Pb(Hf,Ti)O3 BASED HIGH PERFORMANCE POLYCRYSTALLINE PIEZOELECTRIC MATERIALS

Abstract
A ternary polycrystalline material based on lead hafnate (PbHfO3) and having improved dielectric, piezoelectric, and/or thermal stability properties. The Pb(Hf,Ti)O3 based material can exhibit enhanced electromechanical coupling factors when compared to PZT based ceramics and can be used as high performance actuators, piezoelectric sensors and/or ultrasonic transducers. The ternary polycrystalline material can have a perovskite crystal structure with an ABO3 formula and can be characterized by a substitution of heterovalent acceptor and donor ions at A or B (Zr/Hf) sites.
Description
FIELD OF THE INVENTION

The present invention is related to a piezoelectric material, and in particular, a high performance polycrystalline piezoelectric material based on lead hafnate.


BACKGROUND OF THE INVENTION

For the past 60 years, perovskite Pb(ZrxTi1-x)O3 (PZT) piezoelectric ceramics have dominated the commercial market of piezoelectric sensors, actuators and medical ultrasonic transducers due to their high dielectric, piezoelectric and electromechanical coupling factor properties. In addition, the properties of PZT piezoelectric ceramics can be further modified with different additives and/or dopants. In particular, PZT piezoelectric ceramics with compositions in the vicinity of a morphotropic phase boundary (MPB) that separates a rhombohedral phase from a tetragonal ferroelectric phase can exhibit anomalously high dielectric and piezoelectric properties. The high properties are the result of enhanced polarizability from the coupling between two equivalent energy states, i.e. between a tetragonal phase and a rhombohedral phase, which allows optimum domain reorientation during poling.


Numerous PZT formulations/compositions have been engineered for specific characteristics that enhance their use in many applications. For example, Tables I and II list the properties of commercially available soft PZT ceramics, and FIGS. 1 and 2 provide plots of dielectric permittivity and piezoelectric coefficient d33 versus Curie temperature (TC) for such materials. As shown by the data, polycrystalline materials with higher Curie temperatures generally possess lower dielectric and piezoelectric properties.









TABLE I







Piezoelectric, dielectric and ferroelectric


properties of commercial PZT5A type ceramics.




















Pr




d33
kp

tanδ
TC
(μC/
EC


PZT5H
(pC/N)
(%)
εr
(%)
(° C.)
cm2)
(kV/cm)





TRS200HD1
400
0.66
2000
1.8
340
/
/


3195STD2
350
0.63
1800
1.8
350
39
14.9


3295HD2
390
0.65
1900
1.8
350
39
12.0


PIC2553
400
0.62
1750
2.0
350
/
/


PIC1553
360
0.62
1450
2.0
345
/
/


PKI5024
425
0.60
2000
1.5
350
/
/


PZ235
328
0.52
1500
1.3
350
/
/


PZ275
425
0.59
1800
1.7
350
/
/


PZT5A16
410
0.62
1875
2.0
370
/
/


PZT5A36
374
0.60
1700
2.0
365
/
/






1TRS Technologies;




2CTS;




3PIceramic;




4Piezo-kinetics;




5Ferroperm;




6Morgan.














TABLE II







Piezoelectric, dielectric and ferroelectric


properties of commercial PZT5H type ceramics.




















Pr




d33
kp

tanδ
TC
(μC/
EC


PZT5H
(pC/N)
(%)
εr
(%)
(° C.)
cm2)
(kV/cm)





TRS610HD1
690
0.70
3900
1.8
210
/
/


CTS3203STD2
550
0.69
3250
2.0
235
37
10.6


CTS3203HD2
650
0.70
3800
2.0
225
39
 8.0


PIC1513
500
0.62
2400
2.0
250
/
/


PIC1533
600
0.62
4200
3.0
185
/
/


PKI5324
490
0.63
2700
2.0
220
/
/


PKI5524
600
0.67
3400
2.2
200
/
/


PZ215
640
0.60
3980
1.6
218
/
/


PZ295
570
0.64
2870
1.6
235
/
/


PZT5H16
620
0.60
3400
1.8
200
/
/


PZT5H26
590
0.65
3400
2.5
195
/
/






1TRS Technologies;




2CTS;




3PIceramic;




4Piezo-kinetics;




5Ferroperm;




6Morgan.







