JP7071772B2 - How to adjust the frequency of the crystal device - Google Patents

Description

The present invention relates to a frequency adjusting method for a quartz device provided with an adjusting region capable of finely adjusting the frequency.

For quartz devices, the dimensions and excitation electrode patterns of each part are set at the time of design so that the target oscillation frequency can be obtained. However, even if the product is manufactured based on such a design value, the frequency may be adjusted at the final stage of the manufacturing because the target value may be deviated depending on the manufacturing conditions and the surrounding environment.

The oscillation frequency of the tuning fork type crystal device is adjusted by changing the weight of the tip of the vibrating arm (Patent Documents 1 and 2). Such adjustment methods include a method of adjusting in a direction of lowering the frequency while gradually increasing the weight by depositing a metal film on the tip of the vibrating arm, and a method of scraping off the tip of the vibrating arm with a laser beam or an ion beam. There is a method of adjusting in the direction of increasing the frequency while making it lighter. Particularly in a small crystal device, an adjustment method using a laser beam is widely used because the accuracy of the adjustment position can be easily obtained.

In many crystal devices, a crystal vibration element is mounted on a ceramic package with a lead electrode that connects from an external terminal to the inside of the cavity with a conductive adhesive, and then the final frequency adjustment is performed using a laser beam or ion beam. After that, it is completed by vacuum sealing with a lid such as a metal lid.

As described in Patent Document 3, the method of adjusting the frequency before vacuum-sealing the crystal vibrating element with the lid is described as follows, after the crystal vibrating element is vacuum-sealed, the lid or the like. A method of performing final frequency adjustment by irradiating a laser beam from the outside of the is known.

Japanese Patent Application Laid-Open No. 2003-332871 Japanese Patent Application Laid-Open No. 2003-332872 Japanese Unexamined Patent Publication No. 2011-082736

Oscillation variations before frequency adjustment of a crystal device are often caused by dimensional deviations in the shape processing of crystal vibration pieces. This is because, as the size is reduced, the influence of the dimensional deviation becomes relatively large, and as a result, the frequency variation becomes large. Since the frequency adjustment amount tends to be larger as the size is smaller, the frequency adjustment in the initial stage is often performed by beam irradiation such as a laser.

In the conventional manufacturing process of a quartz device, frequency adjustment is performed by irradiating a predetermined position of a quartz vibrating element housed in a package such as ceramic with a laser beam or an ion beam in a high vacuum sealing device. .. After that, a metal lid is placed on the package via a brazing material or the like, and the brazing material is melted by an electron beam to vacuum-seal the quartz device.

However, in the above method, the frequency adjusted in vacuum may fluctuate due to the influence of heat, gas, etc. generated in the subsequent sealing step. Therefore, even if frequency offset is performed, the frequency value will differ between before and after sealing due to individual differences in the crystal vibrating element and changes in the external environment during sealing. .. As a result, there has been a problem that the final frequency value of the quartz device varies and the product yield is lowered.

In this regard, as disclosed in Patent Document 3, in the method of irradiating the laser beam from the outside of the lid in which the crystal vibrating element is sealed, adjustment is performed for the crystal device as the final product. Therefore, it is possible to suppress the final variation. However, since the sealed crystal vibration element cannot be visually recognized from the outside, it is necessary to accurately detect the position where the laser beam is irradiated by infrared rays or the like, and there is a problem that control and a process for that purpose are required. Further, in Patent Document 3, since the lid side is the irradiation surface of the laser beam and the package side is the external electrode surface to which the probe for measurement is applied, it is complicated to adjust the frequency while irradiating the laser beam.

Therefore, an object of the present invention is to enable the formation of frequency fine adjustment marks in at least the second region of a mass-adjusting metal film having a first region shielded by an external electrode and a second region not shielded. By doing so, it is possible to finely adjust the frequency without causing insulation failure or the like, and it is an object of the present invention to provide a frequency adjustment method for a crystal device capable of obtaining a good yield.

