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JPH0412645B2 - - Google Patents
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JPH0412645B2 - - Google Patents

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Publication number
JPH0412645B2
JPH0412645B2 JP57170732A JP17073282A JPH0412645B2 JP H0412645 B2 JPH0412645 B2 JP H0412645B2 JP 57170732 A JP57170732 A JP 57170732A JP 17073282 A JP17073282 A JP 17073282A JP H0412645 B2 JPH0412645 B2 JP H0412645B2
Authority
JP
Japan
Prior art keywords
circuit
source
potential
mosfet
output terminal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP57170732A
Other languages
Japanese (ja)
Other versions
JPS5961205A (en
Inventor
Masunori Sugimoto
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.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP57170732A priority Critical patent/JPS5961205A/en
Publication of JPS5961205A publication Critical patent/JPS5961205A/en
Publication of JPH0412645B2 publication Critical patent/JPH0412645B2/ja
Granted legal-status Critical Current

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  • Amplifiers (AREA)
  • Manipulation Of Pulses (AREA)
  • Logic Circuits (AREA)

Description

【発明の詳細な説明】 本発明はFETで構成されるレベルシフト回路
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a level shift circuit composed of FETs.

MOSFETで構成されるリニア回路に於ては、
入力信号の直流電位を回路が動作する入力電圧範
囲に移動させるためにレベルシフ回路を必要とす
る場合がしばしばある。典型的な例はソース接地
回路を用いる場合である。一般にソース接地回路
は動作をする入力電圧の範囲が極めて狭く、入力
しようとする信号の直流電位がその範囲に存在し
ない場合が多い。この場合、入力信号を一旦レベ
ルシフト回路を通過させ、その直流電位をソース
接地回路が動作する範囲に移動させた後にソース
接地回路に加えるということがよく行なわれる。
このようなレベルシフト回路には、それを置いた
事による周波数特性の劣化を小さく抑えるため
に、出力抵抗が充分小さい事が要求される。
In a linear circuit composed of MOSFETs,
Level shifting circuits are often required to move the DC potential of the input signal into the input voltage range in which the circuit will operate. A typical example is when a common source circuit is used. In general, the input voltage range in which a common source circuit operates is extremely narrow, and the DC potential of the signal to be input is often not within that range. In this case, it is often done that the input signal is once passed through a level shift circuit, its DC potential is moved to a range where the source grounded circuit operates, and then applied to the source grounded circuit.
Such a level shift circuit is required to have a sufficiently small output resistance in order to minimize deterioration of frequency characteristics due to its placement.

従来、レベルシフト回路としてはソースフオロ
ワ回路が広く用いられてきた。その一例を第1図
に示す。
Conventionally, source follower circuits have been widely used as level shift circuits. An example is shown in FIG.

第1図に於てMOSFET1のドレイン電極は第
1の電源5に接続され、ゲート電極は入力端子3
に接続され、ソース電極は出力端子4に接続され
ている。またMOSFET2のドレイン電極は出力
端子4に接続され、ゲート電極はバイアス電位を
与える電源7に接続され、ソース電極は第2の電
源6に接続さている。入力端子3に加えられる信
号は、MOSFET1と2の利得係数とMOSFET
2のゲート電極のバイアス電位によりほぼ決定さ
れる大きさだけ電位移動され、出力端子4に現わ
れる。
In FIG. 1, the drain electrode of MOSFET 1 is connected to the first power supply 5, and the gate electrode is connected to the input terminal 3.
The source electrode is connected to the output terminal 4. Further, the drain electrode of the MOSFET 2 is connected to the output terminal 4, the gate electrode is connected to a power source 7 that provides a bias potential, and the source electrode is connected to a second power source 6. The signal applied to input terminal 3 is the gain coefficient of MOSFETs 1 and 2 and the MOSFET
The potential is shifted by an amount approximately determined by the bias potential of the gate electrode 2 and appears at the output terminal 4.

MOSFET1のトランスコンダクタンスをgm1
とすると、第1図のレベルシフト回路の出力抵抗
はほぼ1/gm1となる。ところがトランスコンダ
クタンスgm1は、電位移動の大きさと消費電流で
決定されてしまう。
The transconductance of MOSFET1 is gm1
Then, the output resistance of the level shift circuit shown in FIG. 1 is approximately 1/gm1. However, transconductance gm1 is determined by the magnitude of potential shift and current consumption.

