JPS6149517A - Pulse generating circuit - Google Patents

Pulse generating circuit

Info

Publication number
JPS6149517A
JPS6149517A JP59172011A JP17201184A JPS6149517A JP S6149517 A JPS6149517 A JP S6149517A JP 59172011 A JP59172011 A JP 59172011A JP 17201184 A JP17201184 A JP 17201184A JP S6149517 A JPS6149517 A JP S6149517A
Authority
JP
Japan
Prior art keywords
circuit
differential amplifier
output
trs
inputted
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.)
Pending
Application number
JP59172011A
Other languages
Japanese (ja)
Inventor
Harunori Sato
里 治則
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
Original Assignee
Mitsubishi Electric 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 filed Critical Mitsubishi Electric Corp
Priority to JP59172011A priority Critical patent/JPS6149517A/en
Publication of JPS6149517A publication Critical patent/JPS6149517A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K5/00Manipulating of pulses not covered by one of the other main groups of this subclass

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Pulse Circuits (AREA)
  • Manipulation Of Pulses (AREA)

Abstract

PURPOSE:To improve the cost performance by constituting a semiconductor integrated circuit as the pulse generating circuit composed of a differential amplifier to which an input signal is inputted, a slow differential amplifier, a fast differential, an AND circuit, and an OR circuit. CONSTITUTION:An unipolar input Vin is supplied to the 1st differential amplifier consisting of transistors (TR) Q3 and Q4 to generate outputs Va and Va'. Then, they are inputted to the 2nd slow differential amplifier consisting of TRs Q5 and Q6 through the level shifting circuit composed of TRs Q3 and Q4 and converted into polarity-inverted outputs Vb and Vb' a certain time later. Further, they are inputted to the 3rd fast differential amplifier consisting of TRs Q7 and Q8 and converted into polarity-inverted rectangular waves Vc and Vc'. The waves are inputted to the OR circuit composes of a resistance R10 through respective AND circuits composed of TRs Q9-Q11 and Q12-Q14, thereby generating a pulse output. Thus, the pulse width is determined by the delay time and the cost performance is improved.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、半導体集積回路における矩形波の立上り、
立下りの各時点でパルスを発生させる際、外部にコンデ
ンサ、抵抗体を設けないで構成できるよ51CLy、:
パルス発生−路に関するものである。
[Detailed Description of the Invention] [Technical Field of the Invention] This invention relates to the rise of a rectangular wave in a semiconductor integrated circuit,
When generating a pulse at each falling point, it can be configured without providing an external capacitor or resistor.51CLy:
It concerns the pulse generation path.

〔従来技術〕[Prior art]

従来、矩形波の立上り、立下り部から各々パルスを発生
させるときは、極性反転回路と単安定マルチバイブレー
タのような2組のパルス化回路と、パルス幅tきめるC
(コンデンサ)、R(抵抗体ン素子等が必要であった。
Conventionally, when generating pulses from the rising and falling parts of a rectangular wave, two sets of pulsing circuits such as a polarity inverting circuit and a monostable multivibrator are used, and a C which determines the pulse width t is used.
(capacitor), R (resistor element, etc.) were required.

従来のパルス発生回路Z、半導体集積回路によって構成
するとき、パルス幅と、立上り、立下り時のベアリング
等を揃えるためには、外部KC。
When constructing a conventional pulse generating circuit Z using a semiconductor integrated circuit, an external KC is required in order to match the pulse width and the bearings at rise and fall.

R等のg子v設けてパルス幅ン設定していに0このため
、ICのピンの増加と外部素子が増加し、コストアップ
の要因となる欠点があった。
This has the drawback that the number of IC pins and external elements increases, which increases the cost, since the pulse width is set by providing a gate such as R and the like.

