JPH02150112A - 90× phase shifter - Google Patents

90× phase shifter

Info

Publication number
JPH02150112A
JPH02150112A JP30455988A JP30455988A JPH02150112A JP H02150112 A JPH02150112 A JP H02150112A JP 30455988 A JP30455988 A JP 30455988A JP 30455988 A JP30455988 A JP 30455988A JP H02150112 A JPH02150112 A JP H02150112A
Authority
JP
Japan
Prior art keywords
frequency
harmonic
fundamental wave
voltage controlled
controlled 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.)
Granted
Application number
JP30455988A
Other languages
Japanese (ja)
Other versions
JP2516250B2 (en
Inventor
Yasushi Yamao
泰 山尾
Hiroichi Ishida
博一 石田
Kazuya Oki
沖 和也
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Nippon Telegraph and Telephone Corp
Original Assignee
Mitsubishi Electric Corp
Nippon Telegraph and Telephone Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp, Nippon Telegraph and Telephone Corp filed Critical Mitsubishi Electric Corp
Priority to JP63304559A priority Critical patent/JP2516250B2/en
Publication of JPH02150112A publication Critical patent/JPH02150112A/en
Application granted granted Critical
Publication of JP2516250B2 publication Critical patent/JP2516250B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To inexpensively obtain a 90 deg. phase shifter with high accuracy with simple constitution by taking out a second harmonic via a band-pass filter, and performing inversion, non-inversion and 1/2-frequency division at an amplifier circuit and a filp-flop. CONSTITUTION:The fundamental wave f1 of a voltage controlled oscillator 11 is supplied to a synthesizer 12 and a reception demodulation part 13, and simultaneously, the second harmonic f2 of the fundamental wave f1 is supplied to the amplifier circuit 15 via the band-pass filter 14. And inversion and non- inversion output obtained at the amplifier circuit 15 are supplied to the flip-flops 16 and 17, and are 1/2-frequency divided, and a signal having a phase difference of 90 deg. is taken out, then, it is outputted to a modulator 20. In such a way, it is possible to obtain the 90 deg. phase shifter with high accuracy with the simple constitution and as attaining the reduction of power consumption.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、無線機の電圧制御発振器で発生する基本周
波数の第2高調波から正確に90度の位相差を持った2
つの信号を出力する90度移相器に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is directed to generating two waves with a phase difference of exactly 90 degrees from the second harmonic of the fundamental frequency generated in a voltage controlled oscillator of a radio.
This relates to a 90 degree phase shifter that outputs two signals.

[従来の技術] 第6図は90度位相が異なる2つの信号を取り出す従来
の90度分配器を示すブロック接続図であり、図におい
て、1.2はDフリップフロップで、これがデータ端子
りに°H°°または°°L”レベルの信号が加わってい
る状態でトリガ端子Tに“H”レベルの信号が入ると、
Q端子にD端子の情報を出力し、一方向端子にはD端子
の信号を反転した信号を出力する。3はクロック入力端
子、5.7は出力端子である。
[Prior Art] Fig. 6 is a block connection diagram showing a conventional 90-degree divider that takes out two signals having a phase difference of 90 degrees. In the figure, 1.2 is a D flip-flop, which is connected to a data terminal. When a “H” level signal is input to the trigger terminal T while a “H°°” or “°°L” level signal is being applied,
Information of the D terminal is output to the Q terminal, and a signal obtained by inverting the signal of the D terminal is output to the one-way terminal. 3 is a clock input terminal, and 5.7 is an output terminal.

次に動作について、第7図のタイミング図について説明
する。まず、クロック入力端子3に、第7図(a)に示
すクロックパルスを入力すると、各Dフリップフロップ
1,2のQ端子に、第7図(b)、(c)に示す信号が
出力され、上記クロックパルス4個で、各Q端子に1周
期の波形を出力する。
Next, the operation will be explained with reference to the timing chart shown in FIG. First, when the clock pulse shown in FIG. 7(a) is input to the clock input terminal 3, the signals shown in FIG. 7(b) and (c) are output to the Q terminal of each D flip-flop 1 and 2. , a one-cycle waveform is output to each Q terminal using the four clock pulses.

