JP4453017B2 - Manufacturing method of crystal unit - Google Patents

Description

The present invention relates to a configured electronic equipment comprises at least a display section and a crystal oscillator. In particular, it comprises an optimal crystal oscillator as a clock source or reference signal source, and further comprises at least two crystal oscillators, two of which comprise crystal oscillators composed of crystal oscillators of different vibration modes. It was about the electronic equipment.

One of the conventional crystal oscillators used in electronic devices is well known as a crystal oscillator composed of an amplifier, a capacitor, a resistance element, and a tuning fork-type bending crystal resonator in which electrodes are arranged on the upper and lower surfaces and side surfaces of the tuning fork arm. FIG. 11 shows an overview of a tuning-fork-shaped bent quartz crystal resonator 200 used in this conventional crystal oscillator. In FIG. 11, the crystal resonator 200 includes two tuning fork arms 201 and 202 and a tuning fork base 230. FIG. 12 shows a cross-sectional view of the tuning fork arm of FIG. As shown in FIG. 12, the excitation electrodes are arranged on the upper and lower surfaces and side surfaces of the tuning fork arm. An electrode 203 is disposed on the upper surface of the cross-section of one tuning fork arm, and an electrode 204 is disposed on the lower surface. Electrodes 205 and 206 are provided on the side surfaces. An electrode 207 is arranged on the upper surface of the other tuning fork arm, an electrode 208 is arranged on the lower surface, and electrodes 209 and 210 are arranged on the side surfaces to form a two-electrode terminal HH ′ structure. Now, when a DC voltage is applied between H-H ', the electric field works in the direction of the arrow. As a result, when one tuning fork arm is bent inward, the other tuning fork arm is also bent inward. This is because the direction of the electric field component Ex in the x-axis direction is opposite in each tuning fork arm. By applying an alternating voltage, vibration can be sustained. Patent Documents 1 to 3 disclose a tuning fork arm with a groove and an electrode configuration.
JP-A-56-65517 JP 2000-223992 (P2000-223992A) International Publication No. 00/44092

The tuning-fork type flexural quartz crystal resonator, the more the electric field component Ex is greater losses equivalent series resistance R ₁ becomes smaller, the quality factor Q value increases. However, as shown in FIG. 12, the tuning fork-type bent quartz crystal resonator that has been used conventionally has electrodes arranged on the upper and lower surfaces and side surfaces of each tuning fork arm. Therefore, the electric field does not work linearly, and if the tuning fork type bent quartz resonator is reduced in size, the electric field component Ex becomes smaller, the loss equivalent series resistance R ₁ becomes larger, the quality factor Q value becomes smaller, etc. The problem was left. At the same time, there remains a problem to obtain a bent crystal resonator that has high accuracy as a time reference, that is, has high frequency stability and suppresses harmonic mode vibration. As a method for solving the above-mentioned problem, for example, Patent Document 1 discloses a groove on the tuning fork arm, and discloses a groove configuration and an electrode configuration. However, the configuration of the groove, disclose any Figa of merit M relating to relationships and the frequency stability of the equivalent series resistance R _n of the harmonic mode vibration and equivalent series resistance R ₁ of the vibration mode and fundamental mode vibration and dimension It has not been. In addition, when a crystal oscillation circuit is configured by connecting a conventional crystal resonator or a resonator with a groove to a conventional circuit, the output signal of the fundamental vibration mode is affected by the impact or vibration, and the output signal vibrates in the harmonic mode. There has been a problem such as a change or detection of the frequency of the electronic device, and a problem that the electronic device does not operate normally. For this reason, there has been a demand for a crystal oscillator including a tuning-fork-shaped bent quartz crystal that vibrates in a fundamental wave mode that suppresses harmonic mode vibration that is not affected by shock or vibration. . Furthermore, in order to reduce the current consumption of the crystal oscillator, and to reduce the load capacitance C _L liable to vibration harmonic mode, problems such as not to obtain the output frequency of the fundamental mode oscillation has been left. Thus, a tiny vibrating at the fundamental mode, a small equivalent series resistance R _1, comprising a flexural quartz crystal tuning fork shape quality factor Q value increases, the output signal at the frequency of the fundamental mode oscillation, high A crystal oscillator having frequency stability (high time accuracy) and low current consumption has been desired. In particular, there is no report regarding a crystal oscillator including a width longitudinal mode crystal resonator having a small equivalent series resistance R ₁ and a high Q value.

  The present invention relates to an electronic apparatus including a tuning fork-shaped crystal resonator, a width-longitudinal mode crystal resonator, or a thickness-slip mode crystal resonator that vibrates in a bending mode, which advantageously solves the conventional problems by the following method. Is intended to provide.

That is, the first aspect of the method for manufacturing a quartz unit of the present invention, in a method for manufacturing a quartz unit configured to include a crystal oscillator and the case and the lid, before Symbol crystal oscillator, a tuning fork base portion and its fork It comprises at least a first tuning fork arm and a second tuning fork arm connected to the base , and a two electrode terminal having a first electrode terminal and a second electrode terminal having a different electrical polarity from the first electrode terminal. a that tuning-fork flexural crystal oscillator, the tuning-fork flexural quartz crystal resonator includes the fundamental mode vibration and second harmonic mode vibration, the fundamental mode vibration of the full Iga of merit M ₁ is the secondary to be larger than the full Iga of merit M ₂ harmonic mode vibration, tuning fork comprising the step of determining the dimensions of the tuning fork and the groove and the electrode, the second fork arm and the first fork arm and the fork base forming a shape, Forming a groove in each of the upper and lower surfaces of the tuning fork arms of serial the first fork arm second tuning fork arms, in order to form the first electrode terminal of said second electrode terminal, before Symbol first In order to form the second electrode terminal of the two electrode terminals, the step of arranging the electrode so that the electrode on the side surface of one tuning fork arm and the electrode of the groove of the second tuning fork arm have the same polarity , a step of the electrode side of the groove electrode and the second tuning fork arms of said first fork arm to place the electrodes so that the same poles, the tuning-fork flexural crystal vibrating configured with the second electrode terminal to configure and fixing a conductive adhesive to a fixed portion of the casing for accommodating the child, a crystal unit with said and said and said tuning-fork flexural crystal oscillator case lid, said case the lid And a step of connecting to the crystal unit .

According to a second aspect of the crystal unit manufacturing method of the present invention, in the first aspect, each of the upper and lower surfaces of each tuning fork arm of the first tuning fork arm and the second tuning fork arm of the tuning fork type quartz crystal resonator. The grooves formed in the first tuning fork arm and the second tuning fork arm are formed on both sides of the neutral line on each of the upper and lower surfaces of each tuning fork arm, and the partial width including the neutral line is 0.05 mm. This is a manufacturing method of a crystal unit formed to be smaller .

  As described above, the present invention is an electronic device including a crystal oscillator composed of a tuning fork-shaped bent crystal resonator, a width-longitudinal mode crystal resonator, or a thickness-shear mode crystal resonator, and in particular, the relationship between the amplifier circuit and the feedback circuit. By showing the shape and cut angle of the crystal resonator, an electronic device including a crystal oscillator having high frequency stability can be obtained.

