Piezoelectric resonator and electronic component using the same resonator

Abstract: A piezoelectric resonator having a small spurious resonance, a large frequency difference ΔF between the resonant frequency and the anti-resonant frequency, adjustable capacitance, and a high level of flexibility in designing the characteristics. Also disclosed is an electronic component using such a resonator. The piezoelectric resonator has a base member formed by laminating, for example, piezoelectric layers and internal electrodes. When the length, width, and thickness of the base member are indicated by L, W and T, respectively, the dimensions of the member are determined to satisfy the conditions of L≥2W and L≥2T. The base member is polarized at both ends of each internal electrode in opposite directions. A groove is formed on one lateral surface of the base member, and at both sides of the groove, the internal electrodes are covered with two insulating films alternately. The two insulating films are respectively formed to cover the different internal electrodes. External electrodes are formed on both sides of the groove of the base member and are connected to the internal electrodes.

Description: BACKGROUND OF THE INVENTION The present invention as defined in claims 1-7 relates to a piezoelectric resonator which uses the mechanical resonance of a piezoelectric member, and more particularly, to a piezoelectric resonator comprising a base member having a longitudinal direction, an active section composed of polarized piezoelectric member and constituting at least a part of the base member, and a pair of external electrodes provided with the active section. The present invention also relates to electronic components for use with the piezoelectric resonator, such as an oscillator, a discriminator, and a filter. Fig. 15 is a perspective view of a typical known type of piezoelectric resonator. An example of such a resonator is diclosed in Patent Abstract of Japan, vol. 009, no. 212 (E-339), 29 August 1985 & JP-A-60 074 709. A piezoelectric resonator generally indicated by 1 has a piezoelectric substrate 2 having, for example, a rectangularly planar shape, as viewed from the top. The substrate 2 is polarized in the thickness direction. Electrodes 3 are formed on both surfaces of the substrate 2. A signal is input between the electrodes 3, 3 so as to apply an electric field to the substrate 2 along its thickness, causing the substrate 2 to vibrate in the longitudinal direction. Also, in Fig. 16. there is shown a piezoelectric resonator 1 in which electrodes 3 are formed on both surfaces of a piezoelectric substrate 2 having a square planar shape, as viewed from the top. In this resonator 1, as well as the resonator 1 shown in Fig. 15, the piezoelectric substrate 2 is polarized in the thickness direction. A signal is input between the electrodes 3, 3 of the resonator 1 so as to apply an electric field to the substrate 2 along its thickness, thereby causing the substrate 2 to vibrate in the square-type vibration mode. These piezoelectric resonators 1, 1 are of an unstiffened type, in which the direction of vibration differs from the direction of polarization and the electric field. The electromechanical coupling coefficient of such an unstiffened piezoelectric resonator is lower than that of a stiffened piezoelectric resonator, in which the direction of vibration, the direction of polarization, and the direction in which an electric field is applied, are the same. Accordingly, an unstiffened resonator has a relatively small frequency difference ΔF between the resonant frequency and the anti-resonant frequency. This leads to a drawback in which a bandwidth in use is narrow when an unstiffened frequency resonator is used as a filter or an oscillator. Thus, flexibility in designing the characteristics is low in the above type of piezoelectric resonator and electronic components using such a resonator. The piezoelectric resonator 1 shown in Fig. 15 utilizes the first-order (basic) resonance in the longitudinal mode. At the same time, however, the resonator 1 also generates due to its structure large spurious resonances in the odd-number-order higher harmonic modes, such as the third-order and fifth-order modes, and in the width mode. Some measures to suppress these spurious resonances may be considered, such as polishing, increasing mass, and changing the shape of the electrode. These measures, however, increase the manufacturing cost. Additionally, since the piezoelectric substrate is formed in a rectangular planar shape as viewed from the top, the substrate cannot be made too thin due to restrictions in strength. Accordingly, the distance between the electrodes cannot be reduced and a capacitance between terminals cannot be made large. This is extremely inconvenient for achieving impedance matching with an external circuit. Further, to form a ladder filter by connecting a plurality of piezoelectric resonators alternately in series and in parallel, the capacitance ratio of the series resonator to the parallel resonator needs to be made large in order to increase attenuation. However, large attenuation cannot be obtained due to limitations in the shape of the resonators as described above, resulting in a low level of flexibility in respect of the characteristics, such