JP2014168145A - Quartz oscillation element - Google Patents

Quartz oscillation element Download PDF

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JP2014168145A
JP2014168145A JP2013039077A JP2013039077A JP2014168145A JP 2014168145 A JP2014168145 A JP 2014168145A JP 2013039077 A JP2013039077 A JP 2013039077A JP 2013039077 A JP2013039077 A JP 2013039077A JP 2014168145 A JP2014168145 A JP 2014168145A
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crystal piece
crystal
excitation electrode
convex portion
main surface
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JP6017350B2 (en
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Koichi Iwata
浩一 岩田
Kohei Sasaoka
康平 笹岡
Masatoshi Yumura
雅俊 湯村
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Kyocera Crystal Device Corp
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Abstract

PROBLEM TO BE SOLVED: To obtain a stabilized low CI value.SOLUTION: A quartz oscillation element includes a tabular crystal piece, an elliptical protrusion provided on the principal surface of the crystal piece, an excitation electrode provided on both principal surfaces of the crystal piece, and covering the protrusion, and a routing pattern provided at one end of the crystal piece, and connected with the excitation electrode. The excitation electrode has a side, directing the short side of the crystal piece, formed in a curved shape and the side, directing the long side, formed linearly. The protrusion provided on one principal surface of the crystal piece has the same or shorter minor axis and a longer major axis as compared with the protrusion provided on the other principal surface.

Description

本発明は、水晶デバイスに用いられる水晶振動素子に関する。   The present invention relates to a crystal resonator element used in a crystal device.

従来より、水晶デバイスには水晶片に金属膜からなる励振電極を設けて構成された水晶振動素子が用いられている。
この水晶片は、例えば、ATカットの水晶ウェハを従来周知のフォトリソグラフィ技術とエッチング技術を用いることで形成することができる。
このような水晶振動素子は、四角形に形成され主面に凸部が形成された水晶片と、この水晶片の両主面中央に設けられる楕円形状の励振電極と、この励振電極と接続され水晶片の一方の端部に設けられる引き回しパターンとから構成されている。
ここで、水晶片の主面には四角形状の凸部が設けられており、この凸部の平面中心が水晶片の平面中心に合わせて設けられている。
また、励振電極は、水晶片に設けられた凸部の平面内に設けられており、平面中心を凸部の平面中心と一致させた位置に設けられている(例えば、特許文献1参照)。
なお、凸部と励振電極とが楕円形状となる水晶振動素子も提案されている(例えば、特許文献2参照)。
このような水晶振動素子は、ウェットエッチングにより凸部の側面が水晶の軸方向によって異なる傾斜角度を有した形状となる。この傾斜角度がついている部分を残差と呼んでいる。
2. Description of the Related Art Conventionally, a quartz crystal element in which an excitation electrode made of a metal film is provided on a quartz piece has been used in a quartz device.
This crystal piece can be formed, for example, by using an AT-cut crystal wafer by using a conventionally known photolithography technique and etching technique.
Such a crystal resonator element includes a crystal piece having a quadrangular shape and a convex portion formed on the main surface, an elliptical excitation electrode provided at the center of both main surfaces of the crystal piece, and a crystal piece connected to the excitation electrode. It is comprised from the routing pattern provided in one edge part of a piece.
Here, a quadrangular convex portion is provided on the main surface of the crystal piece, and the plane center of the convex portion is provided in accordance with the plane center of the crystal piece.
Moreover, the excitation electrode is provided in the plane of the convex part provided in the crystal piece, and is provided in the position which made the plane center correspond with the plane center of a convex part (for example, refer patent document 1).
In addition, a crystal resonator element in which the convex portion and the excitation electrode are elliptical has been proposed (see, for example, Patent Document 2).
Such a crystal resonator element has a shape in which the side surface of the convex portion has an inclination angle that varies depending on the axial direction of the crystal by wet etching. The portion with this inclination angle is called the residual.