Embodiments of the present invention will be specifically described below with reference to the drawings.
FIG. 1 shows an example of an electronic apparatus according to the present invention, which is an example of a block diagram of a facsimile. That is, it comprises a modem, an audio circuit, a clock circuit, a printing unit, a capturing unit, an operation unit, and a display unit. In this principle, first, the reflected light of the light projected on the document by the capturing unit is sensed and scanned by the charge coupled device (CCD). The detected shade of reflected light is converted into a digital signal, modulated by a modem, and sent to a telephone line. On the receiving side, the received signal is demodulated by a modem and printed on a recording sheet in synchronization with the transmitting side by a printing unit. As shown in FIG. 1, the crystal oscillator is used for a CPU clock of a control unit and a printing unit, a clock of a voice synthesis IC of a voice circuit, a synchronous clock of a modem, a time reference of a clock circuit, and the like. That is, they constitute a crystal oscillator and the output signal is used. For example, it is used as a signal for displaying time on the display unit. In order for a facsimile which is one of the electronic devices of this embodiment to operate normally, an accurate output signal of a crystal oscillator used in this device is required. In the present embodiment, a facsimile is shown as an example of the electronic device, but the electronic device of the present invention includes all devices configured to include a crystal oscillator. For example, a mobile phone, a telephone, a television, a camera, a video, a video camera, a pager, a personal computer, a printer, a CD player, an MD player, an electronic musical instrument, car navigation, car electronics, a clock, an IC card, and the like. Hereinafter, the crystal oscillator used in the electronic apparatus of the present invention will be described in detail.

  FIG. 2 is an example of a crystal oscillation circuit diagram constituting a crystal oscillator used in the electronic apparatus of the present invention. In this embodiment, the crystal oscillation circuit 1 includes an amplifier (CMOS inverter) 2, a feedback resistor 4, a drain resistor 7, capacitors 5 and 6, and a tuning fork-shaped bent crystal resonator 3. That is, the crystal oscillation circuit 1 includes an amplifier circuit 8 including an amplifier 2 and a feedback resistor 4, a drain resistor 7, capacitors 5 and 6, and a feedback circuit 9 including a bent crystal resonator 3. Further, the output signal of the crystal oscillation circuit 1 including the tuning fork-shaped bent crystal resonator 3 that vibrates in the fundamental wave mode is output from the drain side through a buffer circuit (not shown). That is, the frequency of the fundamental mode vibration is output as an output signal through the buffer circuit. In the present invention, the frequency of the fundamental mode vibration is 10 KHz to 200 KHz. In the present invention, the frequency obtained by dividing or multiplying the frequency of the output signal by a divider circuit or a multiplier circuit is also included in the fundamental mode vibration frequency. More specifically, the crystal oscillator according to the present embodiment includes a crystal oscillation circuit and a buffer circuit. In other words, the crystal oscillation circuit is composed of an amplifier circuit and a feedback circuit, the amplifier circuit is composed of at least an amplifier, and the feedback circuit is composed of at least a tuning-fork-shaped bent crystal resonator and a capacitor. Further, the tuning-fork-shaped bent crystal resonator used in the crystal oscillator of this embodiment will be described in detail with reference to FIGS.

FIG. 3 shows the feedback circuit diagram of FIG. Now, the angular frequency of the tuning-fork-shaped quartz crystal vibrating in the bending mode is ω _i , the resistance of the drain resistor 7 is R _d , the capacitances of the capacitors 5 and 6 are C _g and C _d , and the crystal impedance of the crystal is R _ei , When the input voltage is V ₁ and the output voltage is V ₂ , the feedback rate β _i is defined by β _i = | V ₂ | _i / | V ₁ | _i . However, i represents the vibration order of the bending mode vibration. For example, when i = 1, fundamental mode vibration, when i = 2, second harmonic mode vibration, when i = 3, third harmonic mode It is vibration. That is, when i = n, it is n-order harmonic mode vibration, but hereinafter simply referred to as harmonic mode vibration. Further, the load capacity C _L is given by C _L = C _g C _d / (C _g + C _d ). When C _g = C _d = C _gd and R _d >> R _ei , the feedback rate β _i is β _i = 1 / (1 + kC _L ² ). However, k is represented by a function of ω _i , R _d, R _ei . R _ei is approximately equal to the equivalent series resistance R _i .

Thus, from the relationship between the feedback rate β _i and the load capacitance C _L , it is well understood that the feedback rates of the resonance frequencies of the fundamental vibration mode and the harmonic vibration mode increase as the load capacitance C _L decreases. Therefore, when the load capacity _CL is reduced, the harmonic mode vibration is more likely to oscillate than the fundamental mode vibration. The reason is that since the maximum vibration amplitude of the harmonic mode vibration is smaller than the maximum vibration amplitude of the fundamental mode vibration, the amplitude condition and the phase condition which are oscillation continuation conditions are satisfied simultaneously.

The crystal oscillator used in the electronic apparatus of the present invention provides a crystal oscillator having a fundamental mode vibration frequency with low current consumption and high frequency stability (high time accuracy). It is aimed. Therefore, in order to reduce current consumption, in the present embodiment, the load capacitance C _L is used under 10pF. In order to further reduce the current consumption, since the current consumption is proportional to the load capacity, C _L = 8 pF or less is preferable. The capacitances C _g and C _{d referred to} here are numerical values that do not include the stray capacitance of the circuit, but actually there are stray capacitances depending on the circuit configuration. Therefore, in this embodiment, the load capacitance C _L containing the stray capacitance of this circuit configuration uses the following 18 pF. Further, in order to suppress the harmonic mode vibration and the output signal of the oscillator obtains the frequency of the fundamental mode vibration, the main signal is satisfied so that α ₁ / α _n > β _n / β ₁ and α ₁ β ₁ > 1 are satisfied. The crystal oscillation circuit of the embodiment is configured. However, α ₁ and α _n are amplification factors of the fundamental wave mode vibration and the harmonic mode vibration amplification circuit, and β ₁ and β _n are feedback rates of the feedback circuit of the fundamental wave mode vibration and the harmonic mode vibration. That is, when n = 2 and 3, they are the second and third harmonic mode vibrations, respectively.

In other words, the ratio of the amplification factor α ₁ of the fundamental mode vibration of the amplifier circuit and the amplification factor α _n of the harmonic mode vibration is the feedback factor β _n of the harmonic mode vibration of the feedback circuit and the feedback factor of the fundamental mode vibration. greater than the ratio of the beta _1, and the product of the feedback factor beta ₁ amplification factor alpha ₁ and the fundamental mode vibration of the fundamental wave mode vibration is configured to be greater than 1. With such a configuration, it is possible to realize a crystal oscillator that consumes less current and whose output signal has a frequency of fundamental mode vibration. Further, high frequency stability will be described later.