〔発明の概要〕[Summary of the invention]

この発BAは、上記のような従来の欠点を除去するため
、トランジスタのおくn時rkQY利用し、外部用ビン
と、外部C,R等の素子を省略できるよ5Kして、簡単
で安価なパルス発生回路を提供丁゛るものである。以下
、この発明の一実施例乞図面によって説明する。
In order to eliminate the above-mentioned drawbacks of the conventional BA, this BA uses the n-time rkQY of the transistor, and is simple and inexpensive by using 5K, which can omit external bins and elements such as external C and R. This provides a pulse generation circuit. Hereinafter, one embodiment of the present invention will be explained with reference to the drawings.

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

第1図はこの発明の一実施例χ示す回路図で、Via”
入力、vrel kl基準電圧源であり、Q、、Q2は
トランジスタ、R1+R2&′f、負荷抵抗体+Cs+
は定電流源であり、コtt、らQ+ −Qx 、R+ 
、R2およびC,lで第1の差動増幅i−+が構成さn
る。
FIG. 1 is a circuit diagram showing an embodiment of this invention.
Input, vrel kl reference voltage source, Q,, Q2 are transistors, R1+R2&'f, load resistor +Cs+
is a constant current source, and Cott et al. Q+ −Qx , R+
, R2 and C,l constitute a first differential amplifier i-+ n
Ru.

また、レベルシフト回路が、トランジスタQ3゜Q4と
、レベルシフト用抵抗体R3,R4および定電流源Cm
2r 0g3で構成さn、遅延時間τpd(propa
gation  delay time) Y発生させ
る定めの第2の差動増幅器がトランジスタQs 、Qa
 と負荷抵抗体Rs HR6、レベルソフト用抵抗体R
7゜ダイオードD3.定電流源C,4で構成さnる。さ
らにτ、d/2という安定した遅延時間を得る几めに波
形整形を行うための第3の差動増幅器がトランジスタQ
7.Q、、°負荷抵抗体Rs r  Rs + ダイオ
ードD21 定電流源0.5で構成さn、負論理のAN
D回路がトランジスタQ e + Q+o+ Q+++
定電流源C1で構成さn、同じく負論理のAND回路が
、トランジスタQ+z jQ+z l Q101 定電
流源C,gで構成さnる。なお、VreL2は基準電圧
源、To  は出力端子、vc!は電源電圧である。
Further, the level shift circuit includes transistors Q3 and Q4, level shift resistors R3 and R4, and constant current source Cm.
2r 0g3 n, delay time τpd (propa
(delay time) The second differential amplifier designed to generate Y is the transistors Qs and Qa.
and load resistor Rs HR6, level soft resistor R
7° diode D3. It consists of a constant current source C,4. Furthermore, the third differential amplifier is a transistor Q to perform waveform shaping to obtain a stable delay time of τ, d/2.
7. Q,, °Load resistor Rs r Rs + diode D21 Consists of constant current source 0.5 n, negative logic AN
D circuit is transistor Q e + Q+o+ Q+++
A constant current source C1 constitutes a negative logic AND circuit, and a negative logic AND circuit consists of transistors Q+z jQ+z l Q101 constant current sources C and g. Note that VreL2 is a reference voltage source, To is an output terminal, and vc! is the power supply voltage.

また、第2図は第1図の動作説明用の波形図で、横軸に
時間軸乞とり、縦軸に入力vIfi、第1の差動増幅器
の出力v、、η、遅n時間τd”を発生させる定めの第
2の差動増幅器の出力vb  、可、波形整形のための
第3の差動増幅器の出力ve。
FIG. 2 is a waveform diagram for explaining the operation of FIG. 1, where the horizontal axis is the time axis, the vertical axis is the input vIfi, the output v, η, and the delay n time τd of the first differential amplifier. The output vb of a predetermined second differential amplifier for generating , and the output ve of a third differential amplifier for waveform shaping.

η、負論理のAND回路の出力vd + ve および
OR回路の出力To ’を示している。
η, the output vd + ve of the negative logic AND circuit, and the output To' of the OR circuit.

