JPS59153303A - High frequency oscillator - Google Patents
High frequency oscillatorInfo
- Publication number
- JPS59153303A JPS59153303A JP58028195A JP2819583A JPS59153303A JP S59153303 A JPS59153303 A JP S59153303A JP 58028195 A JP58028195 A JP 58028195A JP 2819583 A JP2819583 A JP 2819583A JP S59153303 A JPS59153303 A JP S59153303A
- Authority
- JP
- Japan
- Prior art keywords
- high frequency
- power
- circuit
- frequency oscillator
- output
- 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
Links
- 230000010355 oscillation Effects 0.000 claims abstract description 18
- 230000003321 amplification Effects 0.000 claims description 14
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 14
- 230000005669 field effect Effects 0.000 claims description 7
- 238000001020 plasma etching Methods 0.000 abstract description 6
- 230000002265 prevention Effects 0.000 abstract 1
- 239000003990 capacitor Substances 0.000 description 11
- 239000013078 crystal Substances 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 238000001514 detection method Methods 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 238000005530 etching Methods 0.000 description 3
- 230000015556 catabolic process Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000007274 generation of a signal involved in cell-cell signaling Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 210000003127 knee Anatomy 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000178 monomer Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000013077 target material Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L5/00—Automatic control of voltage, current, or power
- H03L5/02—Automatic control of voltage, current, or power of power
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
- H03B5/00—Generation of oscillations using amplifier with regenerative feedback from output to input
- H03B5/30—Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element being electromechanical resonator
- H03B5/32—Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element being electromechanical resonator being a piezoelectric resonator
- H03B5/36—Generation of oscillations using amplifier with regenerative feedback from output to input with frequency-determining element being electromechanical resonator being a piezoelectric resonator active element in amplifier being semiconductor device
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
- H03B2200/00—Indexing scheme relating to details of oscillators covered by H03B
- H03B2200/006—Functional aspects of oscillators
- H03B2200/0094—Measures to ensure starting of oscillations
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03B—GENERATION OF OSCILLATIONS, DIRECTLY OR BY FREQUENCY-CHANGING, BY CIRCUITS EMPLOYING ACTIVE ELEMENTS WHICH OPERATE IN A NON-SWITCHING MANNER; GENERATION OF NOISE BY SUCH CIRCUITS
- H03B2200/00—Indexing scheme relating to details of oscillators covered by H03B
- H03B2200/006—Functional aspects of oscillators
- H03B2200/0098—Functional aspects of oscillators having a balanced output signal
Landscapes
- Oscillators With Electromechanical Resonators (AREA)
- Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
- Plasma Technology (AREA)
Abstract
Description
【発明の詳細な説明】
(部業1の利用分野)
4・発明は易にプラズマエツチングを行うだめの1’;
F+出ノ1電力用の便j周波発振器に関する。[Detailed description of the invention] (Application field of division 1) 4. The invention facilitates plasma etching 1';
This invention relates to a frequency oscillator for F+output 1 power.
(IY 来 」〈こ セト了 )
九時、集(6回路の製造技術ト最も重要々ものとしてプ
ラズマによるエツチング技術が利用さニア’l−’Cい
る。この技術の概要は例えば密閉さjtだ反応器内部の
ガスに接して置かハた平行平板電極の負極側平板上に所
定パターンのマスクを施した被処理付和を置き、導入し
たモノマーか当該平行半板電極の間でプラズマ化され、
当該被処理材$−1の十に有機薄膜を形成するものであ
り、ガスをプラズマ状態に励起するだめの外部エイ・ル
キには高周波′に源が一般に用いられる。(6 o'clock) The most important part of circuit manufacturing technology is plasma etching technology.The outline of this technology is, for example, hermetic A target to be treated with a mask of a predetermined pattern is placed on the negative electrode side of the parallel plate electrode placed in contact with the gas inside the reactor, and the introduced monomer is turned into plasma between the parallel half plate electrodes.
An organic thin film is formed on the target material, and a radio frequency source is generally used as an external source for exciting the gas into a plasma state.