Further, the amplifying part of the amplifying circuit constituting the crystal oscillation circuit of the present embodiment can exhibit the characteristic by a negative resistance -RL _i . When i = 1, it is a negative resistance of fundamental mode vibration, and when i = n, it is a negative resistance of harmonic mode vibration. That is, when n = 2, 3, it is the negative resistance of the second and third harmonic mode vibration. In the crystal oscillator according to the present embodiment, the ratio of the absolute value | −RL ₁ | of the negative resistance of the fundamental mode vibration of the amplifier circuit to the equivalent series resistance R ₁ of the fundamental mode vibration is negative of the harmonic mode vibration of the amplifier circuit. The crystal oscillation circuit is configured so as to be larger than the ratio of the absolute value | -RL _n | of the resistive resistor and the equivalent series resistance R _n of the harmonic mode vibration. That is, it is configured to satisfy | −RL ₁ | / R ₁ > | −RL _n | / R _n . By configuring the crystal oscillation circuit in this way, the oscillation activation of the harmonic mode vibration is suppressed, and as a result, the oscillation activation of the fundamental wave mode vibration is obtained, so that the frequency of the fundamental wave mode vibration is obtained as the output signal.

  FIG. 4 shows an external view of a tuning-fork-shaped bent crystal resonator 10 that vibrates in a bending mode used in the crystal oscillator of the first embodiment constituting the electronic apparatus of the present invention and its coordinate system. An O-xyz including a coordinate system O, an electric axis x, a mechanical axis y, and an optical axis z is configured. The tuning fork-shaped bent quartz crystal resonator 10 according to this embodiment includes a tuning fork arm 20, a tuning fork arm 26 and a tuning fork base 40, and the tuning fork arm 20 and the tuning fork arm 26 are connected to the tuning fork base 40. The tuning fork arm 20 and the tuning fork arm 26 have an upper surface, a lower surface, and a side surface, respectively. Further, a groove 21 is provided on the upper surface of the tuning fork arm 20 with a neutral line interposed therebetween, that is, so as to include the neutral line, and a groove 27 is provided on the upper surface of the tuning fork arm 26 in the same manner as the tuning fork arm 20. Further, the tuning fork base 40 is provided with a groove 32 and a groove 36. The angle θ is a rotation angle around the x axis, and is usually selected in the range of 0 to 10 °. Further, grooves on the lower surfaces of the tuning fork arms 20 and 26 are provided in the same manner as the upper surface.

  FIG. 5 is a cross-sectional view of the tuning fork base 40 of the tuning fork-shaped bent quartz crystal resonator 10 of FIG. 5, the cross-sectional shape and electrode arrangement of the tuning fork base 40 of the crystal resonator of FIG. 4 will be described in detail. The tuning fork base 40 connected to the tuning fork arm 20 is provided with grooves 21 and 22. Similarly, the tuning fork base 40 connected to the tuning fork arm 26 is provided with grooves 27 and 28. Further, a groove 32 and a groove 36 are further provided between the groove 21 and the groove 27. A groove 33 and a groove 37 are also provided between the groove 22 and the groove 28. The electrodes 21 and 24 are disposed in the grooves 21 and 22, the electrodes 34, 35, 38, and 39 are disposed in the grooves 32, 33, 36, and 37, and the electrodes 29 and 30 are disposed in the grooves 27 and 28, respectively. Electrodes 25 and 31 are disposed on both side surfaces of the tuning fork base 40. Specifically, electrodes are disposed on the side surfaces of the grooves, and electrodes having different polarities are disposed to oppose the electrodes.

Further, the bent quartz resonator 10 of the tuning fork has a thickness t, groove has a thickness t _1. The thickness t ₁ here refers to the thickness of the deepest part of the groove. The reason for this is that quartz is an anisotropic material, and the etching speed varies depending on the direction of each crystal axis in the chemical etching method. Therefore, the chemical etching method causes variations in the depth of the groove, and it is extremely difficult to process the uniform shape shown in FIG. In the present embodiment, the ratio (t ₁ / t) between the groove thickness t ₁ and the tuning fork arm or the tuning fork arm and the tuning fork base thickness t is preferably less than 0.79. A groove is formed in the tuning fork arm or the tuning fork arm and the tuning fork base so as to be 79. In particular, in order to increase the distortion of the tuning fork base, it is preferable to set the ratio of the groove thickness of the tuning fork base and the thickness of the tuning fork base to 0.01 to 0.025. By forming in this way, the electric field Ex between the tuning fork arm or the tuning fork arm and the groove side surface electrode of the tuning fork base and the side electrode facing it increases. That is, a flexural vibrator with good electromechanical conversion efficiency can be obtained. That is, a tuning fork-shaped bent quartz crystal resonator with a small capacity ratio can be obtained. Furthermore, in this embodiment, since the grooves 32, 33, 36, and 37 are further provided between the grooves of the tuning fork base, the electric field strength is further increased and the electromechanical conversion efficiency is further improved. . Further, in this embodiment, the grooves 32 and 36 are provided on the upper surface of the tuning fork base 40 and the grooves 33 and 37 are provided on the lower surface, but they may be provided only on one side.

Further, the electrodes 25, 29, 30, 34, and 35 are arranged to have one same polarity, and the electrodes 23, 24, 31, 37, 38, and 39 are arranged to have the other same polarity. -E '. That is, the groove electrode that opposes the z-axis direction has the same polarity, and the electrode that opposes the x-axis direction has a different polarity. Now, when a DC voltage is applied to the two-electrode terminal EE ′ (the positive electrode is applied to the E terminal and the negative electrode is applied to the E ′ terminal), the electric field Ex works as indicated by the arrows shown in FIG. Since the electric field Ex is drawn perpendicularly to the electrodes by the electrodes arranged on the side surface of the crystal unit and the side surface in the groove, that is, linearly, the electric field Ex is increased, and as a result, the amount of distortion generated is large. Become. Therefore, even when the tuning fork-shaped bent quartz crystal is reduced in size, a tuning-fork-shaped quartz crystal that vibrates in a bending mode having a small equivalent series resistance R ₁ and a high quality factor Q value can be obtained.

FIG. 6 shows a top view of the tuning-fork-shaped bent quartz crystal resonator 10 of FIG. In FIG. 6, the arrangement and dimensions of the grooves 21 and 27 will be particularly described in detail. A groove 21 is provided so as to sandwich the neutral line 41 of the tuning fork arm 20. The other tuning fork arm 26 is also provided with a groove 27 so as to sandwich the neutral line 42. Further, in the tuning fork-shaped bent quartz crystal resonator 10 of this embodiment, the groove 32 and the groove 36 are also provided in the portion of the tuning fork base 40 sandwiched between the groove 21 and the groove 27. By providing the grooves 21 and 27 and the grooves 32 and 36, the electric field Ex acts on the tuning fork-shaped bent quartz resonator 10 as indicated by the arrow shown in FIG. Is drawn perpendicularly to the electrodes by the electrodes arranged on the side surface of the crystal unit and the side surface in the groove, that is, linearly, and in particular, the electric field Ex of the tuning fork base is increased, and as a result, the amount of distortion generated is also increased. growing. As described above, the shape and electrode configuration of the tuning-fork-shaped bent quartz crystal resonator 10 of this embodiment are excellent in electrical characteristics even when the tuning-fork-shaped bent quartz resonator is downsized, that is, equivalent series resistance R _A crystal resonator with a small quality factor Q of ₁ can be realized.