In order to solve the above problems, in the frequency adjusting method of the crystal device of the present invention, a plurality of crystal vibrating pieces are formed on the vibrating piece wafer, and a mass adjusting metal film provided on the first plane of each crystal vibrating piece is formed. The step of irradiating a beam to roughly adjust the frequency and the vibrating piece wafer in which each crystal vibrating piece is roughly adjusted is sandwiched between a pair of case wafers from both sides, and each crystal vibrating piece is hermetically sealed in the case. A step of forming an external electrode electrically connected to each of the crystal vibrating pieces on the outer surface of the case wafer facing the first plane of each of the crystal vibrating pieces for each case. A step of attaching a dicing tape to the outer surface of the other case wafer different from the one case wafer on which the external electrode is formed among the pair of case wafers, and dicing the pair of case wafers for each case. From the outer surface side of each of the diced cases , the coarsely adjusted mass-adjusted metal film is irradiated with a beam while the dicing tape is still attached to the outer surface of the case wafer. It includes a step of finely adjusting the frequency.

According to the frequency adjustment method of the crystal device of the present invention, the frequency fine adjustment mark is at least in the second region with respect to the mass adjusting metal film having the first region shielded by the external electrode and the second region not shielded. By making it possible to form the frequency, it is possible to finely adjust the frequency without causing insulation defects and the like, and a good yield can be obtained.

According to the frequency adjustment method of the crystal device of the present invention, after the step of performing rough adjustment on the vibrating piece wafer before being sealed by the case wafer, fine adjustment is made on the vibrating piece wafer sealed by the case wafer. Has a process of performing. As a result, since the vibrating piece wafer is not affected when it is sealed, the final frequency can be finely adjusted precisely.

It is a perspective view (b) of the crystal device (a) of a two-terminal structure of this invention, and the crystal device of a four-terminal structure. It is a plan view and the sectional view (c) of AA of the crystal device (a) of a two-terminal structure, and the crystal device (b) of a four-terminal structure. It is a top view which shows the coarse adjustment region and the fine adjustment region in each of the crystal device (a) of a two-terminal structure and the crystal device (b) of a four-terminal structure. It is a top view which shows the formation position of the frequency fine adjustment mark in each of the crystal device (a) of a 2-terminal structure and the crystal device (b) of a 4-terminal structure. The conceptual diagram (a) showing the scattering state of the mass-adjusting metal film when the frequency fine adjustment mark is provided at the predetermined position specified in the present invention, and the case where the frequency fine adjustment mark is provided at a position deviating from the predetermined position. It is a conceptual diagram (b) which shows the scattering state of a mass-adjusting metal film. Cross-sectional view of beam irradiation of a crystal device in which the mass-adjusting metal film is formed only on the first plane (a) and cross-section of beam irradiation of a crystal device in which the mass-adjusting metal film is formed on both the first plane and the second plane. It is a figure (b). It is a top view of the collective wafer which has a plurality of crystal devices of a two-terminal structure in which a frequency fine adjustment is performed with a dicing tape attached. It is a top view of the collective wafer which has a plurality of crystal devices of a 4-terminal structure in which a frequency fine adjustment is performed with a dicing tape attached. It is explanatory drawing which shows the frequency fine adjustment method in each of the crystal device (a) of a 2-terminal structure and the crystal device (b) of a 4-terminal structure. A graph (a) showing the frequency distribution when the package is sealed after frequency adjustment in the conventional ceramic package, and a graph showing the frequency distribution when the package is sealed after frequency adjustment in the conventional wafer level package (a). b) It is a graph (c) which shows the frequency distribution when the frequency is adjusted after the package is sealed in the wafer level package of this invention.

Hereinafter, embodiments of the crystal device of the present invention will be described. FIG. 1A shows a crystal device 10a having two external electrodes 20a and 20b, and FIG. 1B shows a crystal device 10b having four external electrodes 20a to 20d. The crystal devices 10a and 10b differ only in the number of external electrodes 20, and each is a wafer level package (WLP) including a crystal vibrating piece 11 and a pair of case members that sandwich the crystal vibrating piece 11 from both sides. Is formed by. At least a part of the case member is transparent. In this embodiment, at least one of the case members is made of quartz. The 2 terminals do not have a GND terminal to which the lid shield pattern is connected.

