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JP4370577B2 - Signal extraction method and signal extraction circuit - Google Patents
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JP4370577B2 - Signal extraction method and signal extraction circuit - Google Patents

Signal extraction method and signal extraction circuit Download PDF

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JP4370577B2
JP4370577B2 JP2005034315A JP2005034315A JP4370577B2 JP 4370577 B2 JP4370577 B2 JP 4370577B2 JP 2005034315 A JP2005034315 A JP 2005034315A JP 2005034315 A JP2005034315 A JP 2005034315A JP 4370577 B2 JP4370577 B2 JP 4370577B2
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signal extraction
target signal
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carrier wave
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JP2006222736A (en
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達也 上野
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Azbil Corp
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Description

本発明は、搬送波に微小な信号が重畳した変調波から上記信号の成分を抽出するに好適な信号抽出方法および信号抽出回路に関する。   The present invention relates to a signal extraction method and a signal extraction circuit suitable for extracting a component of the signal from a modulated wave in which a minute signal is superimposed on a carrier wave.

比較的低い周波数を持つ搬送波に比較的高い周波数を持つ微小な信号を重畳させた変調波は、様々な分野で用いられている。尚、一般的な意味での“信号”と区別するべく、上述したように搬送波に重畳された信号をここでは特に“対象信号”と称することにする。そして上述した変調波から対象信号を抽出するに際しては、演算増幅器(いわゆるオペアンプ)を利用した微分回路を用いることが考えられている。   A modulated wave in which a minute signal having a relatively high frequency is superimposed on a carrier wave having a relatively low frequency is used in various fields. In order to distinguish from a “signal” in a general sense, a signal superimposed on a carrier wave as described above is specifically referred to as a “target signal” herein. When extracting a target signal from the above-described modulated wave, it is considered to use a differentiation circuit using an operational amplifier (so-called operational amplifier).

ちなみに一般的な微分回路は、例えば図8において破線枠内に示すように、信号が入力される反転入力端子IN-、基準電圧Vrefが入力される非反転入力端子IN+、および正負の直流電源入力端子とを備えた演算増幅器(オペアンプ)OPと、この演算増幅回路OPの反転入力端子に直列接続された微分用コンデンサC1および入力抵抗器R1と、上記演算増幅器OPの出力端子と反転入力端子IN-との間に接続された帰還抵抗器R2および高周波除去用コンデンサCncとを備えて構成される。そして処理対象とする変調波を上記入力抵抗器R1からコンデンサC1を介して演算増幅器OPの反転入力端子IN-に入力し、該演算増幅器OPの出力として対象信号を得るように用いられる。 Incidentally, a general differentiating circuit includes, for example, an inverting input terminal IN to which a signal is input, a non-inverting input terminal IN + to which a reference voltage Vref is input, and a positive / negative DC power supply as shown in a broken line frame in FIG. An operational amplifier (opamp) OP having an input terminal, a differentiation capacitor C1 and an input resistor R1 connected in series to the inverting input terminal of the operational amplifier circuit OP, and an output terminal and an inverting input terminal of the operational amplifier OP iN - configured with connected and a feedback resistor R2 and the high frequency eliminating capacitor Cnc between. The modulated wave to be processed is input from the input resistor R1 through the capacitor C1 to the inverting input terminal IN of the operational amplifier OP, and used as an output of the operational amplifier OP.

ここで上記微分用コンデンサC1の容量をc1、入力抵抗器R1の抵抗値をr1、帰還抵抗器R2の抵抗値をr2、そして高周波除去用コンデンサCncの容量をcncとすると、上記微分回路における微分動作(入力信号の周波数と利得との比例関係)のカットオフ周波数fiは
fi=1/(2π・r1・c1)
となり、また高周波除去のカットオフ周波数foは
fo=1/(2π・r2・cnc)
となる。このような微分回路を前述した対象信号の抽出に用いる場合、上記微分上限周波数fiは搬送波の周波数よりも高く、且つ対象信号の周波数よりも低くなるように設定される。また高周波除去のカットオフ周波数foは対象信号の周波数よりも高くなるように設定される。
Here, when the capacitance of the differentiation capacitor C1 is c1, the resistance value of the input resistor R1 is r1, the resistance value of the feedback resistor R2 is r2, and the capacitance of the high frequency removing capacitor Cnc is cnc, the differentiation in the differentiation circuit is performed. Cut-off frequency fi of operation (proportional relationship between input signal frequency and gain) is fi = 1 / (2π · r1 · c1).
The cutoff frequency fo for high frequency rejection is fo = 1 / (2π · r 2 · cnc)
It becomes. When such a differentiation circuit is used for the extraction of the target signal described above, the differentiation upper limit frequency fi is set to be higher than the frequency of the carrier wave and lower than the frequency of the target signal. Further, the cutoff frequency fo for high frequency removal is set to be higher than the frequency of the target signal.

ところでこのように構成された微分回路に、例えば図9(a)に示すような矩形波からなる搬送波を微小な対象信号で変調した変調波を入力すると、その出力信号は図9(b)に信号波形aとして示すようになる。即ち、時刻Aにおいて変調波が大きく変化すると、演算増幅器OPの出力信号が瞬時に増加する。これに伴ってコンデンサC1,Cncにそれぞれ電荷が蓄積され、これらのコンデンサC1,Cncにそれぞれ蓄積された電荷は、入力抵抗器R1および帰還抵抗器R2をそれぞれ通して徐々に放電される。これ故、信号波形aに示すように上記出力信号がそのベースライン(0V)付近まで復帰するまでに多大な時間が掛かることが否めない。つまり出力信号の復帰時間が長いので、ベースラインを基準として対象信号を判別できるようになるまでに長い時間を要することになる。   By the way, when a modulated wave obtained by modulating a carrier wave composed of a rectangular wave as shown in FIG. 9A, for example, with a minute target signal is input to the differentiating circuit configured as described above, the output signal is shown in FIG. 9B. This is shown as a signal waveform a. That is, when the modulation wave changes greatly at time A, the output signal of the operational amplifier OP increases instantaneously. Accordingly, charges are accumulated in the capacitors C1 and Cnc, respectively, and the charges accumulated in these capacitors C1 and Cnc are gradually discharged through the input resistor R1 and the feedback resistor R2, respectively. Therefore, it cannot be denied that it takes a long time for the output signal to return to the vicinity of the base line (0 V) as shown in the signal waveform a. That is, since the return time of the output signal is long, it takes a long time before the target signal can be determined with reference to the baseline.

ちなみに帰還抵抗器R2の値を小さくすると、その出力信号は図9(b)に信号波形bとして示すようになり、ベースラインへの復帰時間を短縮することができる。しかしその反面、信号振幅が小さくなるので対象信号の検出が困難になる。即ち、一般的な微分回路においては、復帰時間短縮への要請と増幅率増大への要請とが相反するという問題がある。このような問題は上述した矩形波の場合のみならず、三角波や鋸歯状波等のようにその不連続点で大きな変化を持つ搬送波、換言すれば不連続点で大きな微分値を持つ搬送波を用いる場合にも同様に生じる。   Incidentally, when the value of the feedback resistor R2 is reduced, the output signal is shown as a signal waveform b in FIG. 9B, and the return time to the baseline can be shortened. However, on the other hand, since the signal amplitude becomes small, it becomes difficult to detect the target signal. That is, in a general differentiation circuit, there is a problem that a request for shortening the recovery time and a request for increasing the amplification factor conflict. Such a problem is not limited to the rectangular wave described above, but a carrier wave having a large change at the discontinuity point, such as a triangular wave or a sawtooth wave, in other words, a carrier wave having a large differential value at the discontinuity point is used. It happens in the same way.

特に図10(a)(b)(c)に矩形波、三角波、および正弦波をそれぞれ搬送波とした変調波を1階微分、および2階微分したときの出力信号波形をそれぞれ示すように、従来一般的な増幅器を用いた微分回路においては、その搬送波成分を十分に除去できないことのみならず、微小な信号成分を十分に増幅して抽出することができないと言う不具合がある。しかも搬送波の不連続点において、微分波形のレベルが大きく変化すると言う不具合がある。   In particular, as shown in FIGS. 10A, 10B, and 10C, output signal waveforms obtained when first-order differentiation and second-order differentiation are performed on a modulated wave having a rectangular wave, a triangular wave, and a sine wave as carrier waves, respectively. In a differentiating circuit using a general amplifier, there is a problem that not only the carrier component cannot be sufficiently removed but also a minute signal component cannot be sufficiently amplified and extracted. Moreover, there is a problem that the level of the differential waveform changes greatly at the discontinuous points of the carrier wave.

また搬送波の振幅と、この搬送波に重畳される対象信号の振幅との間に大きな差がある場合、一般的な微分回路を用いた場合には搬送波成分を十分に減衰させることができないので、出力信号中に搬送波成分が雑音として残ってしまうと言う問題がある。具体的には最も一般的な微分回路において搬送波と対象信号の周波数の比がx[dB]であっても、その振幅の比が1/x[dB]であると、そのSN比は[1]となってしまう。尚、微分回路よりも減衰傾度の大きいフィルタ回路も存在するが、応答性能が悪いので上述した問題を解決することはできない。しかも上述した方形波、三角波、鋸波等のように不連続点で大きな変化をもつ搬送波のみならず、正弦波のように滑らかな波形の搬送波の場合であっても同様な問題が生じる。   Also, if there is a large difference between the amplitude of the carrier wave and the amplitude of the target signal superimposed on this carrier wave, the carrier component cannot be sufficiently attenuated using a general differentiating circuit. There is a problem that the carrier component remains as noise in the signal. Specifically, even if the frequency ratio between the carrier wave and the target signal is x [dB] in the most general differentiating circuit, if the amplitude ratio is 1 / x [dB], the SN ratio is [1]. ]. Although there are filter circuits having a greater attenuation slope than the differentiation circuit, the above-mentioned problem cannot be solved because of poor response performance. Moreover, the same problem occurs not only in the case of a carrier wave having a large change at a discontinuous point such as the above-described square wave, triangular wave, and sawtooth wave, but also in the case of a carrier wave having a smooth waveform such as a sine wave.