ように構成される。又、溝幅Ｗ_２はＷ_２≧Ｗ_１，Ｗ_３を満足する条件で構成される。更に具体的に述べると、本実施例では、溝幅Ｗ_２と音叉腕幅Ｗとの比（Ｗ_２／Ｗ）が０．３５より大きく、１より小さくなるように、好ましくは、０．３５〜０．９５で、溝の厚みｔ_１と音叉腕の厚みｔ又は音叉腕と音叉基部の厚みｔとの比（ｔ_１／ｔ）が０．７９より小さくなるように、好ましくは、０．０１〜０．７９となるように溝が音叉腕に形成されている。このように形成することにより、音叉腕の中立線４１と４２を基点とする慣性モーメントが大きくなる。即ち、電気機械変換効率が良くなるので、等価直列抵抗Ｒ_１の小さい、Ｑ値の高い、しかも、容量比の小さい音叉形状の屈曲水晶振動子を得る事ができる。Further, assuming that the partial widths W ₁ and W ₃ and the groove width W ₂ , the arm width W of the tuning fork arms 20 and 26 is W = W ₁ + W _2.

Configured as follows. Further, the groove width W ₂ is configured under the condition that satisfies W ₂ ≧ W ₁ and W ₃ . More specifically, in this embodiment, the ratio (W ₂ / W) of the groove width W ₂ to the tuning fork arm width W is larger than 0.35 and smaller than 1, preferably 0.35. The ratio (t ₁ / t) between the groove thickness t ₁ and the tuning fork arm thickness t or the tuning fork arm and tuning fork base thickness t (t ₁ / t) is preferably less than 0.79. Grooves are formed in the tuning fork arm so as to be 01 to 0.79. By forming in this way, the moment of inertia with the tuning fork arm neutral lines 41 and 42 as base points is increased. That is, since the electro-mechanical conversion efficiency is improved, a small equivalent series resistance R _1, a high Q value, moreover, it is possible to obtain a bending crystal oscillator of a small tuning fork capacity ratio.

On the other hand, with respect to the length l ₁ of the groove 21 and the groove 27, in this embodiment, the grooves 21 and 27 extend from the tuning fork arms 20 and 26 to the length l ₂ of the tuning fork base 40, The dimensions are such that the length l ₃ is obtained. Therefore, the length of the groove provided in the tuning fork arms 20 and 26 is given by (l ₁ −l ₃ ), and in order to obtain a vibrator having a small R ₁ , (l ₁ −l ₃ ) / (l− l ₂ ) has a value of 0.4 to 0.8. Further, the overall length l of the tuning fork-shaped bent quartz crystal resonator 10 is determined from the required frequency, the size of the storage container, and the like. At the same time, in order to obtain a good tuning-fork-shaped bent quartz crystal resonator that vibrates in the fundamental wave mode, there is a close relationship between the groove length l ₁ and the total length l.

That is, the ratio (l ₁ / l) between the tuning fork arms 20 and 26 or the tuning fork arms 20 and 26 and the length l _{1 of the} groove provided in the tuning fork base 40 and the total length l of the tuning fork-shaped bent crystal resonator is 0. The length of the groove is provided to be 2 to 0.78. The reason for forming in this way is that it is possible to suppress harmonic mode vibrations, particularly secondary and third harmonic mode vibrations, which are unwanted vibrations, and to improve the frequency stability of fundamental wave mode vibrations. Therefore, a good tuning fork-shaped bent quartz crystal that easily vibrates in the fundamental wave mode can be realized. If More specifically, the equivalent series resistance R ₁ of the bending quartz oscillator tuning fork vibrating at the fundamental mode is smaller than the equivalent series resistance R _n of the harmonic mode vibration. That is, R ₁ <R _n (equivalent series resistance of the second and third harmonic mode vibration when n = 2, 3), and the amplifier (CMOS inverter), the capacitor, the resistance element, and the tuning fork shape of the present embodiment. In a crystal oscillator composed of a bent crystal resonator or the like, a good crystal oscillator in which the resonator easily vibrates in the fundamental wave mode can be realized. Further, the groove length l ₁ may be divided in the length direction of the tuning fork arm, and at least one of them may satisfy the side ratio (l ₁ / l) or may be divided. It is sufficient that the length of the added groove in the length direction of the groove satisfies the side ratio (l ₁ / l).

Further, in this embodiment, the tuning fork base 40 is the entire lower part of the length l ₂ of the vibrator 10 in FIG. 6, and the tuning fork arm 20 and the tuning fork arm 26 are the same as those of the vibrator 10 in FIG. there is a whole upper portion from the portion of the length l _2. In this embodiment, the tuning fork fork has a rectangular shape. However, the present invention is not limited to the shape described above, and the tuning fork fork may have a U-shape. In this case, as in the rectangular shape, the dimensional relationship between the tuning fork arm and the tuning fork base is the same as that described above. Further, in this embodiment, the groove is provided in the tuning fork arm and the tuning fork base, but the present invention is not limited to this, and the groove may be provided only in the tuning fork arm, and the same effect can be obtained. . In this case, the groove length l ₃ = 0. Further, the length 1 ₁ of the groove in the present invention, when the grooves only in the tuning fork arms are provided, the ratio of the groove width W ₂ and the tuning fork arm width W (W 2 _{/ W)} is than 0.35 The length of the groove formed to be larger and smaller than 1. Further, when the groove provided in the tuning fork arm extends to the tuning fork base, and a groove is further provided between the grooves extending to the tuning fork base, the length including the groove length l ₃ is set. l ₁ . However, when the tuning fork arm groove extends to the tuning fork base, but no further groove is provided between the grooves, the length l ₁ is the length of the tuning fork arm groove.

In other words, at least one groove is provided in the length direction on the upper and lower surfaces of the tuning fork arm that includes the neutral line, ie, the tuning fork arm including the neutral line, and electrodes are formed on both sides of the groove. Are arranged such that the electrode on the side surface of the groove and the electrode on the side surface of the tuning fork arm that opposes the electrode are different from each other, and at least one of each of the electrodes is provided so that the moment of inertia generated in the tuning fork arm increases. The ratio (W ₂ / W) of the groove width W ₂ of at least one of the grooves to the tuning fork arm width W is larger than 0.35 and smaller than 1, and the thickness t _{1 of the} groove and the thickness of the tuning fork arm The groove is formed so that the ratio (t ₁ / t) to t is smaller than 0.79.

するように構成され、間隔Ｗ_４は０．０５ｍｍ〜０．３５ｍｍで、溝幅Ｗ_２は０．０３ｍｍ〜０．１２ｍｍの値を有する。このように構成する理由は超小型の屈曲水晶振動子で、かつ、音叉形状と音叉腕の溝とをフオトリソグラフィ技術を用いて別々（別々の工程）に形成でき、更に、基本波モード振動の周波数安定性が高調波モード振動の周波数安定性より高くすることができる。この場合、厚みｔは通常０．０５ｍｍ〜０．１２ｍｍの水晶ウエハが用いられる。しかし、本発明は本実施例に限定されるものでなく、０．１２ｍｍより厚い水晶ウエハを使用してもよい。

Configured to, spacing _{W 4} is 0.05 mm to 0.35 mm, the groove width _{W 2} has a value of 0.03Mm～0.12Mm. The reason for this configuration is an ultra-compact bent quartz crystal resonator, and the tuning fork shape and the tuning fork arm groove can be formed separately (separate steps) using photolithography technology. The frequency stability can be made higher than the frequency stability of the harmonic mode vibration. In this case, a quartz wafer having a thickness t of usually 0.05 mm to 0.12 mm is used. However, the present invention is not limited to this embodiment, and a quartz wafer thicker than 0.12 mm may be used.