当該高周波電源である高周波発振器は通常水晶発振回路
にて1.:156 Ml−fzの高周波を発生シフ、こ
れをトランジスタ、あるいは高出力電力用の」烏合には
真空管を用いて増幅し、1.00 Wの小出力から1ハ
ル以上の高出力の高周波電力を得ている0ところで、上
記の如く高出力電力用の発振器を構成する場合は高電力
増幅を行うことから通常真空管を用いるが、真空管には
特命が比較的短いという根本的な欠点があり、実際の使
用に於ては数千時間で真空管自体の交換、あるいは再調
整を強いられエツチング作業上大きな障害となっている
。The high-frequency oscillator, which is the high-frequency power source, is usually a crystal oscillation circuit. :156 Ml-fz high frequency is generated, and this is amplified using a transistor or a vacuum tube for high output power, and high output high frequency power of more than 1 hull is generated from a small output of 1.00 W. However, when constructing an oscillator for high output power as mentioned above, vacuum tubes are usually used because they perform high power amplification, but vacuum tubes have a fundamental drawback that their special mission is relatively short, and in reality In use, the vacuum tube itself must be replaced or readjusted after several thousand hours, which is a major hindrance to etching work.
一方、トランジスタ、一般的には増幅用半導体デバイス
は前記真空管の如く寿命の障害はないけれども高周波用
素子に於て、高耐圧、高出方用の素子を得ることは技術
的に困難であり、壕だ、二次降伏に弱いことから電力用
としては不適当である。On the other hand, although transistors, generally semiconductor devices for amplification, do not have the same lifespan problems as vacuum tubes, it is technically difficult to obtain high-voltage and high-output devices for high-frequency devices. It is a trench, and is unsuitable for power use because it is vulnerable to secondary surrender.
しかしなから、最近MO8FET (MO8型電界効果
トトランジスタ進歩により高周波高電力用の高性能素子
が実用化されるに至っており、斯かる電力用MO8FE
Tはトランジスタの如く二次降伏がなく大電力用に製造
可能であるという特長をもっている。However, recently, with the advancement of MO8FET (MO8 type field effect transistor), high-performance devices for high frequency and high power have been put into practical use.
Unlike transistors, T has the advantage of not having secondary breakdown and can be manufactured for high power applications.
なお、冒頭で述べた如く、特にプラズマを利用してエツ
チングを行う技術分野に於ては使用する1質周波発振器
は特に十数MHz の高周波を扱うこと、数KWもの
高電力を扱うこと、安定で高精度の正弦波を発生するこ
と、及びこの状態で容易に目つ大幅に出力電力の大きさ
を可変せしめ得ること等の諸性能が要求されるものであ
り、現在に於て斯かる要求を十分に満足する電力用MO
8FETを利用した高周波発振器が開発されるに至って
ぃ々い。As mentioned at the beginning, especially in the technical field of etching using plasma, the single-frequency oscillator used must handle high frequencies of more than 10 MHz, high power of several kilowatts, and stability. Various performances are required, such as being able to generate a high-precision sine wave in this state, and being able to vary the magnitude of the output power easily and significantly, and these requirements are currently not met. MO for power that fully satisfies
A high frequency oscillator using 8FET has just been developed.
(発明の目的)
本発明は上記要求に答えるもので、電力用MO8FET
を利用することにより高周波高電力用で、容易、且つ正
確、更には大幅な出力電力の制御を行うことができる特
にプラズマエツチングの技術分野における高周波発振器
の提供を目的とするものである。(Object of the invention) The present invention is intended to meet the above-mentioned requirements.
The object of the present invention is to provide a high frequency oscillator, particularly in the technical field of plasma etching, which can be used for high frequency and high power, and can easily and accurately control the output power to a large extent.
(発明の構成及び作用)
本発明は発振回路と電力増幅回路を備える高周波発振器
に適用し、特に蟲該電力増幅回路は高電力用MO8FE
Tを利用した増幅段を構成する。(Structure and operation of the invention) The present invention is applied to a high frequency oscillator comprising an oscillation circuit and a power amplification circuit, and in particular, the power amplification circuit is a high power MO8FE.
Construct an amplification stage using T.
そして、本発明の主要部は上記した発振回路の増幅素子
、例えば高周波用l・ランンスタに接続し、アノード電
圧により尚該高周波用トランジスタのバイアスを可変せ
しめる制御用電界効果トランジスタ(FET )を備え
、このFETのベースに印加する制御用直流信号、例え
ば出力電力に対応した直流検出信号を得る検出手段から
の当該信刊、あるいは任意に可変せしめ得る外部からの
出力1J”変信号を印加することによりクローズトルー
プによる出力電力の安定化、オープンルーズによる出力
電力の可変制御等を行うことができるようにしたことを
特徴とする。The main part of the present invention includes a control field effect transistor (FET) which is connected to the amplification element of the oscillation circuit described above, for example, a high frequency transistor, and which allows the bias of the high frequency transistor to be varied by an anode voltage. By applying a control DC signal applied to the base of this FET, for example, the signal from a detection means that obtains a DC detection signal corresponding to the output power, or an output 1J'' variable signal from an external source that can be arbitrarily varied. It is characterized by being able to stabilize the output power using a closed loop and variable control of the output power using an open loop.