いま、2つのQ端子の信号波形に注目すると、上記クロ
ックパルスの1周期は各Q端子の出力波形に対して1/
4周期となり、角度で示すと、π/2ラジアン、90度
となる。また、各Q端子の出力波形の位相差はクロック
パルス波形の1周期分のずれであるので、90度の位相
差を取り出せることになる。
Now, if we pay attention to the signal waveforms of the two Q terminals, one period of the clock pulse is 1/1 of the output waveform of each Q terminal.
There are four periods, and the angle is π/2 radian or 90 degrees. Furthermore, since the phase difference between the output waveforms of each Q terminal is a shift of one period of the clock pulse waveform, a phase difference of 90 degrees can be extracted.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来の90度移相器は以上のように構成されているので
、基本波である周波数fの90度位相差を取り出す場合
には、周波数fの4倍周波数のクロックパルスを必要と
するためDフリップフロップ1.2での消費電力が大き
くなるほか、周波数fが高くなると4倍の周波数を取り
出すのが容易でなくなるなどの問題点があった。
Since the conventional 90-degree phase shifter is configured as described above, in order to extract the 90-degree phase difference of the frequency f, which is the fundamental wave, a clock pulse with a frequency four times the frequency f is required. In addition to the increased power consumption in the flip-flop 1.2, there were other problems such as it became difficult to extract four times the frequency as the frequency f became higher.

なお近似技術として昭和55年度電子通信学会通信部門
全国大会No、 473に記載のものがある。
As an approximation technique, there is one described in 1981 IEICE Communications Division National Conference No. 473.

この発明は上記のような問題点を解消するためになされ
たもので、従来使用されていない無線機の電圧制御発振
器が出力する第2高調波を原信号として、これを1/2
分周することで、消費電流の低減を図りながら安定な9
0度位相差の出力信号を取り出すことができる90度移
相器を得ることを目的とする。
This invention was made to solve the above-mentioned problems, and uses the second harmonic output from the voltage controlled oscillator of a wireless device, which has not been used in the past, as the original signal, and converts it to 1/2.
By dividing the frequency, it is possible to reduce current consumption while maintaining stable 9
The object of the present invention is to obtain a 90-degree phase shifter that can extract an output signal with a 0-degree phase difference.

〔課題を解決するための手段〕 この発明に係る90度移相器は、電圧制御発振器からの
第2高調波をバンドパスフィルタを通して基本波とは分
離して取り出し、この取り出した第2高調波から、上記
基本波を基準にして90度の位相差の非反転信号および
反転信号を、増幅回路およびフリップフロップを通して
取り出すようにしたものである。
[Means for Solving the Problems] A 90 degree phase shifter according to the present invention extracts the second harmonic from a voltage controlled oscillator separately from the fundamental wave through a bandpass filter, and extracts the second harmonic from the voltage controlled oscillator separately from the fundamental wave. , a non-inverted signal and an inverted signal having a phase difference of 90 degrees with respect to the fundamental wave are extracted through an amplifier circuit and a flip-flop.

〔作用〕[Effect]

この発明における増幅回路および2つのフリップフロッ
プは、電圧制御発振器が発振する第2高調波の非反転信
号および反転信号を1/2分周して、上記電圧制御発振
器の基本波に等しい90度の位相差をもつ周波数出力と
して取り出すように作用する。
The amplifier circuit and two flip-flops of the present invention divide the second harmonic non-inverted signal and inverted signal oscillated by the voltage controlled oscillator into 1/2, and divide the frequency of the second harmonic non-inverted signal and the inverted signal into 90 degrees, which is equal to the fundamental wave of the voltage controlled oscillator. It acts to extract a frequency output with a phase difference.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を図について説明する。第1
図において、11は90度移相器30を構成する電圧制
御発振器 ##≠ポで、外部から入力される制御電圧に応じ、発振
周波数を変化させることができる。
An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, reference numeral 11 denotes a voltage controlled oscillator ##≠PO constituting the 90-degree phase shifter 30, which can change the oscillation frequency according to a control voltage input from the outside.