2A shows a plan view of the crystal device 10a in FIG. 1A, and FIG. 2B shows a plan view of the crystal device 10b in FIG. 1B. Further, since the crystal vibration piece 11 in the middle stage has the same structure as that of 10a and 10b, they will be described below with the same reference numerals. The crystal vibration piece 11 is formed by a vibration main body portion 13 and a frame portion 14 that supports the vibration main body portion 13. Further, as shown in FIG. 2C, the case 12 has a cavity 15 for freely accommodating the vibration main body portion 13 and is in close contact with the frame portion 14 of the crystal vibration piece 11.

As shown in FIGS. 2A and 2B, the vibration main body portion 13 is formed by a base portion 17 and a pair of vibrating arms 18 extending from the base portion 17. The base 17 is connected to the inner end of the frame 14 via a connection 19 extending from one end. The pair of vibrating arms 18 extend parallel to the side surface opposite to the direction in which the connecting portion 19 of the base portion 17 extends. The pair of vibrating arms 18 are symmetrical.

The pair of vibrating arms 18 are integrally formed by a first vibrating portion 21 having a first width W1 extending from a base 17 and a second vibrating portion 22 having a second width W2 wider than the first width W1. There is. The first vibrating portion 21 is provided with one or a plurality of groove portions 23 along the longitudinal direction, and an excitation electrode (not shown) is formed along the wall surface of the groove portions 23. The second vibrating portion 22 is provided as a weight portion for frequency adjustment, and a mass adjusting metal film 25 is formed on the surface thereof. The mass-adjusting metal film 25 adjusts the mass of the second vibrating portion 22 by removing a part of the mass-adjusting metal film 25 by beam irradiation, and as shown in FIG. , A second region E2 for fine adjustment is set. The first region E1 is a region for adjusting the crystal vibration piece 11 so as to roughly approach the target frequency in the step before being sealed by the case 12. The second region E2 is a region for final adjustment so as to match the frequency within the range of the product warranty in the process after sealing with the case 12.

As shown in FIG. 3, the first region E1 has a region partially shielded by the predetermined external electrode 20, and the second region E2 has a region not shielded by the predetermined external electrode 20. are doing. At least the frequency fine adjustment mark 26 removed by beam irradiation is formed in the second region E2. The frequency fine adjustment mark 26 is different for each crystal device depending on the range of the frequency to be adjusted.

As shown in FIG. 4, the frequency fine adjustment mark 26 is defined in relation to the first vibrating portion 21 and the predetermined external electrode 20, and when the first vibrating portion 21 is used as a reference, FIG. 4 (a). ), (B), it is provided at a position separated by at least a first predetermined distance L1 from the end portion 23a of the groove portion 23 formed in the first vibrating portion 21. Further, when the predetermined external electrode 20 is used as a reference, the external electrode 20 is provided at a position separated from the end portion 20a1 of the external electrode 20a by at least a second predetermined distance L2, and in FIG. 4B, the external electrode is provided. It is provided at a position separated from the respective ends 20a1 and 20c1 of the 20a and 20c by at least a second predetermined distance L2.

In one embodiment of the present invention, as shown in FIG. 4, the first predetermined distance L1 is set to 40 μm and the second predetermined distance L2 is set to 20 μm. This assumes an ultra-small crystal device with a volume of 2 mm square x 0.5 mmt or less, and is the size of the second vibrating part of the built-in crystal vibrating piece, or the misalignment in the manufacturing process such as vapor deposition or sputtering. It is decided in consideration of such things. Further, when the frequency adjustment is performed by beam irradiation, when the beam is irradiated to the second region E2 which is the frequency adjustment region after sealing, it is assumed that about 20 μm of metal scraps are scattered by this irradiation. On the other hand, the position accuracy of the beam irradiation is about 10 μm, and the spread of this beam is limited to about φ20 μm.