一方、一般的な微分回路において、過大な微分成分を含む信号が入力されたときの復帰時間が長いという問題を解決するべく、例えば図11に示すように前述した帰還抵抗器R2と並列に、互いに逆並列接続された2つのダイオード(帰還形電圧制限手段)D1,D2を設けることが提唱されている(例えば特許文献1を参照)。上記ダイオードD1,D2は、出力信号の振幅(電圧)が上記ダイオードD1,D2の順方向バイアス電圧VLを超えたときにその出力を制限し、順方向バイアス電圧VLを超えない場合にだけ上述の従来技術とほぼ同様の動作を行わせるように機能する。
特開昭64−43765号公報
On the other hand, in order to solve the problem of a long recovery time when a signal including an excessive differential component is input in a general differential circuit, for example, as shown in FIG. 11, in parallel with the feedback resistor R2 described above, It has been proposed to provide two diodes (feedback voltage limiting means) D1 and D2 connected in antiparallel with each other (see, for example, Patent Document 1). The diodes D1 and D2 limit the output when the amplitude (voltage) of the output signal exceeds the forward bias voltage VL of the diodes D1 and D2, and only when the output signal does not exceed the forward bias voltage VL. It functions so as to perform almost the same operation as in the prior art.
JP-A 64-43765

しかしながら特許文献1に記載される微分回路は、変調波から微小な対象信号を抽出する用途への適用を想定してなされたものではない。しかし、敢えてこの種の用途に特許文献1に示される微分回路を適用することを想定すると、次のような問題が生じる。即ち、前述した図8に示した従来一般的な微分回路において、電源能力の限界に達して演算増幅器OPの出力が飽和するほどの過大な微分成分を含む信号が入力されたときには、その出力信号は、例えば図12に信号波形cとして示すようになり、その復帰時間が長くなる。この点、特許文献1に示される微分回路によれば、入力信号に過大な微分成分が含まれるときには前述した帰還形電圧制限手段(ダイオードD1,D2)によって出力信号が抑制されるので、その出力信号は図12に信号波形dとして示すようになる。従って入力信号に過大な微分成分が含まれないときと比べてその復帰時間があまり増加することはない。   However, the differentiating circuit described in Patent Document 1 is not intended for application to extract a minute target signal from a modulated wave. However, assuming that the differentiating circuit shown in Patent Document 1 is applied to this type of application, the following problems arise. In other words, in the conventional general differentiation circuit shown in FIG. 8 described above, when a signal including an excessive differential component that reaches the limit of the power supply capacity and saturates the output of the operational amplifier OP is input, Is, for example, shown as a signal waveform c in FIG. 12, and its recovery time becomes longer. In this regard, according to the differentiation circuit disclosed in Patent Document 1, when an excessive differential component is included in the input signal, the output signal is suppressed by the feedback voltage limiting means (diodes D1, D2) described above. The signal is shown as a signal waveform d in FIG. Therefore, the recovery time does not increase much compared to when the input signal does not contain an excessive differential component.

換言すれば帰還形電圧制限手段(ダイオードD1,D2)を備えることによって入力信号に過大な微分成分が含まれる場合には、図8に示した従来一般的な微分回路に比較して復帰時間を短縮することができる。しかしそれ以外の場合には、図12に示す信号波形dが前述した図9(b)に示す信号波形aに相当するように、従来回路とほぼ同様に動作するので、前述した復帰時間短縮の要請と増幅率増大の要請とのトレード・オフの関係が依然として残る。これ故、搬送波成分の影響により微小な対象信号を正確に抽出できないと言う問題を解消することはできない。   In other words, when the input signal includes an excessive differential component by providing the feedback voltage limiting means (diodes D1, D2), the recovery time is shorter than that of the conventional general differential circuit shown in FIG. It can be shortened. However, in other cases, since the signal waveform d shown in FIG. 12 corresponds to the signal waveform a shown in FIG. 9B, the operation is almost the same as that of the conventional circuit. The trade-off relationship between the demand and the demand for increasing the amplification factor still remains. Therefore, the problem that a minute target signal cannot be accurately extracted due to the influence of the carrier component cannot be solved.

本発明はこのような事情を考慮してなされたもので、その目的は、搬送波に重畳した微小な対象信号を増幅して確実に抽出することのできる簡易な構成の信号抽出方法および信号抽出回路を提供することにある。   The present invention has been made in consideration of such circumstances, and its object is to provide a signal extraction method and a signal extraction circuit with a simple configuration capable of amplifying and reliably extracting a minute target signal superimposed on a carrier wave. Is to provide.

本発明の基本的な技術的思想は、変調波から微小な対象信号を抽出するに際して、上述した復帰時間短縮への要請を捨てて復帰時間を長くすると共に、出力信号の絶対値が減少する方向への変化に対してはその反応を敏感にし、逆に出力信号の絶対値が増加する方向への変化に対してはその反応を鈍感にし、これによって変調波に含まれる対象信号成分のうち、ベースラインに近い側を強調して捉えようとするものである。   The basic technical idea of the present invention is that, when a minute target signal is extracted from a modulated wave, the request for shortening the recovery time described above is discarded, the recovery time is lengthened, and the absolute value of the output signal is decreased. Sensitive to the change to, and conversely insensitive to the change to the direction in which the absolute value of the output signal increases, among the target signal components included in the modulated wave, It tries to emphasize the side closer to the baseline.

即ち、一般的な微分回路に対する要請は、専ら、増幅率を大きくし、放電時定数を短くすることであるが、本発明においては微分回路の増幅率を極大化すると共に、その放電時定数も極大化するようにしている。そして一般的な微分回路において搬送波を除去する場合には、専ら『搬送波の変化が小さいときには、その出力をできるだけ早くゼロにする』ようにしているが、本発明においては『搬送波の変化が小さいとき、出力の変化をできるだけ小さくする』ものとなってる。これらの技術思想の違いは、出力の“値”に注目するか、その“変化”に注目するかの違いである。   That is, the request for a general differentiation circuit is to increase the amplification factor and shorten the discharge time constant, but in the present invention, the amplification factor of the differentiation circuit is maximized and the discharge time constant is also increased. I try to maximize it. When removing a carrier wave in a general differentiating circuit, exclusively, “when the change in the carrier wave is small, the output is made zero as soon as possible”, but in the present invention, “when the carrier wave change is small , Make changes in output as small as possible. The difference between these technical ideas is whether to focus on the “value” of the output or on the “change”.

ちなみに搬送波の不連続点では搬送波と信号成分のSN比は略[1]であり、その区別が付き難い。しかし搬送波に変化がないところでは、信号成分に対する増幅率を十分大きく取れば、搬送波の影響は単に不連続点直後における出力のベクトルがどこからスタートするかと言うことだけであり、その初期値が多少ずれるに過ぎない。従って搬送波の変化が小さいとき、出力の変化をできるだけ小さくすることで信号成分を確実に抽出することが可能となる。   By the way, at the discontinuity point of the carrier wave, the SN ratio of the carrier wave and the signal component is approximately [1], and it is difficult to distinguish them. However, when there is no change in the carrier wave, if the amplification factor for the signal component is sufficiently large, the influence of the carrier wave is simply to say where the output vector immediately after the discontinuity starts, and its initial value deviates somewhat. Only. Therefore, when the change in the carrier wave is small, the signal component can be reliably extracted by making the change in the output as small as possible.

そこで本発明に係る信号抽出方法は、請求項1に記載するように対象信号よりも低い基本周波数成分を有し、且つ上記対象信号よりも大きい微分値、または前記対象信号よりも大きい振幅を含む搬送波に前記対象信号を重畳した変調波、例えば矩形波や三角波に微小信号を重畳した変調波から前記対象信号(微小信号)の信号成分を抽出するに際して、上記変調波を微分処理した後、得られた微分値が大きいときには対数変換機能を支配的にすると共に、前記微分値が小さいときには積分機能を支配的にして前記微分値に対して対数変換処理積分処理とを同時に施すことを特徴としている。 Therefore, the signal extraction method according to the present invention includes a fundamental frequency component lower than that of the target signal and includes a differential value larger than the target signal or an amplitude larger than the target signal. When extracting a signal component of the target signal (micro signal) from a modulated wave in which the target signal is superimposed on a carrier wave, for example, a modulated wave in which a micro signal is superimposed on a rectangular wave or a triangular wave, the modulation signal is obtained after differential processing. The logarithmic conversion function is dominant when the differential value is large, and the integral function is dominant when the differential value is small , and logarithmic conversion processing and integration processing are simultaneously performed on the differential value . Yes.

ちなみに上記対数変換処理および積分処理は、自己インピーダンスが高いとき(高抵抗領域)には積分機能が支配的となり、自己インピーダンスが低いとき(低抵抗領域)には対数変換機能が支配的となる対数変換特性を有する増幅器を用いて同時に実行する。尚、上記「支配的」とは、前記微分値に対して積分機能と対数変換機能のどちらが強く作用するかを指す。また上記対象信号の信号成分とは、対象信号そのものを抽出することのみならず、対象信号が持つ情報の一部、具体的には対象信号が閾値(例えばベースライン)を横切るタイミングとその変化の方向の情報を抽出するような場合を示している。 By the way, in the logarithmic transformation process and the integration process, when the self-impedance is high (high resistance region), the integration function is dominant, and when the self-impedance is low (low resistance region), the logarithmic transformation function is dominant. Simultaneously using an amplifier having conversion characteristics . The term “dominant” refers to which of the integration function and the logarithmic conversion function strongly acts on the differential value. The signal component of the target signal not only extracts the target signal itself, but also a part of the information held by the target signal, specifically, the timing at which the target signal crosses a threshold (for example, the baseline) and the change in the information. This shows a case where direction information is extracted.

