CN115694405B - A structure and method for generating flexoelectricity - Google Patents
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Abstract
Description
技术领域Technical Field
本发明属于力电耦合领域,更具体地,涉及一种产生挠曲电的结构和方法。The present invention belongs to the field of electromechanical coupling, and more specifically, relates to a structure and method for generating flexoelectricity.
背景技术Background Art
随着微电子技术的快速发展,在微纳尺度下利用力电耦合效应来调控器件的性能引起了研究人员的广泛关注。力电耦合作用包括传统的压电耦合效应和挠曲电耦合效应。传统的力电耦合效应指的是压电效应,它是电极化与均匀应变之间的线性耦合。而挠曲电效应是电介质材料中的一种高阶力电耦合效应,它通常指电介质材料由于受到非均匀变形而引起的电极化,即应变梯度引起的电极化。挠曲电效应相比压电效应来讲存在的优势在于:第一,产生挠曲电效应的电介质材料不再仅限于非中心对称的晶体,挠曲电效应存在于所有的电介质中;第二,挠曲电效应与温度无关;第三,由于应变梯度和材料的特征尺寸成反比,当器件微缩至纳米尺度时,挠曲电效应会更加的显著。基于这些优势,挠曲电效应受到了越来越多的关注。With the rapid development of microelectronics technology, the use of electromechanical coupling effects to regulate the performance of devices at the micro-nano scale has attracted widespread attention from researchers. Electromechanical coupling effects include traditional piezoelectric coupling effects and flexoelectric coupling effects. The traditional electromechanical coupling effect refers to the piezoelectric effect, which is a linear coupling between electric polarization and uniform strain. The flexoelectric effect is a high-order electromechanical coupling effect in dielectric materials. It usually refers to the electric polarization caused by non-uniform deformation of dielectric materials, that is, the electric polarization caused by strain gradient. The advantages of the flexoelectric effect over the piezoelectric effect are: first, the dielectric materials that produce the flexoelectric effect are no longer limited to non-centrosymmetric crystals, and the flexoelectric effect exists in all dielectrics; second, the flexoelectric effect is independent of temperature; third, since the strain gradient is inversely proportional to the characteristic size of the material, the flexoelectric effect will be more significant when the device is miniaturized to the nanoscale. Based on these advantages, the flexoelectric effect has received more and more attention.
目前已有利用弯曲悬臂梁、弯曲薄膜、使用金字塔样品、梯形样品等方法产生挠曲电效应,并指出挠曲电效应具有明显的尺寸依赖关系,但是上述方法都是在准静态产生挠曲电的方法。由此可见,亟需发展以动态的方式产生挠曲电效应,为未来挠曲电效应在动态和中高频方向调控电子器件的性能奠定基础。At present, there are methods such as bending cantilever beams, bending films, using pyramid samples, trapezoidal samples, etc. to produce flexoelectric effect, and it is pointed out that flexoelectric effect has obvious size dependence, but the above methods are all methods of generating flexoelectricity in quasi-static state. It can be seen that it is urgent to develop a dynamic way to generate flexoelectric effect, so as to lay a foundation for the future flexoelectric effect to control the performance of electronic devices in dynamic and medium-high frequency directions.
发明内容Summary of the invention
针对现有技术的以上缺陷或改进需求,本发明提供了一种产生挠曲电的结构和方法,其目的在于为挠曲电效应在动态和中高频方向调控电子器件的性能奠定基础。In response to the above defects or improvement needs of the prior art, the present invention provides a structure and method for generating flexoelectricity, the purpose of which is to lay a foundation for regulating the performance of electronic devices in dynamic and medium and high frequency directions by the flexoelectric effect.
