The present invention relates to an actuator comprising a piezoelectric film and a method for driving the actuator.
As shown in
As shown in
However, when a potential difference is applied to the prior actuator, a stress due to a piezoelectric effect is generated uniformly in the plane of the piezoelectric layer. Accordingly, as shown in
The purpose of the present invention is to provide a method for driving an actuator in which unnecessary deformation is suppressed.
The present invention provides a method for driving an actuator, comprising the following steps (a) and (b):
a step (a) of preparing the actuator, wherein the actuator comprises a first electrode, a piezoelectric layer composed of (Bi,Na,Ba)TiO3, and a second electrode, the piezoelectric layer is interposed between the first electrode (5) and the second electrode, +X direction, +Y direction, and +Z direction denote [100] direction, [01-1] direction, and [011] direction, respectively, and the piezoelectric layer is preferentially oriented along the +Z direction; and
a step (b) of applying a potential difference between the first electrode and the second electrode to drive the actuator.
The present invention provides a method for driving an actuator in which the amount of the displacement along the X direction is much greater than the amount of the deformation along the Y direction.
An embodiment of the present invention is described below with reference to figures.
The example of the support 13 is a silicon substrate with an oxidized surface. The example of the third electrode 25 is a stacked electrode composed of a gold layer and a titanium layer. The stacked electrode may be formed by patterning a titanium film on which gold films are deposited repeatedly with a dry-etching method. The third electrode 25 is not required to be disposed on the support 13. LX and LY denote a length of the actuator 1 along the X direction and a width thereof along the Y direction, respectively.
In
The first electrode 5 is preferentially oriented along the +Z direction. The first electrode 5 may be composed of, for example, a metal film or an oxide electric conductive film. More than one film may be used. The metal includes platinum (Pt), palladium (Pd), and gold (Au). The oxide electric conductor includes nickel oxide (NiO), ruthenium oxide (RuO2), iridium oxide (IrO2), strontium ruthenate (SrRuO3), and lanthanum nickelate (LaNiO3).
The piezoelectric layer 7 is composed of (Bi, Na, Ba) TiO3. The piezoelectric layer 7 may contain a little amount of impurities such as manganese and iron to improve the property of the piezoelectric layer 7. The piezoelectric layer 7 is preferentially oriented along the +Z direction, namely, the [011] axis direction. This characterizes the present invention. The piezoelectric layer 7 may be formed with a spattering method.
Preferably, the second electrode 9 is formed of gold.
The first electrode 5 is electrically connected with the third electrode 25. The third electrode 25 may be provided to apply a voltage to the first electrode 5. However, the third electrode 25 is provided optionally. The support 13 immobilizes the one end of the laminate 11. The support 13 may be adhered to the laminate 11. Epoxy resin or solder may be used. A portion of the substrate 3 may be etched to form the support 13.
The actuator 1 according to the first embodiment comprises the first electrode 5, the piezoelectric layer 7 composed of (Bi, Na, Ba) TiO3, and the second electrode 9. The piezoelectric layer 7 is interposed between the first electrode 5 and the second electrode 9. A voltage is applied between the first electrode 5 and the second electrode 9 to drive the actuator 1. The one end portion of the laminate 11 is immobilized, whereas the other end portion is displaced along the Z direction in the cross-section view of XZ plane.
The method for driving the actuator 1 is described below.
However, when the voltage is applied between the first electrode 5 and the second electrode 9, the other end portion of the actuator 1 is deformed along the Y direction, as shown in
The broken line shows an ideal state (hereinafter, “non-deformation state”) where the center portion of the actuator 1 exists on the line segment, which connects both of the ends of the actuator 1, when the actuator 1 is seen from the +X direction. On the other hand, in
As shown in
In other words, hz denotes the distance along the Z direction between the center portion of the imaginary line segment which connects both ends of the actuator 1, and the center portion of the actuator 1, when the actuator 1, to which the potential difference is applied, is seen from the +X direction.
