摘要:
A surface acoustic wave device includes a three-dimensional substrate having an annular curved surface enabling to propagate a surface acoustic wave, and an electro-acoustic transducing element, which excites and propagates the surface wave along the surface, and receives the propagated surface wave. The substrate is made of a Li2B4O7, Bi12SiO20, LiNbO3, LiTaO3, or quartz crystal, and the element propagates the surface wave along a line of intersection between a crystal face of the crystal and the surface, and the line of intersection is defined as an outermost circumferential line of the surface. An environmental difference detecting apparatus uses the device having a plurality of propagating surface zones and compares surface acoustic wave reception signals of electro-acoustic transducing elements in the propagating surface zones of the device with each other, and detects an environmental difference in space portions with which the propagating surface zones come into contact.
摘要:
The invention provides an in-plane rotational ST-cut SAW resonator that is formed of an in-plane rotational ST-cut crystal plate having Eulerian angles of (0°, 113° to 135°, and ±(40° to 49°)). The in-plane rotational ST-cut SAW resonator can include an interdigital transducer (IDT) electrode for exciting a Rayleigh wave on the main surface. The ratio Lt/Pt of the electrode width Lt and the interelectrode pitch Pt of the IDT electrode is 0.5 or more and 0.65 or less. Accordingly, a reduction in the fluctuation in resonance frequency relative to the variations in an IDT electrode of a surface acoustic wave device by using the in-plane rotated ST-cut crystal plate around the Z′-axis can be achieved.
摘要:
A compact and wide band surface acoustic wave device for intermediate-frequency is disclosed. A piezoelectric substrate for use in a surface acoustic wave device having high electromechanical coupling factor and low SAW velocity is also disclosed. The surface acoustic wave device is constituted of a piezoelectric substrate 1 and inter-digital electrodes 2, 2 formed on the piezoelectric substrate 1. The piezoelectric substrate 1 has a crystal structure of Ca3Ga2Ge4O14 and is represented by the chemical formula, Ca3TaGa3Si2O14. A cut angle of the piezoelectric substrate 1 cut out of the single crystal and a direction of propagation of surface acoustic waves on the piezoelectric substrate represented in terms of Euler's angles (null, null, null) are found in an area represented by null2.5nullnullnullnull2.5null, 30nullnullnullnull90null, and null65nullnullnullnull65null.
摘要翻译:公开了一种用于中频的紧凑且宽带声表面波装置。 还公开了一种用于具有高机电耦合系数和低SAW速度的表面声波装置中的压电基片。 表面声波装置由压电基片1和形成在压电基片1上的数字间电极2,2构成。压电基片1具有Ca 3 Ga 2 Ge 4 O 14的晶体结构,由化学式Ca 3 Ta Ga 3 Si 2 O 14表示。 从欧姆角(phi,θ,psi)表示的压电基板上切出的压电基板1的切割角和压电基板上的表面声波的传播方向在-2.5° <= phi <= 2.5°,30°<=θ<= 90°,-65°<= psi <= 65°。
摘要:
The invention provides an in-plane rotational ST-cut SAW resonator that is formed of an in-plane rotational ST-cut crystal plate having Eulerian angles of (0null, 113null to 135null, and null(40null to 49null)). The in-plane rotational ST-cut SAW resonator can include an interdigital transducer (IDT) electrode for exciting a Rayleigh wave on the main surface. The ratio Lt/Pt of the electrode width Lt and the interelectrode pitch Pt of the IDT electrode is 0.5 or more and 0.65 or less. Accordingly, a reduction in the fluctuation in resonance frequency relative to the variations in an IDT electrode of a surface acoustic wave device by using the in-plane rotated ST-cut crystal plate around the Znull-axis can be achieved.
摘要:
An object of the invention is to achieve a wider passband and reduction in size of a surface acoustic wave device. The surface acoustic wave device comprises a piezoelectric substrate (1) and a pair of interdigitated electrodes (2) provided on one main surface of the piezoelectric substrate (1). As the material of the piezoelectric substrate (1), a single crystal belonging to the point group 32, having a crystal structure of Ca3Ga2Ge4O14 type, containing Ca, Nb, Ga, Si and O as main components, and being represented by the chemical formula Ca3NbGa3Si2O14 is used. The cut angle of the substrate (1) and the propagation direction can be selected as appropriate to thereby realize the substrate (1) which has a large electromechanical coupling coefficient that is effective to achieve a wider passband and a low SAW velocity that is effective to reduce the size of a surface acoustic wave device.
摘要翻译:本发明的一个目的是实现更大的通带和减小声表面波装置的尺寸。 表面声波装置包括压电基片(1)和设置在压电基片(1)的一个主表面上的一对叉指电极(2)。 作为压电基板(1)的材料,属于具有Ca 3 Ga 2 Ge 4 O 14型晶体结构的点组32的单晶,含有Ca,Nb,Ga,Si和O作为主要成分,并且由化学式 使用Ca3NbGa3Si2O14。 可以适当选择基板(1)的切割角度和传播方向,从而实现具有大的机电耦合系数的基板(1),其有效地实现更宽的通带和低的SAW速度, 减小声表面波器件的尺寸。
摘要:
A sapphire single crystal wafer 11 having a diameter not less than two inches and having an off-angled surface which is obtained by rotating an R (1-102) surface about an axis in a negative direction by a given off-angle not less than 2° is introduced in a CVD apparatus. While the sapphire substrate is kept at a temperature of about 950° C., a buffer layer made of gallium nitride or aluminum-gallium nitride is first deposited with an average thickness of 0.1-0.2 &mgr;m, and then an aluminum nitride single crystal layer is deposited with an average thickness not less than 2 &mgr;m. The thus obtained aluminum nitride single crystal layer does not have a significant amount of cracks, has an excellent piezoelectric property, and has a high propagating velocity.