特に本発明に係る信号抽出方法は、請求項2に記載するように前記対数変換処理および積分処理については、抽出する対象信号の経時的な変化が、その抽出された対象信号が山から谷、または谷から山へ移行する際、必ず一定の閾値を通過するように実行することが望ましい。尚、上述した一定の閾値とは典型的には0Vのベースラインであるが、ベースラインからオフセットを与えたものであっても良い。   In particular, in the signal extraction method according to the present invention, as to the logarithmic transformation process and the integration process, the change over time of the target signal to be extracted is such that the extracted target signal is a mountain to valley, Alternatively, it is desirable to execute so as to pass through a certain threshold value when shifting from a valley to a mountain. Note that the above-described constant threshold is typically a baseline of 0V, but may be an offset from the baseline.

また請求項3に記載するように前記微分処理をコンデンサを用いて実行すると共に、前記対数変換処理および積分処理を、少なくとも逆並列接続された一対の半導体接合を用いて帰還インピーダンスを定めた帰還形増幅器を用いて実行することが望ましい。更には請求項4に記載するように抽出された信号を変調波と看做して、上述した信号抽出方法を複数回繰り返すことも有用である。   In addition, the differential processing is performed using a capacitor as described in claim 3, and the logarithmic conversion processing and integration processing are performed using a feedback type in which feedback impedance is determined using at least a pair of semiconductor junctions connected in antiparallel. It is desirable to carry out using an amplifier. Furthermore, it is also useful to repeat the signal extraction method described above a plurality of times by regarding the extracted signal as a modulated wave as described in claim 4.

また本発明に係る信号抽出回路は、請求項5に記載するように対象信号よりも低い基本周波数成分を有し、且つ上記対象信号よりも大きい微分値、または前記対象信号よりも大きい振幅を含む搬送波に前記対象信号を重畳した変調波から前記対象信号の信号成分を抽出するものであって、信号入力端子および基準入力端子を備えると共に、コンデンサを介して入力された変調波を増幅して出力する増幅器と、この増幅器の出力を該増幅器の信号入力端子に帰還する帰還手段とを備え、前記帰還手段を、前記増幅器の入出力間の電圧が小さいときにはインピーダンスが大きくなり、前記増幅器の入出力間の電圧が大きいときにはインピーダンスが大きくなるように自己のインピーダンスを指数関数的に変化させるものとして構成することを特徴としている。 The signal extraction circuit according to the present invention includes a fundamental frequency component lower than that of the target signal and includes a differential value larger than the target signal or an amplitude larger than the target signal. A signal component of the target signal is extracted from a modulated wave in which the target signal is superimposed on a carrier wave. The signal component includes a signal input terminal and a reference input terminal, and amplifies and outputs the modulated wave input through a capacitor. And an amplifier that feeds back the output of the amplifier to a signal input terminal of the amplifier. The feedback means has an impedance that increases when a voltage between the input and output of the amplifier is small. characterized in that the arrangement as to change the self-impedance exponentially so that the impedance becomes large when the voltage between a large It is.

好ましくは請求項6に記載するように前記帰還手段は、逆並列接続された一対の半導体接合(ダイオード)として実現される。また請求項7に記載するように前記増幅器は、その入出力端子間の電圧が前記帰還手段としての逆並列接続された一対の半導体接合の導通電圧よりも小さいときには実質的に演算増幅器として、つまりゲインが一定の線形増幅器として動作し、上記入出力端子間の電圧が前記半導体接合の導通電圧よりも大きいときには実質的に比較器として動作するように構成することが望ましい。   Preferably, the feedback means is realized as a pair of semiconductor junctions (diodes) connected in antiparallel. According to a seventh aspect of the present invention, when the voltage between the input and output terminals of the amplifier is smaller than the conduction voltage of the pair of semiconductor junctions connected in reverse parallel as the feedback means, that is, as an operational amplifier, that is, It is desirable to operate as a linear amplifier with a constant gain and to operate substantially as a comparator when the voltage between the input and output terminals is larger than the conduction voltage of the semiconductor junction.

更には請求項8に記載するように前記帰還形演算増幅器における帰還手段を、逆並列接続された一対の半導体接合およびこれらの半導体接合に並列接続された高周波除去用のコンデンサだけにより構成するようにしても良い。但し、帰還手段をダイオードで構成することにより、帰還形演算増幅器を双方向のピークホールド回路と同等の機能を持つようにすることができる。この場合、帰還形演算増幅器のピークホールド動作を、概略的には積分動作と看做すことができるので、上述した高周波除去用のコンデンサを省略することも可能である。   Further, as described in claim 8, the feedback means in the feedback operational amplifier is constituted by only a pair of semiconductor junctions connected in antiparallel and a high frequency removing capacitor connected in parallel to these semiconductor junctions. May be. However, by configuring the feedback means with a diode, the feedback operational amplifier can have the same function as the bidirectional peak hold circuit. In this case, since the peak hold operation of the feedback operational amplifier can be roughly regarded as an integration operation, the above-described high frequency removing capacitor can be omitted.

また請求項9に記載するように上述した構成の信号抽出回路をひとつの構成単位として、複数の構成単位を多段に接続して用いることも有用である。この場合、ノイズ除去を行うべく、後段の微分回路において増幅制限用の抵抗を前述したダイオードと並列に設けるようにしても良い。ちなみに抵抗がない場合には、ノイズも大きく増幅されて信号と見分けが付かなくなってしまう。従ってダイオードと並列に抵抗を入れてその増幅率を制限することで、ノイズと信号との区別を容易化することが望ましい。   It is also useful to use a signal extraction circuit having the above-described configuration as one structural unit, and connect a plurality of structural units in multiple stages. In this case, in order to remove noise, an amplification limiting resistor may be provided in parallel with the aforementioned diode in the subsequent differentiation circuit. By the way, when there is no resistance, the noise is greatly amplified and cannot be distinguished from the signal. Therefore, it is desirable to facilitate the distinction between noise and signal by limiting the amplification factor by putting a resistor in parallel with the diode.

本発明に係る信号抽出方法によれば、変調波を微分処理した後、得られた微分値に対して対数変換処理および積分処理を施すので、微分処理により搬送波の不連続点で生じる大きな微分波形を抑え、上記搬送波に重畳した微小な信号成分だけを大きな増幅率で増幅することが可能となる。特に微分により不連続点での大きな変化を抑えた信号を対数変換処理および積分処理するので、その微分極性の変化に伴って上記信号を大きな増幅率で増幅して抽出することが可能となる。また対象信号の経時的な変化が、その抽出された対象信号が山から谷、または谷から山へ移行する際、必ずベースライン等の一定の閾値を通過するように対数変換処理および積分処理を実行するので、上記閾値を基準として対象信号を確実に判別することが可能となる。   According to the signal extraction method of the present invention, after differential processing of the modulated wave, logarithmic conversion processing and integration processing are performed on the obtained differential value, so that a large differential waveform generated at the discontinuity point of the carrier by the differentiation processing It is possible to amplify only a minute signal component superimposed on the carrier wave with a large amplification factor. In particular, since a signal in which a large change at a discontinuous point is suppressed by differentiation is subjected to logarithmic conversion processing and integration processing, the signal can be amplified and extracted with a large amplification factor in accordance with the change in the differential polarity. In addition, logarithmic transformation processing and integration processing are performed so that the change over time of the target signal always passes a certain threshold such as the baseline when the extracted target signal transitions from peak to valley or from valley to peak. As a result, the target signal can be reliably discriminated based on the threshold value.

また上記構成の信号抽出回路によれば、コンデンサを介して入力される信号を増幅する増幅器は、その入力信号の振幅が大きいときには増幅率を小さくし、上記入力信号の振幅が小さいときには増幅率を大きくすることで上記入力信号を対数変換する。これ故、搬送波に微小な信号成分が重畳した変調波を前記コンデンサを介して入力した場合、コンデンサによる微分処理により前記搬送波の不連続点で生じる大きな微分波形が抑えられ、一方、上記搬送波に重畳した微小な信号成分だけが大きな増幅率で増幅されることになる。従って搬送波の成分を抑制(除去)して上記搬送波に重畳している微小な信号成分を効果的に増幅して抽出することが可能となる。   According to the signal extraction circuit having the above configuration, the amplifier that amplifies the signal input through the capacitor reduces the amplification factor when the amplitude of the input signal is large, and increases the amplification factor when the amplitude of the input signal is small. The input signal is logarithmically converted by increasing the value. Therefore, when a modulated wave in which a minute signal component is superimposed on a carrier wave is input through the capacitor, a large differential waveform generated at the discontinuous point of the carrier wave is suppressed by the differentiation process by the capacitor, while being superimposed on the carrier wave. Only the small signal component thus amplified is amplified with a large amplification factor. Accordingly, it is possible to effectively amplify and extract a minute signal component superimposed on the carrier wave by suppressing (removing) the carrier wave component.