従つて、第1図に示す従来回路を特に広帯域の
回路を用いようとする場合、回路の帯域幅は出力
抵抗に反比例するから、出力抵抗を充分に小さく
できない従来のレベルシフト回路では、必要な帯
域幅が得られないことが実際にしばしばある。
Therefore, when trying to use the conventional circuit shown in Figure 1 as a particularly wide-band circuit, the circuit bandwidth is inversely proportional to the output resistance, so the conventional level shift circuit, which cannot reduce the output resistance sufficiently, will In practice, it is often the case that bandwidth is not available.

本発明は、この点に鑑み、出力抵抗が従来回路
よりもはるかに小さいレベルシフト回路の提供を
目的とする。
In view of this point, the present invention aims to provide a level shift circuit whose output resistance is much smaller than that of conventional circuits.

本発明によるレベルシフト回路は、ドレイン電
極を第1の電源に接続しゲート電極を入力端子に
接続しソース電極を接続点に接続した第1の
EFTと、ドレイン電極を前記接続点に接続しソ
ース電極を第2の電源に接続しゲート電極を第3
の電源に接続した第2のFETと、ドレイン電極
を前記第1の電源に接続しゲート電極を第4の電
源に接続しソース電極を出力端子に接続した第3
のEFTと、ドレイン電極を前記出力端子に接続
しソース電極を前記第2の電源に接続した第4の
EFTと、前記接続点の電位変化と前記出力端子
の電位変化とを加え合わせて前記第4のEFTの
ゲート電極に印加する回路とを備えて構成され
る。
The level shift circuit according to the present invention includes a first circuit having a drain electrode connected to a first power supply, a gate electrode connected to an input terminal, and a source electrode connected to a connection point.
EFT, the drain electrode is connected to the connection point, the source electrode is connected to the second power source, and the gate electrode is connected to the third power source.
a second FET connected to a power source, and a third FET whose drain electrode is connected to the first power source, whose gate electrode is connected to a fourth power source, and whose source electrode is connected to the output terminal.
and a fourth EFT whose drain electrode is connected to the output terminal and whose source electrode is connected to the second power supply.
The fourth EFT is configured to include an EFT and a circuit that adds the potential change at the connection point and the potential change at the output terminal and applies the sum to the gate electrode of the fourth EFT.

以下図面を参照して本発明を詳細に説明する。 The present invention will be described in detail below with reference to the drawings.

第2図は本発明の一実施例を示す回路図であ
る。MOSFET11のドレイン電極は第1の電源
19に接続され、ゲート電極は入力端子16に接
続され、ソース電極は接続点18に接続されてい
る。MOSFET12のドレイン電極は接続点18
に接続され、ゲート電極はバイアス電位を与える
電源21に接続され、ソース電極は第2の電源2
0に接続されている。MOSFET13のドレイン
電極は第1の電源19に接続されゲート電極はバ
イアス電位を与える電源22に接続され、ソース
電極は出力端子17に接続されている。
MOSFET14のドレイン電極は出力端子17に
接続され、ソース電極は第2の電源20に接続さ
れている。15は出力端子17と接続点18の電
位変化を加算してMOSFET14のゲート電極に
印加するアナログ加算回路である。第2図で用い
ているFETはすべて同一導電型である。
FIG. 2 is a circuit diagram showing one embodiment of the present invention. A drain electrode of the MOSFET 11 is connected to a first power supply 19 , a gate electrode is connected to an input terminal 16 , and a source electrode is connected to a connection point 18 . The drain electrode of MOSFET 12 is the connection point 18
The gate electrode is connected to a power supply 21 that provides a bias potential, and the source electrode is connected to a second power supply 21.
Connected to 0. A drain electrode of the MOSFET 13 is connected to a first power source 19, a gate electrode is connected to a power source 22 that provides a bias potential, and a source electrode is connected to an output terminal 17.
The drain electrode of the MOSFET 14 is connected to the output terminal 17, and the source electrode is connected to the second power supply 20. Reference numeral 15 denotes an analog addition circuit that adds the potential changes at the output terminal 17 and the connection point 18 and applies the result to the gate electrode of the MOSFET 14. All FETs used in Figure 2 are of the same conductivity type.