It is appreciated that innovations in electronic devices have been the driving force for new developments in piezoelectric ceramics. In fact, and in order to meet the newly developed electromechanical devices, materials with Curie temperatures equivalent to heretofore developed materials but with higher dielectric and piezoelectric properties, and/or materials with similar dielectric and piezoelectric properties but higher Curie temperatures, are desired.


In addition to the above, the electromechanical coupling factor—the square of which is closely related to output power density—is known to be an important material parameter in ultrasonic transducer applications and the dielectric variation for prior art PZT based materials is relatively broad and on the order of 2000-8000 ppm/° C. Therefore, a new polycrystalline piezoelectric material with increased electromechanical coupling factor and reduced dielectric variation would also be desirable.


SUMMARY OF THE INVENTION

Ternary polycrystalline materials based on lead hafnate (PbHfO3) and having improved dielectric, piezoelectric, and/or thermal stability properties are provided. In addition, the PbHfO3 based materials can exhibit enhanced electromechanical coupling factors when compared to PZT based ceramics. The inventive materials can be used as high performance actuators, piezoelectric sensors and/or ultrasonic transducers.


In particular, the ternary polycrystalline materials provide piezoelectric ceramic materials based on lead hafnium titanate, e.g. PbHfO3—PbTiO3 (PHT), that have a perovskite crystal structure with an ABO3 formula and are characterized by a substitution of heterovalent acceptor and donor ions at Zr/Hf sites. In addition, Pb(MI3+,MII5+)O3—PHT ternary systems are provided that have: (1) equivalent Curie temperatures as prior art PZT based ceramics but exhibit higher dielectric and piezoelectric properties when compared thereto; and/or (2) comparable dielectric and piezoelectric properties as prior art PZT based ceramics but exhibit higher Curie temperatures when compared thereto.


In some instances, the ternary polycrystalline materials have a formula of Pb1-xMx [(MI,MII)O3]1-y-zHfzTiyO3, where M is Ba2+, Ca2+, Sr2+, La3+ and the like; MI is Mg2+, Zn2+, Ni3+, Yb3+, Sc3+, In3+ and the like; MII is Nb5+, Ta5+, Sb5+ and the like; x is greater than or equal to 0.0 and less than 0.2; y is greater than 0.3 and less than 0.7; and z is greater than 0.3 and less than 0.7. In other instances, the ternary piezoelectric polycrystalline material has a formula of Pb1-xMx [(MI3+,MII5+)O3]1-y-zHfzTiyO3, where Hf 4+ or Ti4+ ions are at least partially replaced with donor dopants or acceptor dopants. The donor dopants can be Nb5+, Ta5+, W5+ and the like and the acceptor dopants can be Fe2+,3+, Co2+,3+, Mn2+,3+ and the like.


The inventive material can have a Curie temperature in the range of 180° C. to 280° C. and a piezoelectric coefficient d33 greater than 600 pC/N, a Curie temperature of greater than 300° C. and a piezoelectric coefficient d33 greater than 500 pC/N, a Curie temperature in the range of 260-300° C. and a piezoelectric coefficient d33 in the range of 450-680 pC/N, and/or a Curie temperature greater than 120° C. and a piezoelectric coefficient d33 greater than 800 pC/N. In addition, the material can have electromechanical coupling k33 greater than or equal to 78-80%.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is a graphical plot illustrating dielectric permittivity as a function of Curie temperature for PZT piezoelectric ceramics;



FIG. 2 is a graphical plot illustrating piezoelectric coefficient d33 as a function of Curie temperature for PZT piezoelectric ceramics;



FIG. 3 is a graphical plot illustrating Curie temperature versus amount of PMN for pellets having a composition formula of (1-x)Pb(Hf1-yTiy)O3-xPMN with various levels of lead titanate (PT);



FIG. 4 is an isothermal map of Currie temperature (TC) for (1-x)Pb(Hf1-yTiy)O3-xPMN;



FIG. 5
a is a graphical plot illustrating piezoelectric coefficient d33 as a function of PMN content;



FIG. 5
b is a graphical plot illustrating planar electrochemical coupling kp as a function of PMN content;



FIG. 6 is a graphical plot with data from the inventive materials shown in Tables III-V superimposed on data shown in FIG. 1;



FIG. 7 is a graphical plot with data from the inventive materials shown in Tables III-V superimposed on data shown in FIG. 2; and



FIG. 8 is a graphical plot of electromechanical coupling factor squared (k332) as a function of Currie temperature for prior art PZT based ceramics and the inventive PHT based ceramics disclosed herein.





