JPH0680979B2 - Voltage-controlled surface acoustic wave oscillator - Google Patents
Voltage-controlled surface acoustic wave oscillatorInfo
- Publication number
- JPH0680979B2 JPH0680979B2 JP11444289A JP11444289A JPH0680979B2 JP H0680979 B2 JPH0680979 B2 JP H0680979B2 JP 11444289 A JP11444289 A JP 11444289A JP 11444289 A JP11444289 A JP 11444289A JP H0680979 B2 JPH0680979 B2 JP H0680979B2
- Authority
- JP
- Japan
- Prior art keywords
- surface acoustic
- acoustic wave
- voltage
- delay line
- wave oscillator
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000010897 surface acoustic wave method Methods 0.000 title claims description 37
- 230000010355 oscillation Effects 0.000 description 13
- 238000010586 diagram Methods 0.000 description 7
- 239000003990 capacitor Substances 0.000 description 2
- 230000010363 phase shift Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
Landscapes
- Oscillators With Electromechanical Resonators (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、弾性表面波遅延線を用いた電圧制御型弾性
表面発振器に関する。Description: TECHNICAL FIELD The present invention relates to a voltage-controlled surface acoustic wave oscillator using a surface acoustic wave delay line.
この種の電圧制御型弾性表面波発振器の典型的な例を第
3図に示す 即ちこの弾性表面波発振器は、基本的には、増幅器2と
移相器4と弾性表面波遅延線6とをループ状に接続して
構成されている。出力の取出しには、方向性結合器8や
コンデンサ等が使われる。A typical example of this type of voltage control type surface acoustic wave oscillator is shown in FIG. 3, that is, this surface acoustic wave oscillator basically comprises an amplifier 2, a phase shifter 4, and a surface acoustic wave delay line 6. It is configured by connecting in a loop. A directional coupler 8 and a capacitor are used to extract the output.
移相器4は、発振条件を成立させるためのものである
が、ここではこれを可変容量ダイオードを含む電圧制御
型にして、それに供給する制御電圧Vtによって当該弾性
表面波発振器の発振周波数を変化させることができるよ
うにしている。The phase shifter 4 is for satisfying the oscillation condition. Here, this is a voltage control type including a variable capacitance diode, and the oscillation frequency of the surface acoustic wave oscillator is changed by the control voltage Vt supplied to it. I am allowed to do it.
ところが、このような電圧制御型弾性表面波発振器にお
いては、従来、その制御電圧Vtに対する発振周波数特性
の直線領域(即ち発振周波数をFとするとdF/dVtが一定
になる領域)が狭いという問題があった。より具体的に
は例えば第4図に示すように、制御電圧Vtが低い方の端
部および高い方の端部に非直線部AおよびBがそれぞれ
存在していた。However, in such a voltage control type surface acoustic wave oscillator, conventionally, there is a problem that the linear region of the oscillation frequency characteristic with respect to the control voltage Vt (that is, the region where dF / dVt is constant when the oscillation frequency is F) is narrow. there were. More specifically, for example, as shown in FIG. 4, the non-linear portions A and B are present at the lower end and the higher end of the control voltage Vt, respectively.
これを詳述すると、第4図のカーブは、具体的には、弾
性表面波遅延線6の位相特性と移相器4の制御電圧Vtに
対する位相特性との合成で決定される。More specifically, the curve in FIG. 4 is specifically determined by combining the phase characteristic of the surface acoustic wave delay line 6 and the phase characteristic of the phase shifter 4 with respect to the control voltage Vt.
ところが通常は、弾性表面波遅延線6はその位相特性が
例えば第5図に示すような直線になるように設計されて
いるので、第4図のカーブは具体的には移相器4の特性
で決定されている。However, since the surface acoustic wave delay line 6 is usually designed so that its phase characteristic becomes a straight line as shown in FIG. 5, for example, the curve of FIG. Has been decided by.