次に第2図に示す回路の動作を説明する。
MOSFET11と12は第1図の回路と同じソー
スフオロワ回路を構成する。入力端子16に加え
られる信号は、MOSFET11と12の利得係数
とMOSFET12のゲート電極のバイアス電位に
より決定される大きさだけ電位移動を受け、接続
点18に現われる。一方MOSFET13と14は
インバータ回路を構成し、その利得はMOSFET
13と14のトランスコンダクタンスの比により
ほぼ決定される。この利得が充分大きく、かつア
ナログ加算回路15の利得が1の近傍またはそれ
以上あるときは、出力端子17からMOSFET1
4のゲート電極への負帰還により、MOSFET1
4のゲート電極の電位の変化は常に小さく抑えら
れる。従つて、接続点18の電位変化と出力端子
17の電位変化との和はほぼ零になる。この結
果、出力端子17には接続点18の電位変化とほ
ぼ同じ大きさで移送が反対の電位変化が現われ
る。すなわち出力端子17には入力端子16に加
わる信号とほぼ同じ大きさで位相が反対の電位変
化が得られるから、本回路はレベルシフト回路と
して動作する。そして、この回路の電位移動の大
きさは、MOSFET11及び12を流れる電流、
MOSFET13のゲート・ソース間電圧(VGS)
並びに電源22のバイアス電位によつて定まる。
Next, the operation of the circuit shown in FIG. 2 will be explained.
MOSFETs 11 and 12 constitute a source follower circuit similar to the circuit shown in FIG. The signal applied to input terminal 16 undergoes a potential shift by an amount determined by the gain coefficients of MOSFETs 11 and 12 and the bias potential of the gate electrode of MOSFET 12, and appears at connection point 18. On the other hand, MOSFETs 13 and 14 constitute an inverter circuit, and the gain is
It is approximately determined by the ratio of the transconductances of 13 and 14. When this gain is sufficiently large and the gain of the analog adder circuit 15 is near or above 1, the MOSFET 1 is connected to the output terminal 17.
Due to negative feedback to the gate electrode of MOSFET 1
Changes in the potential of the gate electrode No. 4 are always kept small. Therefore, the sum of the potential change at the connection point 18 and the potential change at the output terminal 17 becomes approximately zero. As a result, a potential change appears at the output terminal 17 which is approximately the same magnitude as the potential change at the connection point 18 and whose transfer is opposite. That is, since the output terminal 17 obtains a potential change that is approximately the same magnitude and opposite in phase to the signal applied to the input terminal 16, this circuit operates as a level shift circuit. The magnitude of the potential shift in this circuit is determined by the current flowing through MOSFETs 11 and 12.
MOSFET13 gate-source voltage (VGS)
It is also determined by the bias potential of the power supply 22.

次に第2図の回路の出力抵抗を第1図の回路と
比較に於て考察する。出力抵抗は入力信号を零に
したときの出力端子に印加した電位変化と、それ
によつて生じる出力電流の変化量の比である。第
1図に於て、出力端子4に電位変化を印加したと
きに生じる電流の変化は、MOSFET1を流れる
電流の変化によるものがほとんどであり、従つて
出力抵抗は前述の通りほぼ1/gm1となる。これ
に対して第2図の回路に於て、出力端子に電位変
化を印加した場合は、MOSFET13を流れる電
流の変化の他に、アナログ加算回路15を通して
MOSFET14のゲート電位が変化することによ
るMOSFET14を流れる電流の変化があり、し
かも普通後者の方がはるかに大きい。従つて第2
図の回路の出力抵抗はほぼ1/(A・gm14)と
なる。但し、Aは帰還回路15の利得であり、
gm14はMOSFET14のトランスコンダクタン
スである。さて、飽和領域にあるMOSFETのト
ランスコンダクタンスgmは近似的に次式で表わ
されことは能く知られている。
Next, the output resistance of the circuit shown in FIG. 2 will be considered in comparison with the circuit shown in FIG. Output resistance is the ratio of the change in potential applied to the output terminal when the input signal is set to zero and the amount of change in output current caused by the change. In Figure 1, the change in current that occurs when a potential change is applied to output terminal 4 is mostly due to the change in the current flowing through MOSFET 1, and therefore the output resistance is approximately 1/gm1 as described above. Become. On the other hand, in the circuit shown in FIG. 2, when a potential change is applied to the output terminal, in addition to the change in the current flowing through the MOSFET 13, the current changes through the analog adder circuit 15.
There is a change in the current flowing through MOSFET 14 due to a change in the gate potential of MOSFET 14, and the latter is usually much larger. Therefore, the second
The output resistance of the circuit shown in the figure is approximately 1/(A·gm14). However, A is the gain of the feedback circuit 15,
gm14 is the transconductance of MOSFET14. Now, it is well known that the transconductance gm of a MOSFET in the saturation region is approximately expressed by the following equation.