为实现上述目的,按照本发明的第一方面,提供了一种产生挠曲电的结构,包括:集成设置于压电衬底上表面的叉指换能器Ⅰ、叉指换能器Ⅱ及位于所述叉指换能器Ⅰ、叉指换能器Ⅱ之间的至少一个薄膜器件;所述叉指换能器Ⅰ、叉指换能器Ⅱ的材料、尺寸和频率均相同;To achieve the above object, according to a first aspect of the present invention, there is provided a structure for generating flexoelectricity, comprising: an IDT I and an IDT II integrated on the upper surface of a piezoelectric substrate and at least one thin film device located between the IDT I and the IDT II; the IDT I and the IDT II are of the same material, size and frequency;
所述叉指换能器Ⅰ、叉指换能器Ⅱ被同时施加频率、幅值、相位均相同的正弦电压信号时产生XY平面内振动的声表面波驻波,使所述至少一个薄膜器件受到周期性的拉伸,从而产生挠曲电效应。When sinusoidal voltage signals with the same frequency, amplitude and phase are applied to the IDT I and IDT II simultaneously, standing surface acoustic waves vibrating in the XY plane are generated, causing the at least one thin film device to be periodically stretched, thereby generating a flexoelectric effect.
优选地,所述至少一个薄膜器件位于所述声表面波驻波波腹处,与所述叉指换能器Ⅰ、叉指换能器Ⅱ之间的位置满足以下关系式:Preferably, the at least one thin film device is located at the antinode of the surface acoustic wave standing wave, and the position between the IDT I and IDT II satisfies the following relationship:
Δx=n(a+b)Δx=n(a+b)
其中,a表示叉指换能器指条的宽度;b表示叉指换能器指间的间距;Δx表示叉指换能器I最后一根叉指电级中心点和第n个薄膜器件中心点的间距,n为整数。Wherein, a represents the width of the fingers of the IDT; b represents the spacing between the fingers of the IDT; Δx represents the spacing between the center point of the last finger electrode of the IDT I and the center point of the nth thin film device, and n is an integer.
优选地,所述薄膜器件的介电层的厚度为10nm~20nm。Preferably, the thickness of the dielectric layer of the thin film device is 10 nm to 20 nm.
优选地,所述薄膜器件的尺寸小于所述声表面波的波长。Preferably, the size of the thin film device is smaller than the wavelength of the surface acoustic wave.
优选地,所述叉指换能器Ⅰ、叉指换能器Ⅱ的电极材料为Cr和Au。Preferably, the electrode materials of the IDT I and IDT II are Cr and Au.
优选地,所述压电衬底的上表面为抛光面,所述下表面为粗糙面。Preferably, the upper surface of the piezoelectric substrate is a polished surface, and the lower surface is a rough surface.
优选地,所述压电衬底的材料为64°Y方向切割、X方向传播的LiNbO3单晶片。Preferably, the material of the piezoelectric substrate is a LiNbO 3 single crystal crystal cut at 64° in the Y direction and propagated in the X direction.
按照本发明的第二方面,提供了一种产生挠曲电的方法,应用于如第一方面所述的结构,包括:According to a second aspect of the present invention, there is provided a method for generating flexoelectricity, which is applied to the structure as described in the first aspect, comprising:
对所述叉指换能器Ⅰ、叉指换能器Ⅱ同时施加频率、幅值、相位均相同的正弦电压信号,以产生XY平面内振动的声表面波驻波,使至少一个薄膜器件受到周期性的拉伸,从而产生挠曲电效应。Sinusoidal voltage signals with the same frequency, amplitude and phase are applied to the IDT I and IDT II simultaneously to generate standing surface acoustic wave waves vibrating in the XY plane, so that at least one thin film device is periodically stretched, thereby generating a flexoelectric effect.
通过探针台扎针的方法将处于驻波波腹处薄膜器件(3)和测量仪器相连接,通过测量仪器测量在挠曲电作用下产生的电压信号。The thin film device (3) at the antinode of the standing wave is connected to a measuring instrument by a probe station needle piercing method, and the voltage signal generated under the flexoelectric effect is measured by the measuring instrument.
优选地,所述测量仪器为示波器。Preferably, the measuring instrument is an oscilloscope.