無線機の電圧制御発振器11は周波数が非常に安定で、
選択度の高い周波数を発振する。この電圧制御発振器1
1の発振スペクトルは、第2図に示すように、基本周波
数のN倍の周波数(高調波)を発振し、選択度(△fに
対する中心周波数Nflに比例)が高い。この電圧制御
発振器11は通常第2図に示す基本波f1のみ出力する
が、この発明では、基本波f1と基本波f1の第2高調
波(2x f−=f2)である周波数f2を90度移相
して取り出す。14はバンドパスフィルタで、第2図に
示すように、90度移相するための第2高調波f2を選
択的に取り出す。なお、周波数スペクトルで、第2図の
通り基本波f1と第3高調波f3との間は第2高調波f
2のみであるため、バンドパスフィルタ14の帯域幅は
f1/2と広い。
The voltage controlled oscillator 11 of the radio has a very stable frequency.
Oscillates a highly selective frequency. This voltage controlled oscillator 1
As shown in FIG. 2, the oscillation spectrum of No. 1 oscillates at a frequency (harmonic) that is N times the fundamental frequency, and has high selectivity (proportional to the center frequency Nfl with respect to Δf). This voltage controlled oscillator 11 normally outputs only the fundamental wave f1 shown in FIG. Phase shift and take out. Reference numeral 14 denotes a bandpass filter that selectively extracts the second harmonic f2 for phase shifting by 90 degrees, as shown in FIG. In addition, in the frequency spectrum, as shown in Figure 2, there is a second harmonic f between the fundamental wave f1 and the third harmonic f3.
2, the bandpass filter 14 has a wide bandwidth of f1/2.

15は第2高調波f2を増幅または後段のフリップフロ
ップに信号を伝えるバッファ回路としての増幅回路であ
る。なお、この増幅回路15の特性としで、前段のバン
ドパスフィルタ14を外し、本回路にバンドパスフィル
タ特性を持たせても良い。ここでは、この増幅回路15
は反転、非反転出力波形を遅延時間に差の出にくい出力
として同時に取り出す差動増幅回路としである。
Reference numeral 15 denotes an amplifier circuit as a buffer circuit that amplifies the second harmonic f2 or transmits the signal to the flip-flop at the subsequent stage. Note that the characteristics of this amplifier circuit 15 may be determined by removing the band-pass filter 14 at the previous stage and giving this circuit a band-pass filter characteristic. Here, this amplifier circuit 15
This is a differential amplifier circuit that simultaneously takes out inverted and non-inverted output waveforms as outputs with little difference in delay time.

16.17はJK型、D型などのフリップフロップで、
増幅回路15の出力を1/2分周する。
16.17 are flip-flops such as JK type and D type.
The output of the amplifier circuit 15 is divided into 1/2.

20はフリップフロップ16.17からの90度位相差
信号を受け、変調を行う変調器であり、周波数はflで
ある。
A modulator 20 receives the 90 degree phase difference signal from the flip-flops 16 and 17 and performs modulation, and the frequency is fl.

一方、12は電圧制御発振器11を含むシンセサイザで
、プリスケーラ23、分周器24、位相比較回路2・6
および温度補償発振器25からなり、チャネル制御周波
数に従った周波数安定化回路として機能する。また、1
3は受信復調部であり、受信周波数f 11と、電圧制
御発振器11の出力周波数f+をミキシングすることで
、f II−f、周波数を取り出す。
On the other hand, 12 is a synthesizer including a voltage controlled oscillator 11, a prescaler 23, a frequency divider 24, and phase comparator circuits 2 and 6.
and a temperature compensated oscillator 25, and functions as a frequency stabilizing circuit according to the channel control frequency. Also, 1
3 is a reception demodulation section, which mixes the reception frequency f11 and the output frequency f+ of the voltage controlled oscillator 11 to extract the frequency fII-f.

