High-power piezoelectric ceramics

Abstract

The disclosed invention relates to piezoelectric rare earth doped Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds including (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is ≦0.95, 0.40

Description

This application in a continuation in part of International Patent Application PCT/US01/47950, filed Dec. 13, 2001.

FIELD OF THE INVENTION

[0002] The invention relates to high power piezoelectric ceramics, more particularly, to piezoelectric ceramic compositions for use in ultrasonic motors, ultrasonic vibrators, piezoelectric actuators, and the like.

BACKGROUND OF THE INVENTION

[0003] The art has explored the high-power characteristics of piezoelectric materials for use in devices such as ultrasonic motors, piezoelectric actuators and piezoelectric transformers. It is preferred in the art that the piezoelectric materials used in these types of devices have a high mechanical quality factor, low heat generation, a high piezoelectric constant, as well as high vibrational velocities (vo) when subjected to low AC electric fields. The art has found it difficult, however, to achieve a piezoelectric material which has both a high mechanical quality factor and a high piezoelectric constant, as well as high vibrational velocity.

[0004] It is known in the art that the vo in lead-zirconate-titanate (PZT) compounds which have the ABO3 perovskite structure can be increased by introducing lower valent dopants such as Fe on the B-site, and that vo can be decreased by introducing higher valent dopants such as Nb on the B-site. The lower valent dopants tend to produce “hardening” effects on the base PZT type compounds by increasing the mechanical quality factor (Qm) while decreasing the electromechanical coupling factor (k). In contrast, higher valent substituents tend to decrease the Qm while increasing the (k) value.

[0005] It also is known in the art that the vibrational velocity (vo)of a piezoelectric material is restricted by heat generation within the piezoelectric material when subjected to an electric field (Eac). Heat generation under an electric field is known to be a function of vibrational velocity (vo). The value of vo is directly proportional to Qm and to the electromechanical coupling factor (k) under constant Eac. Development of a piezoelectric material with significantly higher vo, however, has not been successful in the art since each of Qm and k are increased at the expense of the other.

[0006] A need therefore exists for a piezoelectric material which has both increased Qm and increased k values, as well as increased vibrational velocity for high-power applications.

SUMMARY OF THE INVENTION

[0007] This invention relates to piezoelectric compositions for manufacture of rare earth (“RE”) doped Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds which have increased vibrational velocity as well as increased Qm and (k) values. The invention further relates to piezoelectric compounds corresponding to the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is ≦0.95, preferably about 0.90, 0.4≦w≦0.6, preferably 0.50≦w≦0.54, more preferably about 0.52, and where RE is a rare earth cation dopant, and 0<x<5%, preferably 0<x<2%.

[0008] The RE dopants employed advantageously generate both “hardening” and “softening” effects in the doped Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds. Examples of RE dopants which may be employed include Eu+3, Yb+3, Ce3+, Er3+, Tm3+, Ho3+ and Dy3+, and mixtures thereof, preferably Eu+3, and Yb+3, most preferably Yb+3. The Eu and Yb dopants advantageously produce both “hardening” and “softening” effects in Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds such as 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3. Doping of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 with any of Eu and Yb produces increased Qm, d31, and k31 relative to undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3. Under high Eac conditions, Eu and Yb doping of Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 type compounds such as 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 advantageously produces an increased vo relative to undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3. These doped compounds include compounds of formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.90, w is 0.52, RE is Yb and x is about 0.1 to about 0.3%. Advantageously, Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 type compounds such as 0.90Pb(Zr0.52Ti0.48O)3−0.10Pb(Mn1/3Sb2/3)O3, when doped with about 0.1 to about 2.0 wt. % Yb, preferably about 0.1% to about 0.2% Yb, produces a high-power piezoelectric material.