总体而言,通过本发明所构思的以上技术方案与现有技术相比,能够取得下列有益效果:In general, the above technical solutions conceived by the present invention can achieve the following beneficial effects compared with the prior art:
1、本发明提供的产生挠曲电的结构和方法,将叉指换能器和薄膜器件进行片上集成,同时给两侧的叉指换能器施加频率、相位、幅值相同的正弦波,由于薄膜器件的上电极未施加任何载荷,在声表面波的周期性拉伸的作用下薄膜器件的介质层会产生应变梯度,周期性变化的应变梯度会产生极化电荷,即产生了挠曲电效应,为挠曲电效应在动态和中高频方向调控电子器件的性能提供了新思路。此外,本发明提供的方法能够通过这种结构产生挠曲电效应对薄膜器件的表面无损伤,对挠曲电能量采集、挠曲电传感等方面的应用发展具有重要的意义。1. The structure and method for generating flexoelectricity provided by the present invention integrates the interdigital transducer and the thin film device on a chip, and simultaneously applies a sine wave with the same frequency, phase, and amplitude to the interdigital transducers on both sides. Since no load is applied to the upper electrode of the thin film device, the dielectric layer of the thin film device will produce a strain gradient under the periodic stretching of the surface acoustic wave. The periodically changing strain gradient will produce polarization charge, that is, the flexoelectric effect is generated, which provides a new idea for the flexoelectric effect to control the performance of electronic devices in the dynamic and medium and high frequency directions. In addition, the method provided by the present invention can generate the flexoelectric effect through this structure without damaging the surface of the thin film device, which is of great significance to the application development of flexoelectric energy collection, flexoelectric sensing, etc.
2、本发明提供的产生挠曲电的结构和方法,将至少一个薄膜器件设置于叉指换能器Ⅰ、叉指换能器叉指换能器Ⅱ在被施加频率、相位、幅值相同的正弦波时产生的声表面波驻波的波腹处,位于波腹处的薄膜器件在声表波的作用下受到的拉伸强烈,产生的挠曲电效果更强。2. The structure and method for generating flexoelectricity provided by the present invention arranges at least one thin film device at the antinode of the standing surface acoustic wave generated by the interdigital transducer I and the interdigital transducer II when a sinusoidal wave with the same frequency, phase and amplitude is applied. The thin film device located at the antinode is strongly stretched under the action of the surface acoustic wave, and the flexoelectric effect generated is stronger.
3、本发明提供的产生挠曲电的结构和方法,薄膜器件单元的尺寸小于声表面波的波长,薄膜器件的上电极未施加任何载荷,在声表面波的周期性拉伸的作用下薄膜器件的介质层会产生应变梯度,应变梯度会引起电极化,当薄膜器件的单元尺寸小于声表面波的波长时,产生的电极化不会相互抵消。3. The structure and method for generating flexoelectricity provided by the present invention have a unit size of the thin film device that is smaller than the wavelength of the surface acoustic wave, and no load is applied to the upper electrode of the thin film device. Under the action of the periodic stretching of the surface acoustic wave, the dielectric layer of the thin film device will produce a strain gradient, and the strain gradient will cause electric polarization. When the unit size of the thin film device is smaller than the wavelength of the surface acoustic wave, the generated electric polarization will not cancel each other out.
4、本发明提供的产生挠曲电的结构和方法,可设计不同频率的叉指换能器,由于波长决定了应变梯度的大小,因此波长较小的高频声表面波驻波产生的挠曲电效应更强烈,因此,可通过改变叉指换能器的频率来改变声表面波驻波的波长,从而改变挠曲电效应的强度,因此可以通过挠曲电效应在动态和中高频方向调控电子器件的性能。4. The structure and method for generating flexoelectricity provided by the present invention can be used to design interdigital transducers of different frequencies. Since the wavelength determines the size of the strain gradient, the flexoelectric effect generated by a high-frequency surface acoustic wave standing wave with a smaller wavelength is stronger. Therefore, the wavelength of the surface acoustic wave standing wave can be changed by changing the frequency of the interdigital transducer, thereby changing the intensity of the flexoelectric effect. Therefore, the performance of electronic devices can be regulated in the dynamic and medium and high frequency directions through the flexoelectric effect.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
图1为本发明实施例提供的产生挠曲电的结构示意图。FIG1 is a schematic diagram of a structure for generating flexoelectricity provided in an embodiment of the present invention.