この移相器4の具体的な回路構成を第6図に示すが、前
述したように可変容量ダイオード41が用いられており、
この可変容量ダイオード41においては一般的に制御電圧
Vtが低いときには容量変化が大きく、制御電圧Vtが高い
ときには容量変化が小さくなる。その結果、移相器4の
制御電圧Vtに対する位相シフト量は例えば第7図に示す
ようになり、制御電圧Vtが低い所ではカーブの傾きが急
になり(A1部)、制御電圧Vtが高い所ではカーブの傾き
が緩やかになる(B1)。第4図のカーブにおる非直線部
AおよびBは、このような非直線部A1およびB1が反映さ
れたものである。なお、第6図中における42および43は
RFC、44および45はDCカット用コンデンサである。A concrete circuit configuration of the phase shifter 4 is shown in FIG. 6. As described above, the variable capacitance diode 41 is used,
In this variable capacitance diode 41, the control voltage is generally
The capacitance change is large when Vt is low, and the capacitance change is small when the control voltage Vt is high. As a result, the amount of phase shift with respect to the control voltage Vt of the phase shifter 4 becomes as shown in FIG. 7, for example, where the control voltage Vt is low, the slope of the curve becomes steep (A 1 part) and the control voltage Vt becomes The slope of the curve becomes gentle at high places (B 1 ). The non-linear portions A and B in the curve of FIG. 4 reflect such non-linear portions A 1 and B 1 . 42 and 43 in FIG. 6 are
RFC, 44 and 45 are capacitors for DC cutting.
電圧制御型弾性表面発振器の発振周波数の上記のような
非直線性は、当該発振器を、搬送波の周波数そのものを
変化させる本来の電圧制御発振器(VCO)の機能の他
に、FM音声変調を同時にかける(即ち制御電圧Vtに変調
信号を加える)例えば携帯電話、自動車電話等の用途に
用いる場合に特に問題になる。The above-mentioned non-linearity of the oscillation frequency of the voltage-controlled surface acoustic oscillator causes the oscillator to simultaneously perform FM voice modulation in addition to the function of the original voltage-controlled oscillator (VCO) that changes the carrier frequency itself. (That is, the modulation signal is added to the control voltage Vt) For example, when it is used for a mobile phone, a car phone, etc., it becomes a problem.
これは、制御電圧Vtに対する発振周波数の特性が第4図
のような場合、A、Bの中間部分では直線性が良いた
め、ここでFM変調をかけた場合は変調度は中程度である
が、もっとも周波数の低い非直線部AでFM変調をかけた
場合、カーブの傾きが急なためそのチャンネルの変調度
は深くなる。逆に周波数の高い非直線部Bではカーブの
傾きが緩いためそのチャンネルでの変調度は浅くなる。
このことは、非直線部AおよびBを含まない狭い周波数
範囲ではこの発振器は使えるが、非直線部AおよびBを
含む広い周波数範囲ではチャンネル間の変調度の偏差が
大きくなるため使えないことを意味している。This is because when the characteristic of the oscillation frequency with respect to the control voltage Vt is as shown in FIG. 4, the linearity is good in the intermediate portion between A and B, so that the modulation degree is medium when FM modulation is applied here. When FM modulation is applied to the non-linear portion A having the lowest frequency, the modulation degree of that channel becomes deep because the slope of the curve is steep. On the contrary, since the slope of the curve is gentle in the non-linear portion B having a high frequency, the modulation degree in that channel becomes shallow.
This means that this oscillator can be used in a narrow frequency range that does not include the non-linear portions A and B, but cannot be used in a wide frequency range that includes the non-linear portions A and B because the deviation of the modulation degree between channels becomes large. I mean.
そこでこの発明は、制御電圧に対する発振周波数特性の
直線領域が広い電圧制御型弾性表面波発振器を提供する
ことを主たる目的とする。Therefore, it is a primary object of the present invention to provide a voltage control type surface acoustic wave oscillator having a wide linear range of oscillation frequency characteristics with respect to a control voltage.
上記目的を達成するため、この発明の電圧制御型弾性表
面波発振器は、前記弾性表面波遅延線の位相特性を、前
記移相器の制御電圧に対する位相特性の非直線部を打ち
消すような非直線部を有するものにしたことを特徴とす
る。In order to achieve the above object, the voltage-controlled surface acoustic wave oscillator of the present invention has a phase characteristic of the surface acoustic wave delay line that is non-linear so as to cancel a non-linear portion of the phase characteristic with respect to the control voltage of the phase shifter. It is characterized by having a part.