ちなみに、例えば図9(b)に示したように微分回路における通常の出力は、演算増幅器が飽和しているときには微小な信号成分も飽和するので、搬送波に重畳した微小な信号成分だけを増幅して抽出することはできない。しかし前述した構成の本発明に係る信号抽出回路(搬送波除去回路)によれば、搬送波の不連続点で生じる大きな微分波形の出力だけを抑えることができるので、搬送波に重畳した微小な信号成分を効果的に増幅して抽出することができる。   Incidentally, for example, as shown in FIG. 9B, the normal output in the differentiation circuit also saturates a minute signal component when the operational amplifier is saturated. Therefore, only the minute signal component superimposed on the carrier wave is amplified. Cannot be extracted. However, according to the signal extraction circuit (carrier wave removal circuit) according to the present invention having the above-described configuration, it is possible to suppress only the output of a large differential waveform generated at the discontinuity point of the carrier wave. It can be amplified and extracted effectively.

また上述した微分回路を、その主体をなす演算増幅器と、この演算増幅器の入力端子と出力端子との間に並列接続されて上記入力端子への入力信号レベルに応じてインピーダンスが変化するインピーダンス制御手段とにより構成すれば、具体的には上記インピーダンス制御手段に、入力信号レベルが小さいときにはインピーダンスが大きくなり、信号レベルが大きいときにはインピーダンスが小さくなるような指数関数的な変化特性を持たせることにより、対数変換特性を有する増幅器簡易に構築することができる。特にインピーダンス制御手段を、逆並列接続された一対のダイオードにより実現すれば、そのインピーダンスは微小な入力信号に対しては略無限大となり、また振幅の大なる入力信号に対しては略零[0]となるので、容易に対数変換特性を付与することが可能となる。 The differential circuit described above is an operational amplifier that is the main component of the differential circuit, and impedance control means that is connected in parallel between the input terminal and the output terminal of the operational amplifier so that the impedance changes according to the level of the input signal to the input terminal. Specifically, the impedance control means has an exponential change characteristic such that the impedance increases when the input signal level is small, and the impedance decreases when the signal level is large. an amplifier having a logarithmic conversion characteristic can be constructed easily. In particular, when the impedance control means is realized by a pair of diodes connected in antiparallel, the impedance becomes substantially infinite for a minute input signal, and substantially zero [0 for an input signal with a large amplitude. Therefore, logarithmic conversion characteristics can be easily provided.

以下、図面を参照して本発明の実施形態に係る信号抽出方法および信号抽出回路について説明する。
図1は本発明に係る信号抽出方法の処理概念を示している。この信号抽出方法は、図1に示すように搬送波に対象信号を重畳した変調波を微分処理した後、その微分波形を対数変換処理および積分処理することで上記対象信号に関する信号成分をその出力として得ることにより実施される。後述するように上記微分処理は、例えばコンデンサを用いて実行される。また対数変換処理および積分処理は、対数変換特性を有する増幅器を用いて実行される。
Hereinafter, a signal extraction method and a signal extraction circuit according to an embodiment of the present invention will be described with reference to the drawings.
FIG. 1 shows a processing concept of a signal extraction method according to the present invention. In this signal extraction method, as shown in FIG. 1, a modulated wave in which a target signal is superimposed on a carrier wave is subjected to differential processing, and then the differential waveform is subjected to logarithmic conversion processing and integration processing to thereby output a signal component related to the target signal as its output. It is implemented by obtaining. As will be described later, the differentiation process is performed using, for example, a capacitor. The logarithmic conversion process and the integration process are performed using an amplifier having logarithmic conversion characteristics.

ちなみに処理対象とする変調波V(t)は、矩形波や三角波等の搬送波に微小な対象信号を重畳したものであって、特に上記搬送波は対象信号よりも低い基本周波数成分を有し、且つ対象信号よりも大きい微分値(絶対値)を含むもの、或いは対象信号よりも大きい振幅を含むものからなる。尚、対象信号よりも大きい微分値(絶対値)を含む搬送波とは、少なくとも搬送波の1周期分の期間について搬送波と対象信号とをそれぞれ時間的に微分して比較したとき、その期間内での搬送波の微分値(絶対値)の最大値が対象信号の微分値(絶対値)の最大値よりも大きいことを意味する。また対象信号よりも大きい振幅を含む搬送波とは、少なくとも搬送波の1周期分の期間について搬送波と対象信号とをそれぞれ比較したとき、その期間内での搬送波の振幅の最大値が対象信号の振幅の最大値よりも大きいことを意味する。   Incidentally, the modulation wave V (t) to be processed is obtained by superimposing a minute target signal on a carrier wave such as a rectangular wave or a triangular wave. In particular, the carrier wave has a lower fundamental frequency component than the target signal, and The signal includes a differential value (absolute value) larger than that of the target signal or a signal including an amplitude larger than that of the target signal. Note that a carrier wave including a differential value (absolute value) larger than the target signal means that the carrier wave and the target signal are temporally differentiated and compared for at least one period of the carrier wave. It means that the maximum value of the differential value (absolute value) of the carrier wave is larger than the maximum value of the differential value (absolute value) of the target signal. In addition, a carrier wave having an amplitude larger than that of the target signal means that when the carrier wave and the target signal are compared for at least one period of the carrier wave, the maximum value of the carrier wave amplitude within that period is the amplitude of the target signal. Means greater than the maximum value.

また上述した対数変換処理および積分処理は、自己インピーダンスが高い高抵抗領域においては積分回路の機能を支配的にし、自己インピーダンスが低い低抵抗領域において対数変換機能を支配的にして同時に実行される。また上記信号抽出処理の出力として得る対象信号に関する信号成分とは、対象信号そのものを示すことのみならず、対象信号が持つ情報の一部、具体的には対象信号が閾値を横切るタイミングとその変化の方向の情報等を示している。 Further, the logarithmic conversion process and the integration process described above are executed simultaneously with the function of the integrating circuit dominant in the high resistance region where the self impedance is high and the logarithmic conversion function dominant in the low resistance region where the self impedance is low . The signal component related to the target signal obtained as the output of the signal extraction processing not only indicates the target signal itself, but also a part of information of the target signal, specifically, the timing at which the target signal crosses the threshold and its change The direction information is shown.

さて上述した信号処理方法を実行する信号抽出回路は、概略的には、例えば図2に示すように1段の微分回路10を用いてその入力信号Vinを1階微分するように、或いは図3に示すように2つの微分回路10,20を直列に接続した2段構成の微分回路により入力信号Vinを2階微分するように構成される。特にこれらの各微分回路10,20は、それぞれ演算増幅器(オペアンプ)OPを主体として構成されるものであって、基本的には入力信号Vin(Vin')を微分して演算増幅器OPの反転入力端子IN-に導くコンデンサCin(微分処理機能)と、上記演算増幅器OPの反転入力端子IN-とその出力端子との間に並列接続されて上記演算増幅器OPに対数変換処理機能と積分処理機能とを持たせたインピーダンス制御手段Zとを備えて構成される。尚、ここで言う演算増幅器OPは一般に普及しているものであり、反転入力端子・非反転入力端子・出力端子・電源入力端子を有する差動増幅器で、その入力インピーダンスおよび裸の増幅率が共に極めて大きいという特徴を持つものである。 Now, the signal extraction circuit for executing the above-described signal processing method is schematically shown, for example, in such a manner that the input signal Vin is first-order differentiated using a one-stage differentiation circuit 10 as shown in FIG. As shown in FIG. 2, the input signal Vin is second-order differentiated by a two-stage differentiating circuit in which two differentiating circuits 10 and 20 are connected in series. In particular, each of the differentiating circuits 10 and 20 is composed mainly of an operational amplifier (op-amp) OP. Basically, the input signal Vin (Vin ′) is differentiated to input the inverting input of the operational amplifier OP. A capacitor Cin (differential processing function) leading to the terminal IN , and a logarithmic conversion processing function and an integration processing function are connected in parallel between the inverting input terminal IN of the operational amplifier OP and its output terminal. And an impedance control means Z provided with. Note that the operational amplifier OP mentioned here is generally popular, and is a differential amplifier having an inverting input terminal, a non-inverting input terminal, an output terminal, and a power supply input terminal, and has both an input impedance and a bare amplification factor. It has the characteristic of being extremely large.

尚、ここでは図3に示す2つの微分回路10,20を直列に接続して2階微分を実行する搬送波除去用の信号抽出回路(微小信号抽出回路)を例に説明するが、図2に示したように微分回路10(20)を単独で用いて1階微分を実行する信号抽出回路であっても同様に機能する。またこの微小信号抽出回路が処理対象とする変調波は、前述したように信号成分の変動幅よりも大なる振幅の搬送波(矩形波,三角波,正弦波)に信号成分(対象信号)が重畳した信号、またはその微分成分が前記信号成分よりも大なる搬送波(矩形波,正弦波)に微小な信号成分が重畳したもの、或いはこれらの信号を合成した信号(合成波)からなる。そして微分回路10(20)により実現される信号抽出回路は、矩形波や三角波、或いは正弦波等の搬送波に微小な信号成分が重畳した変調波を入力し、この変調波から搬送波の影響を低減して微小な信号成分を効率よく抽出する役割を担う。   Here, a signal extraction circuit for removing a carrier wave (micro signal extraction circuit) that performs two-order differentiation by connecting two differentiating circuits 10 and 20 shown in FIG. 3 in series will be described as an example. As shown, even a signal extraction circuit that performs first-order differentiation using the differentiating circuit 10 (20) alone functions similarly. In addition, as described above, the modulated wave to be processed by the minute signal extraction circuit has a signal component (target signal) superimposed on a carrier wave (rectangular wave, triangular wave, sine wave) having an amplitude larger than the fluctuation range of the signal component as described above. The signal, or a differential component of the carrier wave (rectangular wave, sine wave) whose differential component is larger than the signal component, or a signal (combined wave) obtained by synthesizing these signals. The signal extraction circuit realized by the differentiation circuit 10 (20) inputs a modulated wave in which a minute signal component is superimposed on a carrier wave such as a rectangular wave, a triangular wave, or a sine wave, and reduces the influence of the carrier wave from the modulated wave. Thus, it plays a role of efficiently extracting minute signal components.