特開2009−135830号公報JP 2009-135830 A 特開2012‐74860号公報JP 2012-74860 A

水晶振動素子は、励振電極で振動エネルギーを最大にして、水晶片の縁付近で振動エネルギーを閉じ込めるのが理想状態となる。
しかしながら、水晶片に形成される凸部には、凸部の形成の際に生じるウェットエッチングによる残渣が形成されるので、均一な厚みが形成されず、不要な振動を発生させるものと考えられる。これにより、水晶片に楕円形状の凸部を形成した上に励振電極を形成した場合、温度変化によるCI値(クリスタルインピーダンス値)の変動が発生しやすくなっていた。この変動は、CIディップと呼ばれ、周波数温度特性をグラフ化した場合に、所定の温度範囲においてCI値変動が大きく現れた状態となる。
The ideal state of the crystal resonator element is to maximize the vibration energy by the excitation electrode and confine the vibration energy near the edge of the crystal piece.
However, since the residue formed by the wet etching that occurs during the formation of the protrusion is formed on the protrusion formed on the crystal piece, it is considered that a uniform thickness is not formed and unnecessary vibration is generated. As a result, when the excitation electrode is formed after the elliptical convex portion is formed on the crystal piece, the CI value (crystal impedance value) fluctuates easily due to a temperature change. This variation is called a CI dip, and when the frequency-temperature characteristic is graphed, a variation in the CI value appears greatly in a predetermined temperature range.

そこで、本発明は、安定した低いCI値を得る水晶振動素子を提供することを課題とする。   Therefore, an object of the present invention is to provide a crystal resonator element that obtains a stable low CI value.

前記課題を解決するため、本発明は、水晶振動素子であって、平板状の水晶片と、この水晶片の主面に設けられる楕円形状の凸部と、この水晶片の両主面に設けられ前記凸部を覆う励振電極と、この水晶片の一方の端部に設けられ、前記励振電極と接続する引き回しパターンとを備え、前記励振電極が、水晶片の短辺側を向く辺が曲線状に形成されつつ長辺側を向く辺が直線状に形成され、前記水晶片の一方の主面に設けられる凸部が前記水晶片の他方の主面に設けられる凸部よりも同じ短径でかつ長い長径となって構成されることを特徴とする。   In order to solve the above-mentioned problems, the present invention provides a crystal resonator element, which is provided on a plate-like crystal piece, an elliptical convex portion provided on the main surface of the crystal piece, and both main surfaces of the crystal piece. An excitation electrode that covers the convex portion, and a routing pattern that is provided at one end of the crystal piece and is connected to the excitation electrode. The excitation electrode has a curved side that faces the short side of the crystal piece. The side facing the long side is formed in a straight line, and the convex portion provided on one main surface of the crystal piece is the same short diameter as the convex portion provided on the other main surface of the crystal piece And having a long major axis.

また、本発明は、水晶振動素子であって、平板状の水晶片と、この水晶片の主面に設けられる楕円形状の凸部と、この水晶片の両主面に設けられ前記凸部を覆う励振電極と、この水晶片の一方の端部に設けられ、前記励振電極と接続する引き回しパターンとを備え、前記励振電極が、水晶片の短辺側を向く辺が曲線状に形成されつつ長辺側を向く辺が直線状に形成され、前記水晶片の一方の主面に設けられる凸部が前記水晶片の他方の主面に設けられる凸部よりも短い短径でかつ長い長径となって構成されることを特徴とする。   Further, the present invention is a crystal resonator element, comprising a plate-shaped crystal piece, an elliptical convex portion provided on a main surface of the crystal piece, and the convex portions provided on both main surfaces of the crystal piece. An excitation electrode to be covered and a routing pattern provided at one end of the crystal piece and connected to the excitation electrode, and the excitation electrode is formed in a curved shape with a side facing the short side of the crystal piece The side facing the long side is formed in a straight line, and the convex part provided on one main surface of the crystal piece has a short diameter and a long major axis shorter than the convex part provided on the other main surface of the crystal piece. It is characterized by comprising.

このような水晶振動素子では、水晶片の両主面に設ける凸部の形状について、水晶片の一方の主面に設けられる凸部が、水晶片の他方の主面に設けられる凸部よりも同じ短径でかつ長い長径となって構成されるので、従来よりも凸部に形成されるエッチング残渣による厚みのばらつきが減少することで不要な振動の発生を防ぎ、CIディップのない安定したCI値温度特性を得ることができる。   In such a crystal resonator element, with respect to the shape of the protrusions provided on both main surfaces of the crystal piece, the protrusion provided on one main surface of the crystal piece is more than the protrusion provided on the other main surface of the crystal piece. Since it is configured with the same short diameter and a long long diameter, the variation in thickness due to the etching residue formed on the convex portion is reduced as compared with the prior art, thereby preventing the occurrence of unnecessary vibration and stable CI without CI dip. Value temperature characteristics can be obtained.