次に動作について説明する。まず、シンセサイザ12で
は、電圧制御発振器11の出力周波数f1を受け、プリ
スケーラ23で分周し、さらに、チャネル制御信号に応
じた分周比に分周器24を固定して周波数分周を行い、
この分周出力と温度補償発振器25の出力との位相比較
(周波数比較)を位相比較回路26にて行い。位相差に
応じた出力にもとづき、電圧制御発振器11の発振周波
数を制御し、シンセサイザ12として安定な発振周波数
を出力する。
Next, the operation will be explained. First, in the synthesizer 12, the output frequency f1 of the voltage controlled oscillator 11 is received, the frequency is divided by the prescaler 23, and the frequency divider 24 is fixed to a frequency division ratio according to the channel control signal to perform frequency division.
The phase comparison circuit 26 performs a phase comparison (frequency comparison) between this frequency-divided output and the output of the temperature compensation oscillator 25. The oscillation frequency of the voltage controlled oscillator 11 is controlled based on the output according to the phase difference, and a stable oscillation frequency is output as the synthesizer 12.

また、電圧制御発振器11は第2図に示す周波数スペク
トルの通り、基本波で1のN倍の周波数の信号を出力し
、f1/△fに比例する選択度が非常に高い特徴がある
。この発明では、電圧制御発振器11の出力波形図中、
基本波であるflを上記シンセサイザ12と受信復調部
13に取り込み、受信周波数f、から周波数f、引いた
f。
Further, as shown in the frequency spectrum shown in FIG. 2, the voltage controlled oscillator 11 outputs a signal having a frequency of 1 N times as a fundamental wave, and has a very high selectivity proportional to f1/Δf. In this invention, in the output waveform diagram of the voltage controlled oscillator 11,
The fundamental wave fl is taken into the synthesizer 12 and the reception demodulator 13, and the frequency f is subtracted from the reception frequency f.

f+の周波数を、この受信復調部13のミクサ27を通
して取り出す。
The f+ frequency is extracted through the mixer 27 of the receiving demodulator 13.

また、シンセサイザ12の電圧制御発振器11を含む9
0度移相器30は、電圧制御発振器11から発生する第
2図に示す波形から、基本波f1の2倍周波数である第
2高調波f、を、バンドパスフィルタ14を通して取り
出す。この第2高調波f2は基本波で1と同様選択度の
高い安定した周波数で、その第2高調波f2を増幅回路
15で増幅しくフリップフロップ16.17が駆動でき
れば1倍以下の増幅度でも良い)、第3図(a)、(b
)に示すように、第2高調波f2から非反転、反転信号
を非反転出力端子31および反転出力端子32より出力
する。
In addition, 9 including the voltage controlled oscillator 11 of the synthesizer 12
The 0 degree phase shifter 30 extracts the second harmonic f, which is twice the frequency of the fundamental wave f1, from the waveform shown in FIG. 2 generated by the voltage controlled oscillator 11 through the bandpass filter 14. This second harmonic f2 is a fundamental wave and has a stable frequency with high selectivity like the first harmonic, and if the second harmonic f2 can be amplified by the amplifier circuit 15 and the flip-flops 16 and 17 can be driven, even if the amplification degree is 1 times or less. Good), Figure 3 (a), (b
), non-inverted and inverted signals from the second harmonic f2 are output from the non-inverted output terminal 31 and the inverted output terminal 32.

そして、フリップフロップ16.17はこれらの信号を
受けて出力端子18.19に、第3図(C)、(d)に
示す信号を出力する。これら第3図(c)、(d)に示
す信号波形は基本波f1の周波数で、この基本波f1の
周波数を基準にして、90度の位相差を持つことになる
The flip-flops 16.17 receive these signals and output the signals shown in FIGS. 3(C) and 3(d) to the output terminals 18.19. The signal waveforms shown in FIGS. 3(c) and 3(d) have the frequency of the fundamental wave f1, and have a phase difference of 90 degrees with respect to the frequency of the fundamental wave f1.

このように、電圧制御発振器11が非常に安定した周波
数で、基本波f1のN倍しか出ないことから、バンドパ
スフィルタ4のフィルタ特性が少々悪くても、f2の領
域さえ通過する特性であれば、第3図の第2高調波f2
の波形は正弦波に近く、反転、非反転波形に遅延時間の
差が生じない。また、フリップフロップ16.17は同
一回路を使用することから、非常に精度の高い90度移
相器を提供できる。
In this way, since the voltage controlled oscillator 11 outputs only N times the fundamental wave f1 at a very stable frequency, even if the filter characteristics of the bandpass filter 4 are a little bad, the characteristics can pass even the f2 region. For example, the second harmonic f2 in Fig. 3
The waveform is close to a sine wave, and there is no difference in delay time between inverted and non-inverted waveforms. Furthermore, since the flip-flops 16 and 17 use the same circuit, a highly accurate 90 degree phase shifter can be provided.