The first predetermined distance L1 and the second predetermined distance L2 defined in the present embodiment are defined in consideration of the scattering distance of metal debris due to beam irradiation. Here, the assumed scattered state of metal debris will be described with reference to FIGS. 5 (a) and 5 (b) in which the vicinity of the external electrode 20a in FIG. 4 (b) is enlarged. FIG. 5A is a schematic diagram assuming a scattered state of the mass adjusting metal film 25 when the frequency fine adjustment mark 26 is formed at the positions defined as the first predetermined distance L1 and the second predetermined distance L2. 5 (b) shows the scattered state of the mass adjusting metal film 25 when the frequency fine adjustment mark 26 is formed outside the range defined by the first predetermined distance L1 and the second predetermined distance L2. It is an assumed schematic diagram. As shown in FIG. 5B, when the first predetermined distance L1 becomes equal to or less than the above set value, scattered metal scraps 35 are formed in the first vibrating portion 21 as shown as a short-circuit defective portion 36. It may adhere to the space between the pair of excitation electrodes 24, resulting in a short circuit. Further, when the second predetermined distance L2 becomes equal to or less than the above set value, the inner surface of the transparent case 12a (FIG. 6) in which the scattered metal scraps 35 are on the back surface side of the external electrode 20a, as shown as the misaligned portion 37. The metal scraps 35 that adhere to (see) and are scattered when viewed from the outside may be recognized in an overlapping state as if they were a part of the external electrode 20a. Therefore, at the time of completion inspection of the crystal device, when the external electrodes 20a are aligned to align the product orientation, the shape of the external electrodes may be determined to be defective.

In response to the above problem, according to FIG. 5A, the frequency fine adjustment mark 26 is formed within the range defined by the first predetermined distance L1 and the second predetermined distance L2 from the adjacent external electrode 20a. This prevents the scattered metal debris 35 from adhering between the pair of excitation electrodes 24 formed in the first vibrating portion 21 and prevents the external electrode 20a from appearing to be deformed from the outside. be able to. As a result, when finely adjusting the frequency, it is possible to prevent problems such as short circuits and ensure alignment of the external electrodes. In FIG. 5, the external electrode 20a has been described as an example, but the same applies to the other external electrodes 20c.

FIG. 6 is a cross-sectional view showing an embodiment of the mass adjusting metal film 25 formed on the second vibrating portion 22. Here, the second vibrating portion 22 has a second plane F2 on the opposite side of the first plane F1, and the second plane F2 is at least the plane of the portion corresponding to the second region E2 of the mass adjusting metal film 25. It has a structure that exposes. The first plane F1 and the second plane F2 are crystal surfaces, and the mass-adjusting metal film 25 is formed via an excitation electrode 24 adhered to the crystal surface.

In the embodiment shown in FIG. 6A, the mass adjusting metal film 25 is provided on the first plane F1 of the second vibrating portion 22 facing the case 12a on which the external electrode 20 is formed, while the first plane. The mass adjusting metal film 25 is not provided on the second plane F2 on the opposite side of F1, and the entire second plane F2 is exposed. This is because when the excitation electrode 24 and the mass adjusting metal film 25 are provided on the second plane F2, the beam B irradiated from the first plane F1 exits from the second plane F2, and the excitable electrode is removed. 24 and the mass adjusting metal film 25 are removed, and the removed metal debris may be scattered in the case 12b and reattached to the vibrating arm or the like. As a result, problems such as frequency fluctuations and short circuits may occur. On the other hand, in the present embodiment, since the excitation electrode 24 and the mass adjusting metal film 25 are not formed on the second plane F2 facing the mass adjusting metal film 25, such a problem does not occur. The beam B is irradiated substantially perpendicular to the case 12a.

In the embodiment shown in FIG. 6B, the mass adjusting metal film 25 is provided on the first plane F1 of the second vibrating portion 22 facing the case 12a on which the external electrode 20 is formed, and the first plane is provided. The mass adjusting metal film 25 is also provided on the second plane F2 on the opposite side of F1. However, the excitation electrode 24 and the mass adjusting metal film 25 are not formed on the second plane F2 at the portion where the beam B irradiated from the first plane F1 penetrates, and the second plane F2 at that portion is not formed. Is exposed. In this embodiment, the mass adjusting metal film 25 is formed not only on the first plane F1 but also on the second plane F2 in order to set a wide frequency adjustment range, but at least the beam B penetrates. By removing the excitation electrode 24 and the mass adjusting metal film 25 in advance, the amount of metal debris scattered on the case 12b side can be reduced.