このような水晶振動素子では、水晶片の両主面に設ける凸部の形状について、水晶片の一方の主面に設けられる凸部が、水晶片の他方の主面に設けられる凸部よりも短い短径でかつ長い長径となって構成されるので、従来よりも凸部に形成されるエッチング残渣による厚みのばらつきが減少することで不要な振動の発生を防ぎ、CIディップのない安定したCI値温度特性を得ることができる。   In such a crystal resonator element, with respect to the shape of the protrusions provided on both main surfaces of the crystal piece, the protrusion provided on one main surface of the crystal piece is more than the protrusion provided on the other main surface of the crystal piece. Since it is configured with a short minor axis and a long major axis, the variation in thickness due to etching residue formed on the convex portion is reduced as compared with the prior art, thereby preventing the occurrence of unnecessary vibration and stable CI without CI dip. Value temperature characteristics can be obtained.

(a)は本発明の実施形態に係る水晶振動素子の一例を示す模式図であり、(b)は水晶片の短辺側を誇張して示した側面図であり、(c)は水晶片の長辺側を誇張して示した側面図である。(A) is a schematic diagram which shows an example of the crystal oscillation element which concerns on embodiment of this invention, (b) is the side view which exaggerated and showed the short side of the crystal piece, (c) is a crystal piece It is the side view which exaggerated and showed the long side of this. 本発明の実施形態に係る水晶振動素子の変形例を示す模式図である。It is a mimetic diagram showing the modification of the crystal oscillation element concerning the embodiment of the present invention. 本発明の実施形態に係る水晶振動素子のCI値温度特性の一例を示すグラフである。It is a graph which shows an example of CI value temperature characteristic of the crystal oscillation element concerning the embodiment of the present invention. 本発明の実施形態に係る水晶振動素子との比較に用いた水晶振動素子を示し、(a)は水晶振動素子の平面図であり、(b)は側面図であり、(c)は他の水晶振動素子の平面図である。The crystal oscillation element used for the comparison with the crystal oscillation element which concerns on embodiment of this invention is shown, (a) is a top view of a crystal oscillation element, (b) is a side view, (c) is other It is a top view of a crystal oscillation element. 本発明の実施形態に係る水晶振動素子との比較に用いた水晶振動素子のCI値温度特性の一例を示すグラフである。It is a graph which shows an example of the CI value temperature characteristic of the crystal oscillation element used for comparison with the crystal oscillation element which concerns on embodiment of this invention. 本発明の実施形態に係る水晶振動素子との比較に用いた他の水晶振動素子のCI値温度特性の一例を示すグラフである。It is a graph which shows an example of the CI value temperature characteristic of the other crystal oscillation element used for the comparison with the crystal oscillation element which concerns on embodiment of this invention.

次に、本発明を実施するための最良の形態(以下、「実施形態」という。)について、適宜図面を参照しながら詳細に説明する。なお、各構成要素について、状態をわかりやすくするために、誇張して図示している。また、水晶片の主面という場合、水晶片に現れる平面のうち最も広い面とこの広い面と並行する面を主面とする。   Next, the best mode for carrying out the present invention (hereinafter referred to as “embodiment”) will be described in detail with reference to the drawings as appropriate. Note that each component is exaggerated for easy understanding of the state. Further, when referring to the main surface of the crystal piece, the main surface is defined as the widest surface of the planes appearing on the crystal piece and a surface parallel to the wide surface.

図1(a)〜(c)に示すように、本発明の実施形態に係る水晶振動素子11は、四角形状で凸部が設けられた水晶片1とこの水晶片1の両主面に設けられる励振電極2と、この励振電極2と接続し水晶片1の一方の端部へ引き回されている引き回しパターン3とから構成されている。
この本発明の実施形態に係る水晶振動素子11は、水晶片1の長辺の中心を通る中心線と水晶片1の短辺の中心を通る中心線との交点が水晶片1の平面中心C1であり、凸部の平面中心C2と水晶片の平面中心C1とが一致させて形成され、励振電極2の平面中心C3が水晶片1の引き回しパターン3が設けられない短辺側にずらして形成されている。
As shown in FIGS. 1A to 1C, a crystal resonator element 11 according to an embodiment of the present invention is provided on a crystal piece 1 having a quadrangular shape and provided with convex portions and both main surfaces of the crystal piece 1. And a routing pattern 3 connected to the excitation electrode 2 and routed to one end of the crystal piece 1.
In the crystal resonator element 11 according to this embodiment of the present invention, the intersection of the center line passing through the center of the long side of the crystal piece 1 and the center line passing through the center of the short side of the crystal piece 1 is the plane center C1 of the crystal piece 1. The plane center C2 of the convex portion and the plane center C1 of the crystal piece are formed to coincide with each other, and the plane center C3 of the excitation electrode 2 is formed to be shifted to the short side where the routing pattern 3 of the crystal piece 1 is not provided. Has been.