More specifically, the Figer of Merit M _i representing the inductivity, electromechanical conversion efficiency, and quality factor of the bent quartz resonator is the ratio of the quality factor Q _i value to the capacity ratio r _i (Q _i / r _i ). Defined by (fundamental vibration when i = 1, second harmonic vibration when i = 2, third harmonic vibration when i = 3), and mechanical series resonance independent of the parallel capacitance of the bent quartz crystal frequency difference Delta] f of the series resonance frequency f _r which depends on the parallel capacitance and the frequency f _s is inversely proportional to the off Iga of merit M _i, Delta] f becomes smaller as the value M _i is large. Therefore, as M _i is large, the resonance frequency of the bending crystal oscillator does not influenced by the parallel capacitance, the frequency stability of a flexural quartz crystal resonator is improved. That is, a tuning fork-shaped bent quartz crystal with high time accuracy can be obtained.

Specifically, due to the configuration of the tuning fork shape, groove, electrode, and dimensions thereof, the fibre-of-merit M ₁ of the fundamental mode vibration is larger than the fibre-of-merit M _n of the harmonic mode vibration. That is, M ₁ > M _n . However, n represents the vibration order of the harmonic mode vibration, and when n = 2 and 3, it is the fibre of merit of the second and third harmonic mode vibration. As an example, the frequency of the fundamental mode vibration is 32.768 kHz, W ₂ /W=0.5, t ₁ /t=0.34. When l ₁ /l=0.48, variations due to manufacturing occur, but M ₁ and M ₂ of the tuning-fork-shaped bent quartz crystal resonator are M ₁ > 65 and M ₂ <30, respectively. That is, (a small equivalent series resistance R ₁₎ Good high inductive electromechanical conversion efficiency, can be obtained flexural quartz oscillator that vibrates at a large fundamental mode of the quality factor. As a result, the frequency stability of the fundamental wave mode vibration becomes better than the frequency stability of the second harmonic mode vibration, and the second harmonic mode vibration can be suppressed. Therefore, the crystal oscillator composed of the bent crystal resonator of this embodiment can obtain the frequency of the fundamental mode vibration as an output signal and has high frequency stability (excellent time accuracy). Further, the reference frequency of the fundamental wave mode vibration of the present invention is 10 kHz to 200 kHz. In particular, 32.768 kHz is widely used.

FIG. 7 is a top view of a tuning-fork-shaped crystal resonator 45 that vibrates in a bending mode used in the crystal oscillator according to the second embodiment constituting the electronic apparatus of the present invention. The tuning fork-shaped bent quartz crystal unit 45 includes tuning fork arms 46 and 47 and a tuning fork base 48. That is, one end of the tuning fork arms 46 and 47 is connected to the tuning fork base 48. In this embodiment, the tuning fork base 48 is provided with notches 53 and 54. Further, the tuning fork arms 46 and 47 are provided with grooves 49 and 50 with (including) the neutral lines 51 and 52, respectively. Further, the grooves 49 and 50 in this embodiment is provided in a part of the tuning fork arms 46 and 47, the grooves 49 and 50 each have a width _{W 2} and length _{l 1.} More specifically, the groove area S = W ₂ × ₁₁ is shown, and S is configured to have a value of 0.025 to 0.12 mm ² . The reason for configuring the groove area in this way is that it is easy to form a groove by a chemical etching method, and it is possible to form a groove with improved electromechanical conversion efficiency. At the same time, a tuning fork-shaped crystal resonator that vibrates in a bending mode having a high quality factor Q value of fundamental mode vibration can be obtained. As a result, it is possible to realize a crystal oscillator whose output signal has a frequency of fundamental mode vibration.

In the groove area S, the groove and the tuning fork arm can be processed in separate steps. However, in processing the tuning fork arms and grooves provided in it at the same time, should there be an interval W ₄ and the area S of the thickness t and groove width W ₂ and the tuning fork arm of the tuning fork arms to the optimum dimensions. In other words, the tuning fork arms of thickness t when 0.06Mm～0.15Mm, within the groove width _{W 2} is 0.02Mm～0.068Mm, further area S of 0.023mm ² ~0.088mm ² in the range, the interval _{W 4} is configured to be 0.05 mm to 0.35 mm. The reason for such a configuration is that the crystallinity of quartz is used, and from the crystallinity, a groove (including a groove divided in the length direction of the tuning fork arm) and a tuning fork shape can be formed simultaneously. Although not shown in FIG. 7, grooves are also provided on the lower surfaces of the tuning fork arms 46 and 47 at positions facing the grooves 49 and 50.

た、切り欠き部５３、５４も振動子の固定による振動部のエネルギー損失を小さくすることができる。図７で示されている音叉腕の腕幅Ｗ、部分幅Ｗ_１、Ｗ_３、溝幅Ｗ_２と間隔Ｗ_４及び溝の長さｌ_１と音叉振動子の全長ｌとの関係は図６で述べられているので、ここでは省略する。Furthermore, the width of the tuning fork portion of the cutout portions 53 and 54 provided in the fork base 48 is given by W _5, the dimensions of the end of the cutout portions 53 and 54 is given by W _6. And when it is fixed to the surface mount type case or cylindrical case by solder or adhesive on the end side of the tuning fork base 48

The notches 53 and 54 can also reduce the energy loss of the vibration part due to the fixation of the vibrator. The relationship between the arm width W, the partial widths W ₁ and W ₃ , the groove width W ₂ , the gap W _{4, the} groove length ₁₁ and the overall length l of the tuning fork vibrator shown in FIG. Is omitted here.

  FIG. 8 is a top view (a) and a side view (b) of a width-longitudinal mode crystal resonator used in the crystal oscillator of the third embodiment constituting the electronic apparatus of the present invention. The width-longitudinal mode crystal resonator 62 includes support portions 67 and 80 including a vibration portion 63, connection portions 66 and 69, and mount portions 68 and 81, respectively. Furthermore, the support part 67 and the support part 80 are provided with a hole 67a and a hole 80a, respectively. More specifically, the first connecting portion 66 and the second connecting portion 69 are provided at the end portion of the vibrating portion 63 positioned opposite to the length direction. That is, one first support part 67 is connected to the vibration part 63 via the first connection part 66, and the other second support part 80 is connected to the vibration part 63 via the second connection part 69. Yes. Moreover, the electrode 64 and the electrode 65 are arrange | positioned facing the upper surface and lower surface of the vibration part 63, and these electrodes are comprised so that it may become a different polarity. That is, a pair of electrodes are arranged. Further, the electrode 64 is disposed so as to extend to the second mount portion 81 through one second connection portion 69. Further, the electrode 65 is arranged to extend to the first mount portion 68 through the other first connection portion 66. In the present embodiment, the electrode 64 and the electrode 65 arranged in the vibrating part 63 extend in different directions and are arranged up to the mount part. However, even if arranged so as to extend in the same direction, as a vibrator The same characteristics are obtained. In the vibrator of this embodiment, the mount parts 68 and 81 are fixed to the case or lid fixing part of the unit by an adhesive or solder.