A plurality of the crystal devices 10a and 10b can be collectively produced from a large-sized collective wafer. FIG. 7 is a plan view of an aggregate wafer 30a in which a plurality of crystal devices 10a shown in FIG. 1A are formed and then diced, and FIG. 8 is an assembly in which a plurality of crystal devices 10b shown in FIG. 1B are formed and then diced. It is a top view of the wafer 30b. The assembled wafers 30a and 30b are formed by a vibrating piece wafer and a pair of case wafers that sandwich the vibrating piece wafer.

A plurality of crystal vibrating pieces 11 shown in FIG. 2 are formed in an array on the vibrating piece wafer. Further, in the case wafer, a plurality of cases 12 having a cavity 15 for freely accommodating the vibration main body portion 13 formed in the vibration piece wafer are formed in an array. As shown in FIG. 6A, each of the crystal vibrating pieces 11 in this embodiment is mass-adjusted to the first plane F1 of the second vibrating portion 22 facing the case 12a on which the external electrode 20 is formed. The metal film 25 is provided, and the mass adjusting metal film 25 is not provided on the second plane F2 opposite to the first plane F1. Hereinafter, each step of frequency adjustment in the crystal devices 10a and 10b formed by the assembled wafers 30a and 30b will be described. The procedure and the like shown in each step are examples, and the procedure is not limited thereto.

In the first step, in the vibrating piece wafer before being sealed by the pair of case wafers, the mass of at least the first plane F1 of the second vibrating portion 22 of each crystal vibrating piece 11 formed on the vibrating piece wafer. The adjusting metal film 25 is irradiated with a beam. By this beam irradiation, the frequency is roughly adjusted by removing a predetermined amount of the mass adjusting metal film 25. By performing this rough adjustment centering on the mass-adjusting metal film formed on the tip side of the second vibrating portion 22 having a high frequency volatility, it can be quickly dropped to the vicinity of the target frequency, and after sealing, which will be described later. It becomes easy to make fine adjustments. It is also possible to form the mass adjusting metal film 25 again in the portion removed by the rough adjustment as long as it can be finely adjusted in the subsequent step.

In the second step, from both sides of the coarsely adjusted vibrating piece wafer, each crystal vibrating piece 11 is sandwiched between a pair of case wafers in which a plurality of cases 12 are arranged, and as shown in FIG. 2 (c). , Each crystal vibration main body 13 is hermetically sealed in the cavity 15 of each case 12.

In the third step, an external electrode 20 electrically connected to the crystal vibrating piece 11 is formed on the outer surface of the case 12 corresponding to the first plane F1 side of each crystal vibrating piece 11. The external electrode 20 has two terminals and four terminals depending on the package specifications. The crystal device 10a shown in FIG. 1A is formed with a pair of external electrodes 20a and 20b that serve as signal terminals having both polarities. Further, in the crystal device 10b shown in FIG. 1B, in addition to a pair of external electrodes 20a and 20b serving as signal terminals having both polarities, external electrodes 20c and 20d serving as GND or NC (unconnected) are formed. Has been done.

In the fourth step, the case wafer on which the external electrode 20 is not formed is attached to the dicing tape 33 held by the dicing frame 32, and vibrates along the regions of the individual crystal devices 10a and 10b. The three-layer structure aggregate wafers 30a and 30b composed of a single wafer and a pair of case wafers are diced. This dicing is performed along a plurality of dicing streets 31 set along the X-axis direction and the Y'axis direction with the case wafer on which the external electrodes 20a to 20d are formed facing up. ..

In the fifth step, the dicing tape 33 is still attached from the outside of each of the diced cases 12, and is shielded by the external electrodes 20 of the first plane F1 on which the mass adjusting metal film 25 is formed. A predetermined portion of the second region E2 that has not been formed is irradiated with a beam for a predetermined time. This beam irradiation is performed toward the crystal vibration piece 11 from a direction substantially orthogonal to the case 12. A frequency fine adjustment mark 26 reduced by a predetermined amount remains in the beam-irradiated portion, and the size of the frequency fine adjustment mark 26 corresponds to the frequency fine adjustment amount. Since the mass adjusting metal film 25 is not formed on the second plane F2 opposite to the first plane F1 to be irradiated with the beam, even when the beam penetrates the second vibrating portion 22. It is possible to suppress the adhesion of metal debris in the cavity 15 of the lower case 12.