水晶片1は、例えばATカットの水晶ウェハから四角形状でかつ平板状に形成されている。
なお、この水晶片1は、長辺がX軸と平行であり、短辺がZ´軸と平行であり、厚みがY´軸方向と平行に形成されている。
また、図1(a)〜(c)に示すように、この水晶片1の両主面には、凸部1a,1bが設けられている。これら凸部1a,1bの平面中心C2は、平面視における水晶片1の投影面の中心C1に一致した位置となっている。
The crystal piece 1 is formed in a rectangular shape and a flat plate shape from, for example, an AT-cut crystal wafer.
The crystal piece 1 has a long side parallel to the X axis, a short side parallel to the Z ′ axis, and a thickness parallel to the Y ′ axis direction.
Further, as shown in FIGS. 1A to 1C, convex portions 1 a and 1 b are provided on both main surfaces of the crystal piece 1. The plane center C2 of the convex portions 1a and 1b is a position that coincides with the center C1 of the projection surface of the crystal piece 1 in plan view.

また、水晶片1の両主面に設けられる凸部1a,1bは、楕円形状に形成されており、楕円の長径を水晶片11の長辺と平行となり、楕円の短径を水晶片11の短辺と平行となるように設けられる。
ここで、水晶片1の一方の主面に設けられる凸部1bは、水晶片1の他方の主面に設けられる凸部1aよりも同じ短径でかつ長い長径となるように設けられる。つまり、凸部1bは、凸部1aに対して長く形成された状態となる。
The convex portions 1 a and 1 b provided on both main surfaces of the crystal piece 1 are formed in an elliptical shape, the major axis of the ellipse is parallel to the long side of the crystal piece 11, and the minor axis of the ellipse is It is provided so as to be parallel to the short side.
Here, the convex part 1b provided in one main surface of the crystal piece 1 is provided so that it may have the same short diameter and a long long diameter as the convex part 1a provided in the other main surface of the crystal piece 1. That is, the convex part 1b will be in the state formed long with respect to the convex part 1a.

この水晶片1は、従来周知のフォトリソグラフィ技術とエッチング技術を用いて形成することができる。なお、水晶片1は、側面に水晶の結晶面が形成されている。なお、水晶片1の側面に形成される残渣は省略する。
なお、水晶片1は、引き回しパターン3が設けられる端部をX軸の+X方向とし、反対側の端部を−X方向としている。
This crystal piece 1 can be formed using a conventionally known photolithography technique and etching technique. The crystal piece 1 has a crystal face of crystal on the side surface. The residue formed on the side surface of the crystal piece 1 is omitted.
The crystal piece 1 has an end portion where the routing pattern 3 is provided as the + X direction of the X axis and an opposite end portion as the −X direction.

このとき、図1(b)に示すように、Z軸方向において凸部1aは、凸部1aの内側に入り込む傾斜角度が付いた残渣が側面に生じており、Z軸方向に沿ったこの側面と反対側では、外側にはみ出る傾斜角度がついた残渣が側面生じている。
これに対し、凸部1bは、凸部1aの内側に入り込む傾斜角度が付いた残渣が生じている側面と対向する位置に外側にはみ出る傾斜角度がついた残渣が側面生じており、凸部1aの外側にはみ出る傾斜角度がついた残渣が生じている側面と対向する位置に、凸部1bの内側に入り込む傾斜角度が付いた残渣が側面に生じている。
At this time, as shown in FIG. 1 (b), in the Z-axis direction, the convex portion 1a has a residue with an inclination angle that enters the inside of the convex portion 1a, and this side surface along the Z-axis direction. On the opposite side, a residue with a tilt angle that protrudes outward is produced on the side surface.
On the other hand, the convex portion 1b has a side surface with a residue having an inclination angle that protrudes outside at a position opposite to the side surface where the residue with an inclination angle entering the inside of the convex portion 1a is generated. The residue with the inclination angle which enters the inside of the convex part 1b is generated on the side surface at a position opposite to the side surface where the residue with the inclination angle protruding outside the surface is generated.