DETAILED DESCRIPTION OF THE INVENTION

Inventive lead hafnium titanate-lead magnesium niobate (PHT-PMN) ternary ceramics with compositions of (1-x)Pb(Hf1-yTiy)O3-xPb(Mg1/3Nb2/3)O3 ((1-x)Pb(Hf1-yTiy)O3-xPMN, x=0˜0.5, y=0.515˜0.7) are provided. For example and for illustrative purposes only, an example of how typical PHT-PMN ternary ceramics according to one or more embodiments of the present invention were produced and associated properties are described below.


The inventive materials were prepared using a two-step precursor method. Raw materials of MgCO3 (99.9%, Alfa Aesar, Ward Hill, Mass.), Nb2O5 (99.9%, Alfa Aesar), HfO2 (99.9%, Alfa Aesar) and TiO2 (99.9%, Ishihara, San Francisco, Calif.) were used to synthesize columbite precursors of MgNb2O6 and Hf0.45Ti0.55O2 at 1000° C. and 1200° C., respectively. Thereafter, Pb3O4 (99%, Alfa Aesar) and the MgNb2O6 and Hf0.45Ti0.55O2 percursor powders were batched stoichiometrically by wet-milling in alcohol for 24 hours (h). Dried mixed powders of the Pb3O4, MgNb2O6 and Hf0.45Ti0.55O2 were then calcined at 800° C. for 4 h to produce synthesized powders which were subsequently vibratory milled in alcohol for 12 h. The synthesized powders were then granulated and pressed into pellets having a 12 mm diameter, followed by a binder burnout at 550° C. and sintering in a sealed crucible at 1250° C. In order to minimize PbO evaporation during sintering, PbZrO3 was used as a lead (Pb) source in the sealed crucible.


Sintered pellets were tested for temperature dependence of dielectric permittivity with FIG. 3 illustrating Curie temperature (TC) versus amount of PMN for pellets having a composition formula of (1-x)Pb(Hf1-yTiy)O3-xPMN with various levels of lead titanate (PT). As shown in the figure, increasing the PMN content resulted in a monotonic TC decrease from 360-285° C., 340-270° C., 320-255° C., 328-243° C. and 234-186° C. for the different PT levels corresponding to y=0.515, 0.534, 0.555, 0.574 and 0.7, respectively. Furthermore, with increasing PMN content, the ternary solid solution exhibited more relaxor-like characteristics, showing broadened dielectric peaks and dispersive dielectric behavior with respect to frequency.


Based on the above results, an isothermal map of Currie temperature (TC) for (1-x)Pb(Hf1 -yTiy)O3-xPMN was developed and is shown in FIG. 4. It is appreciated that along the MPB line from the PH-PT side towards the PMN-PT side, TC gradually decreases from 325° C. to 200° C. It is appreciated that this decrease in TC could be due to an increase of PMN content in the sintered pellets that were tested.


The dielectric, piezoelectric and electromechanical properties of all studied (1-x)Pb(Hf1-yTiy)O3-xPMN compositions are summarized in Table III. In addition, the piezoelectric coefficient d33 and planar electromechanical coupling kp as a function of PMN are shown in FIGS. 5a and 5b, respectively. As shown in the figures, optimum piezoelectric and electromechanical properties where exhibited for specific compositions and it is appreciated that the optimum properties could be due to enhanced polarizability arising from coupling between tetragonal and rhombohedral phases. In addition, the optimum piezoelectric and electromechanical properties were achieved for the composition 0.8Pb(Hf0,445Ti0,555)O3-0.2Pb(Mg1/3Nb2/3)O3, with dielectric permittivity εr, piezoelectric coefficient d33, planar electromechanical coupling kp and TC being on the order of 2870, 680 pC/N, 70% and 276° C., respectively.









