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    • 1. 发明专利
    • SURFACE ACOUSTIC WAVE FILTER AND COMMUNICATION EQUIPMENT USING SAME
    • JPH03163904A
    • 1991-07-15
    • JP30210389
    • 1989-11-22
    • HITACHI LTD
    • HIKINO OSAMUSHIBA TAKASHITAKEMA TAKEMITSUYAMADA JUN
    • H03H9/64H03H9/145
    • PURPOSE:To suppress diffraction effect and to improve the frequency characteristic of an element by obtaining all desired surface acoustic wave exciting strength only by paired opposite electrode digits equipped with electrode digits crossing width longer than the central wavelength of a surface acoustic wave to be propagated on a substrate. CONSTITUTION:At an arbitrary position x' in a surface acoustic wave propagating direction (x) of interdigital electrodes 4 and 5 (bus bars 10 and 11), respective electrode digit width w1 and w2 is made longer than the central wavelength of the surface acoustic wave to be propagated on the substrate. Then, the lower interdigital electrode 5 applies the exciting strength of the same phase as the desired surface acoustic wave and the upper interdigital electrode 4 applies the exciting strength of the reverse phase. The difference between the length of the crossing width w2 of the lower interdigital electrode 5 and the length of the crossing width w1 of the upper interdigital electrode 4 is equal to the crossing width in the conventional case being not divided the electrode. Since the phases of the surface acoustic waves to be excited by the vertically divided interdigital electrodes are made reverse, and the desired surface acoustic wave exciting strength can be realized by an aperture length longer than the central wavelength of the surface acoustic wave to be propagated on the substrate, the diffraction effect can be suppressed.
    • 2. 发明专利
    • SURFACE ACOUSTIC WAVE DUPLEX MODE FILTER AND COMMUNICATION EQUIPMENT USING SAME
    • JPH03163903A
    • 1991-07-15
    • JP30210289
    • 1989-11-22
    • HITACHI LTD
    • TAKEMA TAKEMITSUSHIBA TAKASHIYAMADA JUN
    • H03H9/64H03H9/145
    • PURPOSE:To enlarge frequency band width by forming one part of interdigital electrodes arranged close and parallel to a direction rectangular to a surface acoustic wave propagating direction to be meander electrode structure, and bringing the end part of more than one interdigital electrode into contact with a straight line drawn parallel to the interdigital electrode between these adjacent and parallel interdigital electrodes. CONSTITUTION:A common electrode 3 and an electrode finger connected to the electrode 4 are formed to be the structure of a meander electrode 6. Therefore, the central common electrode is eliminated and further, the respective interdigital electrodes close and parallel to the direction rectangular to the surface acoustic wave propagating direction get contact with a straight line 5-5' drawn parallel to the both electrodes between the both electrodes. Thus, the distance of a surface acoustic wave propagation path to be excited by the respective interdigital electrodes 3, namely, a gap G becomes 0. Accordingly, the frequency difference of two modes is enlarged, and the frequency band width of a surface acoustic wave duplex mode filter can be enlarged.
    • 3. 发明专利
    • SURFACE ACOUSTIC WAVE ELEMENT
    • JPS6327112A
    • 1988-02-04
    • JP16970786
    • 1986-07-21
    • HITACHI LTD
    • TAKEMA TAKEMITSUHOSAKA NORIOKUMISAWA YUKOYUHARA AKITSUNASAITO MASAKATSU
    • H03H9/145H03H9/25
    • PURPOSE:To decrease the phase change within a desired band by arranging an input electrode and an output electrode respectively on different planes existing nearby and in parallel with each other to approach the center distance between the input/output electrodes independently of the shape of the electrodes. CONSTITUTION:A slant electrode 1 formed by the photo lithography technology is arranged on a molten quartz substrate 4, the 1st layer ZnO piezoelectric thin film 2, a shield film 3 and the 2nd layer ZnO piezoelectric thin film 2 are formed on the electrode 1 by the sputtering method and a slant electrode 1 formed by the photo lithography technology is arranged on the 2nd layer ZnO piezoelectric thin film 2 and a sound absorbing member 5 is formed to the edge of the plane on which the slant electrode 1 is arranged. Through the layerd structure above, the output electrode is arranged beneath the input electrode, the center distance between the input and output electrodes is /2 (is the wavelength of a surface acoustic wave) or below so as to reduce the phase change in the band.
    • 4. 发明专利
    • ACOUSTO-OPTICAL DEVICE
    • JPS62242922A
    • 1987-10-23
    • JP8594186
    • 1986-04-16
    • HITACHI LTD
    • TAKEMA TAKEMITSUFUJITA YUJIHOSAKA NORIOSHIBA TAKASHIYAMADA JUN
    • G02F1/335G02F1/11G02F1/125G02F1/1339G02F1/33
    • PURPOSE:To enlarge an angle of polarization and width of polarization by constituting an interdigital electrode of a slant type, so that all surface acoustic waves satisfy a Bragg condition against incident light beams, and also, placing a high frequency surface acoustic wave exciting part in the incident light side. CONSTITUTION:On a piezoelectric substrate 1, an optical waveguide 2 is formed, and on said waveguide, an interdigital electrode 3 is formed. As for this electrode 3, a slant type electrode having a wide band characteristic is used. Also, as for its structure, each electrode finger is curved so that a surface acoustic wave satisfies a Bragg condition. Moreover, a high frequency exciting part of the slant type electrode is placed in the incident side of the optical waveguide so that light beams which have been deflected by a high frequency surface acoustic wave do not cross each other. According to said constitution, in a light beam 5 which is propagated in the optical waveguide 2 by a surface acoustic wave radiated from the electrode 3, deflection light beams 6 which have been brought to Bragg diffraction is obtained. In this way, an enlargement of a deflection angle, an improvement of a deflection efficiency, and an enlargement of deflection width can be realized.