このような凸部1aと凸部1bとを有する本発明の実施形態に係る水晶振動素子11は、凸部1aと凸部1bとに生じた残渣による厚みの異なる部分について、その厚みの異なるZ軸方向の長さ部分を△W1としたとき、このZ軸方向の長さ部分△W1を従来よりも小さくすることができる。
したがって、従来よりも凸部に形成されるエッチング残渣による厚みのばらつきが減少するので不要な振動の発生を防ぐことができる。これにより、本発明の実施形態に係る水晶振動素子10は、CIディップのない安定したCI値温度特性を得ることができる。
In the crystal resonator element 11 according to the embodiment of the present invention having the convex portion 1a and the convex portion 1b, Z portions having different thicknesses are formed on portions having different thicknesses due to the residues generated on the convex portions 1a and 1b. When the length portion in the axial direction is ΔW1, the length portion ΔW1 in the Z-axis direction can be made smaller than the conventional one.
Therefore, since the thickness variation due to the etching residue formed on the convex portion is reduced as compared with the conventional case, unnecessary vibration can be prevented. Accordingly, the crystal resonator element 10 according to the embodiment of the present invention can obtain a stable CI value temperature characteristic without CI dip.

なお、凸部1aと凸部1bとは、変形例として、図2に示すように、水晶片1の一方の主面に設けられる凸部1bが、水晶片1の他方の主面に設けられる凸部1aよりも短い短径でかつ長い長径となるように設けて水晶振動素子12を構成しても良い。つまり、凸部1bは、凸部1aに対して細くかつ長く形成された状態となる。
このように構成しても従来よりも凸部に形成されるエッチング残渣による厚みのばらつきが減少するので不要な振動の発生を防ぐことができる。これにより、本発明の実施形態に係る水晶振動素子10は、CIディップのない安定したCI値温度特性を得ることができる。
In addition, as a modification, the convex part 1a and the convex part 1b are provided with the convex part 1b provided on one main surface of the crystal piece 1 on the other main surface of the crystal piece 1 as shown in FIG. The crystal resonator element 12 may be configured to have a short diameter shorter than the convex portion 1a and a long long diameter. That is, the convex part 1b will be in the state formed thinly and long with respect to the convex part 1a.
Even if comprised in this way, since the dispersion | variation in the thickness by the etching residue formed in a convex part reduces conventionally, generation | occurrence | production of an unnecessary vibration can be prevented. Accordingly, the crystal resonator element 10 according to the embodiment of the present invention can obtain a stable CI value temperature characteristic without CI dip.

図1(a)に示すように、励振電極2は、凸部1a,1bを覆うように水晶片1上に設けられている。この励振電極2は、水晶片1の短辺側を向く辺が曲線状に形成されて、水晶片1の長辺側を向く辺が直線状に形成されている。
前記凸部1a,1bを覆って設けられるこの励振電極2は、楕円形状を用いて形成しても良く、楕円形状のうち短径側を直線に形成した形状で構成しても良い。
As shown in FIG. 1A, the excitation electrode 2 is provided on the crystal piece 1 so as to cover the convex portions 1a and 1b. In the excitation electrode 2, the side facing the short side of the crystal piece 1 is formed in a curved shape, and the side facing the long side of the crystal piece 1 is formed in a straight line.
The excitation electrode 2 provided so as to cover the convex portions 1a and 1b may be formed using an elliptical shape, or may be configured in a shape in which the minor axis side is formed in a straight line in the elliptical shape.

引き回しパターン3は、水晶片1の一方の端部に設けられ、励振電極2と接続している。この引き回しパターン3は、水晶片1の主面の縁に沿って設けられている。   The routing pattern 3 is provided at one end of the crystal piece 1 and is connected to the excitation electrode 2. The routing pattern 3 is provided along the edge of the main surface of the crystal piece 1.