as the frequency difference ΔF and the capacity. In the piezoelectric resonator 1 illustrated in Fig. 16, large spurious resonances such as those in the thickness mode and in the triple-wave mode in the plane direction are generated. Further, since this type of resonator needs a large size as compared with a piezoelectric resonator using longitudinal vibration in order to obtain the same resonant frequency, it is difficult to reduce the size of the former type of resonator. Also, when a ladder filter is formed by a plurality of piezoelectric resonators, in order to increase the capacitance ratio between the series resonator and the parallel resonator, the resonators connected in series are made thick, and electrodes are formed only on part of a piezoelectric substrate to decrease the capacitance as well. In this case, since the electrodes are only partially formed, not only the capacitance, but also the difference ΔF between the resonant frequency and the anti-resonant frequency, are reduced. The resonators connected in parallel are accordingly required to have a small frequency difference ΔF. As a consequence, the piezoelectricity of the piezoelectric substrate cannot be effectively used, and the pass bandwidth of the filter cannot be increased. In light of the above problems, a laminated piezoelectric resonator was proposed by the present inventor, for example, in Japanese Patent Application No. 8-122725. This resonator is a stiffened type, in which the direction of vibration and the direction in which an electric field is applied are the same. The resonator has more factors that contribute to filter characteristics, such as the width and thickness of the resonator, and the number of laminated layers used in the resonator, as compared with a known type of piezoelectric resonator formed of only a single substrate. Then, an examination was made whether good filter characteristics would be obtained by adjusting the above-described factors when this type of laminated piezoelectric resonator is applied to an electronic component, such as a ladder filter. Through this study it was revealed that the frequency difference ΔF is seriously decreased, and spurious resonances are increased, depending on the dimensions, such as the length, width and thickness, of the resonator. This further proves that the determination of the dimensions of the resonator is an important factor. SUMMARY OF THE INVENTION Accordingly, it is the main object of the present invention to provide a piezoelectric resonator having a small spurious resonance, a large difference ΔF between the resonant frequency and the anti-resonant frequency, adjustable capacitance, and high flexibility of designing the characteristics of the resonator, and also to provide an electronic component for use with the above piezoelectric resonator. In order to achieve the above object, the present invention provides a piezoelectric resonator of the above mentioned kind, which is characterized in that at least one pair of internal electrodes disposed in the active section such that the internal electrodes are perpendicular to the longitudinal direction of the base member and are connected to the pair of external electrodes respectively, the active section is polarized in the longitudinal direction of the base member, said base member excites a longitudinal mode basic vibration when an electric field is applied to the longitudinal direction of the base member via the internal electrodes, and the piezoelectric resonator has a rectangular planar shape viewed from the top thereof, and satisfies the conditions of L≧2W and L≧2T when L, W, T indicate the length, width, and thickness of said piezoelectric resonator, respectively. In the above piezoelectric resonator, ends of the internal electrodes may be exposed at a side face of the base member, a first insulating film may be provided to cover exposed portions of internal electrodes among the internal electrodes at one end of the side face of the base member, a second insulating film may be provided to cover exposed portions of internal electrodes among the internal electrodes which are not covered by the first insulating film at the other end of the side face of the base member, the pair of external electrodes may be respectively extended in the longitudinal direction at said one and the other ends of the side face of the base member and connected to said internal electrodes which are not covered by said first and second insulating films at each end of the side face of said base member. Or, ends of the internal electrodes may be partially exposed at a side face of the base member such that the exposed portions of the internal electrodes adjacent to each other are electrically connected to the pair of external electrodes respectively. In the above piezoelectric resonators, an inactive section, in which vibration is not excited when the electric field is applied, may constitute the other part of the base member. In the above piezoelectric resonators, a support member may be provided at a center of the base member in the longitudinal direction. This invention also provides an electronic component for use with the above described piezoelectric resonator, which is characterized in that the support member is provided on a insulating substrate, and a pattern