当該電圧制御型弾性表面波発振器の制御電圧に対する発
振周波数特性は、前述したように、弾性表面波遅延線の
位相特性と移相器の制御電圧に対する位相特性との合成
で決定される。従って、弾性表面波遅延線の位相特性を
上記のようなものにすれば、互いに非直線部が相殺され
るので、当該電圧制御型弾性表面波発振器の制御電圧に
対する発振周波数特性の直線領域が広くなる。The oscillation frequency characteristic of the voltage controlled surface acoustic wave oscillator with respect to the control voltage is determined by combining the phase characteristic of the surface acoustic wave delay line and the phase characteristic of the phase shifter with respect to the control voltage, as described above. Therefore, if the phase characteristics of the surface acoustic wave delay line are set as described above, the non-linear portions are offset from each other, so that the linear region of the oscillation frequency characteristic with respect to the control voltage of the voltage controlled surface acoustic wave oscillator is wide. Become.
この実施例に係る電圧制御型弾性表面波発振器も、回路
構成的には第3図のようなものであるのでそれを参照す
るものとし、以下においては従来例との相違点を主に説
明する。The voltage control type surface acoustic wave oscillator according to this embodiment also has a circuit configuration as shown in FIG. 3, and therefore, the description will be made with reference to it. In the following, differences from the conventional example will be mainly described. .
一般的に弾性表面波遅延線6においては、周知のよう
に、その振幅特性と位相特性とを相互独立に設計するこ
とができる。Generally, in the surface acoustic wave delay line 6, its amplitude characteristic and phase characteristic can be designed independently of each other, as is well known.
従って、移相器4の特性が例えば前述した第7図に示す
ように非直線部A1およびB2を有している場合、弾性表面
遅延線6の位相特性を例えば第1図に示すように上記非
直線部A1およびB1をそれぞれ打ち消すような非直線部A2
およびB2を有するものにすると、当該発振器の制御電圧
Vtに対する発振周波数特性は、前述したように弾性表面
波遅延線6の位相特性と移相器4の位相特性との合成で
決定されるから、互いに非直線部が相殺されて、例えば
第2図に示すように直線領域の広いものになる。この実
施例ではそのような特性の弾性表面波遅延線6を設計し
て用いている。Therefore, when the characteristic of the phase shifter 4 has the non-linear portions A 1 and B 2 as shown in FIG. 7, for example, the phase characteristic of the elastic surface delay line 6 is as shown in FIG. 1, for example. to the non-linear portion a 1 and B 1 as the cancel each such non-linear portion a 2
And when the one having a B 2, the control voltage of the oscillator
Since the oscillation frequency characteristic with respect to Vt is determined by the combination of the phase characteristic of the surface acoustic wave delay line 6 and the phase characteristic of the phase shifter 4 as described above, the non-linear portions are canceled by each other. As shown in, the linear area becomes wide. In this embodiment, the surface acoustic wave delay line 6 having such characteristics is designed and used.
尚、弾性表面波遅延線6を構成するIDTが中心に対して
点対称の場合(重み付けをした場合)、あるいは正規形
IDTの場合(これは当然線対称である)、当該弾性表面
波遅延線6の位相特性は第5図に示したように直線にな
る。従って弾性表面波遅延線6の位相特性に上記のよう
な非直線部A2およびB2を持たせるには、具体的には、例
えばIDTに対する重み付けを点対称から若干ずらせる等
すれば良い。It should be noted that if the IDT that constitutes the surface acoustic wave delay line 6 is point-symmetric with respect to the center (when weighted), or if it is in the normal form.
In the case of IDT (which is naturally line symmetric), the phase characteristic of the surface acoustic wave delay line 6 becomes a straight line as shown in FIG. Therefore, in order to give the phase characteristics of the surface acoustic wave delay line 6 the above-mentioned non-linear portions A 2 and B 2 , specifically, for example, the weighting for the IDT may be slightly shifted from the point symmetry.
以上のようにこの発明によれば、弾性表面遅延線の位相
特性を、移相器の制御電圧に対する位相特性の非直線部
を打ち消すような非直線部を有するものにしたので、当
該電圧制御型弾性表面波発振器の制御電圧に対する発振
周波数特性の直線領域が広くなる。As described above, according to the present invention, the phase characteristic of the surface acoustic delay line has the non-linear portion that cancels the non-linear portion of the phase characteristic with respect to the control voltage of the phase shifter. The linear region of the oscillation frequency characteristic with respect to the control voltage of the surface acoustic wave oscillator becomes wider.