摘要:
A surface acoustic wave element includes a LiNbxTa1−xO3 (‘x’ is 0 or more and 1 or less) film on a (012) sapphire substrate, in which a Love wave is propagated as a surface acoustic wave in a specific direction of the LiNbxTa1−xO3 film. Preferably, a crystal axis of the sapphire substrate and a crystal axis of a (012) LiNbxTa1−xO3 film (‘x’ is 0 or more and 1 or less) are parallel to each other; a surface acoustic wave propagation direction is within a range of ±20 degrees around an axis vertical to a C-axis projection line direction of a crystal axis of the sapphire substrate or the (012) LiNbxTa1−xO3 film. Alternatively, a C-axis projection line direction of a crystal axis of the sapphire substrate and a C-axis direction of a crystal axis of a (100) LiNbxTa1−xO3 film (‘x’ is 0 or more and 1 or less) are parallel to each other, and the surface acoustic wave propagation direction is within a range of ±35 degrees around an axis vertical to a C-axis projection line direction of a crystal axis of the sapphire substrate. A piezoelectric substrate preferably has an intermediate layer including of a metal or a metal oxide between the sapphire substrate and the (100) LiNbxTa1−xO3 (‘x’ is 0 or more and 1 or less).
摘要翻译:表面声波元件包括在(012)蓝宝石衬底上的LiNb x Ta 1-x O 3(“x”为0以上且1以下)的膜,其中,爱波作为表面声波在特定方向上传播 LiNb x Ta 1-x O 3膜优选蓝宝石衬底的晶轴和(012)LiNb x Ta 1-x O 3膜的晶轴(“x”为0以上且1以下)彼此平行; 表面声波传播方向在与蓝宝石衬底或(012)LiNb x Ta 1-x O 3膜的晶轴的C轴投影线方向垂直的轴的±20度的范围内。 或者,蓝宝石基板的晶轴的C轴投影线方向和(100)LiNb x Ta 1-x O 3膜(“x”为0以上且1以下)的晶轴的C轴方向为 彼此平行,弹性表面波传播方向在与蓝宝石基板的晶轴的C轴投影线方向垂直的轴的±35度的范围内,压电基板优选具有中间层, 的蓝宝石衬底和(100)LiNb x Ta 1-x O 3之间的金属或金属氧化物(“x”为0以上且1以下)。
摘要:
A sapphire single crystal wafer 11 having a diameter not less than two inches and having an off-angled surface which is obtained by rotating an R (1-102) surface about a �11-20! axis by a given off-angle is introduced in a CVD apparatus, and a double-layer structure of first and second aluminum single crystal layers 12 and 13 is deposited on the off-angled surface of the sapphire single crystal wafer by MOCVD. The thus deposited aluminum single crystal layer 13 has (1-210) surface. The first aluminum nitride single crystal layer 12 serves as a buffer layer and has a thickness of 5-50 nm, and the second aluminum nitride single crystal layer 13 has a thickness not less than 1 .mu.m. The off-angle is preferably set to a value not less than .+-.1.degree., much preferably a value .+-.2.degree., more preferably a value not less than -3.degree., and particularly preferable to a value within a range from -2.degree.-+10.degree.. The thus obtained aluminum nitride single crystal layer 12, 13 has no clack formed therein, has an excellent piezo-electric property, and has a high propagating velocity for surface acoustic wave.
摘要:
A surface acoustic wave device comprises lithium tetraborate single crystal substrate to make use of surface acoustic waves with higher propagation velocities and smaller propagation losses, whereby frequencies to be signal-processed can be as high as above 1 GHz. The surface acoustic wave device comprises a metal film formed on a surface of a lithium tetraborate single crystal substrate, the metal film being for exciting, receiving, reflecting and/or propagating surface acoustic waves, the metal film being so formed that a cut angle of the substrate, and a propagation direction of the surface acoustic waves are in an Eulerian angle representation of (39.degree.-51.degree., 66.degree.-114.degree., -20.degree.-20.degree.) and directions equivalent thereto. In this propagation direction few Rayleigh waves exit, and only surface acoustic waves of high propagation velocity are generated. Propagation losses can be eliminated.
摘要:
A surface acoustic wave device has been developed, such as a surface acoustic wave filter in which a plurality of electroacoustic interdigital electrodes are formed, as thin films made principally of aluminum, on the surface of a Li.sub.2 B.sub.4 O.sub.7 single crystal substrate and a surface acoustic wave resonator, in which a plurality of electroacoustic interdigital electrodes and grating reflectors for reflecting the surface acoustic wave are formed, as thin films made principally of aluminum, on the surface of a Li.sub.2 B.sub.4 O.sub.7 single crystal substrate. Here, a cut angle, at which the substrate is cut from the Li.sub.2 B.sub.4 O.sub.7 single crystal, and the propagation direction of the surface acoustic wave are so set that, when the Eulerian angle representation is (90.degree..+-..lambda., 90.degree..+-..mu., 90.degree..+-..theta.), .lambda.=38.degree. to 52.degree., .mu.=0.degree. to 5.degree. and .theta.=0.degree. to 10.degree., whereby the TCD of the surface acoustic wave device is below .+-.5 ppm/.degree.C. and coupling coefficient K.sup.2 is about 1.0%, and the propagation speed suffers almost no angular dependence.