electrode is provided on the insulating substrate and connected to the external electrodes of the piezoelectric resonator. The above described electronic component may be a ladder filter in which the plurality of pattern electrodes are provided on the insulating substrate and connected to the external electrodes of the plurality of piezoelectric resonators such that the piezoelectric resonators are connected each other in a ladder shape. In the above piezoelectric resonator, since the dimensions of the resonator are set to satisfy the conditions of L/W≧2 and L/T≧2, ΔF/F a is increased (a difference between the resonant frequency and the anti-resonant frequency, ΔF, is increased), and spurious resonances are decreased. Through the experiment made by the present inventor, Fig. 4 shows that ΔF/F a is sharply decreased if L is smaller than two times W i.e., L/W<2. Similarly, Fig. 5 indicates that ΔF/F a sharply drops if L is smaller than two times T i.e., L/T<2. Further, Figs. 6 and 7 reveal that smaller spurious resonances can be achieved when L/W and L/T are equal to 4(within the conditions L/W≧2 and L/T≧2) as compared with a case when L/W and L/T are equal to 1 (out of the conditions L/W≧2 and L/T≧2). It is thus possible to obtain a piezoelectric resonator having small spurious resonances and an electronic component using such a resonator. Also, in this piezoelectric resonator, it is possible to adjust ΔF unlike conventional piezoelectric resonators, which further makes it possible to regulate the bandwidth of the resonator. Additionally, since the capacitance of the resonator is adjustable, it is easy to achieve impedance matching with an external circuit in a case when the resonator is mounted on, for example, a circuit board. Namely, in this invention, ΔF and the capacitance are adjustable, and thus, a piezoelectric resonator having high flexibility in designing the characteristics and an electronic component for use with such a resonator can be provided. Moreover, an electronic component, such as a filter, a discriminator, or an oscillator, using the above type of piezoelectric resonator can be produced by the following process. The resonator is mounted on a support substrate on which pattern electrodes are formed, and preferably the resonator is then covered with a cap. Thus, a chip-type electronic component can be completed. During this process, the resonator can be mounted on the pattern electrodes disposed on the support substrate without needing to use a lead wire by virtue of the face bonding structure. Additionally, support members have been formed at the center of the base member, and thus, the node of the resonator can be positively supported when the resonator is mounted on the pattern electrodes. Thus, an electronic component using this resonator can be produced with reduced cost because the resonator can be connected via support members to the pattern electrodes formed on a support substrate without needing to use a lead wire. The support members have been provided for the piezoelectric resonator, so that vibrations of the resonator are not impeded, thereby obtaining piezoelectric components having good characteristics. In particular, by utilizing a plurality of piezoelectric resonators, a ladder filter exhibiting good characteristics can be produced with reduced cost. Since a chip-type electronic component can be made by the use of the above piezoelectric resonator, it can be readily mounted on a circuit board. In this electronic component, as well as the above piezoelectric resonator, the capacitance can be regulated by constructing the resonator with a laminated structure, and it is easy to achieve impedance matching between such a component and an external circuit. Additionally, in a ladder filter formed by connecting a plurality of the piezoelectric resonators alternately in series and in parallel, attenuation can be adjusted by changing the ratio of the capacitance of the resonators connected in series to the capacitance of the resonators connected in parallel. The above-described object, other objects, other features, and other advantages of the present invention will be apparent in the following detailed description of the embodiments of the present invention in conjunction with the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1A is a perspective view of a piezoelectric resonator according to an embodiment of the present invention. Fig. 1B is a perspective view of an example of modifications of the piezoelectric resonator shown in Fig. 1A. Fig. 2 illustrates the internal construction of the piezoelectric resonator shown in Figs. 1A and 1B. Fig. 3 is a plan view of the piezoelectric resonator shown in Figs. 1A and 1B having insulating films on the base member. Fig. 4 is a diagram illustrating the relationship between the dimension ratio L/W and the frequency difference ratio ΔF/F a of a piezoelectric resonator. Fig. 5 is a diagram illustrating the relationship between the dimension ratio L/T and the frequency difference ratio ΔF/F a of a piezoelectric resonator. Fig. 6 is a diagram illustrating the relationship between the frequency and the impedance of a piezoelectric resonator when L/W is equal to 1. Fig. 7 is a diagram illustrating the relationship between the frequency and the impedance of a piezoelectric resonator