Next, the relationship between the cut angle of the width-longitudinal mode crystal resonator and its coordinate system will be described. When the coordinate system is an origin O, an electric axis x, a mechanical axis y, and an optical axis z, it constitutes O-xyz. First, consider a quartz plate perpendicular to the x-axis, so-called X-plate quartz. At this time, the width W ₀ , the length L ₀ , and the thickness T ₀ , which are the dimensions of the X-plate quartz, respectively coincide with the y-axis, z-axis, and x-axis directions. Further, this X-plate crystal is rotated around the x-axis by an angle θ _x = −25 ° to + 25 °, and further rotated around a new y-axis y′-axis by an angle θ _y = −30 ° to + 30 °. The At this time, the new axis of the x-axis is rotated about the x′-axis and the z-axis is rotated about the two axes, so that the new axis is z ″. The width longitudinal mode crystal resonator of this embodiment is the above-described rotating crystal. In addition, the definition of the electric axis + x axis in this embodiment is in accordance with JIS standard, and the counterclockwise rotation angle is positive (plus), and the vertex temperature of the vibrator is set around room temperature. Angle θ _x is θ _x = −12 ° to −13.5 °, −18.5 ° to −19.8 °, or angles θ _x and θ _y are θ _x = −13 ° to − 18 °, θ _y = + / − (0.5 ° to 30 °) In this example, the X-plate quartz is first rotated at an angle θ _x = −25 ° to + 25 ° around the x axis. Next, the angle θ _y is rotated about −30 ° to + 30 ° around the y ′ axis, but first, the angle θ _{x is} rotated about −25 ° to + 25 ° around the x axis, and then , The new axis z 'about the angle _{θ z = -15 ° ~ + 15} ° rotated may be. This embodiment of the shaft axis, has been described cut angle of the quartz plate used for forming the width longitudinal mode crystal oscillator The cut angle of the vibrator of the present invention is not limited to this, and the formed width-longitudinal mode crystal vibrator may be a vibrator having the angle described above, and the present invention includes those vibrators. For example, in-plane rotation is performed with a mask or the like used for forming a vibrator without rotating the quartz plate in-plane.

More specifically, the thickness direction of the width-longitudinal mode crystal unit is aligned with the electric axis x-axis direction, the width direction is matched with the mechanical axis y-axis direction, and the length direction is matched with the optical axis z-axis direction. the longitudinal mode quartz crystal resonator first be angle theta _x as a rotation axis in the thickness direction axis (x-axis), then, as a rotation axis in the width direction of the axis (new axis y 'axis of the rotated y-axis) The angle θ _{y is} rotated, or the width-longitudinal mode crystal resonator is first rotated by an angle θ _x with the axis in the thickness direction (x axis) as the rotation axis, and then the axis in the length direction (optical axis z axis) The new axis z′-axis) after rotation is rotated by an angle θ _z , and the angles θ _x , θ _y and θ _z are θ _x = −25 ° to + 25 ° and θ _y = −30 ° to +30, respectively. The width-longitudinal mode crystal resonator is formed so as to have °, θ _z = −15 ° to + 15 °. By combining these cut angles, the vertex temperature can be set over a wide temperature range.

Furthermore, the vibrating portion 63 has a width _{W 0,} has a length dimension _{L 0,} and the thickness _{T 0,} the width _{W 0,} length _{L 0,} and the thickness _{T 0} respectively y 'axis, z "axis, and x That is, the electrode 64 and the electrode 65 are disposed on the upper surface and the lower surface of the vibrating portion 63 that are perpendicular to the x ′ axis, and the electrode 65 opposed to the electrode 64 is different. Furthermore, the length L ₀ of the vibration part 63 is designed to be larger than the width W ₀ and the thickness T ₀ is smaller than the width W _0. That is, the width longitudinal mode vibration and In order to obtain a width longitudinal mode crystal resonator having a small equivalent series resistance R ₁ by making the coupling with the length longitudinal mode vibration negligibly small and increasing the electrode area of the vibration part, the width W ₀ the ratio _W 0 / _{L 0} length _{L 0} is smaller than 0.8, and, by increasing the electric field _{E x,} equivalent series To obtain a small width longitudinal crystal oscillator of anti R _1, the ratio T _{0 /} W ₀ of the thickness T ₀ and width W ₀ is required to be smaller than 0.85. Actual these dimensions The determination depends on the characteristics required for the width-longitudinal mode crystal resonator, and the thickness T ₀ is usually set to 250 μm or less.

More specifically, the resonance frequency of the width-longitudinal mode crystal resonator is inversely proportional to the width dimension W ₀ and hardly depends on other dimensions (length, thickness, connection portion and support portion). Therefore, by reducing the width W ₀ , the size can be reduced and the frequency can be increased. In addition, a width-longitudinal mode crystal resonator that vibrates in a single vibration mode without unnecessary vibration can be obtained from the above-described dimensional relationship. At the same time, by arranging the electrodes in the vibrating portion so that an electric field is applied in the thickness direction, the vibration orders of the fundamental wave mode vibration and the overton mode vibration of the width-longitudinal mode crystal resonator do not depend on the piezoelectric constant. That is, the vibration part and the electrode disposed thereon are configured so that the vibration order of the fundamental wave mode vibration and the overton mode vibration does not depend on the piezoelectric constant. Therefore, since the resonance frequency of the width-longitudinal mode crystal resonator of the present invention does not depend on the piezoelectric constant, it has a remarkable effect that the design of the resonator becomes very easy.

Next, a description will be given values of the piezoelectric constants e ₁₂ required to drive the width longitudinal mode crystal oscillator of the present embodiment. As the value of the piezoelectric constant e ₁₂ is large, the electromechanical conversion efficiency is high. The absolute value of piezoelectric constant _{e 12} of width longitudinal mode crystal oscillator of this embodiment has a 0.095~0.18C / ^{m 2.} That is, since the width longitudinal mode quartz crystal resonator of this embodiment has a high electromechanical conversion efficiency, a small equivalent series resistance R _1, high quality factor Q value, moreover, to obtain a wide longitudinal mode quartz resonator miniature be able to.

Now, when an alternating voltage is applied between the electrode 64 and the electrode 65 of FIG. 8, the electric field E _x is acting alternately in the thickness direction as shown by the solid line and dotted arrows in the side view of FIG. 8 (b). As a result, the vibration part 63 vibrates to expand and contract in the width direction. That is, it is possible to obtain a so-called lateral effect type width longitudinal mode crystal resonator that vibrates in a direction perpendicular to the electric field direction. The resonance frequency of the main (longitudinal width) vibration is a vibrator that does not depend on the piezoelectric constant. Further, the width-longitudinal mode crystal resonator of the present embodiment is a resonator different from the KT-cut width-mode crystal resonator that vibrates in parallel with the electric field direction. At the same time, the KT cut quartz crystal resonator is a so-called longitudinal effect type resonator whose vibration order depends on the piezoelectric constant. That is, the resonator whose resonance frequency depends on the piezoelectric constant. In this embodiment, the width-longitudinal mode crystal resonator is described. However, instead of this resonator, a thickness-slip mode crystal resonator whose frequency depends on the thickness of the resonator may be used in the electronic apparatus of the present invention.