例えば、引き回しパターン3は、2つ一対の接続パッド3aと引き回し配線3bとから構成されている。接続パッド3aは、水晶片1の両主面の角部に並んで設けられており、1つの接続パッド3aが一方の主面に設けられた励振電極2と引き回し配線3bを介して接続し、他の接続パッド3aが他方の主面に設けられた励振電極2と引き回し配線3bを介して接続している。
また、引き回し配線3bは、水晶片1の主面の縁に沿って直線で形成されており、励振電極2から接続パッド3aまで設けられている。
For example, the routing pattern 3 includes two pairs of connection pads 3a and routing wirings 3b. The connection pads 3a are provided side by side at the corners of both main surfaces of the crystal piece 1, and one connection pad 3a is connected to the excitation electrode 2 provided on one main surface via the lead wiring 3b. Another connection pad 3a is connected to the excitation electrode 2 provided on the other main surface via the lead wiring 3b.
Further, the routing wiring 3b is formed in a straight line along the edge of the main surface of the crystal piece 1, and is provided from the excitation electrode 2 to the connection pad 3a.

このように構成される本発明の実施形態に係る水晶振動素子11は、例えば、図3に示すようにCIディップが発生せず、CI値が約40Ωから50Ωの間に入る値となり、安定したCI値温度特性を得ることができた。   In the crystal resonator element 11 according to the embodiment of the present invention configured as described above, for example, as shown in FIG. 3, CI dip does not occur, and the CI value becomes a value that falls between about 40Ω to 50Ω and is stable. CI value temperature characteristics could be obtained.

これに対し、例えば、図4(a)及び(b)に示すように、水晶片1の両主面に楕円形状の凸部を設け、水晶片1の一方の主面の凸部より他方の主面の凸部の短径と長径とを大きく形成した水晶振動素子21を検討した。
この水晶振動素子21は、図4(b)に示すように、水晶片の両主面に設けられた凸部に生じた残渣による厚みの異なる部分について、その厚みの異なるZ軸方向の長さ部分を△W2及び△W3としたとき、このZ軸方向の長さ部分△W2と△W3との距離は異なって対称性がなくなっており、△W2と△W3とを合わせた長さが本発明の実施形態に係る水晶振動素子11の厚みの異なるZ軸方向の長さ部分△W1+△W1よりも長くなっている。
この水晶振動素子21の場合、図5に示すように、−10℃のあたりで急激にCI値が増加するCIディップが発生した。
On the other hand, for example, as shown in FIGS. 4A and 4B, elliptical convex portions are provided on both main surfaces of the crystal piece 1, and the other convex portion is provided on one main surface of the crystal piece 1. The crystal resonator element 21 in which the minor axis and the major axis of the convex portion of the main surface are formed large was examined.
As shown in FIG. 4B, the quartz resonator element 21 has different lengths in the Z-axis direction for portions having different thicknesses due to residues generated on the convex portions provided on both main surfaces of the quartz piece. When the portions are ΔW2 and ΔW3, the distance between the length portions ΔW2 and ΔW3 in the Z-axis direction is different and the symmetry is lost, and the total length of ΔW2 and ΔW3 is The quartz resonator element 11 according to the embodiment of the present invention is longer than the length portions ΔW1 + ΔW1 in the Z-axis direction having different thicknesses.
In the case of this crystal resonator element 21, as shown in FIG. 5, a CI dip in which the CI value suddenly increases around -10 ° C. occurred.

また、例えば、図4(c)に示すように、水晶片の両主面に楕円形状の凸部を設け、水晶片の一方の主面の凸部と他方の主面の凸部とを同一形状で形成した水晶振動素子22を検討した。
この水晶振動素子21の場合、図6のように、CIディップは発生しなかったが、CI値が約80Ωから100Ωの間に入る値となった。
なお、図4、図5、図6の横軸において、「Temp(℃)」は温度を意味し、縦軸において、「CI(Ω)」はCI値を意味する。
Also, for example, as shown in FIG. 4C, an elliptical convex portion is provided on both main surfaces of the crystal piece, and the convex portion of one main surface of the crystal piece and the convex portion of the other main surface are the same. The crystal resonator element 22 formed in a shape was examined.
In the case of this crystal resonator element 21, CI dip did not occur as shown in FIG. 6, but the CI value became a value between about 80Ω and 100Ω.
4, 5, and 6, “Temp (° C.)” means temperature, and on the vertical axis, “CI (Ω)” means CI value.

これにより、本発明の実施形態に係る水晶振動素子11は、CIディップのない安定したCI値温度特性を得ることができる。   Accordingly, the crystal resonator element 11 according to the embodiment of the present invention can obtain a stable CI value temperature characteristic without CI dip.

以上、本発明の実施形態について説明したが、本発明は前記実施形態には限定されない。   As mentioned above, although embodiment of this invention was described, this invention is not limited to the said embodiment.