TABLE III







Piezoelectric, dielectric and ferroelectric properties of (1 −


x)Pb(Hf1−yTiy)O3-xPMN ternary ceramics.















d33
kp

tanδ
TC
Pr
EC


(1 − x)Pb(Hf1−yTiy)O3-xPMN
(pC/N)
(%)
εr
(%)
(° C.)
(μC/cm2)
(kV/cm)


















y = 0.515
x = 0
210
37
1220
1.1
360
13
13.2



x = 0.05
280
41
1560
1.6
333
25
11.9



x = 0.1
430
62
1100
2.1
306
37
8.8



x = 0.15
330
58
870
2.4
285
39
8.3


y = 0.534
x = 0.05
190
32
1350
1.4
340
18
14.4



x = 0.1
450
58
2030
1.4
312
32
15



x = 0.15
600
69
2330
1.9
291
40
9.4



x = 0.2
320
59
960
2.2
271
36
8.1


y = 0.555
x = 0.1
360
37
1300
1.4
321
23
17.3



x = 0.15
430
57
2120
1.4
296
32
15.2



x = 0.18
580
65
2770
1.5
286
37
11.3



x = 0.19
640
68
2810
1.5
278
40
10.3



x = 0.2
680
70
2870
1.7
276
40
9.9



x = 0.21
590
69
2040
1.6
271
42
9.3



x = 0.22
490
68
1630
1.8
268
40
8.4



x = 0.25
340
60
1020
2.2
255
38
7.9


y = 0.574
x = 0.1
160
32
1050
1.3
328
22
19.9



x = 0.15
300
49
1550
1.2
304
31
19.4



x = 0.2
440
58
2360
1.4
283
34
13.3



x = 0.24
670
69
2960
1.4
263
41
9.5



x = 0.25
640
65
2470
1.6
262
38
9.3



x = 0.26
580
65
1900
1.6
/
41
8.6



x = 0.3
230
48
1120
2.2
243
28
7.1


y = 0.7
x = 0.4
330
46
2360
0.8
234
26
10.7



x = 0.45
390
54
2050
1.1
213
30
7.3



x = 0.47
540
66
2090
1.3
201
37
7



x = 0.5
400
60
1420
1.8
186
36
5.9









The main properties of other systems, such as (1-x)Pb(Hf1-yTiy)O3-xPb(Ni1/3Nb2/3)O3 (PHT-PNN), (1-x)Pb(Hf1-yTiy)O3-xPb(Sc0.5Nb0.5)O3 (PHT-PSN) and (1-x)Pb(Hf1-yTiy)O3-xPb(Zn1/3Nb2/3)O3 (PHT-PZN), are given in Tables IV and V below, respectively.









TABLE IV







Piezoelectric, dielectric and ferroelectric properties of (1 −


x)Pb(Hf1−yTiy)O3-xPNN ternary ceramics.















d33
kp

loss
TC
Pr
Ec


Samples
(pC/N)
(%)
K
(%)
(° C.)
(μC/cm2)
(kV/cm)



