第3図は第2の差動増幅器の立上り時間、立下り時間が
異なるときの動作説明用の波形図であり、Vb# VB
  Y実線と破線で重ねてあられし定もので、横軸に時
間t、縦軸l1cva + vb + ’b l Ve
を示している。
FIG. 3 is a waveform diagram for explaining the operation when the rise time and fall time of the second differential amplifier are different.
The Y solid line and the broken line are superimposed, and the horizontal axis is time t, and the vertical axis is l1cva + vb + 'b l Ve
It shows.

次に動作忙ついて説明する。Next, I will explain about the operation.

第1図において、入力V1mなる矩形波が第1の差動増
幅器に加えらnると、その負荷抵抗体RI。
In FIG. 1, when a rectangular wave input V1m is applied to the first differential amplifier, its load resistor RI.

R2およびバッファ用のトランジスタQ、、Q4を通っ
て、v、 、  v、 なる両極性の出力が得らnる。
Through R2 and buffer transistors Q, , Q4, bipolar outputs v, , v, are obtained.

レベルシフト用抵抗体R1、R4’を介して、前記出力
V m +  V A ハ各々Rs Iz 、R4Is
だけレベルシフトさrる。この場合、元の矩形波の出力
v1.籍 と時間軸上では同じ位相で、遅n時間は無視
できるものとする。次に、出力V、 、 V。
Through the level shift resistors R1 and R4', the outputs V m + V A are Rs Iz and R4Is, respectively.
level shift. In this case, the output of the original square wave v1. It is assumed that the phase is the same as that on the time axis, and the delay n time can be ignored. Then the output V, , V.

は遅延時間7発生させるための第2の差動増幅器忙加え
られてvl、、9bなる出力が得らnる。各々の立上り
、立下りの傾斜電圧vbr+π、およびVbfl 昂は
等しい。
is added to the second differential amplifier to generate the delay time 7, and an output of vl, , 9b is obtained. The respective rising and falling slope voltages vbr+π and Vbfl are equal.

次K、出力Vb+’bは波形整形する定めの第3の差動
増幅器に加えらn、立上り、立下りの各傾斜電圧Vbr
と四の電圧レベルが等しい時間1゜および立下り、立上
りの各傾斜電圧vbtと可が等しい時間t3で反転し、
その出力電圧がVer−マ)となる出力が得らn、v、
、  v、より各々r(l++τD2遅rしる。ここで
vbl vl、の各々の立上Cハ立下り時間は牛導体集
積回路化したときは寄生容量の影響等で異なるが、トラ
ンジスタQIllQ61抵抗体R5−R6の特性を揃え
てバランスがとnnば、前述のように立上り電圧Vbr
 + τ1同士と立下り電圧vbf +  951同士
は等しくでき、こrlらの条件下で遅延時間τ。1.τ
D2が等しくなることt第3図を用いて説明する。
The next K, output Vb+'b is applied to a predetermined third differential amplifier for waveform shaping, and each rising and falling slope voltage Vbr
and four voltage levels are equal, and each falling and rising slope voltage vbt is reversed at a time t3, which is equal to
An output whose output voltage is Ver-ma) is obtained, n, v,
, v, respectively r (l + + τD2 delay r. Here, the rise and fall times of vbl and vl, respectively, differ due to the influence of parasitic capacitance when integrated circuits are implemented, but transistors QIll and Q61 resistors If the characteristics of R5-R6 are aligned and balanced, the rising voltage Vbr will increase as described above.
+ τ1 and falling voltage vbf + 951 can be made equal, and under these conditions the delay time τ. 1. τ
The fact that D2 becomes equal will be explained using FIG. 3.

第1図の定電流源C,4Tl−流nるバイアス電流工。Constant current source C in FIG. 1, 4Tl-current bias current generator.