具体的には前記微分回路10(20)は、演算増幅器OPの反転入力端子IN-に、入力抵抗Rinと上記コンデンサCinとの直列回路を介して入力信号Vin(Vin')を微分処理して入力し、また演算増幅器OPの非反転入力端子IN+に該演算増幅器OPにおける動作基準レベルを規定するための基準電圧Vrefを抵抗Rrefを介して入力する。そして演算増幅器OPの反転入力端子IN-と出力端子OUTとの間に並列接続されたインピーダンス制御手段Zによりその帰還回路を形成し、前記入力信号Vin(Vin')のコンデンサCinを介して微分された信号を、その振幅に応じた増幅率で増幅して出力するように構成される。 Specifically, the differentiating circuit 10 (20) differentiates the input signal Vin (Vin ′) at the inverting input terminal IN of the operational amplifier OP through a series circuit of the input resistor Rin and the capacitor Cin. The reference voltage Vref for defining the operation reference level in the operational amplifier OP is input to the non-inverting input terminal IN + of the operational amplifier OP via the resistor Rref. The inverting input terminal IN of the operational amplifier OP - and its feedback circuit formed by the parallel-connected impedance control unit Z between the output terminal OUT, and is differentiated through the capacitor Cin of the input signal Vin (Vin ') The received signal is amplified with an amplification factor corresponding to the amplitude and output.

ちなみに前記インピーダンス制御手段Zは、ここでは逆並列接続された一対のダイオードD1,D2および高周波ノイズ除去用コンデンサCncにより実現されている。ダイオードD1,D2は、いずれも順方向の電流値に対応してそのインピーダンスが指数関数的に減少する特性を有する一般的なシリコンダイオードである。またその極性を逆にして並列接続してあるのは、両方向の電流に対応するためである。高周波ノイズ除去用コンデンサCcnは、対象信号よりも周波数の高い雑音のみを帰還するようにその容量が定められており、上記変調波に関する帰還インピーダンスについて考えるときには、実質的にその存在を無視することができる。但し、高周波ノイズ除去用コンデンサCncの容量は、出力のベースラインへの収束を律する時定数に影響を及ぼす。   Incidentally, the impedance control means Z is realized here by a pair of diodes D1, D2 connected in reverse parallel and a high frequency noise removing capacitor Cnc. Each of the diodes D1 and D2 is a general silicon diode having a characteristic that its impedance decreases exponentially in accordance with a forward current value. The reason why the polarities are reversed is that they are connected in parallel in order to cope with currents in both directions. The capacitance of the high-frequency noise removing capacitor Ccn is determined so that only noise having a frequency higher than that of the target signal is fed back. When considering the feedback impedance related to the modulated wave, its existence may be substantially ignored. it can. However, the capacitance of the high frequency noise removing capacitor Cnc affects the time constant governing the convergence of the output to the baseline.

このインピーダンス制御手段Zは、コンデンサCinを介して微分処理されて入力する前記入力信号Vin(Vin')の微分成分の振幅が小さく、そこに流れる電流が小さいときにはダイオードD1,D2のインピーダンスが高いことから、そのインピーダンスを大きく設定することで演算増幅器OPによる上記入力信号Vin(Vin')に対する増幅率を大きくする。逆に上記微分成分の振幅が大きく、そこに流れる電流が大きいときにはダイオードD1,D2のインピーダンスが指数関数的に低くなることから、そのインピーダンスを小さく設定して上記入力信号Vin(Vin')に対する増幅率を小さくする。従ってインピーダンス制御手段Zは、入力信号Vin(Vin')の微分成分の振幅に応じてそのインピーダンスを変化させることで、演算増幅器OPに対数変換特性を付与する役割を担う。   This impedance control means Z is such that the amplitude of the differential component of the input signal Vin (Vin ′) input after being differentially processed through the capacitor Cin is small, and the impedance of the diodes D1 and D2 is high when the current flowing therethrough is small. Therefore, the amplification factor for the input signal Vin (Vin ′) by the operational amplifier OP is increased by setting the impedance large. On the contrary, when the amplitude of the differential component is large and the current flowing therethrough is large, the impedances of the diodes D1 and D2 are exponentially lowered. Therefore, the impedance is set small and the input signal Vin (Vin ') is amplified. Reduce the rate. Therefore, the impedance control means Z plays a role of providing logarithmic conversion characteristics to the operational amplifier OP by changing the impedance according to the amplitude of the differential component of the input signal Vin (Vin ′).

特にインピーダンス制御手段Zは、入力信号Vin(Vin')の微分成分の振幅(電圧)がダイオードD1,D2の順方向バイアス電圧VLに満たないときには、そのインピーダンスが高くなることから演算増幅器OPの増幅率を大きく設定して該演算増幅器OPを通常の線形増幅器として機能させる。また上記入力信号Vin(Vin')の微分成分の振幅(電圧)がダイオードD1,D2の順方向バイアス電圧VLを越えたときには、インピーダンス制御手段Zのインピーダンスが指数関数的に低くなるので演算増幅器OPの増幅率が小さく抑えられ、該演算増幅器OPは実質的に比較器として機能することになる。この結果、演算増幅器OPは対数変換特性を持つことになる。   In particular, the impedance control means Z increases the impedance of the operational amplifier OP because the impedance increases when the amplitude (voltage) of the differential component of the input signal Vin (Vin ′) is less than the forward bias voltage VL of the diodes D1 and D2. The ratio is set to be large so that the operational amplifier OP functions as a normal linear amplifier. When the amplitude (voltage) of the differential component of the input signal Vin (Vin ') exceeds the forward bias voltage VL of the diodes D1 and D2, the impedance of the impedance control means Z decreases exponentially, so the operational amplifier OP Thus, the operational amplifier OP substantially functions as a comparator. As a result, the operational amplifier OP has logarithmic conversion characteristics.

また高周波ノイズ除去用コンデンサCncは、入力信号Vin(Vin')と演算増幅器OPからの反転出力との電位差に応じた電荷を蓄積することで上記入力信号Vin(Vin')を積分する作用を呈する。このインピーダンス制御手段Zにより演算増幅器OPに付与される上記対数変換特性と積分機能は同時に働くものである。しかし演算増幅器OPの増幅率が上述したように入力信号Vin(Vin')の微分成分の振幅が小さいときには大きくなることから、コンデンサCncによる積分機能に比較して対数変換機能が支配的となり、逆に入力信号Vin(Vin')の微分成分の振幅が大きいときには上記増幅率が小さくなることから、コンデンサCncによる積分機能が支配的となる。   Further, the high frequency noise removing capacitor Cnc exhibits an action of integrating the input signal Vin (Vin ′) by accumulating charges according to the potential difference between the input signal Vin (Vin ′) and the inverted output from the operational amplifier OP. . The logarithmic conversion characteristic and the integration function given to the operational amplifier OP by the impedance control means Z work simultaneously. However, since the amplification factor of the operational amplifier OP becomes large when the amplitude of the differential component of the input signal Vin (Vin ′) is small as described above, the logarithmic conversion function becomes dominant as compared with the integration function by the capacitor Cnc, and vice versa. In addition, when the amplitude of the differential component of the input signal Vin (Vin ′) is large, the amplification factor becomes small, so that the integration function by the capacitor Cnc becomes dominant.

上述した構成の微分回路10(20)によれば、コンデンサCinを介して微分された入力信号Vin(Vin')が演算増幅器OPの反転入力端子IN-に加えられるので、入力信号Vin(Vin')の搬送波が大きく変化しても、その不連続点で生じる大きな微分波形が抑えられる。従って演算増幅器OPの反転入力端子IN-には、専ら、搬送波に重畳した対象信号の成分だけが印加される。そして入力信号Vin(Vin')の微分成分が入力される演算増幅器OPにおいては、対象信号の振幅が小さいときには大きな増幅率で該対象信号を増幅し、対象信号の振幅が大きくなるとその増幅率を小さくして該対象信号に相当する電荷を前記コンデンサCncに蓄積する(コンデンサCncの充電による積分作用)。 According to the differentiation circuit 10 (20) having the above-described configuration, the input signal Vin (Vin ′) differentiated through the capacitor Cin is applied to the inverting input terminal IN of the operational amplifier OP, so that the input signal Vin (Vin ′) ), A large differential waveform generated at the discontinuity can be suppressed. Accordingly, only the component of the target signal superimposed on the carrier wave is applied exclusively to the inverting input terminal IN of the operational amplifier OP. In the operational amplifier OP to which the differential component of the input signal Vin (Vin ′) is input, the target signal is amplified with a large amplification factor when the amplitude of the target signal is small, and the amplification factor is increased when the amplitude of the target signal increases. The charge corresponding to the target signal is reduced and accumulated in the capacitor Cnc (integration effect by charging the capacitor Cnc).

この際、搬送波と対象信号波とは同じ取り扱いを受け、僅かな変化でもその出力がベースライン付近に到達する。またコンデンサCinによる微分値が大きいときは、前述したようにインピーダンス制御手段Zのインピーダンスが小さくなるので、搬送波の不連続点においてはその出力に規制が掛かることになる。しかし演算増幅器OP自体が飽和することがないので、信号が潰れることはない。   At this time, the carrier wave and the target signal wave are subjected to the same handling, and the output reaches the vicinity of the baseline even with a slight change. Further, when the differential value by the capacitor Cin is large, the impedance of the impedance control means Z becomes small as described above, so that the output is restricted at the discontinuous point of the carrier wave. However, since the operational amplifier OP itself does not saturate, the signal is not destroyed.

