has a value ranging from 15.degree. to 35.degree..

2. The device according to claim 1, wherein the Euler angle .phi. is proximate 0.degree..

3. A surface acoustic wave device comprising:

a substrate having a substantially planar surface for propagating surface acoustic waves thereon, the substrate formed from a single lanthanum gallium tantalate (langatate) crystal cut for providing a crystal orientation for forming the surface defined by Euler angles having a range of -5.degree..ltoreq..phi.<5.degree., 130.degree..ltoreq..theta.<150.degree., and 15.degree..ltoreq..psi..ltoreq.35.degree.; and

interdigitized electrodes affixed to the surface.

4. The device according to claim 3, wherein the electrodes have an orientation generally perpendicular to a direction of wave propagation generally defined by the crystal orientation Euler angle .psi..

5. A langatate substrate comprising:

a planar SAW propagation surface, wherein a surface wave direction of propagation is defined to be along an X' axis, the substrate further having a Z' axis normal to the surface, and a Y' axis along the surface and perpendicular to the X' axis; and

a crystal orientation defined by crystal axes X, Y, and Z, wherein the relative orientation of the X', Y', and Z' axes is defined by Euler angles .phi. and .THETA., and wherein .phi. has a value ranging from -5.degree. to 5.degree., and .theta. has a value ranging from 130.degree. to 150.degree..

6. The device according to claim 5, wherein the Euler angle .phi. is further within the range of 0.degree..+-.5.degree., and .theta. is within the range of 140.degree..+-.5.degree..

7. The device according to claim 5, wherein the Euler angle .phi. is proximate 0.degree., and .theta. is within the range of 140.degree.35 10.degree..

8. A surface acoustic wave device substrate formed from a langatate single crystal, the substrate comprising:

a planar surface for receiving one or more interdigital transducers having a plurality of electrodes, the interdigital transducers operable for launching and detecting surface acoustic waves propagating generally perpendicular to the electrodes; and

a crystal orientation cut for forming the surface, the crystal orientation defined by Euler angles .phi. and .theta., where .phi. and .theta. define a surface which is crystallographically equivalent to the surface defined by .phi. having a value ranging from approximately -5.degree. to approximately 5.degree. and .theta. having a value ranging from approximately 130.degree. to approximately 150.degree..

9. A method for forming a surface acoustic wave device comprising the steps of:

providing a lanthanum gallium tantalate (langatate) single crystal;

orientating the crystal for cutting a planar surface with a defined direction of propagation, the crystal orientating defined by Euler angles .phi., .theta., and .psi.;

cutting the crystal for forming the planar surface, the cut defined by the Euler angles, wherein .phi. has a value ranging from approximately -5.degree. to approximately 5.degree., and .theta. has a value ranging from approximately 130.degree. to approximately 150.degree.; and

affixing an interdigitized transducer on the surface for propagating and detecting surface acoustic waves propagating in a direction generally along an axis of propagation defined relative to the crystal orientation angle .psi., where .psi. has a value ranging from approximately 15.degree. to approximately 35.degree..

10. The method according to claim 9, wherein the transducer affixing step further comprises the step of orientating electrodes of the transducer generally perpendicular to the axis of propagation.

11. The method according to claim 9, wherein the Euler angles comprise .phi. having a value proximate 0.degree..

12. A method for forming a surface acoustic wave device substrate comprising the steps of:

providing a lanthanum gallium tantalate (langatate) single crystal;

orientating the crystal for cutting a planar surface, the crystal orientating defined by Euler angles .phi., .theta., and .psi.; and

cutting the crystal for forming the planar surface with a defined direction of propagation, the cut defined by the Euler angles, wherein .phi. has a value ranging from approximately -5.degree. to approximately 5.degree., and .theta. has a value ranging from approximately 130.degree. to approximately 150.degree..

13. The method according to claim 12, further comprising the steps of:

affixing interdigitized transducer electrodes on the surface for propagating and detecting surface acoustic waves in a direction generally along an axis of propagation defined relative to the crystal orientation angle .psi., wherein .psi. has a value ranging from approximately 15.degree. to approximately 35.degree.; and

orienting the electrodes generally perpendicular to the axis of propagation.

14. The method according to claim 13, wherein the Euler angles comprise .phi. having a value proximate 0.degree..