when L/W is equal to 4. Fig. 8 is a perspective view illustrating the internal construction of an example of modifications of the piezoelectric resonator shown in Figs. 1A, 1B, 2 and 3. Fig. 9 is a cross sectional view of the base member used in the piezoelectric resonator shown in Fig. 8. Fig. 10 is an exploded perspective view of an example of an electronic component for use with the piezoelectric resonator shown in Figs. 1A, 1B, 2 and 3. Fig. 11 is an exploded perspective view of a method for mounting the piezoelectric resonator on a substrate in the electronic component shown in Fig. 10. Fig. 12 is a plan view of the essential portion of an example of a ladder filter using the piezoelectric resonators of the present invention. Fig. 13 is an exploded perspective view of the essential portion of the ladder filter shown in Fig. 12. Fig. 14 is a diagram illustrating an equivalent circuit of the ladder filter shown in Figs. 12 and 13. Fig. 15 illustrates a known type of unstiffened piezoelectric resonator. Fig. 16 illustrates a known type of stiffened piezoelectric resonator. DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will now be described while referring to the accompanying drawings. A reference will first be made to Figs. 1A, 1B and 2 illustrating a piezoelectric resonator according to an embodiment of the present invention. A piezoelectric resonator generally designated by 10, formed in a rectangular planar shape as viewed from the top, has a base member 12 formed, for example, in a rectangular-prism shape. The base member 12 is made from, for example, a piezoelectric ceramic material. A plurality of internal electrodes 14 are formed in the base member 12 in such a manner that the surfaces of the electrodes 14 are perpendicular to a longitudinal direction of the base member 12. The base member 12 is longitudinally polarized so that the directions of polarization are opposite to each other at both ends of one electrode 14, as indicated by the arrows in Fig. 2. The dimensions of the base member 12 are determined in the following manner. When the length, width, and thickness of the base member 12 are indicated by L, W and T, respectively, the dimensions of the base member 12 are set to satisfy the conditions of L 3 2W and L 3 2T. Namely, the dimensions of the base member 12 are formed to satisfy the conditions of L/W 3 2 and L/T 3 2. Formed on one lateral surface of the base member 12 is a groove 15 extending In the longitudinal direction of the base member 12. The groove 15 is formed in the central portion of the base member 12 in a widthwise direction so as to divide one lateral surface of the base member 12 into two portions. Further, a first insulating film 16 and a second insulating film 18 are provided, as illustrated in Fig. 3, for the lateral surface divided by the groove 15. On one side face of the divided lateral surface of the base member 12, the first insulating film 16 covers the exposed sections of every other electrode 14. On the other side face of the base member 12, the second insulating film 18 covers the exposed sections of every other electrode 14 which are not covered by the first insulating film 16. It should be noted that both ends of the base member 12 are not polarized. Moreover, external electrodes 20 and 22 are disposed on the lateral surface on which the first and second insulating films 16 and 18 are formed, i.e., on both sides of the groove 15. Thus, the electrode 20 is connected to the internal electrodes 14 which are not covered with the first insulating film 16, while the electrode 22 is connected to the internal electrodes 14 which are not covered with the second insulating film 18. Namely, two adjacent electrodes 14 are connected to the external electrodes 20 and 22, respectively. In this embodiment, the exposed sections of the internal electrodes 14 are covered with the first and second insulating films 16 and 18, and the external electrodes 20 and 22 are further formed on the films 16 and 18, respectively. However, the base member 12 is not necessarily grooved, as illustrated in Fig. 1B. More specifically, for example, on one lateral surface of the base member 12 illustrated in Figs. 1A, 2 and 3, the insulating films 16 and 18 may alternately cover the exposed sections of the internal electrodes 14 at both ends of the base member 12 in the widthwise direction, and the external electrodes 20 and 22 may be disposed in two rows to extend along the base member 12 in the longitudinal direction. In this modification, although the base member 12 is not grooved, adjacent internal electrodes 14 are connected to the external electrodes 20 and 22, respectively. The internal electrodes 14 may be configured such that only part of the electrodes 14 connected to the external electrodes 20 and 22 may be exposed from the surface of a laminated block of the piezoelectric resonator 10, and the other portions may not be exposed. In this case, the provision of the insulating films 16 and 18 is not particularly necessary, as illustrated in, for example, Figs. 8 and 9. The above-constructed resonator 10 uses the external electrodes 20 and 22 as input and output electrodes. The base member 12, except for both the ends, becomes piezoelectrically active because an electric field is applied between adjacent internal