このように、この発明では電圧制御発振器11の基本波
f1をシンセサイザ12および受信復調部13に供給す
ると同時に、基本波f1の第2高調波f2を、バンドパ
スフィルタ14を通して増幅回路15に供給し、この増
幅回路15で得た反転、非反転出力をフリップフロップ
16゜17に供給してl/2分周することにより、90
度の位相差を持つ信号を取り出し、これを変調器20へ
出力している。
As described above, in the present invention, the fundamental wave f1 of the voltage controlled oscillator 11 is supplied to the synthesizer 12 and the reception demodulator 13, and at the same time, the second harmonic wave f2 of the fundamental wave f1 is supplied to the amplifier circuit 15 through the bandpass filter 14. , by supplying the inverted and non-inverted output obtained from this amplifier circuit 15 to the flip-flop 16°17 and dividing the frequency by l/2, 90
A signal having a phase difference of degrees is extracted and outputted to the modulator 20.

なお、上記実施例では増幅回路15から反転、非反転信
号の2出力を出す場合について示したが、第4図に示す
ように増幅回路15から非反転信号(または反転信号)
のみを取り出し、フリップフロップ16.17の出力を
一方は立ち下がり、他方は立ち上がるように動作させる
ことにより、上記実施例と同様の効果を得ることができ
る。ここで、33はフリップフロップ16と逆の立ち下
がりまたは、立ち上がり動作するフリップフロップであ
る。
In the above embodiment, the amplifier circuit 15 outputs two outputs, an inverted signal and a non-inverted signal, but as shown in FIG.
The same effect as in the above embodiment can be obtained by taking out only the outputs of the flip-flops 16 and 17 and operating the outputs of the flip-flops 16 and 17 so that one falls and the other rises. Here, 33 is a flip-flop that operates in a falling or rising direction opposite to that of the flip-flop 16.

また、第4図の実施例では2つのフリップフロップ16
.33を設けたものを示したが、第5図に示すようにマ
スタフリップフロップ34とスレーブフリップフロップ
35とを直列接続して、マスタフリップフロップ34の
出力とスレーブフリップフロップ35の出力とから90
度位相差の信号を取り出すようにしてもよく、上記実施
例と同様の効果を奏する。
Further, in the embodiment of FIG. 4, two flip-flops 16
.. Although the master flip-flop 34 and the slave flip-flop 35 are connected in series as shown in FIG.
It is also possible to extract a degree phase difference signal, and the same effect as in the above embodiment can be obtained.

〔発明の効果] 以上のように、この発明によれば従来使用されていなか
った無線機などの電圧制御発振器内の第2高調波をバン
ドパスフィルタを通して取り出し、さらに増幅回路およ
びフリップフロップで反転、非反転しかつ1/2分周す
るように構成したので、非常に高精度な90度移相器を
簡単な構成にて、かつ安価に実現できるものが得られる
効果がある。
[Effects of the Invention] As described above, according to the present invention, the second harmonic in a voltage controlled oscillator of a wireless device, which has not been used in the past, is extracted through a bandpass filter, and further inverted using an amplifier circuit and a flip-flop. Since the structure is configured to perform non-inversion and 1/2 frequency division, there is an effect that a highly accurate 90-degree phase shifter can be realized with a simple structure and at low cost.