具体实施方式DETAILED DESCRIPTION
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。此外,下面所描述的本发明各个实施方式中所涉及到的技术特征只要彼此之间未构成冲突就可以相互组合。In order to make the purpose, technical solutions and advantages of the present invention more clearly understood, the present invention is further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention and are not intended to limit the present invention. In addition, the technical features involved in the various embodiments of the present invention described below can be combined with each other as long as they do not conflict with each other.
本发明实施例提供一种产生挠曲电的结构,如图1所示,包括:集成设置于压电衬底1上表面的叉指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4及位于所述指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4之间的至少一个薄膜器件3;所述叉指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4的材料和尺寸相同,频率相同;An embodiment of the present invention provides a structure for generating flexoelectricity, as shown in FIG1 , comprising: an IDT I2, an IDT II4, and at least one thin film device 3 located between the IDT I2 and the IDT II4, which are integrated on the upper surface of a piezoelectric substrate 1; the IDT I2 and the IDT II4 have the same material and size and the same frequency;
所述叉指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4被同时施加频率、幅值、相位均相同的正弦电压信号时产生XY平面内振动的声表面波驻波5,使所述至少一个薄膜器件3受到周期性的拉伸,从而产生挠曲电效应。When sinusoidal voltage signals with the same frequency, amplitude and phase are applied simultaneously to the IDT I2 and IDT II4, a surface acoustic wave standing wave 5 vibrating in the XY plane is generated, so that the at least one thin film device 3 is periodically stretched, thereby generating a flexoelectric effect.
可以理解的是,本实施例中,所采用薄膜器件3,从下到上依次由下电极(Pt)、功能层(介电层,如SiO2;HfO2)和上电极(W)三部分组成。下电极的厚度为100nm;功能层的厚度为10nm;上电极的宽度为100μm。It can be understood that in this embodiment, the thin film device 3 is composed of three parts from bottom to top: a lower electrode (Pt), a functional layer (dielectric layer, such as SiO 2 ; HfO 2 ) and an upper electrode (W). The thickness of the lower electrode is 100nm; the thickness of the functional layer is 10nm; and the width of the upper electrode is 100μm.
所述薄膜器件3位于叉指换能器Ⅰ2、叉指换能器Ⅱ4之间,叉指换能器Ⅰ2、叉指换能器Ⅱ4产生的声表面波的传播方向上。The thin film device 3 is located between the IDT I2 and the IDT II4, in the propagation direction of the surface acoustic waves generated by the IDT I2 and the IDT II4.
优选地,所述薄膜器件3与压电衬底1之间存在导电黏附层,所述导电黏附层与压电衬底1形成共价键,同时该导电黏附层与薄膜器件3下电极形成金属键。Preferably, there is a conductive adhesive layer between the thin film device 3 and the piezoelectric substrate 1 , the conductive adhesive layer forms a covalent bond with the piezoelectric substrate 1 , and the conductive adhesive layer forms a metal bond with the lower electrode of the thin film device 3 .
优选地,所述薄膜器件3的尺寸小于所述声表面波的波长。Preferably, the size of the thin film device 3 is smaller than the wavelength of the surface acoustic wave.
叉指换能器的指条宽度和指条间距都是100μm。两叉指换能器产生的声表面波波长λ=2×(指条宽度+指条间距)=400μm,声表面波频率f=v/T,v是声表面波速度约为4000m/s,从而声表面波频率为10MHz。两侧的叉指换能器产生声表面波,相向传播的声表面波在两侧叉指换能器之间的区域进行叠加,形成声表面驻波。由于薄膜器件3的上电极未施加任何载荷,且薄膜器件3尺寸小于声表面波的波长,在声表面波的周期性拉伸的作用下薄膜器件3的介质层会产生应变梯度,周期性变化的应变梯度会产生极化电荷,即产生了挠曲电效应。The finger width and finger spacing of the interdigital transducer are both 100μm. The wavelength of the surface acoustic wave generated by the two interdigital transducers is λ=2×(finger width+finger spacing)=400μm, and the surface acoustic wave frequency is f=v/T, where v is the surface acoustic wave velocity of about 4000m/s, so the surface acoustic wave frequency is 10MHz. The interdigital transducers on both sides generate surface acoustic waves, and the surface acoustic waves propagating in opposite directions are superimposed in the area between the interdigital transducers on both sides to form a surface acoustic standing wave. Since no load is applied to the upper electrode of the thin film device 3, and the size of the thin film device 3 is smaller than the wavelength of the surface acoustic wave, the dielectric layer of the thin film device 3 will produce a strain gradient under the periodic stretching of the surface acoustic wave, and the periodically changing strain gradient will produce polarization charge, that is, the flexoelectric effect is generated.