を任意の値に選んで、遅延時間τDl+  τnz’l
ある大きさになるように設定したときの一例が第3図の
如くなったとする。第3図から明らかなように、時間t
0 〜t1 およびt2 〜t3  までのVjr、■
の傾斜が等しく直線であり、時間t0〜t、およびt2
〜t3までのvbt T  ’Ib、の傾斜が等しく直
線の時はその起点から交点までを指子τD1とτD2は
等しい値(こlrLをτ。とする〕となる。
By choosing an arbitrary value, the delay time τDl + τnz'l
Assume that an example of setting a certain size is shown in FIG. 3. As is clear from Fig. 3, time t
Vjr from 0 to t1 and from t2 to t3, ■
are equally straight and the slopes of t0 to t and t2
When the slopes of vbt T'Ib from t3 to t3 are equal and straight, the indicators τD1 and τD2 have the same value (here, lrL is τ) from the starting point to the intersection.

こうして得らnたv、 、  v、’、  ve、−九
 なる矩形波は負論理を構成する2組のAND回路、丁
なわもトランジスタQ 9 a Q1o+  Qllお
よびトランジスタQ lzr Qsx* Q14で、v
ll ・ve = vd 、   v& ・ vc =
 v。
The rectangular waves n, v, , v,', ve, -9 obtained in this way are obtained by two sets of AND circuits forming a negative logic, transistor Q 9 a Q1o+ Qll and transistor Q lzr Qsx* Q14, and v
ll ・ve = vd, v& ・vc =
v.

が得られ、OR回路を構成する抵抗体R1゜の端子に、 v、  =v4  +v。is obtained, and at the terminal of the resistor R1° constituting the OR circuit, v, =v4 +v.

なる出力が得らnる。こ〜で、l4=50μA。An output of n is obtained. Here, l4 = 50 μA.

R,=16にΩ、Rs=16にΩK L rsとき、τ
D中50na が得らnる。
When R,=16 is Ω, and Rs=16 is ΩK L rs, τ
50 na in D is obtained.

この発明によるパルス発生回路はパルス幅を遅延時間に
より決定し、特にパルス幅が細いとき、安定したパルス
幅χもち、入力矩形波の立上りおよび立下り部でパルス
を発生させることができる。
The pulse generating circuit according to the present invention determines the pulse width by the delay time, and when the pulse width is particularly narrow, it has a stable pulse width χ and can generate pulses at the rising and falling parts of the input rectangular wave.

〔発明の効果〕〔Effect of the invention〕

以上説明しLようK、この発明は一極性の入力vInV
cより第1の差動増幅器から両極性の出力vll。
As explained above, this invention has a unipolar input vInV.
Bipolar output vll from the first differential amplifier from c.

η を発生させ、こnらの出力vll、 −−を低速の
第2の差動増幅器を通して、ある時間遅ftケ有し、か
つ極性の反転した出力vb、  Vj に変換し、こn
らの出力vb+  v6 ’を高速の第3の差動増幅器
を通して極性の反転しに矩形波であるv8.ηに変換し
、さらに2組のAND回路を通して7d二v11  ・
Vcl  V、  =7.  ・v8なる出力に変換し
、こnらの出力v4.v、VCよりOR回路を用いてV
O=v、1 +v、なるパルス出力音発生させる回路か
らなっているので、集積回路に構成したとき、パルスの
時間幅?きめるC、R素子および外部端子を削除できる
定め、安価で、コストパフォーマンスの良いパルス発生
回路を構成することができ、産業上の各分野で幅広く用
いることができる利点がある。
These n outputs vll, -- are passed through a low-speed second differential amplifier and converted into outputs vb, Vj with a certain time delay ft and inverted polarity.
The outputs vb+v6' from vb+v6' are passed through a high-speed third differential amplifier to invert the polarity and generate a rectangular wave v8. 7d2v11 ・
Vcl V, =7.・Convert to an output v8, and convert these n outputs v4. v, V using an OR circuit from VC
It consists of a circuit that generates a pulse output sound of O = v, 1 + v, so when it is configured as an integrated circuit, the time width of the pulse? Since the C and R elements and external terminals can be eliminated, an inexpensive pulse generating circuit with good cost performance can be constructed, and there is an advantage that it can be widely used in various industrial fields.