y = 0.55
x =
5
160
35
1050
1.0
337
10
12




10
280
43
1400
1.2
310
16
12




15
340
49
1830
1.8
280
24
10.7




18
495
61
2140
1.7
260
29
8




19
470
61
1970
1.6
256
28
7.5




20
435
61
1870
1.8
250
31
7.5




22
380
60
1250
1.7
238
34
7.3




25
350
60
1180
1.8
222
36
7.2


y = 0.57
x =
10
170

1030
1.1





15
250
39
1280
1.4
292
19
13.7




19
350
47
1950
1.5
266
21
10.2




20
360
49
2000
1.5
257
23
10.2




21
420
57
2100
1.55
252
27
9.8




22
480
57
2600
1.77
246
28
9




23
550
65
2650
1.8
240
32
8.8




25
595
66
2200
1.66
229
34
7.6




20
320
50
2000
1.2
260
24
11.5




22
410
54
2390
1.3
250
28
10.1




23
460
57
2600
1.38
244
29
9.8




24
530
61
2850
1.4
235
31
9.4




25
610
65
3000
1.5
234
33
8.6




26
650
68
2950
1.6
227
35
8.5




26.5
630
67
2430
1.5
225
35
8.4




27
660
68
2200
1.35
221
37
7.5




28
530
65
2270
1.5
215
36
7




30
460
64
2000
1.7
204
36
6.4


y = 0.60
x =
25
570
63
3200
1.46
225
29
9.5




28
650
67
3450
1.5
220
31
9




29
700
69
3610
1.7
214
32
8.3




30
765
70
3800
2.0
210
32
7.4




30.5
795
71
3600
2.0
206
33
7.2




31
760
71
3250
2.0
203
34
7.2




31.5
730
71
2940
1.8

35
6.9




32
690
70
2880
1.75
199
34
6.6




33
640
68
2350
1.75
191
34
6.2


y = 0.70
x =
30
300
47
1900
1.4
208
25
12.5




40
445
51
2700
1.3
184
26
9




42
540
55
3600
1.65
168
26
6




44
650
58
4500
1.85
155
26
6.7




45
725
60
4950
1.98
151
26
6.5




46
800
61
5500
1.8
145
27
5.6




47
865
63
5830
2.3
138
27
5.1




48
940
65
5240
2.4
120
27
3.8




49
970
65
6000
2.5

27
4.2




50
930
65
5930
2.38

27
4.3
















TABLE V







Piezoelectric, dielectric and ferroelectric properties


of (1 − x)Pb(Hf1−yTiy)O3-xPSN and


(1 − x)Pb(Hf1−yTiy)O3-xPZN ternary ceramics.




















Pr



Materials
d33
kp

loss
TC
(μC/
Ec















y
x
(pC/N)
(%)
K
(%)
(° C.)
cm2)
(kV/cm)












(1 − x)Pb(Hf1−yTiy)O3-xPSN















0.60
0.20
550
65
2420
1.5
325
38
10.6


0.575
0.175
600
71
2220
1.6
325
43
9.4


0.55
0.12
590
70
2250
1.6
334
43
9.5


0.55
0.125
560
67
1950
1.7
330
41
9.2









(1 − x)Pb(Hf1−yTiy)O3-xPZN















0.519
0.20
500
70
1650
2.0
292
42
9.1


0.525
0.20
530
69
2060
2.0
295
41
10.3


0.525
0.25
510
68
1900
2.0
280
41
9.9


0.539
0.225
570
68
2300
2.0
292
38
11.6









In order to provide a clearer view of the enhanced properties exhibited by the inventive materials, FIGS. 6 and 7 are plots of data from Tables III-V above compared to the data shown in FIGS. 1 and 2. The data from Tables III-V are labeled as PHT based ceramics, versus the data from FIGS. 1 and 2 which are labeled as PZT based ceramics. As shown in the figures, a comparable dielectric permittivity with significant higher d33 coefficient is exhibited by the inventive materials compared to heretofore polycrystalline piezoelectric materials. In addition, FIG. 8 provides a plot of the electromechanical coupling factor squared (k332) as a function of TC for prior art PZT based ceramics and the inventive PHT based ceramics. Again, a significant improvement in output power density is expected by the ternary PHT polycrystalline piezoelectric materials disclosed herein.


The invention is not restricted to the illustrative examples and embodiments described above. The examples are not intended as limitations on the scope of the invention. Methods, apparatus, compositions, and the like described herein are exemplary and not intended as limitations on the scope of the invention. Changes therein and others will occur to those skilled in the art and, as such, the specification and the appendices should be interpreted broadly.