従って図4(a)に示すように矩形波に微小な信号成分(対象信号)が重畳した変調波Vinが入力されると、微分回路10(20)の出力は図4(b)に示すように演算増幅器OPの動作範囲(電源電圧;−Vd〜+Vd)において大きく変化することになる。特に対象信号の振幅が小さいときには上述した対数変換特性の下での大きな増幅率で増幅され、その出力信号はベースライン(0V)を基準として略電源電圧±Vdのレベルまで変化する。そして対象信号の振幅が大きくなったとき、その増幅率が小さく抑えられることから前記コンデンサCncに蓄積された電荷の量(積分値)に相当する電圧変化を呈する。そして前記コンデンサCncには対象信号の繰り返し変化に伴って次第に電荷が蓄積されていくことから、これに伴って対数変換特性が機能して対象信号を大きな増幅率で増幅する領域(電圧範囲)が次第に低減していく。   Therefore, as shown in FIG. 4A, when a modulated wave Vin in which a minute signal component (target signal) is superimposed on a rectangular wave is input, the output of the differentiating circuit 10 (20) is as shown in FIG. 4B. In the operational range of the operational amplifier OP (power supply voltage: -Vd to + Vd), the operation amplifier OP greatly changes. In particular, when the amplitude of the target signal is small, the signal is amplified with a large amplification factor under the above-described logarithmic conversion characteristics, and the output signal changes to the level of approximately power supply voltage ± Vd with reference to the baseline (0 V). When the amplitude of the target signal is increased, the amplification factor is suppressed to a small value, so that a voltage change corresponding to the amount of charge (integrated value) accumulated in the capacitor Cnc is exhibited. Since the capacitor Cnc gradually accumulates electric charges as the target signal is repeatedly changed, the logarithmic conversion characteristic functions accordingly, and there is a region (voltage range) in which the target signal is amplified with a large amplification factor. Reduce gradually.

従って上述したように構成され、機能する搬送波除去用の信号抽出回路によれば、搬送波に微小な信号成分が重畳した変調波V(t)からなる入力信号Vinを与えると、この入力信号Vinは前段の微分回路10にて微分処理され、その搬送波成分が抑制されると共に上記信号成分が増幅されて出力される(1階微分処理)。そしてこの微分回路10の出力信号が後段の微分回路20に入力されて同様にして微分処理され、更に搬送波成分が抑制されると共に上記信号成分が更に増幅されて出力される(2階微分処理)。この結果、搬送波が矩形波である場合には、例えば図5(a)に示すようにその1階微分波形、および2階微分波形が得られ、入力信号Vinにおける搬送波成分が除去され、その信号成分が増幅されて出力される。   Therefore, according to the signal extracting circuit for removing a carrier wave configured and functioning as described above, when the input signal Vin composed of the modulated wave V (t) in which a minute signal component is superimposed on the carrier wave, the input signal Vin is Differentiating processing is performed by the differentiating circuit 10 in the preceding stage, the carrier wave component is suppressed, and the signal component is amplified and output (first-order differentiation processing). The output signal of the differentiating circuit 10 is input to the subsequent differentiating circuit 20 and subjected to differential processing in the same manner. Further, the carrier wave component is suppressed and the signal component is further amplified and output (second-order differential processing). . As a result, when the carrier wave is a rectangular wave, for example, as shown in FIG. 5A, the first-order differential waveform and the second-order differential waveform are obtained, the carrier wave component in the input signal Vin is removed, and the signal The component is amplified and output.

また搬送波が三角波である場合には、例えば図5(b)に示すようにその1階微分波形、および2階微分波形が得られ、矩形波の場合と同様にその入力信号Vinにおける搬送波成分が除去され、その信号成分が増幅されて出力される。更に搬送波が正弦波である場合には、例えば図5(c)に示すようにその1階微分波形、および2階微分波形が得られ、前述した矩形波や三角波の場合と同様に入力信号Vinにおける搬送波成分が除去され、その信号成分が増幅されて出力されることになる。   When the carrier wave is a triangular wave, for example, as shown in FIG. 5B, the first-order differential waveform and the second-order differential waveform are obtained, and the carrier wave component in the input signal Vin is the same as in the case of the rectangular wave. Then, the signal component is amplified and output. Further, when the carrier wave is a sine wave, for example, as shown in FIG. 5C, the first-order differential waveform and the second-order differential waveform are obtained, and the input signal Vin is the same as in the case of the rectangular wave or the triangular wave described above. Is removed and the signal component is amplified and output.

即ち、本発明に係る搬送波除去用の信号抽出回路によれば、逆並列接続された一対のダイオードD1,D2等によって実現されるインピーダンス制御回路Zにより、演算増幅器OPを主体とする微分回路10,20の増幅率をその入力信号レベルに応じて変化させるので、微分回路10,20からの増幅出力の変動幅を制限し、また高周波ノイズ除去用コンデンサCncが放電する際の時定数を大きくすることができる。従って搬送波の微分値に拘わることなく、その搬送波に重畳した微小な信号成分だけを効率的に増幅して抽出し、また搬送波の成分を効果的に除去することが可能となる。換言すれば高周波ノイズ除去用コンデンサCncが放電する際の時定数を大きくすることで、搬送波の微分値の絶対値が小さいときの出力変化を抑制することができる。特に図10(a)(b)(c)にそれぞれ示した従来回路による信号処理波形(1階微分波形、2階微分波形)と対比すればより明らかなように、上述した構成の信号抽出回路によれば、2階微分処理によって搬送波の成分を略零(0)とすることができるので、搬送波除去効果が非常に良好であると言える。   That is, according to the signal extraction circuit for removing a carrier wave according to the present invention, the impedance control circuit Z realized by a pair of diodes D1, D2 and the like connected in anti-parallel, the differentiation circuit 10, mainly the operational amplifier OP, Since the amplification factor of 20 is changed according to the input signal level, the fluctuation range of the amplified output from the differentiation circuits 10 and 20 is limited, and the time constant when the high frequency noise removing capacitor Cnc is discharged is increased. Can do. Therefore, regardless of the differential value of the carrier wave, it is possible to efficiently amplify and extract only a minute signal component superimposed on the carrier wave and effectively remove the carrier wave component. In other words, the output change when the absolute value of the differential value of the carrier wave is small can be suppressed by increasing the time constant when the high frequency noise removing capacitor Cnc is discharged. In particular, as compared with the signal processing waveforms (first-order differential waveform, second-order differential waveform) by the conventional circuits shown in FIGS. 10 (a), 10 (b), and 10 (c), the signal extraction circuit having the above-described configuration is more apparent. Therefore, it can be said that the carrier wave removal effect is very good because the component of the carrier wave can be made substantially zero (0) by the second-order differentiation process.

尚、一般的な微分回路を用いた場合、搬送波を除去するに必要な微分階数は、専ら、その搬送波の形によって決定される。この点、本発明に係る信号抽出回路においては、その入力信号(変調波)を何階微分するかは、主として信号成分の大きさに依存するだけである。しかもこの信号抽出回路の主たる目的は、変調波に含まれる微小な信号成分を、その対数変換特性を十分に活かして増幅することにある。従って搬送波に重畳した信号成分の振幅が大きく、1階の微分で十分に対数変換が掛かるような場合には1階微分処理だけで十分である。逆に信号成分の振幅が小さい場合には、十分な対数変換が掛かる出力が得られるまで、2階微分3階微分と、その微分処理を繰り返し実行するように微分回路を多段に直列接続して信号抽出回路を構築するようにすれば良い。また必要以上に微分処理を繰り返したとしても、これによって得られる出力信号は対数変換によりその上下が圧縮されるだけなので、その後に上記出力信号をディジタル処理する上で殆ど問題となることはない。   When a general differentiation circuit is used, the differential order necessary for removing the carrier wave is determined solely by the shape of the carrier wave. In this respect, in the signal extraction circuit according to the present invention, the order of differentiation of the input signal (modulated wave) depends mainly on the magnitude of the signal component. Moreover, the main purpose of this signal extraction circuit is to amplify a minute signal component included in the modulated wave by fully utilizing its logarithmic conversion characteristics. Accordingly, when the amplitude of the signal component superimposed on the carrier wave is large and the logarithmic transformation is sufficiently performed by the first-order differentiation, the first-order differentiation process is sufficient. Conversely, if the amplitude of the signal component is small, the differential circuit is connected in series in multiple stages so as to repeatedly execute the second-order differentiation and third-order differentiation and the differentiation process until an output with sufficient logarithmic transformation is obtained. A signal extraction circuit may be constructed. Further, even if the differentiation process is repeated more than necessary, the output signal obtained by this is only compressed at the top and bottom by logarithmic transformation, so that there is almost no problem in the subsequent digital processing of the output signal.

また上述した信号抽出回路は、信号成分よりも大きな搬送波の微分成分(折れ曲がり)は1パルスとして出力信号中に現れ、これを対象信号に基づく出力信号と区別することはできない。その点では完全に搬送波成分を除去するものではないが、対象信号に基づく出力信号のパルス数が多ければ、実質的にはその影響を無視することができる。従って上述した構成の信号抽出回路を用いれば、例えば搬送波に重畳した微小な信号成分を高速フーリエ変換等のディジタル処理技術を用いることなく解析することが可能となる。故に、前述したレーザ光の自己結合効果を利用した距離測定等のセンシング処理に適用して、簡易な構成のセンサ装置を実現する上で非常に有効である。また上述した構成の搬送波除去回路は集積回路化も容易なので、センシング素子と一体化されるセンシングアンプとして用いるにも効果的である。   Further, in the signal extraction circuit described above, the differential component (bending) of the carrier wave larger than the signal component appears in the output signal as one pulse and cannot be distinguished from the output signal based on the target signal. In this respect, the carrier component is not completely removed, but if the number of pulses of the output signal based on the target signal is large, the influence can be substantially ignored. Therefore, if the signal extraction circuit having the above-described configuration is used, for example, a minute signal component superimposed on a carrier wave can be analyzed without using a digital processing technique such as fast Fourier transform. Therefore, the present invention is very effective in realizing a sensor device with a simple configuration by applying to sensing processing such as distance measurement using the self-coupling effect of the laser beam described above. Further, since the carrier wave removal circuit having the above-described configuration can be easily integrated, it is effective for use as a sensing amplifier integrated with a sensing element.