In the fifth step, as shown in FIG. 9, the measurement probe 34 arranged at a position that does not interfere with the irradiation range of the beam B is brought into contact with the external electrodes 20a and 20b, which are signal terminals, and is generated from the crystal vibration piece 11. The mass-adjusting metal film 25 in the second region E2 is reduced and adjusted by irradiating the beam B while measuring the frequency to be measured. As shown in FIG. 4, the position of the frequency fine adjustment mark 26 by beam irradiation is set to a position at least a predetermined distance L1 from the end portion 23a of the groove portion 23 formed in the first vibrating portion 21. When the external electrodes 20a and 20c are used as a reference, the external electrodes 20a and 20c are set at positions separated from the ends 20a1 and 20c1 by at least a second predetermined distance L2.

A crystal device formed by a conventional ceramic package has a crystal vibrating piece mounted with a conductive adhesive, and then the final frequency adjustment is performed by a laser or an ion beam, and then a metal lid that serves as a lid for airtightness, etc. It is sealed with and completed. Especially in the case of tuning fork type crystal vibrating pieces, in order to improve the equivalent series resistance value, which is an important element of electrical characteristics, it is essential to create a high vacuum inside the package at the time of sealing, but this degree of vacuum changes. By doing so, it is known that the frequency also changes at a higher rate than that of AT or the like. Therefore, in the step of covering with the metal lid to create this vacuum airtight state, which is performed after the final frequency adjustment, the influence of heat applied when sealing the lid and the degree of deterioration of the degree of vacuum due to the gasification of the internal liquid Since the individual difference of the crystal vibrating element and the state difference of the package and the adhesive affect, it is difficult to reduce the frequency deviation of the final product even if the frequency offset before encapsulation is performed.

On the other hand, in the present invention, the crystal vibrating piece 11 which has been roughly adjusted before being sealed by the case 12 is finely adjusted from the outside of the case 12 after being airtightly sealed by the case 12. The final fine adjustment can be performed without the influence of gas, heat, etc. generated during the tight sealing. As shown in FIG. 4, the frequency fine adjustment mark 26 is provided at a position separated by a first predetermined distance L1 from the end portion 23a of the groove portion 23 formed in the first vibrating portion 21 of each vibrating arm 18. As a result, the metal debris scattered by the beam irradiation does not adhere to the excitation electrode formed along the groove portion 23. Therefore, it is possible to perform accurate frequency adjustment without affecting the vibration characteristics of the crystal device. Further, the frequency fine adjustment marks 26 are set at positions separated from the respective ends 20a1 and 20c1 of the external electrodes 20a and 20c by a second predetermined distance L2, so that the external electrodes 20a and 20c are damaged by beam irradiation. As shown in FIG. 5B, the metal scraps 35 scattered by the beam irradiation can be prevented from reattaching to the back surface side of the case 12a so as to overlap the external electrodes 20a and 20c. Can be prevented. This makes it possible to reduce recognition errors when aligning the external electrode shapes in the completion inspection device and the assembly device.

Next, the frequency distribution of the crystal device sealed after frequency adjustment in the conventional ceramic package and WLP and the crystal device frequency-adjusted after sealing in the WLP of the present invention will be compared. This comparison was performed using the same measuring instrument under the same sealing conditions. In the case of a crystal device with a conventional ceramic package, the crystal vibration piece before being housed in the package is irradiated with a beam at a predetermined position to adjust the frequency, and then the package is covered with a metal lid that serves as a sealing lid. In a sealing device equipped with a high-vacuum vacuum chamber, the airtight state was maintained by heating (Au wax), seam sealing, electron beam sealing, and the like. In such a method, the frequency adjusted in vacuum changes due to the heat of sealing and the generated gas, etc., and even if the frequency is offset, the individual difference of the crystal vibrating piece and the sealing after sealing are performed. Due to the difference in vacuum state and the like, the frequency deviation as shown in FIG. 10A was generated. Further, as shown in FIG. 10 (b), even if the crystal device is WLP-based, when the crystal device is sealed after frequency adjustment, the frequency has a large variation as compared with FIG. 10 (a). It is a distribution. This is because the effect of sealing the WLP is much greater than that of the metal lid sealed by the electron beam.