[0009] In another aspect, the invention relates to piezoelectric devices such as ultrasonic motors, ultrasonic vibrators, and piezoelectric actuators which include a piezoelectric ceramic compound represented by formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z≦0.95, preferably about 0.90, 0.4≦w≦0.6, preferably 0.50≦w≦0.54, more preferably about 0.52, RE is a rare earth cation such as Yb, Eu and Ce, and 0<x<5%, preferably 0<x<2%.

[0010] In yet another aspect, the invention relates to piezoelectric ceramic compounds represented by formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.9, w is 0.52, RE is a rare earth cation selected from the group consisting of Eu, Lu, Nd and La and x is 0.1%.

DETAILED DESCRIPTION OF THE INVENTION

[0011] In the present invention, rare earth doped, piezoelectric compounds are produced. The compounds correspond to the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is ≦0.95, preferably about 0.90, 0.4≦w≦0.6, preferably 0.50≦w≦0.54, more preferably about 0.52, RE is a rare earth cation dopant, and 0<x<5%, preferably 0<x<2.0%, and even more preferably x is about 0.1% to about 0.5%. These compounds are made by reaction of 98% or higher purity, preferably 99% or higher, oxides of ZrO2, TiO2, MnO, Sb2O5 and a RE oxide. The RE oxide has a purity of 98% or higher. The high purity oxides employed, including the RE dopant oxides, are available from, such as, Alfa Aesar Co., Ward Hill, Mass. (USA)

[0012] The ionic radii of the RE cations of the RE oxides which may be employed are shown in Table 1:

TABLE 1
Ionic Radii
RE Cation Ionic Radius (Angstrom)
Ce3+      1.034
Eu3+      0.947
Yb3+      .0858
Tm3+      0.869
Er3+      0.881
Ho3+      0.901
Dy3+      0.912
Nd3+      0.995
Lu3+      0.848
La3+      1.061

[0013] In manufacture of the RE doped compounds, starting materials in the form of oxides, or precursors thereof such as carbonates and oxalates are employed. The amounts of the starting materials are sufficient to produce a base compound corresponding to the formula zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3, where z is ≦0.95, preferably about 0.90, 0.4≦w≦0.6, preferably 0.50≦w≦0.54, more preferably about 0.52. A RE dopant in the form of an oxide or precursor thereof is added to these starting materials in an amount sufficient to produce a doped compound corresponding to the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is ≦0.95, preferably about 0.90, 0.4≦w≦0.6, preferably 0.50≦w≦0.54, more preferably about 0.52, RE is a rare earth cation dopant, and 0<x<5%, more preferably 0<x<2%, even more preferably x is about 0.1% to about 0.5%. The resulting blend of starting materials and dopant is mixed with a liquid such water or alcohol to form a slurry. Examples of suitable alcohols include but are not limited to C1-C4 alcohols, preferably anhydrous ethyl alcohol. The slurry is milled by ball milling or vibratory milling, preferably vibratory milling, for a time sufficient, typically about 48 hours, to achieve a uniform mixture. The mixture then is sieved to about −80 mesh to about −200 mesh, calcined, and then mixed with a liquid such as water or alcohol to form a slurry that is milled again. The resulting milled material then is dried, sieved to about −80 mesh, preferably about −200 mesh, and mixed with an organic binder to form a material. Useful organic binders include, but are not limited to, acryloid resins, and polyvinyl alcohol, preferably acryloid resins. The resulting material is isostatically cold pressed at about 3000 kg/cm2 to about 3500 kg/cm2 to produce a preform such as rectangular bar. The preform then is sintered to produce the final piezoelectric compound.

[0014] The invention is further illustrated below by reference to the following non-limiting examples. In the examples below, the amount of RE dopant is based on the weight of the base compound zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3.