その結果例えば、当該発振器を用いれば、自動車電話等
のFM式の移動無線においてチャンネル間の変調度の偏差
が少なくなり、質の良い電波を出すことができるように
なる。As a result, for example, when the oscillator is used, the deviation of the modulation degree between channels is reduced in an FM mobile radio such as a car telephone, and a good quality radio wave can be emitted.
また、電圧制御型弾性表面波発振器は一般的に周波数可
変帯域幅が狭いと言われているが、この発明の発振器に
よれば、従来使えなかった部分も可変帯域に加えること
ができるので、周波数可変帯域幅を増加させることがで
きるようになる。Further, it is said that the voltage control type surface acoustic wave oscillator generally has a narrow frequency variable bandwidth. However, according to the oscillator of the present invention, it is possible to add a part which cannot be used conventionally to the variable band. The variable bandwidth can be increased.
第1図は、この発明の一実施例に係る電圧制御型弾性表
面波発振器における弾性表面波遅延線の振幅および位相
特性の一例を示す図である。第2図は、同電圧制御型弾
性表面波発振器の制御電圧に対する発振周波数特性の一
例を示す図である。第3図は、電圧制御型弾性表面波発
振器の一例を示すブロック図である。第4図は、従来の
電圧制御型弾性表面波発振器の制御電圧に対する発振周
波数特性の一例を示す図である。第5図は、従来の電圧
制御型弾性表面波発振器における弾性表面波遅延線の振
幅および位相特性の一例を示す図である。第6図は、第
4図中の移相器の具体的な構成例を示す回路図である。
第7図は、第6図の移相器の制御電圧に対する位相シフ
ト量の一例を示す図である。 2……増幅器、4……移相器、41……可変容量ダイオー
ド、6……弾性表面波遅延線。FIG. 1 is a diagram showing an example of amplitude and phase characteristics of a surface acoustic wave delay line in a voltage control type surface acoustic wave oscillator according to an embodiment of the present invention. FIG. 2 is a diagram showing an example of oscillation frequency characteristics of the same voltage control type surface acoustic wave oscillator with respect to a control voltage. FIG. 3 is a block diagram showing an example of the voltage control type surface acoustic wave oscillator. FIG. 4 is a diagram showing an example of oscillation frequency characteristics with respect to a control voltage of a conventional voltage control type surface acoustic wave oscillator. FIG. 5 is a diagram showing an example of amplitude and phase characteristics of a surface acoustic wave delay line in a conventional voltage control type surface acoustic wave oscillator. FIG. 6 is a circuit diagram showing a specific configuration example of the phase shifter in FIG.
FIG. 7 is a diagram showing an example of the amount of phase shift with respect to the control voltage of the phase shifter of FIG. 2 ... Amplifier, 4 ... Phase shifter, 41 ... Variable capacitance diode, 6 ... Surface acoustic wave delay line.
Claims (1)
を含む電圧制御型の移相器と、弾性表面波遅延線とをル
ープ状に接続して構成された電圧制御型弾性表面波発振
器において、前記弾性表面波遅延線の位相特性を、前記
移相器の制御電圧に対する位相特性の非直線部を打ち消
すような非直線部を有するものにしたことを特徴とする
電圧制御型弾性表面波発振器。1. A voltage control type surface acoustic wave oscillator configured by connecting at least an amplifier, a voltage control type phase shifter including a variable capacitance diode, and a surface acoustic wave delay line in a loop shape. A voltage controlled surface acoustic wave oscillator, wherein the phase characteristic of the surface wave delay line has a non-linear portion that cancels out the non-linear portion of the phase characteristic with respect to the control voltage of the phase shifter.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11444289A JPH0680979B2 (en) | 1989-05-08 | 1989-05-08 | Voltage-controlled surface acoustic wave oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11444289A JPH0680979B2 (en) | 1989-05-08 | 1989-05-08 | Voltage-controlled surface acoustic wave oscillator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02292904A JPH02292904A (en) | 1990-12-04 |
JPH0680979B2 true JPH0680979B2 (en) | 1994-10-12 |
Family
ID=14637838
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11444289A Expired - Lifetime JPH0680979B2 (en) | 1989-05-08 | 1989-05-08 | Voltage-controlled surface acoustic wave oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0680979B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2897661B2 (en) * | 1994-11-11 | 1999-05-31 | 日本電気株式会社 | Voltage controlled SAW oscillator |
-
1989
- 1989-05-08 JP JP11444289A patent/JPH0680979B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH02292904A (en) | 1990-12-04 |
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