An actuator 1 with a small value of hz/dz is requested. Specifically, the value of hz/dz is not more than 0.1. If the value of hz/dz is more than 0.1, the other end portion of the actuator 1 may be broken.
An actuator 1 with greater LY has a greater driving force. An actuator 1 with smaller LX has a greater stiffness. Accordingly, the value of LY/LX is preferred to be greater. Specifically, it is preferred that the value of LY/LX is not less than 0.1.
The maximum value of LY is approximately 20 mm in light of the size of the substrate 3. When LY is 20 mm, the minimum value of LX is approximately 1 mm in light of cutting off the piezoelectric layer 7. Accordingly, it is preferred that the value of LY/LX is not more than 20.
On the contrary, when LY is greater, the value of hz/dz is also greater. This is a collision.
The present actuator 1 is characterized by that the piezoelectric layer 7 is preferentially oriented along the +Z direction, and that the one end along the X direction is immobilized whereas the other end portion is displaced along the Z direction. This allows the value of hz/dz of the present actuator to be smaller than that of the other actuator, even when the value of LY/LX is identical.
The following example gives a more detailed explanation of the present invention.
In example 1, an actuator according to
[Preparation of the Laminate 11]
A Pt layer with [011] axis direction and a thickness of 250 nm was formed with RF magnetron sputtering on the surface of a MgO monocrystalline substrate with (110) plane orientation and a thickness of 0.5 mm. The MgO monocrystalline substrate and the Pt layer correspond to the substrate 3 and the first electrode 5, respectively.
The condition of the RF magnetron sputtering is described below:
Target: Pt metal
Atmosphere: argon (Ar) gas
RF output: 15W
Temperature of the substrate: 300 degrees Celsius.
Next, a (Bi, Na, Ba) TiO3 layer with a thickness of 2.7 μm was deposited with RF magnetron sputtering on the surface of the first electrode 5 to form a piezoelectric layer 7.
The condition of the RF magnetron sputtering is described below:
Target: the above-mentioned composition
Atmosphere: mixed gas with Ar and Oxygen in which a flow ratio of Ar/O2 is 50/50.
RF output: 170W
Temperature of the substrate: 650 degrees Celsius.
The crystalline structure of the piezoelectric layer 7 was analyzed with X-ray diffraction.
Finally, an Au layer with a thickness of 100 nm was formed with deposition on the surface of the piezoelectric layer 7. The Au layer corresponds to the second electrode 9. Thus, the laminate 11 was prepared.
[Evaluation of Piezoelectric Performance]
The piezoelectric performance of the laminate 11 was evaluated as below. The laminate 11 was cut off to form some plates with a length of 20 mm and a width of 2 mm each. The plate was adhered to the support 13 to prepare a cantilever.
The amount of the displacement of the one end portion of the cantilever was measured with a laser displacement gauge, when a potential difference was applied between the first electrode 5 and the second electrode 9.
As understood from
The amount of the displacement when a potential difference of 10 V was applied was converted to a piezoelectric constant d31. The piezoelectric constant d31 according to
In an actuator, it is preferred that an amount of the displacement fails to generate hysteresis relative to an applied voltage. This requires the applied voltage to be not more than 20 V. Therefore, the maximum value of the applied voltage was set to be 10 V in the present example.
[Preparation of the Actuator]
In order to obtain the greater amount of the displacement, the MgO monocrystalline substrate was polished to render the thickness thereof to be 50 μm. The plate cut off from the laminate 11 was adhered with epoxy resin to the support 13 comprising the third electrode 25 to immobilize the laminate 11. The first electrode 5 was electrically connected to third electrode 25 with silver paste. Thus, the actuator 1 was prepared. The amount of the displacement dZ1 was measured with the laser displacement gauge, similarly to
[Research of the Relationship Between the Value of LY/LX and the Value of hz/dz]
The laminate 11 was cut off to form a plurality of plates with various lengths LX and various widths LY. Each of the one end portions of the plates was immobilized to prepare various actuators.