EXAMPLE 1

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Yb3+)

[0015] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure), 1.642 grams Sb2O5 (99.99% pure) are employed as starting materials. These starting materials are milled with 0.06 grams Yb2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is calcined at 800° C. for 4.5 hrs. The calcined powder is ground, and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder)of acryloid resin from Rohm and Hass Co. to form a material. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Yb3+)

EXAMPLE 2

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.2% Yb3+)

[0016] The procedure of example 1 is performed except that 0.0899 grams Yb2O3 (99.9% pure) is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.2% Yb3+)

EXAMPLE 3

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Yb3+)

[0017] The procedure of example 1 is performed except that 0.18 grams Yb2O3 (99.9% pure) is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0 52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Yb3+)

EXAMPLE 4

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Yb3+)

[0018] The procedure of example 1 is performed except that 0.3 grams Yb2O3 (99.9% pure) is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Yb3+)

EXAMPLE 5

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Eu3+)

[0019] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure),and 1.642 grams Sb2O5 (99.99% pure). These starting materials are milled with 0.0536 grams Eu2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound corresponds is a solid solution that to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Eu3+).

EXAMPLE 6

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Eu3+)

[0020] The procedure of example 5 is performed except that 0.161 grams Eu2O3 (99.9%) is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Eu3+).

EXAMPLE 7

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Eu3+)

[0021] The procedure of example 5 is performed except that 0.267 grams Eu2O3 (99.9%) is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Eu3+).

EXAMPLE 8

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Ce3+)

[0022] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO (99% pure), 1.642 grams Sb2O5 (99.99% pure). These starting materials are milled with 0.05 grams CeO2 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Ce3+).

EXAMPLE 9

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Ce3+)

[0023] The procedure of example 7 is performed except that 0.15 grams CeO2 is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.3% Ce3+).

EXAMPLE 10

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Ce3+)

[0024] The procedure of example 7 is performed except that 0.25 grams CeO2 is used. The resulting doped compound is a solid solution that corresponds to the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.5% Ce3+).

EXAMPLE 11

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% La3+)

[0025] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2 (99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure),and 1.642 grams Sb2O5 (99.99% pure) are employed as starting materials. These starting materials are milled with 0.0496 grams La2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound corresponds to a solid solution of the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% La3+).

EXAMPLE 12

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Nd3+)

[0026] 5.30 grams Pb3O4(99% pure), 8.915 grams ZrO(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure),and 1.642 grams Sb2O5 (99.99% pure) are employed as starting materials. These starting materials are milled with 0.0512 grams Nd2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound corresponds to a solid solution of the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Nd3+).

EXAMPLE 13

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Lu3+)

[0027] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure), and 1.642 grams Sb2O5 (99.99% pure) are employed as starting materials. These starting materials are milled with 0.0606 grams Lu2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound corresponds to a solid solution of the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Lu3+)

EXAMPLE 14

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Er3+)

[0028] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure), and 1.642 grams Sb2O5 (99.99% pure) are employed as starting materials. These starting materials are milled with 0.0582 grams Er2O3 (99.9% pure) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled. The resulting doped compound corresponds to a solid solution of the formula (0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Er3+)

[0029] In another aspect of the invention, mixtures of dopants are used. This aspect of the invention is illustrated by the following non-limiting example.

EXAMPLE 15

(0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3+0.1% Yb3+ and 0.1% Eu3+

[0030] A mixture of 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure), 1.642 grams Sb2O5 (99.99% pure). These starting materials are milled with 0.0449 g Yb2O3 (99.9% pure) and 0.0402 g Eu2O3 (99.9%) in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is sieved to −200 mesh and calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting material is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1210° C., maintained at 1210° C. for 2 hrs, and furnace cooled.