また、かかる90度移相器を用いれば電圧制御発振器の
出力周波数f1の2倍であるf2から、90度位相差を
持つf、周波数を作り出し、他方受信復調部に入って来
る周波数f++と上記f、とをミキシングすることで、
周波数を落とす(f++−fl)ことができ、無線機と
して回路の簡単化が容易になるものが得られる効果があ
る。
In addition, if such a 90 degree phase shifter is used, a frequency f having a 90 degree phase difference is created from f2 which is twice the output frequency f1 of the voltage controlled oscillator, and the frequency f++ entering the reception demodulator and the above By mixing f,
This has the effect that the frequency can be lowered (f++-fl) and a radio device whose circuit can be easily simplified.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの本発明の一実施例による90度移相器を示
すブロック接続図、第2図は電圧制御発振器の発振信号
の周波数スペクトラム図、第3図は第1図の回路各部の
信号波形を示すタイミングチャート、第4図は90度移
相器の他の実施例を示すブロック接続図、第5図は90
度移相器のさらに他の実施例を示すブロック接続図、第
6図は従来の90度分配器を示すブロック接続図、第7
図は第6図の各部の信号波形図を示すタイミングチャー
トである。 11は電圧制御発振器 14はバンドパスフィルタ、15は増幅回路、16.1
7.33,34.35はフリップフロップ。 なお、 を示す。 図中、 同一符号は同一、
Figure 1 is a block connection diagram showing a 90 degree phase shifter according to an embodiment of the present invention, Figure 2 is a frequency spectrum diagram of the oscillation signal of the voltage controlled oscillator, and Figure 3 is a signal diagram of each part of the circuit in Figure 1. A timing chart showing waveforms, Fig. 4 is a block connection diagram showing another embodiment of a 90 degree phase shifter, and Fig. 5 shows a 90 degree phase shifter.
FIG. 6 is a block connection diagram showing still another embodiment of the degree phase shifter; FIG. 6 is a block connection diagram showing a conventional 90 degree divider; FIG.
This figure is a timing chart showing signal waveform diagrams of each part in FIG. 6. 11 is a voltage controlled oscillator, 14 is a band pass filter, 15 is an amplifier circuit, 16.1
7.33 and 34.35 are flip-flops. In addition, is shown. In the figure, the same symbols are the same.

Claims (1)

【特許請求の範囲】[Claims] 基本波とこの基本波の第2高調波を発生する無線機の電
圧制御発振器と、上記第2高調波を上記基本波とは分離
して取り出すバンドパスフィルタと、このバンドパスフ
ィルタから得た第2高調波から、上記基本波を基準にし
て90度の位相差の非反転信号および反転信号を取り出
す増幅回路およびフリップフロップとを備えた90度移
相器。
A voltage controlled oscillator of a radio device that generates a fundamental wave and a second harmonic of the fundamental wave; a bandpass filter that extracts the second harmonic separately from the fundamental wave; and a bandpass filter that extracts the second harmonic separately from the fundamental wave; A 90 degree phase shifter comprising an amplifier circuit and a flip-flop for extracting a non-inverted signal and an inverted signal having a phase difference of 90 degrees with respect to the fundamental wave from the second harmonic.
JP63304559A 1988-12-01 1988-12-01 90 degree phase shifter Expired - Lifetime JP2516250B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63304559A JP2516250B2 (en) 1988-12-01 1988-12-01 90 degree phase shifter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63304559A JP2516250B2 (en) 1988-12-01 1988-12-01 90 degree phase shifter

Publications (2)

Publication Number Publication Date
JPH02150112A true JPH02150112A (en) 1990-06-08
JP2516250B2 JP2516250B2 (en) 1996-07-24

Family

ID=17934452

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63304559A Expired - Lifetime JP2516250B2 (en) 1988-12-01 1988-12-01 90 degree phase shifter

Country Status (1)

Country Link
JP (1) JP2516250B2 (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5734729U (en) * 1980-07-31 1982-02-24
JPS59201518A (en) * 1983-04-28 1984-11-15 Shinko Electric Co Ltd Two-phase oscillating circuit
JPS61281627A (en) * 1985-06-06 1986-12-12 Matsushita Electric Ind Co Ltd Receiver

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5734729U (en) * 1980-07-31 1982-02-24
JPS59201518A (en) * 1983-04-28 1984-11-15 Shinko Electric Co Ltd Two-phase oscillating circuit
JPS61281627A (en) * 1985-06-06 1986-12-12 Matsushita Electric Ind Co Ltd Receiver

Also Published As

Publication number Publication date
JP2516250B2 (en) 1996-07-24

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