  FIG. 9 is a cross-sectional view of a crystal unit used in the crystal oscillator of the fourth embodiment constituting the electronic apparatus of the present invention. The crystal unit 170 includes a tuning fork-shaped bent crystal resonator 70, a case 71, and a lid 72. More specifically, the vibrator 70 is fixed to a fixing portion 74 provided on the case 71 with a conductive adhesive 76 or solder. The case 71 and the lid 72 are joined via a joining member 73. In the present embodiment, the vibrator 70 is the same vibrator as one of the tuning-fork-shaped crystal vibrators 10 and 45 that vibrate in the bending mode described in detail in FIGS. In the crystal oscillator of this embodiment, the circuit element is connected to the outside of the crystal unit. That is, only a tuning fork-shaped bent quartz crystal is housed in the unit. At this time, the bent crystal resonator is housed in a vacuum unit. Further, the width-longitudinal mode crystal resonator and the thickness-shear mode crystal resonator described in FIG. 8 are similarly housed in the surface-mount type crystal unit of this embodiment. Usually, the width-longitudinal mode crystal resonator is fixed to the fixed portion at both ends, and the thickness-slip mode crystal resonator is fixed to one end portion.

  Further, the case member is made of ceramics or glass, the lid member is made of metal or glass, and the joining member is made of metal or low-melting glass. Further, the relationship between the vibrator, the case, and the lid described in this embodiment is also applied to the crystal oscillator of FIG. 10 described below.

  FIG. 10 is a sectional view of a crystal oscillator according to a fifth embodiment constituting the electronic apparatus of the present invention. The crystal oscillator 190 includes a crystal oscillation circuit, a case 91, and a lid 92. In this embodiment, the crystal oscillation circuit is housed in a crystal unit composed of a case 91 and a lid 92. The crystal oscillation circuit includes a tuning fork-shaped bent crystal resonator 90, an amplifier 98 including a feedback resistor, a capacitor (not shown), and a drain resistor (not shown). The amplifier 98 is formed by a CMOS inverter. Used.

  Further, in this embodiment, the vibrator 90 is fixed to a fixing portion 94 provided in the case 91 by an adhesive 96 or solder. On the other hand, the amplifier 98 is fixed to the case 91. Further, the case 91 and the lid 92 are joined via a joining member 93. The vibrator 90 of the present embodiment is either the tuning-fork-shaped bent quartz crystal 10 or 45 described in detail in FIGS. 4 and 7, or the width-longitudinal mode crystal resonator 62 or the thickness-sheared crystal described in FIG. The vibrator in the vibrator is used.

  Next, a method for manufacturing a crystal oscillator used in the electronic apparatus of the present invention will be described. The tuning fork-shaped bent quartz crystal resonator is formed by a photolithography method using a semiconductor technique and a chemical etching method. First, metal films (for example, chromium and gold thereon) are formed on the upper and lower surfaces of a polished or polished quartz crystal wafer by sputtering or vapor deposition. Next, a resist is applied on the metal film. Then, after the resist and the metal film are removed while leaving the tuning fork shape by a photolitho process, a tuning fork shape including a tuning fork arm and a tuning fork base is formed by a chemical etching method. When forming this tuning fork shape, a notch may be formed in the tuning fork base. Further, the metal film and resist shown in the above process are applied on the tuning fork-shaped surface, and grooves are formed in the tuning fork arm or the tuning fork arm and the tuning fork base by a photolitho process and a chemical etching method.

  Next, a metal film and a resist are again applied to the tuning fork shape having a groove, and an electrode is formed by a photolitho process. That is, the electrode on the side surface of the tuning fork arm and the electrode on the side surface of the groove are arranged to oppose each other so as to have different polarities. More specifically, the side electrode of the first tuning fork arm and the electrode of the groove of the second tuning fork arm have the same polarity, and the electrode of the groove of the first tuning fork arm and the side electrode of the second tuning fork arm have the same polarity. The electrode of the groove | channel of a 1st tuning fork arm and a side electrode are comprised so that polarity may differ. That is. Two electrode terminals are formed on the vibrator. As a result, by applying an alternating voltage to the two electrode terminals, the tuning fork arm bends and vibrates in reverse phase. In this embodiment, the groove is formed in the tuning fork arm or the tuning fork arm and the tuning fork base after the tuning fork shape is formed. However, the present invention is not limited to the above embodiment, and the groove is first formed. A tuning fork shape may be formed. Or you may form a tuning fork shape and a groove | channel simultaneously.

  By the process of this embodiment, a large number of tuning fork-shaped bent quartz resonators are formed on the quartz wafer. Therefore, in the next step, the initial frequency adjustment is performed by laser or plasma etching or vapor deposition in this wafer state. At the same time, the defective vibrator is marked or removed from the wafer. In this step, the frequency is adjusted so that the frequency deviation is within the range of −9000 PPM to +5000 PPM with respect to the reference frequency of 10 kHz to 200 kHz. Further, in the next step, the formed vibrator is fixed to a lead wire of a surface mount type case, a lid or a cylindrical case with an adhesive or solder. After the fixing, the second frequency adjustment is performed by laser, plasma etching or vapor deposition. In this step, the frequency is adjusted so that the frequency deviation is within the range of −100 PPM to +100 PPM. The fact that the frequency adjustment is performed after fixing in the present invention may be performed immediately after fixing, or may be performed after connecting the case and the lid after fixing. That is, whatever process is performed after fixing, the frequency may be adjusted after that, and the present invention encompasses all of these. The frequency adjustment after the case and the lid are connected is performed with a laser through glass.

  When the third frequency adjustment is performed, the frequency adjustment is performed so that the frequency deviation due to the second frequency adjustment is in the range of −950 PPM to +950 PPM. In the above embodiment, the first frequency adjustment is performed in the state of the wafer, and at the same time, the defective vibrator is marked or removed from the wafer. However, the present invention is not limited to this. The present invention may include a step of inspecting a large number of tuning-fork-shaped bent quartz crystal resonators formed on a quartz wafer in the state of the wafer and inspecting whether the resonator is a good resonator or a defective resonator. That is, the defective vibrator is marked, removed from the wafer, or stored in a computer. By including such a process, a defective vibrator can be found quickly, and since it does not flow to the next process, the yield can be increased. As a result, an inexpensive bent quartz resonator can be obtained.