COMPARISON EXAMPLE

Undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3

[0031] 35.30 grams Pb3O4 (99% pure), 8.915 grams ZrO2(99% pure), 5.248 grams TiO2(99.5% pure), 0.363 grams MnO(99% pure) and 1.642 grams Sb2O5 (99.99% pure) are wet milled in anhydrous ethyl alcohol in a SWECO vibratory mill for 48 hrs. The resulting mixture is calcined at 800° C. for 4.5 hrs. The calcined powders are ground and wet milled again in anhydrous ethyl alcohol in the SWECO mill for 48 hours. The resulting milled powder then is dried, sieved to −200 mesh and mixed with 3 wt. % (based on the weight of the milled powder) of acryloid resin from Rohm and Hass Co. to form a mixture. The resulting mixture is cold isostatic pressed at 3000 kg/cm2 for 10 minutes to produce a preform in the shape of a rectangular bar. The preform then is heated in flowing air at 0.5° C./min to 300° C. and held at 300° C. for 4 hr. The preform then is heated at 2.5° C./min from 300° C. to 550° C., and held at 550° C. for 4 hrs. The preform then is cooled to room temperature. The preform then is heated at 5° C./min to 1230° C., maintained at 1230° C. for 2 hrs, and furnace cooled.

[0032] Property Measurement

[0033] The sintered samples produced in examples 1-9, as well as in the comparison example, are cut into rectangular plates of dimensions 42 mm×7 mm×1 mm. Gold electrodes are sputtered onto the top and bottom surfaces of the plates. The plates then are poled at 2.5 kV/mm for 15 min at 130° C. in silicon oil. Electrical measurements are performed at 36 hrs after poling. Curie Temperature (Tc) is determined by measuring dielectric response as function of temperature and frequency. The measurements are made while cooling at a rate of 2° C./min by using a HP 4275 A LCR meter.

[0034] The piezoelectric properties are determined by impedance spectra under a low-level constant-voltage using a HP4194 impedance analyzer according to IEEE standard on Piezoelectricity (American National Standard, STD 176/1987). By measuring resonance and antiresonance frequencies and other parameters, piezoelectric properties such as d31 and k31 are calculated by known techniques according to this standard.

[0035] The piezoelectric properties also are determined by impedance spectra under various vibration velocities using a constant current method using laser Doppler vibrometer (LDV) models OFV-3001 and OFV-511 from Polytec PI Corp. This constant current method is described by Uchino et al. in the Journal of Electroceramics 2:1, 33-40, 1998. As described therein, this method entails measuring admittance (Y) as a function of frequency to obtain an admittance curve under a constant current. This constant current method of measurement achieves a completely symmetrical impedance peak at high vibrational driving condition. The vo is read directly read from the laser Doppler vibrometer.

[0036] X-ray diffraction patterns of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 doped with 0.1, 0.3, 0.5 wt. % Eu, and with 0.1, 0.3, 0.5 wt. % Yb have a single phase perovskite structure. The piezoelectric properties of doped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3, as well as of undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3, are shown in table 2.

TABLE 2
Piezoelectric properties of doped
0.90Pb(Zr0.52Ti0.48)03-0.10Pb(Mn⅓Sb⅔)O3
							Elastic
Amount & type	Density				|d31|		Compliance
of dopant wt. %	(103 kg/m3)	Qm	K	k31	(pC/N)	Tc	(10−12 (m2/N))
Undoped	7.38	1150	660	0.19	44	290	8.8
0.1 Eu	8.40	—	608	0.24	50	262	8.1
0.3 Eu	8.08	1210	578	0.23	48	265	8.7
0.5 Eu	8.02	1340	565	0.24	51	263	8.8
0.1 Yb	8.20	1250	610	0.23	50	255	8.5
0.2 Yb	8.35	1386	509	0.28	57	—	9.0
0.3 Yb	7.85	1350	490	0.27	53	250	8.8
0.5 Yb	7.70	1330	550	0.26	53	248	9.2
0.1 La	7.62	1484	653	0.22	53	—	9.8
0.1 Nd	7.93	1437	624	0.22	52	—	9.6
0.1 Lu	8.17	1608	566	0.25	53	—	8.8
0.1 Er	8.20	1293	490	0.28	56		8.8