electrodes 14. The member 12 is, however, piezoelectrically inactive at both the ends because it is not polarized therein and also because an electric field is not applied because of the absence of electrodes. As a result, an active section 26, which is responsive to input signals, is formed at the center of the base member 12, while inactive sections 28, which is unresponsive to input signals, are formed at both ends of the member 12. The inactive sections 28 do not generate driving force by input signals. In the inactive portions 28, an electric field may be applied between the internal electrodes 14 as long as they are not polarized. Alternatively, the inactive portions 28 may be constructed in such a manner that the piezoelectric layers may be polarized as long as an electric field is not applied. In this resonator 10, a signal is input to the external electrodes 20 and 22 so as to apply opposite voltages to the piezoelectric layers of the active section 26 polarized in the opposite directions. This causes the piezoelectric layers to expand and contract in the same direction as a whole. Thus, the overall piezoelectric resonator 10 vibrates in the longitudinal direction in the basic mode in which the center of the base member 12 serves as a node. By use of the piezoelectric resonators, such as the resonator 10 shown in Fig. 1A, electronic components, such as oscillators and discriminators, can be produced. Referring to a perspective view of an example of electronic components shown in Fig. 10, an electronic component generally indicated by 30 has an insulating substrate 32. At each of the opposing end portions of the substrate 32, two indentations 34 are formed. Disposed on one surface of the substrate 32 are two pattern electrodes 36 and 38. One pattern electrode 36 is formed between opposing indentations 34 and extends in an "L" shape from a point near one end of the electrode 36 toward the center of the substrate 32. The other electrode 38 is disposed between the other opposing indentations 34 and extends in an "L" shape from a point near one end of the electrode 38 (opposite to the one end of the electrode 36) toward the center of the substrate 32. In the vicinity of the central portion of the substrate 32, the pattern electrodes 36 and 38 are disposed to opposedly face each other with a spacing. The electrodes 36 and 38 are formed to be routed in a roundabout fashion from the ends of the substrate 32 to the reverse surface of the substrate 32. The piezoelectric resonator 10 is mounted on the insulating substrate 32 by support members 24. In other words, the support members 24 are formed at the central portions of the respective external electrodes 20 and 22 in the longitudinal direction. The support members 24 are formed so that they can become conductive. The support members 24 may be made from a conductive material, such as conductive adhesive. Alternatively, an insulator coated with an electrode film may adhere to each of the external electrodes 20 and 22 through a conductive material. Then, the support members 24 formed as noted above are, as illustrated in Fig. 11, connected through, for example, conductive adhesive (not shown), to the ends of the respective pattern electrodes 36 and 38 disposed at the center of the substrate 32. Thus, the external electrodes 20 and 22 of the resonator 10 can be securely mounted on the insulating substrate 32 and also electrically connected to the pattern electrodes 36 and 38, respectively. Referring back to Fig. 10, a metallic cap 40 is placed on the substrate 32 to complete the electronic component 30. In order to prevent the metallic cap 40 being shortcircuited to the pattern electrodes 36 and 38, insulating resin is applied to the insulating substrate 32 and the pattern electrodes 36 and 38 in advance. In this component 30, the pattern electrodes 36 and 38, which are formed to be routed in a roundabout manner from the ends of the substrate 32 to the reverse surface of the substrate 32, are used as input and output terminals for connecting the resonator 10 to external circuits. In this electronic component 30, when the length, width, and thickness of the resonator 10 are indicated by L, W and T, respectively, the dimensions of the piezoelectric resonator 10 are determined to satisfy the conditions of L 3 2W and L 3 2T. Accordingly, a difference between the resonant frequency and the anti-resonant frequency, i.e., ΔF, can be increased. Thus, in this electronic component 30, a large frequency difference ΔF/F a and small spurious resonances can be achieved. Also, in this component 30, since the piezoelectric resonator 10 is held by the support members 24 formed at the central portion of the longitudinal substrate 12, the ends of the resonator 10 can be disposed separately from the substrate 32, so that vibrations are not impeded. Additionally, the central portion of the resonator 10, which serves as a node, can be secured by the support members 24, and the external electrodes 20 and 22 are electrically connected to the pattern electrodes 36 and 38, respectively. Since the support members 24 have been formed on the resonator 10, they can be correctly positioned to the node of the resonator 10. Thus, the node can be supported more correctly by the support members 24 arranged as described above as compared