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

第1図はこの発明の一実施例によるパルス発生回路図、
第2図、第3図は第1図の動作説明の定めの波形図であ
る。 図中、vl。は入力、Vrefl r  Vreflは
基準電圧源、Q8〜Q 14はトランジスタ、R□l 
 R1+ Ra1R6,R81R9は負荷抵抗体・Ra
 、R4,R7ニ はンベルシフト抵抗体、Ca I”−CB 7 k1定
電流源、DI−02はダイオード、To は出力端子、
weeは電源電圧である。 なお、図中の同一符号は同一または相当部分ン示す。 代理人 大岩増雄   (外2名) 第2図 −埼P1t
FIG. 1 is a pulse generation circuit diagram according to an embodiment of the present invention.
FIGS. 2 and 3 are typical waveform diagrams for explaining the operation of FIG. 1. In the figure, vl. is the input, Vrefl r Vrefl is the reference voltage source, Q8 to Q14 are transistors, R□l
R1+ Ra1R6, R81R9 are load resistors/Ra
, R4, R7 is a bell shift resistor, Ca I"-CB7 k1 constant current source, DI-02 is a diode, To is an output terminal,
wee is the power supply voltage. Note that the same reference numerals in the figures indicate the same or corresponding parts. Agent Masuo Oiwa (2 others) Figure 2 - Sait P1t

Claims (1)

【特許請求の範囲】[Claims] 一極性の入力v_i_nにより両極性の出力v_a、@
v_a@を発生させる第1の差動増幅器と、前記出力v
_a、@v_a@からある時間遅れを有しかつ極性の反
転した出力v_b、@v_b@に変換する低速の第2の
差動増幅器と、前記出力v_b、@v_b@により極性
の反転した矩形波である出力v_c、@v_c@に変換
する高速の第3の差動増幅器と、さらにv_d=@v@
_a・@v_c@、v_e=v_a・v_cなる出力に
変換する2組のAND回路と、前記出力v_d、v_e
によりv_0=v_d+v_eなるパルス出力を発生さ
せるOR回路とからなり、前記各差動増幅器、AND回
路およびOR回路を半導体集積回路で構成したことを特
徴とするパルス発生回路。
Unipolar input v_i_n causes bipolar output v_a, @
a first differential amplifier that generates v_a@, and the output v
a low-speed second differential amplifier that converts _a, @v_a@ into an output v_b, @v_b@ with a certain time delay and inverted polarity, and a rectangular wave with inverted polarity due to the output v_b, @v_b@ a high-speed third differential amplifier that converts the output v_c, @v_c@, and further v_d=@v@
_a・@v_c@, two sets of AND circuits that convert the output to v_e=v_a・v_c, and the outputs v_d, v_e
1. A pulse generating circuit comprising an OR circuit that generates a pulse output of v_0=v_d+v_e, wherein each of the differential amplifiers, the AND circuit, and the OR circuit are constructed of semiconductor integrated circuits.
JP59172011A 1984-08-17 1984-08-17 Pulse generating circuit Pending JPS6149517A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59172011A JPS6149517A (en) 1984-08-17 1984-08-17 Pulse generating circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59172011A JPS6149517A (en) 1984-08-17 1984-08-17 Pulse generating circuit

Publications (1)

Publication Number Publication Date
JPS6149517A true JPS6149517A (en) 1986-03-11

Family

ID=15933872

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59172011A Pending JPS6149517A (en) 1984-08-17 1984-08-17 Pulse generating circuit

Country Status (1)

Country Link
JP (1) JPS6149517A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH098616A (en) * 1995-06-19 1997-01-10 Nec Corp Variable delay circuit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH098616A (en) * 1995-06-19 1997-01-10 Nec Corp Variable delay circuit

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