[0037] As shown in Table 2, K decreased with increasing amounts of Eu and Yb dopants. Table 2 also shows that the Qm of Eu doped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 increased from as the amount of Eu dopant increased from 0% to 0.5%. As the amount of Eu dopant increased from 0 to 0.3 wt. %, k31 increased by 17%, and the absolute value of d31 increased from 44 pC/N to 51 pC/N. The Curie Temperature (Tc)decreased from 290° C. to 263° C. at 0.5 wt. % Eu. In addition, upon Eu doping, the elastic constant decreased, and then increased to 8.8×10−12 m2/N at 0.5 wt. % Eu.

[0038] As also shown in Table 2, the Qm of Yb doped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 increased from 1150 to 1350 as the amount of Yb dopant increased from 0% to 0.3%; k31 increased by 39% at 0.3 wt. % Yb, and the 475 absolute value of d31 increased from 44 to 53 pC/N at 0.3 wt. % upon Yb dopant. The Curie Temperature decreased from 290° C. to 250° C. at 0.3 wt. % Yb, and the elastic constant decreased, and then increased to 9.2×10−12 m2/N at 0.5 wt. % Yb.

[0039] The increased values of Qm, together with the decreased values of K, show that Eu and Yb dopants generate “hardening” effects in Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds such as 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3. In addition, the increased values of k31 together with the increased absolute values of d31 show the “softening” effects generated by use of Eu and Yb dopants on Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds such as 0.90Pb(Zr0.52Ti0.48)O3−010Pb(Mn1/3Sb2/3)O3.

[0040] The results in Table 2 show that Eu3+ and Yb3+ dopants generate a combination of “hardening” and “softening” doping effects on Pb(Zr,Ti)O3—Pb(Mn,Sb)O3 compounds such as 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3.

[0041] As is known in the art, for a rectangular sample driven by an electric field under the d31 mode, where both longitudinal ends of the sample are mechanically free, vo is proportional to the product k31Qm. In order to have a maximum vo, both Qm and k31 should be maximized. However, simultaneous achievement of maximum values of Qm and k31 is contrary to conventional prior art concepts of “hardening” and “softening” piezoelectric characteristics. Advantageously, however, the present invention produces such a combination of “hard” and “soft” piezoelectric characteristics.

[0042] Table 3 shows vibrational velocity (vo) as a function of electric field (Eac, rms) and dopant on 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3.

TABLE 3
Vo as function of (Eac, rms) and
dopant in 0.90Pb(Zr0.52Ti0.48)03-0.10Pb(Mn⅓Sb⅔)O3
Dopant/
Eac/Vo	vo1	Eac2	vo1	Eac2	vo1	Eac2	vo1	Eac2	vo1	Eac2	vo1	Eac2	vo1	Eac2	vo1	Eac2
Undoped	0.04	0.7	0.2	2.2	0.38	3.6	0.38	4.1	0.57	5.2	0.58	6.0	0.60	7.0	0.62	10.0
0.1% Yb	0.2	0.7	0.58	2.2	0.71	3.6	0.78	4.1	0.92	5.2	0.96	6.0	1.0	7.0	1.00	10.0
0.2% Yb	0.07	3.4	0.06	6.84	—	—	—	—	—	—	—	20.0	0.92	—	1.00	10.0
0.3% Yb	0.18	0.7	0.60	2.2	0.66	3.6	0.78	4.1	0.84	5.2	0.92	6.0	0.84	7.0	0.90	10.0
0.5% Yb	0.18	0.7	0.57	2.2	0.61	3.6	0.68	4.1	0.69	5.2	0.70	6.0	0.68	7.0	0.82	10.0
0.3% Eu	0.42	1.8	0.58	3.0	0.61	3.6	078	4.6	0.78	6.0	0.90	8.3	0.94	9.6	—	—
0.5% Eu	0.30	1.8	0.44	3.0	0.54	3.6	0.60	4.6	0.64	6.0	0.78	8.3	0.79	9.6	—	—
0.1% La	0.31	0.93	0.51	1.6	0.62	2.1	0.66	3.2	0.74	4.1	0.78	5.3	0.84	6.8	—	—
0.1% Nd	0.2	0.66	0.51	1.9	0.66	2.9	0.73	3.4	0.81	3.8	0.90	5.0	—	—	—	—
0.1% Lu	0.21	0.66	0.30	0.91	0.55	1.8	0.64	2.4	0.68	3.3	0.75	4.1	0.81	5.3	0.85	8.3
0.1% Er	0.19	0.66	0.38	1.5	0.49	2.3	0.55	3.1	0.61	4.0	0.83	5.0	—	—	—	—
1(m/s, rms)
2(kV/m, rms)