On the other hand, in the present invention, after the crystal vibrating piece is WLP-sealed with a pair of cases, the frequency fine adjustment mark 26 made by beam irradiation from the outside of the case is limited to the position shown in FIG. As a result, it is possible to prevent the metal debris scattered by the beam irradiation from adhering to the excitation electrode formed in the first vibrating portion 21, and as shown in FIG. 10 (c), the frequency deviation is also substantially zero. It becomes possible to approach to.

B beam E1 1st region (for rough adjustment)
E2 2nd area (for fine adjustment)
F1 1st plane F2 2nd plane W1 1st width W2 2nd width 10a, 10b Crystal device 11 Crystal vibrating piece 12 Case 13 Vibration main body 14 Frame part 15 Cavity 17 Base 18 Vibration arm 19 Connection part 20 External electrode 20a1 End 20c1 End 21 1st vibrating part 22 2nd vibrating part 23 Groove part 23a End part 24 Excitation electrode 25 Mass adjustment metal film 26 Frequency fine adjustment mark 30a, 30b Collective wafer 31 Dicing street 32 Dicing frame 33 Dicing tape 34 Measurement probe 35 Metal scraps 36 Short defects 37 Alignment defects

Claims (6)

A process of forming a plurality of crystal vibrating pieces on a vibrating piece wafer and irradiating a mass-adjusting metal film provided on the first plane of each crystal vibrating piece with a beam to roughly adjust the frequency.
A step of sandwiching the vibrating piece wafer in which each crystal vibrating piece is roughly adjusted from both sides with a pair of case wafers and airtightly sealing each crystal vibrating piece in the case.
A step of forming an external electrode electrically connected to each crystal vibrating piece on the outer surface of one of the case wafers facing the first plane of each crystal vibrating piece for each case.
A step of attaching a dicing tape to the outer surface of the other case wafer different from the one case wafer on which the external electrode is formed among the pair of case wafers, and dicing the pair of case wafers for each case. ,
From the outer surface side of each of the diced cases , the coarsely adjusted mass-adjusted metal film is irradiated with a beam while the dicing tape is still attached to the outer surface of the case wafer. A process for fine-tuning the frequency and a frequency adjustment method for a crystal device comprising. The crystal device according to claim 1 , wherein the frequency is roughly adjusted by irradiating the mass-adjusting metal film provided on the first plane of the crystal vibrating piece with a beam and removing a predetermined amount of the mass-adjusting metal film. Frequency adjustment method. The first aspect of claim 1 , wherein the coarsely adjusted mass-adjusted metal film is irradiated with a beam to fine-tune the frequency by leaving a frequency fine-tuning mark in which the coarsely-adjusted mass-adjusted metal film is reduced by a predetermined amount. How to adjust the frequency of the crystal device. The mass-adjusting metal film provided on the first plane of the crystal vibrating piece is such that the mass-adjusting metal film after rough adjustment is formed on the outer surface of the case in a plan view. Claim 1 having a first region shielded by an electrode and a second region not shielded, and irradiating the second region of the mass-adjusting metal film after the rough adjustment with a beam to finely adjust the frequency. The method for adjusting the frequency of the crystal device according to any one of 3 to 3 . In the process of fine-tuning the frequency
4. Claim 4 for forming a frequency fine adjustment mark by irradiating the second region of the mass-adjusting metal film after the rough adjustment with the beam while measuring the frequency by bringing the measuring probe into contact with the external electrode. The frequency adjustment method of the crystal device described in. 5. Claim 5 that irradiates the second region with a beam so that the frequency fine adjustment mark formed in the second region is set at a position separated from the end of the external electrode by a predetermined distance in a plan view. The frequency adjustment method of the crystal device described in.

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