将不同频率的叉指换能器和至少一个薄膜器件3在同一个压电衬底1上进行集成(即两个叉指换能器和至少一个薄膜器件3均位于压电衬底1的上表面),对同一压电衬底1上的一对叉指换能器同时施加频率、幅值、相位均相同的正弦波信号,由于逆压电效应,位于所述至少一个薄膜器件3两侧的叉指换能器均产生声表面波,相向传播的声表面波在两侧叉指换能器之间的区域进行叠加,从而在两侧叉指换能器之间的区域形成声表面驻波,在所述声表面驻波的作用下,所述至少一个薄膜器件3会受到周期性的拉伸。由于薄膜器件3的上电极未施加任何载荷,在声表面波的周期性拉伸的作用下,薄膜器件3的介质层发生非均匀的应变,即薄膜器件3的介质层会产生应变梯度,周期性变化的应变梯度会产生极化电荷,即产生了挠曲电效应。The interdigital transducers of different frequencies and at least one thin film device 3 are integrated on the same piezoelectric substrate 1 (i.e., the two interdigital transducers and at least one thin film device 3 are both located on the upper surface of the piezoelectric substrate 1), and a pair of interdigital transducers on the same piezoelectric substrate 1 are simultaneously applied with a sine wave signal with the same frequency, amplitude, and phase. Due to the inverse piezoelectric effect, the interdigital transducers located on both sides of the at least one thin film device 3 both generate surface acoustic waves, and the surface acoustic waves propagating in opposite directions are superimposed in the area between the interdigital transducers on both sides, thereby forming a surface acoustic standing wave in the area between the interdigital transducers on both sides. Under the action of the surface acoustic standing wave, the at least one thin film device 3 will be periodically stretched. Since no load is applied to the upper electrode of the thin film device 3, under the action of the periodic stretching of the surface acoustic wave, the dielectric layer of the thin film device 3 will be non-uniformly strained, that is, the dielectric layer of the thin film device 3 will produce a strain gradient, and the periodically changing strain gradient will produce polarization charge, that is, the flexoelectric effect is produced.
且薄膜器件3的尺寸小于声表面波波长。压电衬底1上的叉指换能器产生声表面波,而薄膜器件3的上电极未施加任何载荷,在声表面波的周期性拉伸的作用下薄膜器件3的介质层会产生非均匀的应变,周期性变化的应变梯度会产生极化电荷,即产生了挠曲电效应。本发明将声表面波和薄膜器件3通过片上集成产生了挠曲电效应,这为挠曲电效应在动态和中高频方向调控电子器件的性能提供了新思路。And the size of the thin film device 3 is smaller than the wavelength of the surface acoustic wave. The interdigital transducer on the piezoelectric substrate 1 generates surface acoustic waves, and the upper electrode of the thin film device 3 does not apply any load. Under the periodic stretching of the surface acoustic wave, the dielectric layer of the thin film device 3 will produce non-uniform strain, and the periodically changing strain gradient will produce polarization charge, that is, the flexoelectric effect. The present invention integrates the surface acoustic wave and the thin film device 3 on a chip to produce the flexoelectric effect, which provides a new idea for the flexoelectric effect to control the performance of electronic devices in the dynamic and medium and high frequency directions.