11,12 水晶振動素子
1 水晶片
1a,1b 凸部
2 励振電極
3 引き回しパターン
C1,C2,C3 平面中心
DESCRIPTION OF SYMBOLS 11, 12 Crystal resonator element 1 Crystal piece 1a, 1b Convex part 2 Excitation electrode 3 Leading pattern C1, C2, C3 Plane center

Claims (2)

平板状の水晶片と、
この水晶片の主面に設けられる楕円形状の凸部と、
この水晶片の両主面に設けられ前記凸部を覆う励振電極と、
この水晶片の一方の端部に設けられ、前記励振電極と接続する引き回しパターンとを備え、
前記励振電極が、水晶片の短辺側を向く辺が曲線状に形成されつつ長辺側を向く辺が直線状に形成され、
前記水晶片の一方の主面に設けられる凸部が前記水晶片の他方の主面に設けられる凸部よりも同じ短径でかつ長い長径となって構成されることを特徴とする水晶振動素子。
A flat crystal piece,
An elliptical convex portion provided on the main surface of the crystal piece;
An excitation electrode provided on both main surfaces of the crystal piece and covering the convex portion;
Provided at one end of this crystal piece, with a routing pattern connected to the excitation electrode,
The excitation electrode is formed such that the side facing the short side of the crystal piece is formed in a curved shape while the side facing the long side is formed in a straight line,
The quartz crystal resonator element, wherein a convex portion provided on one main surface of the crystal piece has a shorter diameter and a longer long diameter than a convex portion provided on the other main surface of the crystal piece. .
平板状の水晶片と、
この水晶片の主面に設けられる楕円形状の凸部と、
この水晶片の両主面に設けられ前記凸部を覆う励振電極と、
この水晶片の一方の端部に設けられ、前記励振電極と接続する引き回しパターンとを備え、
前記励振電極が、水晶片の短辺側を向く辺が曲線状に形成されつつ長辺側を向く辺が直線状に形成され、
前記水晶片の一方の主面に設けられる凸部が前記水晶片の他方の主面に設けられる凸部よりも短い短径でかつ長い長径となって構成されることを特徴とする水晶振動素子。
A flat crystal piece,
An elliptical convex portion provided on the main surface of the crystal piece;
An excitation electrode provided on both main surfaces of the crystal piece and covering the convex portion;
Provided at one end of this crystal piece, with a routing pattern connected to the excitation electrode,
The excitation electrode is formed such that the side facing the short side of the crystal piece is formed in a curved shape while the side facing the long side is formed in a straight line,
A crystal resonator element, wherein a convex portion provided on one main surface of the crystal piece has a shorter and longer major diameter than a convex portion provided on the other main surface of the crystal piece. .
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Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001085970A (en) * 1999-09-10 2001-03-30 Toyo Commun Equip Co Ltd Resonator for high stable piezo-oscillator
JP2007158486A (en) * 2005-12-01 2007-06-21 Epson Toyocom Corp Crystal resonator element, crystal resonator, and crystal oscillator
JP2009135830A (en) * 2007-11-30 2009-06-18 Epson Toyocom Corp Crystal vibration piece, crystal vibrator, and crystal oscillator
JP2011205516A (en) * 2010-03-26 2011-10-13 Seiko Epson Corp Piezoelectric vibrating element and piezoelectric vibrator
JP2012074860A (en) * 2010-09-28 2012-04-12 Kyocera Kinseki Corp Crystal vibration element
JP2012249099A (en) * 2011-05-27 2012-12-13 Daishinku Corp Piezoelectric vibration piece

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001085970A (en) * 1999-09-10 2001-03-30 Toyo Commun Equip Co Ltd Resonator for high stable piezo-oscillator
JP2007158486A (en) * 2005-12-01 2007-06-21 Epson Toyocom Corp Crystal resonator element, crystal resonator, and crystal oscillator
JP2009135830A (en) * 2007-11-30 2009-06-18 Epson Toyocom Corp Crystal vibration piece, crystal vibrator, and crystal oscillator
JP2011205516A (en) * 2010-03-26 2011-10-13 Seiko Epson Corp Piezoelectric vibrating element and piezoelectric vibrator
JP2012074860A (en) * 2010-09-28 2012-04-12 Kyocera Kinseki Corp Crystal vibration element
JP2012249099A (en) * 2011-05-27 2012-12-13 Daishinku Corp Piezoelectric vibration piece

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