[0043] As shown in Table 3, at Eac=10.0 kV/m (rms), vo is 1.0 m/s (rms) for 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 doped with 0.1 wt. % Yb to 0.2 wt. % Yb. As the amount of Yb dopant increased, vo decreased slightly but remained significantly higher than that of the undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 that has a vo of 0.60 m/s rms) at Eac=7 kV/m (rms).). In addition, by introducing Eu dopant, the vo of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 also increased. The vo of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 doped with 0.3 wt. % Eu is 0.94 m/s at E=9.6 kV/m (rms value).

[0044] Another important property of high power piezoelectric materials is heat generation (ΔT). A high-power piezoelectric material desirably has a high vo and low ΔT. Achievement of high vo and low ΔT, however, has been a problem in the art because ΔT is proportional to vo2.

[0045] Table 4 shows vo as a function of ΔT. Heat generation is measured by a thermocouple placed at the nodal point of the vibrating sample.

TABLE 4
(Vo, rms) and T(° C.) as function of dopant in
0.90Pb(Zr0.52Ti0.48)03-0.10Pb(Mn⅓Sb⅔)O3
Dopant	Vo1	T	Vo1	T	Vo1	T	Vo1	T	Vo1	T	Vo1	T	Vo1	T
Undoped	0.2	2.0	0.38	4.8	0.57	8.0	0.62	20	0.65	25	—	—	—	—
0.1% Y	0.2	0.5	0.38	2.0	0.57	4.0	0.65	5.0	0.77	8.0	0.93	0.9	1.0	20
0.2% Y	0.7	0.3	0.86	19	1.0	40.	—	—	—	—	—	—	—	—
0.3% Y	0.52	2.0	0.6	2.2	0.65	2.5	0.77	4.5	0.82	6.0	0.90	10	0.92	20
0.5% Y	0.2	0.5	0.38	1	0.6	3.0	0.77	9.0	0.82	10	0.86	12	0.88	20
0.3% E	0.32	0.5	0.54	1.5	0.61	2.0	0.76	5	0.9	20	—	—	—	—
0.5% E	0.32	2	0.43	6	0.52	7.5	0.62	12	0.73	18	—	—	—	—
0.1% Ce	—	—	—	—	—	—	—	—	—	—	—	—	0.74	20
0.3% Ce	—	—	—	—	—	—	—	—	—	—	—	—	0.79	20
0.5% Ce	—	—	—	—	—	—	—	—	—	—	—	—	0.63	20
0.1% La	0.30	1.5	0.50	5	0.62	7.5	0.66	12	0.74	19.5	0.78	23	—	—
0.1% Nd	0.20	1	0.51	5	0.66	9	0.73	14	0.81	16	0.9	20	—	—
0.1% Lu	0.21	0.5	0.55	3.5	0.64	6	0.68	8	0.81	16.5	0.84	21.5	—	—
0.1% Er	0.19	0.5	0.38	2.5	0.49	5	0.55	7.5	0.61	10	0.83	23	—	—

[0046] Table 4 shows that the maximum vibrational velocity, vo(ΔT=20° C.) is 0.62 m/s for undoped 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3. The 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 compound doped with 0.3 wt. % Eu produces a vo(ΔT=20° C.) of 0.9 m/s. Doping of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 with 0.1 wt. % Yb produces a vo(ΔT=20° C.) of 1.0 m/s. In addition, doping of 0.90Pb(Zr0.52Ti0.48)O3−0.10Pb(Mn1/3Sb2/3)O3 with 0.2 wt. % Yb produces a vo(ΔT=40° C.) of 1.0 m/s.