gm=2×IDS/(VGS−VT) ………(1) ここでIDS、VGS、VTはそれぞれドレイン・
ソース間電流、ゲート・ソース間電圧、闘値電圧
である。第1図に於ては、電位移動の大きさと消
費電流が決定されてしまうと、MOSFET1のゲ
ート・ソース間電圧VGSとドレイン・ソース間
電流IDSが決定されてしまうので、gm1も決定さ
れてしまうのは式(1)より分かる。これに対し第2
図の回路に於ては、電位移動の大きさは
MOSFET14ゲート・ソース間電圧(VGS)に
は依存しないから、MOSFET14のドレイン・
ソース間電流IDSが一定の条件のもとでも、
MOSFET14のゲート電極の電位を第2の電源
に近づけていくことで、電位移動の大きさを変化
させることなく、MOSFET14のゲート・ソー
ス間電圧VGSを闘値電圧VTに幾らでも近づける
ことができる。そこで、式(1)によると原理的には
gm14は幾らでも大きくすることが可能であるこ
とが分る。
gm=2×IDS/(VGS−VT) ………(1) Here, IDS, VGS, and VT are the drain and
These are source current, gate-source voltage, and threshold voltage. In Figure 1, once the magnitude of the potential shift and current consumption are determined, the gate-source voltage VGS and drain-source current IDS of MOSFET1 are determined, so gm1 is also determined. can be seen from equation (1). On the other hand, the second
In the circuit shown in the figure, the magnitude of the potential shift is
Since it does not depend on the MOSFET14 gate-source voltage (VGS), the MOSFET14 drain and
Even under the condition that the source-to-source current IDS is constant,
By bringing the potential of the gate electrode of the MOSFET 14 closer to the second power supply, the gate-source voltage VGS of the MOSFET 14 can be brought closer to the threshold voltage VT as much as possible without changing the magnitude of potential shift. Therefore, according to formula (1), in principle
It turns out that gm14 can be made as large as desired.

従つて、電位移動の大きさと消費電流が決定さ
れた場合、一般にA・gm14はgm1よりはるかに
大きくすることが可能であり、第2図の回路によ
ると第1図の回路に比較しはるかに小さな出力抵
抗を得ることができる。
Therefore, once the magnitude of the potential shift and the current consumption are determined, A·gm14 can generally be made much larger than gm1, and the circuit of FIG. 2 is much larger than the circuit of FIG. Small output resistance can be obtained.

第2図の回路をさらに具体化した一実施例を第
3図に示す。
FIG. 3 shows an embodiment in which the circuit shown in FIG. 2 is further embodied.

デプレツシヨン型MOSFET30と31には電
気的特性が同じものが選んであり、また出力端子
17と接続点18の動作点電位は等しくとられて
いる。出力端子17と接続点18に生じた逆向き
の電位変化に対しては、MOSFET30と31を
流れる電流の合計は変化しないから、MOSFET
14のゲート電極37の電位は変化しない。出力
端子17と接続点18に生じた同じ向きの電位変
化に対しては、MOSFET30と31は
MOSFET32と共にソースフオロワ回路として
働き、MOSFET14のゲート電極37に電位変
化ほぼ1の利得で伝える。従つてMOSFET3
0,31,32からなる回路は第2図のアナログ
加算回路15を実現している。
The depletion type MOSFETs 30 and 31 are selected to have the same electrical characteristics, and the operating point potentials of the output terminal 17 and the connection point 18 are set to be equal. Since the sum of the currents flowing through MOSFETs 30 and 31 does not change in response to an opposite potential change that occurs at the output terminal 17 and the connection point 18, the MOSFET
The potential of the gate electrode 37 of No. 14 does not change. For potential changes in the same direction that occur at the output terminal 17 and the connection point 18, MOSFETs 30 and 31
Together with the MOSFET 32, it functions as a source follower circuit, and transmits potential changes to the gate electrode 37 of the MOSFET 14 with a gain of approximately 1. Therefore MOSFET3
The circuit consisting of 0, 31, and 32 realizes the analog adder circuit 15 of FIG.