优选地,所述正弦电压信号的幅值不超过所述压电衬底1最大承受电压。本实施例中,将压电衬底1非抛光面粘贴在电路板上,并将电路板上的印刷电路通道与叉指换能器进行引线,对两对叉指换能器同时施加幅度为1V,频率为10MHz的正弦电压信号。Preferably, the amplitude of the sinusoidal voltage signal does not exceed the maximum withstand voltage of the piezoelectric substrate 1. In this embodiment, the non-polished surface of the piezoelectric substrate 1 is pasted on a circuit board, and the printed circuit channels on the circuit board are connected to the IDTs, and sinusoidal voltage signals with an amplitude of 1V and a frequency of 10MHz are applied to the two pairs of IDTs simultaneously.
优选地,至少一个薄膜器件3位于所述声表面波驻波5波腹处(即将所述至少一个薄膜器件3设置于压电衬底1上的叉指换能器产生声表面波传播的方向上),与所述叉指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4之间的位置满足以下关系式:Preferably, at least one thin film device 3 is located at the antinode of the surface acoustic wave standing wave 5 (that is, the at least one thin film device 3 is arranged in the direction of propagation of the surface acoustic wave generated by the interdigital transducer on the piezoelectric substrate 1), and the position between the interdigital transducer I2 and the interdigital transducer II4 satisfies the following relationship:
Δx=n(a+b)Δx=n(a+b)
其中,a表示叉指换能器指条的宽度;b表示叉指换能器指间的间距;Δx表示叉指换能器I最后一根叉指电级中心点和第n个薄膜器件3中心点的间距,n为整数。Wherein, a represents the width of the fingers of the IDT; b represents the spacing between the fingers of the IDT; Δx represents the spacing between the center point of the last finger electrode of the IDT I and the center point of the nth thin film device 3, and n is an integer.
具体地,将薄膜器件3与叉指换能器进行片上集成,使得薄膜器件3位于声表面波驻波5的波腹处,位于波腹处的薄膜器件3在声表波的作用下受到的拉伸强烈,产生的挠曲电效果更强。Specifically, the thin film device 3 is integrated on a chip with the interdigital transducer so that the thin film device 3 is located at the antinode of the surface acoustic wave standing wave 5. The thin film device 3 located at the antinode is strongly stretched under the action of the surface acoustic wave, and the flexoelectric effect generated is stronger.
优选地,所述薄膜器件3的介电层的厚度为10nm~20nm。Preferably, the thickness of the dielectric layer of the thin film device 3 is 10 nm to 20 nm.
具体地,薄膜器件3的厚度在纳米量级。由于应变梯度和材料的特征尺寸成反比,当器件微缩至纳米尺度时,挠曲电效应会更加的显著。Specifically, the thickness of the thin film device 3 is in the nanometer range. Since the strain gradient is inversely proportional to the characteristic size of the material, when the device is miniaturized to the nanometer scale, the flexoelectric effect will be more significant.
优选地,所述叉指换能器Ⅰ2、叉指换能器Ⅱ4的电极材料为Cr/Au。Preferably, the electrode material of the IDT I2 and IDT II4 is Cr/Au.
具体地,叉指换能器的电极材料为Cr/Au,厚度一般为50nm-100nm。Specifically, the electrode material of the IDT is Cr/Au, and the thickness is generally 50nm-100nm.
其中金属Cr的作用为Au和压电衬底1的黏附层,即金属Cr可以增加金属薄膜Au与衬底的黏附性。The metal Cr serves as an adhesion layer between Au and the piezoelectric substrate 1 , that is, the metal Cr can increase the adhesion between the metal film Au and the substrate.
优选地,所述叉指换能器Ⅰ2、叉指换能器Ⅱ4与所述压电衬底1的接触面(即压电衬底1的上表面)为抛光面,所述压电衬底1的下表面为粗糙面。Preferably, the contact surfaces of the IDT I2 and IDT II4 with the piezoelectric substrate 1 (ie, the upper surface of the piezoelectric substrate 1) are polished surfaces, and the lower surface of the piezoelectric substrate 1 is a rough surface.
具体地,压电衬底1的上表面为抛光面,有利于声表面波的传播,减小损耗。压电衬底1的下表面为粗糙面,有利于减小声表面波的反射。Specifically, the upper surface of the piezoelectric substrate 1 is a polished surface, which is beneficial to the propagation of surface acoustic waves and reduces losses. The lower surface of the piezoelectric substrate 1 is a rough surface, which is beneficial to reduce the reflection of surface acoustic waves.