Claims

1. A piezoelectric compound of the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z≦0.95, 0.40≦w≦0.60, and where RE is a rare earth cation selected from the group consisting of Eu, Yb, Ce, La, Er, Nd, Lu, Tm, Ho and Dy and 0<x<5.0%.

2. The piezoelectric compound of claim 1 where z is 0.9, 0.5<w<0.54 and 0<x<2.0%.

3. The piezoelectric compound of claim 2 where w is about 0.52.

4. A piezoelectric compound of the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.90, w is 0.52, RE is Yb and x is 0.1 to 0.5%.

5. The piezoelectric compound of claim 4 wherein x is 0.1 to 0.3%.

6. A piezoelectric compound of the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.90, w is 0.52, RE is wherein RE is Eu and x is about 0.1 to 2%.

7. The piezoelectric compound of claim 6 wherein x is about 0.1% to about 0.5%.

8. A composition comprising Pb3O4, ZrO2, TiO2, MnO, and Sb2O5 and a rare earth dopant oxide in amounts sufficient to produce a piezoelectric compound corresponding to the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is ≦0.95, 0.50<w<0.54, RE is a rare earth cation dopant selected from the group consisting of Yb, Eu, La, Nd, Er, Lu and Ce, and 0<x<5.0%

9. A composition comprising Pb3O4, ZrO2, TiO2, MnO, and Sb2O5 and a rare earth dopant oxide in amounts sufficient to produce a piezoelectric compound corresponding to the formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.90, w is 0.52, and RE is a rare earth cation dopant selected from the group consisting of Yb and Eu, and 0≦x≦0.5%

10. The composition of claim 11 wherein 0<x<2%.

11. A piezoelectric device comprising a piezoelectric ceramic compound represented by formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z≦0.95, w is about 0.52, RE is a rare earth cation selected from the group consisting of Yb, Eu, La, Nd, Er, Lu and Ce, and 0≦x≦5.0%.

12. The composition of claim 13 wherein 0<x<2%.

13. The piezoelectric device of claim 12 where z is about 0.90.

14. The piezoelectric device of claim 13 where RE is selected from the group consisting of Yb and Eu.

15. The piezoelectric device of claim 14 where z is about 0.90, w is about 0.52, RE is Yb and x is 0.1 to 0.5%.

16. The piezoelectric device of claim 15 where x is 0.1 to 0.3%.

17. The piezoelectric device of claim 14 where z is 0.90, w is 0.52, RE is Eu and x is about 0.1 to about 0.5%.

18. The piezoelectric device of claim 17 where x is about 0.1 to about 0.3%.

19. A piezoelectric ceramic compound represented by formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+(Ybx+Eux)) where z is 0.9, w is 0.52, and x is 0.1%.

20. A piezoelectric ceramic compound represented by formula (zPb(ZrwTi(1−w))O3−(1−z)Pb(Mn1/3Sb2/3)O3+REx) where z is 0.9, w is 0.52, RE is a rare earth cation selected from the group consisting of Er, Lu, Nd and La and x is 0.1%.

21. The piezoelectric ceramic compound of claim 20 wherein RE is Er.

22. The piezoelectric ceramic compound of claim 20 wherein RE is Lu.

23. The piezoelectric ceramic compound of claim 20 wherein RE is Nd.

24. The piezoelectric ceramic compound of claim 20 wherein RE is La.