デプレツシヨン型MOSFET33とエンハンス
メント型MOSFET34は、MOSFET12及び
MOSFET32のゲート電極にバイアス電位を与
えている。同様にデプレツシヨン型MOSFET3
5とエンハンスメント型MOSFET36は、
MOSFET13のゲート電極にバイアス電位を与
える電源の働きをしている。以上ように第3図の
回路は第2図の回路を具体化した一例となつてい
る。
The depletion type MOSFET 33 and the enhancement type MOSFET 34 are the MOSFET 12 and the enhancement type MOSFET 34.
A bias potential is applied to the gate electrode of MOSFET 32. Similarly, depletion type MOSFET3
5 and enhancement type MOSFET36 are
It functions as a power supply that applies a bias potential to the gate electrode of MOSFET 13. As described above, the circuit shown in FIG. 3 is an example of the circuit shown in FIG. 2.

以上述べた如く本発明によれば、従来のものよ
り出力抵抗のはるかに小さいレベルシフト回路を
得ることができる。従つて、本発明は、
MOSFET集積回路に於けるリニア回路の広帯域
化に大きく寄与することができる。
As described above, according to the present invention, it is possible to obtain a level shift circuit with a much smaller output resistance than the conventional one. Therefore, the present invention
It can greatly contribute to widening the bandwidth of linear circuits in MOSFET integrated circuits.

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

第1図は従来のレベルシフト回路(ソースフオ
ロワ回路)の回路図、第2図は本発明の一実施例
を示す回路図、第3図は第2図をさらに具体化し
た一実施例を示す回路図である。 1,2,11,12,13,14,30,3
1,32,33,34,35,36……
MOSFET、3,16……入力端子、4,17…
…出力端子、5,6,19,20……電源、7,
21,22……バイアス電位を与える電源、15
……アナログ加算回路、18……接続点。
FIG. 1 is a circuit diagram of a conventional level shift circuit (source follower circuit), FIG. 2 is a circuit diagram showing an embodiment of the present invention, and FIG. 3 is a circuit diagram showing an embodiment that further embodies FIG. 2. It is a diagram. 1, 2, 11, 12, 13, 14, 30, 3
1, 32, 33, 34, 35, 36...
MOSFET, 3, 16...Input terminal, 4, 17...
...Output terminal, 5, 6, 19, 20...Power supply, 7,
21, 22...power supply that provides bias potential, 15
...Analog addition circuit, 18...Connection point.

Claims (1)

【特許請求の範囲】[Claims] 1 ドレイン電極を第1の電源に接続しゲート電
極を入力端子に接続しソース電極を接続点に接続
した第1のFETと、ドレイン電極を前記接続点
に接続しソース電極を第2の電源に接続しゲート
電極を第3の電源に接続した第2のFETと、ド
レイン電極を前記第1の電源に接続しゲート電極
を第4の電源に接続しソース電極を出力端子に接
続した第3のFETと、ドレイン電極を前記出力
端子に接続しソース電極を前記第2の電源に接続
した第4のFETと、前記接続点の電位変化と前
記出力端子の電位変化とを加え合わせて前記第4
のFETのゲート電極に印加する回路とを備える
レベルシフト回路。
1 A first FET with a drain electrode connected to a first power source, a gate electrode connected to an input terminal, and a source electrode connected to a connection point, and a first FET with a drain electrode connected to the connection point and a source electrode connected to a second power source. a second FET with a gate electrode connected to a third power source; and a third FET with a drain electrode connected to the first power source, a gate electrode connected to a fourth power source, and a source electrode connected to an output terminal. FET, a fourth FET whose drain electrode is connected to the output terminal and whose source electrode is connected to the second power supply, and the fourth FET which combines the potential change at the connection point and the potential change at the output terminal
A level shift circuit comprising: a circuit for applying voltage to the gate electrode of the FET;
JP57170732A 1982-09-29 1982-09-29 Level shifting circuit Granted JPS5961205A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57170732A JPS5961205A (en) 1982-09-29 1982-09-29 Level shifting circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57170732A JPS5961205A (en) 1982-09-29 1982-09-29 Level shifting circuit

Publications (2)

Publication Number Publication Date
JPS5961205A JPS5961205A (en) 1984-04-07
JPH0412645B2 true JPH0412645B2 (en) 1992-03-05

Family

ID=15910358

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57170732A Granted JPS5961205A (en) 1982-09-29 1982-09-29 Level shifting circuit

Country Status (1)

Country Link
JP (1) JPS5961205A (en)

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* Cited by examiner, † Cited by third party
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CN102427358A (en) * 2011-06-14 2012-04-25 盐城师范学院 Solar power-supply power grounding resistance automatic monitoring liquid filling device

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