with, for example, the following arrangement of support members. That is, support members in the form of, for example, projections, are formed on the pattern electrodes 36 and 38, and the piezoelectric resonator 10 is mounted on the support members. As a consequence, vibration leakage of the resonator 10 can be avoided, thereby obtaining good characteristics. Also, there is no need to use a lead wire to connect the external electrodes 20 and 22 of the resonator 10 to the pattern electrodes 36 and 38, respectively. Hence, the electronic component 30 can be manufactured with reduced cost. The electronic component 30, together with IC chips, can be mounted on a substrate to form an oscillator or a discriminator. Since the electronic component 30 constructed as described above is sealed and protected by the metallic cap 40, it can be used as a chip-type (surface mount) component which is mountable by reflow soldering. When this electronic component 30 using the above type of resonator 10 is employed in an oscillator, spurious vibrations can be suppressed to a low level, which would otherwise cause unusual vibrations. It is also easy to achieve impedance matching with an external circuit since any desired level of capacitance can be set. Particularly when the electronic component 30 is used in an oscillator for voltage-controlled oscillation, a wide frequency variable range can be obtained due to a large frequency difference ΔF, which cannot be conventionally accomplished. Moreover, when this electronic component 30 is used in a discriminator, a wide peak-separation range can be provided due to a large ΔF of the resonator. Additionally, it is easy to achieve impedance matching with an external circuit because of a wide capacitance range of the resonator. A ladder filter may be produced using a plurality of piezoelectric resonators 10. Fig. 12 is a plan view of the essential portion of an electronic component used as a ladder filter having a ladder-shaped circuit. Fig. 13 is an exploded perspective view of the electronic component shown in Fig. 12. In an electronic component generally designated by 50 shown in Fig. 13, four pattern electrodes 56, 58, 60 and 62 are formed on an insulating substrate 52. Five lands are provided for these pattern electrodes 56 through 62 in such a manner that they are disposed in a row with intervals. More specifically, the first land from one end of the substrate 52 is provided for the pattern electrodes 56; the second and fifth lands are formed at the electrode 58; the third land is disposed at the electrode 60; and the fourth land is provided for the electrode 62. Fixed to these lands are support members 24 mounted on the external electrodes 20 and 22 of the individual piezoelectric resonators 10a, 10b, 10c and 10d. In this case, the resonators 10a through 10d are mounted on the substrate 52 in such a manner that the ladder-shaped circuit illustrated in Fig. 14 can be obtained. Then, a metallic cap (not shown) is placed on the substrate 52. The electronic component 50 constructed as described above can thus be used as a ladder filter having a ladder-shaped circuit shown in Fig. 14. Two resonators 10a and 10d may be used as series piezoelectric resonators, while the other two resonators 10b and 10c may serve as parallel piezoelectric resonators. This type of ladder filter is designed so that the capacitance of the parallel resonators 10b and 10c is much larger than the capacitance of the series resonators 10a and 10d. Attenuation in the ladder filter is determined by the capacitance ratio between the series resonators and the parallel resonators. When the lengths, widths, and thicknesses of the resonators 10a through 10d are represented by L, W and T, respectively, this electronic component 50, as well as the previous electronic component 30, is designed to satisfy the conditions of L≥2W and L≥2T. Accordingly, the frequency difference ΔF can be increased. Hence, the electronic component 50 can exhibit large ΔF/F a and small spurious resonances. Further, in this electronic component 50, the capacitance can be adjusted by changing the number of laminated layers used in the piezoelectric resonators 10a through 10d. Thus, a ladder filter having a larger attenuation with fewer piezoelectric resonators can be implemented by changing the capacitance of the resonators 10a through 10d, as compared with a case where conventional unstiffened piezoelectric resonators are employed. Additionally, since the resonators 10a through 10d have a larger ΔF than known piezoelectric resonators, a wider pass bandwidth of a resulting ladder filter can be achieved as compared with a filter using conventional resonators. As discussed in the foregoing embodiment, according to the present invention, when the length, width, and thickness of the piezoelectric resonator 10 are indicated by L, W and T, respectively, the dimensions of the resonator 10 are determined, in particular, to satisfy the conditions of L≥2W and L≥2T. Accordingly, the characteristics of the resonator 10, such as the capacitance, can be regulated. As a consequence, a resonator 10 having a high level of flexibility in designing the characteristics can be obtained. To further develop this resonator 10, the electronic components 30 and 50 using the resonator 10 can be attained.