    • 5. 发明专利
    • SURFACE ACOUSTIC WAVE DEVICE
    • JPS61288509A
    • 1986-12-18
    • JP12980985
    • 1985-06-17
    • HITACHI LTD
    • TAKEMA TAKEMITSUSHIBA TAKASHIHOSAKA NORIOYAMADA JUN
    • H03H9/25H03H3/08
    • PURPOSE:To attain low loss, high Q and miniaturization by so designing that a grating reflector electrode finger width in the surface acoustic wave propagation direction is smaller than the space between grating reflector electrode fingers. CONSTITUTION:As a piezoelectric substrate 1, a 128 deg. Y axis cut lithium niobate single crystal is used and the propagating direction of a surface acoustic wave is taken as the X axis direction. Aluminum is used for the electrode material and the vapor-deposited film is formed by the photolithography technology. Further, the resonance frequency of the resonator is selected as 90MHz, the width of the surface acoustic wave transmission and reception electrode is 10.8.mum, the number of pairs of electrodes for transmission and receiption electrodes 2 is three pairs and number of grating reflector electrodes 3 is 200 electrodes for both right and left electrodes. In this invention, the grating reflector electrode finger width is 10.6mum and the space width between the grating reflector electrode fingers is 11.0mum. That is, the grating reflector electrode finger width is shorter than the space width (l) between the grating reflector electrode fingers.
    • 9. 发明专利
    • VOLTAGE CONTROLLED OSCILLATOR FOR SURFACE ACOUSTIC WAVE
    • JPS63169110A
    • 1988-07-13
    • JP36987
    • 1987-01-07
    • HITACHI LTD
    • HOSAKA NORIOTAKEMA TAKEMITSUSHIBA TAKASHIYAMADA JUN
    • H03H9/42H03B5/30H03H3/08H03H9/44H03H9/64
    • PURPOSE:To obtain a voltage controlled oscillator whose variable frequency band is wide and oscillation characteristic is excellent by constituting an interdigital electrodes so that the delay time varies depending on the frequency and that the gradient of phase within a frequency band comes small. CONSTITUTION:The titled oscillator is constituted of two systems of surface acoustic wave delay lines whose output phases are different from each other, variable gain elements 5, 6, and an amplifier 7; at least either one of the input/ output interdigital electrodes 2-4 of said delay lines are formed with chirp electrode. The input electrode 2 is a normal type electrode common for the respective systems. while the output electrodes 3, 4 are separated respectively for the two systems. The electrodes are so formed that their respective periods of electrode gradually longer along the propagation direction of the surface acoustic wave. Therefore, a delay time for a high frequency wave can be made short, but that for a low frequency wave can be made longer. Thus the gradient of phase within a frequency band can be made less. As a result, the variable band width can be widened without a need for forming the input/output electrodes in extreme closeness or for the decreasing the number of electrode pairs can be eliminated, hence by the performance can be thus improved.
    • 10. 发明专利
    • RESONATOR FILTER FOR SURFACE ACOUSTIC WAVE
    • JPS63155810A
    • 1988-06-29
    • JP30122786
    • 1986-12-19
    • HITACHI LTD
    • TAKEMA TAKEMITSUHOSAKA NORIOSHIBA TAKASHIYAMADA JUN
    • H03H9/25H03H3/08
    • PURPOSE:To set attenuation quantities outside band areas on a high frequency side and a low frequency side at the same level and also to increase them, by performing the cascade connection of resonators in which distances between electrode fingers and centers at respective end of a grating reflector confronting with an interdigital electrode satisfy a prescribed condition. CONSTITUTION:The interdigital electrodes 1 and the grating reflectors 2 are constituted in the three stage cascade connection of two-port type resonators I, II, and III, and are arranged on a substrate 3 as shown in figure. As the resonators, the resonators I and II having frequency characteristics in which attenuation poles are on the high frequency side of a main peak, and the resonator III having the frequency characteristics in which the attenuation pole is on the low frequency side of the main peak, are selected. And the distance lmu between respective confronting electrode finger of the electrode 1 and the reflector 2 is selected so as to satisfy conditional equations I and II. In this case, it is assumed that (l) represents a wavelength in the center frequency of a filter, and (m) and (n) represent natural numbers including 0. By constituting the device in such way, it is possible to set the attenuation quantities outside the band areas on the high and low frequency sides at the same levels and to increase the attenuation quantity further because a peak and a trough in the frequency characteristics of each resonator do not coincide.