尚、本発明は上述した実施形態に限定されるものではない。例えば前述した一対のダイオードD1,D2については、演算増幅器OPを構築する半導体集積回路に同時集積されたPN接合として実現するようにしても良い。またトランジスタ等を用いてインピーダンス可変型の非線形抵抗回路をインピーダンス制御手段Zとして構築することも可能である。またインピーダンス制御手段Zの機能を損なうことのない高い値の抵抗を演算増幅器OPの入出力端子間に並列接続して、その動作安定化を図ることも勿論可能である。また通常の微分回路で搬送波成分を除去する場合には、搬送波が三角波の場合には2階微分、搬送波が矩形波や正弦波の場合には1階微分が必要となるので、本発明に係る搬送波除去回路においても、搬送波の形によらず、信号の大きさに応じて微分処理階数を決定するようにすれば良い。   The present invention is not limited to the embodiment described above. For example, the pair of diodes D1 and D2 described above may be realized as PN junctions that are simultaneously integrated in a semiconductor integrated circuit that constructs the operational amplifier OP. It is also possible to construct a variable impedance nonlinear resistance circuit as the impedance control means Z using a transistor or the like. It is of course possible to stabilize the operation by connecting in parallel between the input and output terminals of the operational amplifier OP, a high value resistor that does not impair the function of the impedance control means Z. Further, when the carrier wave component is removed by an ordinary differentiating circuit, second order differentiation is required when the carrier wave is a triangular wave, and first order differentiation is required when the carrier wave is a rectangular wave or a sine wave. Even in the carrier wave removal circuit, the differential processing rank may be determined in accordance with the signal size regardless of the shape of the carrier wave.

また微分回路を多段に接続する場合、ノイズ除去のために、後段の微分回路において増幅制限用の抵抗を前述したダイオードD1,D2と並列に設けるようにしても良い。ちなみに抵抗がない場合、ノイズも大きく増幅されて信号と見分けが付かなくなる虞があるが、抵抗を入れることにより演算増幅器OPの増幅率を制限し、これによってノイズと信号とが容易に見分けられるようになる。   When differentiating circuits are connected in multiple stages, an amplification limiting resistor may be provided in parallel with the diodes D1 and D2 in the subsequent differentiating circuit in order to eliminate noise. By the way, when there is no resistance, there is a possibility that noise will be greatly amplified and become indistinguishable from the signal, but by inserting a resistance, the amplification factor of the operational amplifier OP is limited, so that noise and signal can be easily distinguished. become.

また演算増幅器OPの帰還回路がダイオードD1,D2で構成されているので、演算増幅器OPは双方向のピークホールド回路と同等の機能を持つことになる。従ってピークホールドの機能をほぼ積分動作と看做すことができるので、前述したノイズ除去用のコンデンサCncを省略しても、実質的に積分機能を持たせることができる。その他、本発明はその要旨を逸脱しない範囲で種々変形して実施することができる。   Further, since the feedback circuit of the operational amplifier OP is composed of the diodes D1 and D2, the operational amplifier OP has a function equivalent to that of the bidirectional peak hold circuit. Therefore, since the peak hold function can be regarded as an almost integral operation, even if the above-described noise removing capacitor Cnc is omitted, the integration function can be substantially provided. In addition, the present invention can be variously modified and implemented without departing from the scope of the invention.

ここで上述した本発明を用いるのに好適な適用例について説明する。
光学的な距離計測技術の1つにレーザ光の自己結合効果(自己混合効果ともいう)[Self mixing Effect]を利用したものがある(例えば特開平10−246782号公報、特開平11−287859号公報を参照)。この手法は、例えば図6に示すように所定の変調信号を用いて駆動したレーザ素子(以下、LD)1から測定対象物2にレーザ光を照射すると共に、測定対象物2により反射されて前記レーザ素子1に戻った反射レーザ光と前記出力レーザ光との自己結合により生じた変調光(変調波)を受光器(以下、PD)3にて受光し、その出力を周波数分析する等して前記測定対象物2までの距離Lを測定するものである。
An application example suitable for using the present invention described above will now be described.
One of optical distance measurement techniques uses a self-coupling effect (also referred to as a self-mixing effect) of laser light (for example, Japanese Patent Laid-Open Nos. 10-246782 and 11-287859). See the publication). In this method, for example, as shown in FIG. 6, a laser element (hereinafter referred to as LD) 1 driven by using a predetermined modulation signal irradiates a measurement object 2 with laser light, and is reflected by the measurement object 2 to reflect the above-mentioned The modulated light (modulated wave) generated by the self-coupling of the reflected laser light returning to the laser element 1 and the output laser light is received by a light receiver (hereinafter referred to as PD) 3, and the output is subjected to frequency analysis or the like. The distance L to the measurement object 2 is measured.

即ち、レーザー素子1から発せられるレーザ光の発振波長を変化させると、或る発振波長において測定対象物2により反射した戻りレーザ光と上記レーザ素子1の出力レーザ光とが共振条件を満たしたとき(自己結合効果)、前記受光器3の出力が増加する。例えば付与される電流値に応じてレーザー光の発振波長が変化するタイプのレーザー素子に対して、図7に示すような三角波α(縦方向が電流値、横方向が時間を表す)を用いて波長変調することができる。即ち、三角波αの一周期分について見ると、時間の経過と共に電流値が連続的に増加するのでこれに応じて放出されるレーザー光の波長も連続的に増加し、電流値がピークに達した後は電流値が連続的に減少するのでこれに応じて放出されるレーザー光の波長も連続的に減少する。このように放射レーザー光の波長が連続的に増減する中で、戻りレーザー光との間の共振条件が何度も満たされるため、その結果として前記受光器3からは上記三角波αに微小な共振成分が重畳したビート波形(変調波)βが得られる。従ってこのビート波形βを解析すれば、上記共振成分の周波数から測定対象物2までの距離Lを求めることが可能となる。   That is, when the oscillation wavelength of the laser beam emitted from the laser element 1 is changed, the return laser beam reflected by the measurement object 2 at a certain oscillation wavelength and the output laser beam of the laser element 1 satisfy the resonance condition. (Self-coupling effect), the output of the light receiver 3 increases. For example, for a type of laser element in which the oscillation wavelength of the laser light changes in accordance with the applied current value, a triangular wave α as shown in FIG. Wavelength modulation can be performed. That is, when looking at one period of the triangular wave α, the current value continuously increases with the passage of time, so the wavelength of the emitted laser light continuously increases accordingly, and the current value reached a peak. After that, since the current value continuously decreases, the wavelength of the emitted laser light correspondingly decreases accordingly. As the wavelength of the emitted laser beam continuously increases and decreases in this manner, the resonance condition with the return laser beam is satisfied many times. As a result, the light receiving device 3 causes a minute resonance in the triangular wave α. A beat waveform (modulated wave) β in which components are superimposed is obtained. Therefore, if this beat waveform β is analyzed, the distance L from the frequency of the resonance component to the measurement object 2 can be obtained.

この計測技術について紹介した公知文献としては、平成6年度電気関係学会東海支部連合大会講演論文集,1994-10-6,No.650,『半導体レーザの自己結合効果を利用した距離計』上田・山田・紫藤や、オーストラリア、クイーンズランド大学論文『Distance Measurement Using External Optical Feedback in a Vertical-Cavity Surface-Emitting Laser』 Student;Garth Niethe,Supervisor;Dr Aleksandar D. Rakic, HYPERLINK "http://innovexpo.itee.uq.edu.au/2000/348657979.htm" http://innovexpo.itee.uq.edu.au/2000/348657979.htm等がある。   The public literature that introduced this measurement technology includes the 1994 Annual Conference of the Tokai Branch Joint Conference on Electrical Engineering, 1994-10-6, No.650, “Distance Meter Using Self-Coupling Effect of Semiconductor Laser”, Ueda, Yamada, Shito, and Queensland University, Australia, “Distance Measurement Using External Optical Feedback in a Vertical-Cavity Surface-Emitting Laser” Student; Garth Niethe, Supervisor; Dr Aleksandar D. Rakic, HYPERLINK "http: //innovexpo.itee .uq.edu.au / 2000 / 348657979.htm "http://innovexpo.itee.uq.edu.au/2000/348657979.htm.

即ち、三角波αの一周期分について見ると、時間の経過と共に電流値が連続的に増加するので、これに応じてレーザー素子1から放出されるレーザー光の強度も連続的に増加する。そして電流値がピークに達した後は電流値が連続的に減少するので、これに応じて前記レーザー素子1から放出されるレーザー光の強度も連続的に減少する。この際、電流値の増減に応じて前記レーザー素子1から放出されるレーザ光の波長も伸び縮みする。このように放射レーザー光の強度が連続的に増減する中で、戻りレーザー光との間の共振条件が何度も満たされるため、その結果として前述したように共振により強度(振幅)が変化した微小な成分(対象信号)が上記連続したレーザ光の強度(搬送波)に重畳することになる。   That is, when looking at one period of the triangular wave α, the current value continuously increases as time passes, and accordingly, the intensity of the laser light emitted from the laser element 1 also increases continuously. Then, since the current value continuously decreases after the current value reaches the peak, the intensity of the laser beam emitted from the laser element 1 is also continuously decreased accordingly. At this time, the wavelength of the laser beam emitted from the laser element 1 expands and contracts according to the increase / decrease of the current value. As the intensity of the emitted laser beam continuously increases and decreases in this way, the resonance condition with the return laser beam is satisfied many times. As a result, the intensity (amplitude) changes due to resonance as described above. A minute component (target signal) is superimposed on the intensity (carrier wave) of the continuous laser beam.