Claims
  • 1. A ternary piezoelectric polycrystalline material comprising: a lead hafnium titanate containing ceramic having a formula of Pb1-xMx [(MI,MII)O3]1-y-zHfzTiyO3, where:M is at least one of Ba2+, Ca2+, Sr2+and La3+;MI is at least one of Mg2+, Zn2+, Ni3+, Yb3+, Sc3+,In3+, Fe3+ and Co3+, etc.;MII is at least one of Nb5+, Sb5+ and Ta5+;x is greater than or equal to 0.0 and less than 0.2;y is greater than 0.2 and less than 0.8; andz is greater than 0.2 and less than 0.8.
  • 2. The composition of claim 1, wherein said lead hafnium titanate containing ceramic has a Curie temperature in the range of 180° C. to 280° C. and a piezoelectric coefficient d33 greater than 600 pC/N.
  • 3. The composition of claim 1, wherein said lead hafnium titanate containing ceramic has a Curie temperature of greater than 300° C., a piezoelectric coefficient d33 greater than 500 pC/N and electromechanical coupling k33 greater than or equal to 78-80%.
  • 4. The composition of claim 1, wherein said lead hafnium titanate containing ceramic has a Curie temperature in the range of 260-300° C. and a piezoelectric coefficient d33 in the range of 450-680 pC/N.
  • 5. The composition of claim 1, wherein said lead hafnium titanate containing ceramic has a Curie temperature greater than 120° C. and a piezoelectric coefficient d33 greater than 800 pC/N.
  • 6. A ternary piezoelectric polycrystalline material comprising a lead hafnium titanate containing ceramic having a formula of Pb1-xMx [(MI3+,MII5+)O3]1-y-zHfzTiyO3, where:Hf4+ or Ti4+ ions are at least partially replaced with donor dopants or acceptor dopants;said donor dopants being at least one of Nb5+, Ta5+ and W5+; andsaid acceptor dopants being at least one of Fe2+,3+, Co2+,3+, Mn2+,3+, Cu+,2+.
  • 7. The composition of claim 6, wherein said lead hafnium titanate containing ceramic has a Curie temperature in the range of 180° C. to 280° C. and a piezoelectric coefficient d33 greater than 600 pC/N.
  • 8. The composition of claim 6, wherein said lead hafnium titanate containing ceramic has a Curie temperature of greater than 300° C., a piezoelectric coefficient d33 greater than 500 pC/N and electromechanical coupling k33 greater than or equal to 78-80%.
  • 9. The composition of claim 6, wherein said lead hafnium titanate containing ceramic has a Curie temperature in the range of 260-300° C. and a piezoelectric coefficient d33 in the range of 450-680 pC/N.
  • 10. The composition of claim 6, wherein said lead hafnium titanate containing ceramic has a Curie temperature greater than 120° C. and a piezoelectric coefficient d33 greater than 800 pC/N.
  • 11. A process for manufacturing a ternary polycrystalline piezoelectric ceramic comprising: providing precursors of columbite and hafnium-titanium oxide;providing a powder of Pb3O4;mixing the precursors of columbite and hafnium-titanium oxide with the powders of Pb3O4;calcining the mixture of columbite and hafnium-titanium oxide precursors and Pb3O4 powder to produce a synthesized powder; andsintering the synthesized powder to produce a ternary polycrystalline piezoelectric ceramic having a formula of Pb1-x,Mx[MI,MII)O3]1-y-zHfzTiyO3, where: M is at least one of Ba2+, Ca2+, Sr2+ and La3+;MI is at least one of Mg2+, Zn2+, Ni3+, Yb3+, Sc3+,In3+, Fe3+ and Co3+, etc.;MII is at least one of Nb5+, Sb5+ and Ta5+;x is greater than or equal to 0.0 and less than 0.2;y is greater than 0.2 and less than 0.8; andz is greater than 0.2 and less than 0.8.
  • 12. The process of claim 11, wherein the ternary polycrystalline piezoelectric ceramic has a Curie temperature in the range of 180° C. to 280° C. and a piezoelectric coefficient d33 greater than 600 pC/N.
  • 13. The process of claim 11, wherein the ternary polycrystalline piezoelectric ceramic has a Curie temperature of greater than 300° C., a piezoelectric coefficient d33 greater than 500 pC/N and electromechanical coupling k33 greater than or equal to 78-80%.
  • 14. The process of claim 11, wherein the ternary polycrystalline piezoelectric ceramic has a Curie temperature in the range of 260-300° C. and a piezoelectric coefficient d33 in the range of 450-680 pC/N.
  • 15. The process of claim 11, wherein the ternary polycrystalline piezoelectric ceramic a Curie temperature greater than 120° C. and a piezoelectric coefficient d33 greater than 800 pC/N.
CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority of U.S. Provisional Application 61/581,365, filed Dec. 29, 2011, the contents of which are incorporated herein by reference.

Provisional Applications (1)
Number Date Country
61581365 Dec 2011 US