  Furthermore, after adjusting the frequency, the vibrator is housed in a unit serving as a case and a lid in a vacuum to obtain a crystal unit. When the lid is made of glass, the third frequency adjustment is performed with a laser after storage. In this step, the frequency is adjusted so that the frequency deviation is within the range of −50 PPM to +50 PPM. In this embodiment, the frequency adjustment is performed in three separate steps, but may be performed in at least two separate steps. For example, the frequency adjustment in the third process may not be performed. Further, in the next step, the two electrode terminals of the vibrator are electrically connected to the amplifier, the capacitor, and the resistance element. In other words, the amplifier circuit is composed of a CMOS inverter and a feedback resistor element, and the feedback circuit is connected to be composed of a tuning fork-shaped bent crystal resonator, a drain resistor element, a gate-side capacitor, and a drain-side capacitor. The third frequency adjustment may be performed after the crystal oscillation circuit is configured.

  Although the present invention has been described based on the illustrated examples, the present invention is not limited to the above-described example. In the above-described embodiment, the tuning fork arm is composed of two, but the present invention has three or more tuning fork arms. Is included. In this case, the electrodes may be configured so that at least two tuning fork arms vibrate in opposite phases.

Further, in this embodiment, the groove is provided on the tuning fork arm so as to sandwich (include) the neutral line, but the present invention is not limited to this, and the groove is formed on both sides of the neutral line. It may be formed. In this case, partial width W ₇ including the neutral line of the tuning fork arms are configured to be less than 0.05 mm. Further, the width of each groove is configured to be smaller than 0.04 mm, and the ratio of the thickness t _{1 of} the groove to the thickness t of the tuning fork arm is configured to be 0.79 or less. With such a configuration, M ₁ can be made larger than M _n .

  Further, the shape of the tuning fork, the groove, and the width longitudinal mode crystal resonator of the bent crystal resonator of this embodiment are processed using at least one of chemical, physical and mechanical methods. In the physical method, for example, ionized atoms and molecules are scattered and processed. In the mechanical method, for example, particles for blasting are scattered and processed. Therefore, in the present invention, the processing method by the physical method and the mechanical method is called processing by the particle method.

As described above, it has already been described that many effects can be obtained by providing the electronic device of the present invention. Among them, the following remarkable effects can be obtained.
(1) using at least the one of the crystal oscillator tuning fork flexural crystal oscillator, full Iga of merit M ₁ of the fundamental mode vibration comprises a full Iga of merit M _n greater than oscillator harmonic mode vibration The crystal oscillator is configured, and the ratio of the absolute value | −RL ₁ | of the negative resistance of the fundamental mode vibration of the amplifier circuit to the equivalent series resistance R ₁ of the fundamental mode vibration is negative of the harmonic mode vibration of the amplifier circuit. Since the crystal oscillator is configured to be larger than the ratio of the absolute value | -RL _n | of the resistive resistor and the equivalent series resistance R _n of the harmonic mode vibration, the output signal of the crystal oscillator is at the frequency of the fundamental mode vibration. And has high frequency stability. As a result, a highly accurate electronic device using the output signal can be realized.
(2) Since a width-longitudinal mode crystal resonator or a thickness-slip mode crystal resonator is used for at least one crystal oscillator, a small and highly accurate output signal can be obtained, and an electronic device can be operated by this output signal. Therefore, an electronic device having high reliability can be realized.

  Since the crystal oscillator of the present invention is ultra-compact and has high frequency stability, it can be applied to electronic devices that particularly require high reliability.

  1 is an example of a block diagram of a facsimile in one embodiment of an electronic device of the present invention.   It is one Example of the crystal oscillation circuit diagram which comprises the crystal oscillator used for the electronic device of this invention.   The feedback circuit diagram of FIG. 2 is shown.   FIG. 2 shows an external view of a tuning-fork-shaped bent crystal resonator used in the crystal oscillator of the first embodiment constituting the electronic apparatus of the present invention and its coordinate system.   FIG. 6 shows a DD ′ cross-sectional view of a tuning fork base of the tuning fork-shaped bent crystal resonator of FIG. 4.   FIG. 5 shows a top view of the tuning fork-shaped bent quartz crystal resonator of FIG. 4.   FIG. 6 is a top view of a tuning-fork-shaped crystal resonator that vibrates in a bending mode used in a crystal oscillator according to a second embodiment that constitutes the electronic apparatus of the present invention.   It is the top view (a) and side view (b) of the width-longitudinal mode crystal resonator used for the crystal oscillator of 3rd Example which comprises the electronic device of this invention.   It is sectional drawing of the crystal unit used for the crystal oscillator of 4th Example which comprises the electronic device of this invention.   It is sectional drawing of the crystal oscillator of 5th Example which comprises the electronic device of this invention.   A perspective view and a coordinate system of a tuning fork-shaped bent quartz resonator used in a quartz oscillator constituting a conventional electronic device are shown.   FIG. 12 is a cross-sectional view of a tuning fork arm of the tuning fork-shaped crystal resonator of FIG. 11.

Explanation of symbols

1, 9 Amplifier circuit, feedback circuit V ₁ , V ₂ input voltage, output voltage W ₂ , t ₁ groove width, groove thickness W, W ₄ tuning fork arm width, tuning fork arm spacing W ₁ , W ₃ tuning fork arm Partial width l ₁ , l ₂ , l Groove length, tuning fork base length, total length of tuning fork-shaped bent quartz resonator t tuning fork arm or tuning fork arm and tuning fork base thickness

Claims (2)

In the production method of the crystal unit configured to include a crystal oscillator and the case and the lid, before Symbol crystal oscillator is provided with at least first tuning fork arms and the second tuning fork arms connected to the fork base and its fork base And a tuning fork-type bending crystal resonator comprising a two-electrode terminal having a first electrode terminal and a second electrode terminal having a second electrode terminal having a different electrical polarity from the first electrode terminal,
The tuning fork type quartz crystal resonator has a fundamental mode vibration and a second harmonic mode vibration.
The tuning fork shape, groove and electrode dimensions are such that the Fibber of merit M (1) of the fundamental mode vibration is larger than the Fibber of merit M (2) of the second harmonic mode vibration. A step of determining
Forming a tuning fork shape comprising the tuning fork base, the first tuning fork arm and the second tuning fork arm;
Forming grooves in each of the upper and lower surfaces of each tuning fork arm of the first tuning fork arm and the second tuning fork arm ;
In order to form the first electrode terminal of the second electrode terminal, and the electrode before Symbol groove electrode and the second fork arm of the side surface of the first tuning fork arm to place the electrodes so that the same poles Process,
In order to form the second electrode terminal of the second electrode terminal, the step of the electrode side of the groove electrode and the second tuning fork arms of said first fork arm to place the electrodes so that the same poles When,
And fixing a conductive adhesive to a fixed portion of the casing for housing the tuning fork type flexural quartz crystal resonator configured with the second electrode terminal,
To configure a crystal unit with said lid and said and said tuning-fork flexural crystal oscillator case, the production method of the crystal unit shall be the; and a step of connecting the cover to the case. The Te claim 1 smell, the groove formed in each of the upper and lower surfaces of the tuning fork arms of said second tuning fork arms and the first tuning fork arms of the tuning fork type flexural quartz crystal resonator, the first tuning fork arms It is formed on both sides of the upper and lower surfaces of each of the neutral line of the tuning fork arms of the second tuning fork arms, partial width, including the neutral line of the crystal unit you characterized by being smaller than 0.05mm Manufacturing method .

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