优选地,所述压电衬底1的材料为64°Y方向切割、X方向传播的LiNbO3单晶片,即64°YX-LiNbO3。Preferably, the material of the piezoelectric substrate 1 is a LiNbO 3 single crystal crystal cut in the Y direction at 64° and propagated in the X direction, that is, 64°YX-LiNbO 3 .
具体地,LiNbO3单晶片的机电耦合系数较大,插入损耗小。在LiNbO3单晶片的抛光面上制备叉指换能器可以降低声表面波的传播损耗。Specifically, the electromechanical coupling coefficient of the LiNbO3 single crystal is large and the insertion loss is small. Fabricating an interdigital transducer on the polished surface of the LiNbO3 single crystal can reduce the propagation loss of the surface acoustic wave.
本实施例中,压电衬底1采用64°YX-LiNbO3,尺寸为30×15×0.5mm,单面抛光。In this embodiment, the piezoelectric substrate 1 is made of 64° YX-LiNbO 3 , has a size of 30×15×0.5 mm, and is polished on one side.
本发明实施例提供一种产生挠曲电的方法,应用于如上述任一实施例所述的结构,包括:An embodiment of the present invention provides a method for generating flexoelectricity, which is applied to the structure described in any of the above embodiments, including:
对所述叉指换能器Ⅰ2、叉指换能器叉指换能器Ⅱ4同时施加频率、幅值、相位均相同的正弦电压信号,以产生XY平面内振动的声表面波驻波5,使所述至少一个薄膜器件3受到周期性的拉伸,从而产生挠曲电效应。Sinusoidal voltage signals with the same frequency, amplitude and phase are applied to the IDT I2 and IDT II4 simultaneously to generate a surface acoustic wave standing wave 5 vibrating in the XY plane, so that the at least one thin film device 3 is periodically stretched, thereby generating a flexoelectric effect.
具体地,对两侧的叉指换能器用时施加频率、幅值均相同的正弦电压信号,由于逆压电效应,两侧的叉指换能器均会产生声表面波,相向传播的声表面波在两侧叉指换能器之间的区域进行叠加,从而形成声表面驻波。Specifically, a sinusoidal voltage signal with the same frequency and amplitude is applied to the IDTs on both sides. Due to the inverse piezoelectric effect, the IDTs on both sides will generate surface acoustic waves. The surface acoustic waves propagating in opposite directions are superimposed in the area between the IDTs on both sides, thereby forming a surface acoustic standing wave.
优选地,所述方法还包括:通过测量仪器测量所述薄膜器件3在挠曲电效应下产生的电压信号;优选地,所述测量仪器为示波器。Preferably, the method further comprises: measuring a voltage signal generated by the thin film device 3 under the flexoelectric effect by means of a measuring instrument; preferably, the measuring instrument is an oscilloscope.
具体地,例如,当所述至少一个薄膜器件3位于驻波波腹处时,通过探针台扎针的方法将处于驻波波腹处薄膜器件3和示波器相连接,由于薄膜器件3的上电极未施加任何载荷,在声表面波的周期性拉伸的作用下薄膜器件3的介质层会产生应变梯度,应变梯度会引起电极化,通过示波器可以测量到薄膜器件3产生的正弦电压信号。Specifically, for example, when the at least one thin film device 3 is located at the antinode of the standing wave, the thin film device 3 at the antinode of the standing wave is connected to an oscilloscope by a probe station needle method. Since no load is applied to the upper electrode of the thin film device 3, the dielectric layer of the thin film device 3 will produce a strain gradient under the action of the periodic stretching of the surface acoustic wave. The strain gradient will cause electric polarization, and the sinusoidal voltage signal generated by the thin film device 3 can be measured by the oscilloscope.
本领域的技术人员容易理解,以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明的保护范围之内。It will be easily understood by those skilled in the art that the above description is only a preferred embodiment of the present invention and is not intended to limit the present invention. Any modifications, equivalent substitutions and improvements made within the spirit and principles of the present invention should be included in the protection scope of the present invention.
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