Claims: Piezoelectric resonator (10), comprising a base member (12) having a longitudinal direction, an active section (26) composed of polarized piezoelectric member and constituting at least a part of said base member (12), and a pair of external electrodes (20,22) provided with said active section (26), characterized in that at least one pair of internal electrodes (14) disposed in said active section (26) such that the internal electrodes (14) are perpendicular to the longitudinal direction of said base member (12) and are connected to said pair of external electrodes (20,22) respectively, said active section (26) is polarized in the longitudinal direction of said base member (12), said base member (12) excites a longitudinal mode basic vibration when an electric field is applied to the longitudinal direction of said base member (12) via said internal electrodes (14), and said piezoelectric resonator (10) has a rectangular planar shape viewed from the top thereof, and satisfies the conditions of L≥2W and L≥2T when L, W, T indicate the length, width, and thickness of said piezoelectric resonator (10), respectively. Piezoelectric resonator (10) according to Claim 1, characterized in that ends of said internal electrodes (14) are exposed at a side face of said base member (12), a first insulating film (16) which covers exposed portions of internal electrodes (14) among said internal electrodes (14) at one end of said side face of said base member (12), a second insulating film (18) which covers exposed portions of internal electrodes (14) among said internal electrodes (14) which are not covered by said first insulating film (16) at the other end of said side face of said base member (12), said pair of external electrodes (20,22) are respectively extended in the longitudinal direction at said one and the other ends of said side face of said base member (12) and connected to said internal electrodes (14) which are not covered by said first and second insulating films (16,18) at each end of said side face of said base member (12). A piezoelectric resonator (10) according to Claim 1, characterized in that ends of said internal electrodes (14) are partially exposed at a side face of said base member (12) such that the exposed portions of said internal electrodes (14) adjacent to each other are electrically connected to said pair of external electrodes (20,22) respectively. Piezoelectric resonator (10) according to one of Claims 1 to 3, characterized in that an inactive section (28), in which vibration is not excited when said electric field is applied, constitutes the other part of said base member (12). Piezoelectric resonator (10) according to one of Claims 1 to 4, characterized in that the piezoelectric resonator (10) further comprises a support member (24) at a center of said base member (12) in the longitudinal direction. An electronic component (30) for use with the piezoelectric resonator (10) according to Claim 4, characterized in that said support member (24) is provided on a insulating substrate (32), and a pattern electrode (36,38) is provided on said insulating substrate (32) and connected to said external electrodes (20,22) of said piezoelectric resonator (10). An electronic component (50) according to Claim 6, characterized in that said electronic component (50) is a ladder filter in which a plurality of said pattern electrodes (56,58,60,62) are provided on said insulating substrate (52) and connected to said external electrodes (20,22) of a plurality of said piezoelectric resonators (10) such that said piezoelectric resonators (10) are connected each other in a ladder shape.

Inventors: BABA TOSHIYUKI, KUSABIRAKI SHIGEMASA, TAKESHIMA TETSUO, UNAMI TOSHIHIKO, YAMAMOTO TAKASHI, YOSHINO HIROHIDE, BABA, TOSHIYUKI, KUSABIRAKI, SHIGEMASA, TAKESHIMA, TETSUO, UNAMI, TOSHIHIKO, YAMAMOTO, TAKASHI, YOSHINO, HIROHIDE
Applicants: MURATA MANUFACTURING CO, MURATA MANUFACTURING CO., LTD.
Application year: 1997
Main classification: H03H9
IPC codes: H01L41, H03H9