従って上述したレーザ光から求められる、三角波αのような振幅の大きい搬送波に微小な共振成分(対象信号)が重畳したビート波形(変調波)βを解析するに際し、高速フーリエ変換(FFT)等のディジタル処理に代えて、本発明を用いて対象信号を抽出し、その出力をカウンタで計数すれば対象信号の周波数を得ることができる。従ってこの対象信号の周波数を解析することでレーザー素子1から測定対象物2までの距離Lを測定することができる。   Accordingly, when analyzing a beat waveform (modulated wave) β obtained by superimposing a minute resonance component (target signal) on a carrier wave having a large amplitude such as a triangular wave α, which is obtained from the laser light described above, a fast Fourier transform (FFT) or the like is used. Instead of digital processing, the frequency of the target signal can be obtained by extracting the target signal using the present invention and counting the output with a counter. Accordingly, the distance L from the laser element 1 to the measurement object 2 can be measured by analyzing the frequency of the target signal.

本発明に係る信号抽出方法の処理概念を示す図。The figure which shows the processing concept of the signal extraction method which concerns on this invention. 本発明の一実施形態に係る信号抽出回路(1階微分処理)の構成例を示す図。The figure which shows the structural example of the signal extraction circuit (1st-order differentiation process) which concerns on one Embodiment of this invention. 本発明の別の実施形態に係る信号抽出回路(2階微分処理)の構成例を示す図。The figure which shows the structural example of the signal extraction circuit (2nd-order differentiation process) which concerns on another embodiment of this invention. 図3に示す信号処理回路による変調波の微分出力波形の例を示す図。The figure which shows the example of the differential output waveform of the modulation wave by the signal processing circuit shown in FIG. 本発明に係る信号処理回路による入力変調波とその1階微分処理波形、および2階微分処理波形の例を示す図。The figure which shows the example of the input modulation wave by the signal processing circuit which concerns on this invention, its 1st-order differentiation processing waveform, and 2nd-order differentiation processing waveform. レーザ光の自己結合効果を利用した距離計の概略的な構成例を示す図。The figure which shows the schematic structural example of the distance meter using the self-coupling effect of a laser beam. レーザ光に対する周波数変調信号(搬送波)と、自己結合効果により生じたレーザ光のビート波形(変調波)の例を示す図。The figure which shows the example of the frequency modulation signal (carrier wave) with respect to a laser beam, and the beat waveform (modulation wave) of the laser beam produced by the self-coupling effect. 従来一般的な微分回路の例を示す図。The figure which shows the example of a conventional general differentiation circuit. 図8に示す微分回路による変調波の微分出力波形の例を示す図。The figure which shows the example of the differential output waveform of the modulation wave by the differentiating circuit shown in FIG. 従来一般的な微分回路による入力変調波とその1階微分処理波形、および2階微分処理波形の例を示す図。The figure which shows the example of the input modulation wave by the conventional general differentiation circuit, its 1st-order differentiation processing waveform, and 2nd-order differentiation processing waveform. 公知技術を適用した従来の微分回路の別の例を示す図。The figure which shows another example of the conventional differentiation circuit to which a well-known technique is applied. 図11に示す微分回路の微分出力波形の例を示す図。The figure which shows the example of the differential output waveform of the differentiating circuit shown in FIG.

符号の説明Explanation of symbols

10,20 微分回路
OP 演算増幅器
Cin 微分用コンデンサ
Cnc 高周波ノイズ除去用コンデンサ
Rin 入力抵抗
D1,D2 ダイオード(帰還回路;インピーダンス制御手段)
10,20 Differentiation circuit OP Operational amplifier Cin Differentiation capacitor Cnc High frequency noise elimination capacitor Rin Input resistance D1, D2 Diode (feedback circuit; impedance control means)

Claims (9)

対象信号よりも低い基本周波数成分を有し、且つ上記対象信号よりも大きい微分値、または前記対象信号よりも大きい振幅を含む搬送波に前記対象信号を重畳した変調波から前記対象信号の信号成分を抽出するに際し、
上記変調波を微分処理した後、得られた微分値が大きいときには対数変換機能を支配的にすると共に、前記微分値が小さいときには積分機能を支配的にして前記微分値に対して対数変換処理積分処理とを同時に施すことを特徴とする信号抽出方法。
The signal component of the target signal is derived from a modulated wave having a fundamental frequency component lower than that of the target signal and having a differential value larger than the target signal or a carrier wave including an amplitude larger than the target signal. When extracting
After differentiating the modulated wave, with when obtained differential value is large to dominate the logarithmic conversion function, wherein when the differential value is small and the logarithmic conversion process on the differential value in the dominant integral function A signal extraction method characterized by performing integration processing simultaneously .
前記対数変換処理および前記積分処理は、抽出する対象信号の経時的な変化が、その抽出された対象信号が山から谷、または谷から山へ移行する際、必ず一定の閾値を通過するように実行することを特徴とする請求項1に記載の信号抽出方法。 The logarithmic conversion process and the integration process, temporal change of the target signal to be extracted, when the extracted target signal transitions valley peak or from trough, to the mountain, as always to pass a certain threshold The signal extraction method according to claim 1, wherein the signal extraction method is executed. 前記微分処理をコンデンサを用いて実行すると共に、
前記対数変換処理および積分処理を、少なくとも逆並列接続された一対の半導体接合を用いて帰還インピーダンスを定めた帰還形増幅器を用いて実行することを特徴とする請求項1または2に記載の信号抽出方法。
While performing the differentiation process using a capacitor,
3. The signal extraction according to claim 1, wherein the logarithmic conversion process and the integration process are performed using a feedback amplifier that determines a feedback impedance by using at least a pair of semiconductor junctions connected in antiparallel. Method.
抽出された信号を変調波とみなして請求項1〜3のいずれかに記載の信号抽出方法を複数回繰り返すことを特徴とする信号抽出方法。   4. The signal extraction method according to claim 1, wherein the extracted signal is regarded as a modulated wave and the signal extraction method according to claim 1 is repeated a plurality of times. 対象信号よりも低い基本周波数成分を有し、且つ上記対象信号よりも大きい微分値、または前記対象信号よりも大きい振幅を含む搬送波に前記対象信号を重畳した変調波から前記対象信号の信号成分を抽出する信号抽出回路であって、
信号入力端子および基準入力端子を備えると共に、コンデンサを介して入力された変調波を増幅して出力する増幅器と、この増幅器の出力を該増幅器の信号入力端子に帰還する帰還手段とを備え、
前記帰還手段は、前記増幅器の入出力間の電圧が小さいときにはインピーダンスが大きくなり、前記増幅器の入出力間の電圧が大きいときにはインピーダンスが大きくなるように自己のインピーダンスを指数関数的に変化させるものであることを特徴とする信号抽出回路。
The signal component of the target signal is derived from a modulated wave having a fundamental frequency component lower than that of the target signal and having a differential value larger than the target signal or a carrier wave including an amplitude larger than the target signal. A signal extraction circuit for extracting,
An amplifier that has a signal input terminal and a reference input terminal, amplifies and outputs the modulated wave input through the capacitor, and feedback means that feeds back the output of the amplifier to the signal input terminal of the amplifier,
The feedback means changes its impedance exponentially so that the impedance increases when the voltage between the input and output of the amplifier is small, and the impedance increases when the voltage between the input and output of the amplifier is large. A signal extraction circuit characterized by being.
前記帰還手段は、逆並列接続された一対の半導体接合である請求項5に記載の信号抽出回路。   6. The signal extraction circuit according to claim 5, wherein the feedback means is a pair of semiconductor junctions connected in antiparallel. 前記増幅器は、その入出力端子間の電圧が前記帰還手段としての逆並列接続された一対の半導体接合の導通電圧よりも小さいときには実質的に演算増幅器として動作し、上記入出力端子間の電圧が前記半導体接合の導通電圧よりも大きいときには実質的に比較器として動作するものである請求項5に記載の信号抽出回路。   The amplifier operates substantially as an operational amplifier when the voltage between its input / output terminals is smaller than the conduction voltage of a pair of semiconductor junctions connected in reverse parallel as the feedback means, and the voltage between the input / output terminals is 6. The signal extraction circuit according to claim 5, wherein the signal extraction circuit substantially operates as a comparator when the conduction voltage is higher than the semiconductor junction. 前記帰還形演算増幅器における帰還手段は、逆並列接続された一対の半導体接合およびこれらの半導体接合に並列接続された高周波除去用のコンデンサだけからなる請求項5〜7のいずれかに記載の信号抽出回路。   8. The signal extraction according to claim 5, wherein the feedback means in the feedback operational amplifier comprises only a pair of semiconductor junctions connected in antiparallel and a high-frequency removing capacitor connected in parallel to these semiconductor junctions. circuit. 請求項5〜8のいずれかに記載の信号抽出回路をひとつの構成単位として、複数の構成単位を多段に接続したことを特徴とする信号抽出回路。   9. A signal extraction circuit, wherein the signal extraction circuit according to claim 5 is used as one structural unit, and a plurality of structural units are connected in multiple stages.
JP2005034315A 2005-02-10 2005-02-10 Signal extraction method and signal extraction circuit Expired - Fee Related JP4370577B2 (en)

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