Table 1 shows the relationship between the value of LY/LX and the value of hz/dz, both of which each of actuators 1 according to the present example 1 has. The actuator 1 comprised the MgO monocrystalline substrate 3 with a thickness of 50 μm. The hz was the value measured when the potential difference between the first electrode 5 and the second electrode 9 is 10 V.
As shown in Table 1, when the value of LY/LX increases, the value of hz/dz also increases. When the value of LY/LX is 0.1 such that the minimum condition to obtain a driving force is satisfied, the value of hz/dz was so small (<0.01) that it was not able to be measured. Even when the value of LY/LX is 2.0, the value of hz/dz was 0.10. The inequality hz/dz≦0.1 was satisfied. Accordingly, the actuators according to the example 1 had a greater amount of the displacement and a smaller amount of the deformation.
The actuator according to comparative example 1 was prepared similarly to the example 1 except only that MgO monocrystalline substrate with (100) plane orientation was used in place of MgO monocrystalline substrate with (110) plane orientation. Both of the first electrode 5 and the piezoelectric layer 7 oriented along the [001] axis direction in accordance with the (100) plane direction of the substrate 3.
Similarly to the example 1, a piezoelectric constant d31 was evaluated. The piezoelectric constant d31 of the piezoelectric layer 7 according to the comparative example 1 is −130 pC/N along the [100] axis direction, which is in-plane. The piezoelectric constant d31 along the [010] axis direction, which orthogonal to the [100] axis direction is also −130 pC/N. This means that the piezoelectric layer 7 according to the comparative example 1 had an in-plane isotropic piezoelectric property.
Table 2 shows the relationships between the value of LY/LX and the value of hZ/dZ of the actuators according to the comparative example 1.
Because the piezoelectric property is isotropic, in Table 2, when the value of LY/LX is identical, the value of hz/dz was greater than that of Table 1. For this reason, the upper limit value of LY/LX which satisfies that the value of hz/dz is less than 0.1 was approximately 0.5. The upper limit value is one-fourth times as great as the upper limit value of LY/LX according to the example 1 (approximately, 2.0). Furthermore, the actuators according to the comparative example 1 have about one-fourth times driving forth, compared to the actuators according to the example 1.
An actuator according to the present invention may be used preferably for MEMS (Micro Electro Mechanical Systems) because of its great driving force.
Number | Date | Country | Kind |
---|---|---|---|
2010-185762 | Aug 2010 | JP | national |
This application is continuation of International Application No. PCT/JP2011/003400, filed on Jun. 15, 2011, which in turn claims the benefit of Japanese Application No. 2010-185762, filed on Aug. 23, 2010, the disclosures of which applications are incorporated by reference herein.
Number | Name | Date | Kind |
---|---|---|---|
5966787 | Nakayama et al. | Oct 1999 | A |
7965021 | Harigai et al. | Jun 2011 | B2 |
20050127795 | Torii et al. | Jun 2005 | A1 |
20060119229 | Koizumi et al. | Jun 2006 | A1 |
20090273652 | Kazama et al. | Nov 2009 | A1 |
20100194245 | Harigai et al. | Aug 2010 | A1 |
20110143146 | Harigai et al. | Jun 2011 | A1 |
Number | Date | Country |
---|---|---|
05-187867 | Jul 1993 | JP |
11180769 | Jul 1999 | JP |
2005-203725 | Jul 2005 | JP |
2007266346 | Oct 2007 | JP |
2008186985 | Aug 2008 | JP |
2008192672 | Aug 2008 | JP |
2009-049065 | Mar 2009 | JP |
2009-049065 | Mar 2009 | JP |
2009-286119 | Dec 2009 | JP |
Number | Date | Country | |
---|---|---|---|
20120043857 A1 | Feb 2012 | US |
Number | Date | Country | |
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Parent | PCT/JP2011/003400 | Jun 2011 | US |
Child | 13282089 | US |