(実施例)
以下には本発明を更に具体化した好適な実施例を挙げ図
面を参照して詳細に説明する0図面に於て、第1図は本
発明に係る高周波発振器の電気回路図、第2図は第1図
中制御用FETの入力端子対出力電圧特性図をそれぞれ
表している○
先ず、第1図を参照して発振器全体の概略構成について
説明する○同図中1は発振回路を示し、高周波用npn
l・ランジスタQ11 Qii 、及び水晶発振イXを
利用した水晶発振回路を構成する。トランジスタQ1及
びC2はいずれもエミッタ接地で1、ランジスタQ1の
ベース側に接続した水晶発振子Xにて1 :3.56
MI−(zの高周波を発生する。そして、l−ランジス
クQ1及びC2にて増幅し、トランジスタQ2のコレク
タ側に接続i・た用カドランス゛r1から出力信号を取
り出す。なお、l−ランス゛r2及び調整用可変コンデ
ンサC1は上記水晶発振子Xに直列接続−シた発振用素
子であり、−まだ、符号R,、R2,l(3,)14.
i(5,R6,R7’及びR8はトランジスタQ1又は
C2の7<イアス用抵抗を示し、C2+ C/81 C
4+ C5及びc、、 (#i〕(イノぐス又はカップ
リング用のコンデンサを示し、これら各抵抗、コンデン
サは設計上任意に選定されるものである。(Embodiments) Below, preferred embodiments of the present invention will be described in detail with reference to the drawings. In the drawings, FIG. 1 is an electrical circuit diagram of a high frequency oscillator according to the present invention; Figure 2 shows the input terminal vs. output voltage characteristic diagram of the control FET in Figure 1. First, the overall configuration of the oscillator will be explained with reference to Figure 1. Figure 1 in the figure shows the oscillation circuit. , high frequency npn
A crystal oscillation circuit using the transistor Q11 Qii and the crystal oscillation IX is constructed. Transistors Q1 and C2 both have their emitters connected to 1, and crystal oscillator X connected to the base side of transistor Q1 has a value of 1:3.56.
A high frequency of MI-(z is generated. Then, it is amplified by L-transistors Q1 and C2, and the output signal is taken out from I-transistor r1, which is connected to the collector side of transistor Q2. In addition, L-transistor R2 and adjustment The variable capacitor C1 is an oscillation element connected in series with the crystal oscillator X, and has symbols R, , R2, l(3,)14.
i (5, R6, R7' and R8 are the resistances for transistor Q1 or C2 for 7 < IA, C2+ C/81 C
4+ C5 and c, , (#i) (Indicates a capacitor for insulation or coupling, and these resistors and capacitors are arbitrarily selected based on the design.
ところで、プラズマを発生させるだめに使用される高周
波発振器は前述した如く被処理利料の加工精度が高く要
求されることから供給する高周波の波形も歪の少ない安
定した正弦波か要求されるとともにこの種の高周波発振
器は用途上出力電力を大幅に可変する必要がある。この
ため本発明に於てはトランジスタQ1及びC2の各エミ
ッタ間にコンデンサC4を接続するとともにトランジス
タQ2のエミッタに後述する制御用F E Tの出力で
ある制御用の直流電圧を印加することにより、発振回路
1の出力か高精度の正弦波を維持し、[−4つこの状態
で容易、更に正確に出力電月三の大きさを可変せしめる
ことができるようにしている。具体的にに↓l・ランジ
スタQ2 のエミッタに印加する直流電圧の1可変で発
振回路1の出力、即ちカップリング川のコンデンサC9
の出力を零から最大値−まで[1丁亥することができる
。By the way, as mentioned above, the high-frequency oscillator used to generate plasma is required to have a high processing precision of the processed material, so the waveform of the high-frequency wave supplied is also required to be a stable sine wave with little distortion. For some high-frequency oscillators, it is necessary to vary the output power to a large extent. Therefore, in the present invention, a capacitor C4 is connected between the emitters of transistors Q1 and C2, and a control DC voltage, which is the output of a control FET to be described later, is applied to the emitter of transistor Q2. The output of the oscillation circuit 1 is maintained as a highly accurate sine wave, and in this state it is possible to easily and more accurately vary the magnitude of the output power. Specifically, the output of the oscillation circuit 1, that is, the capacitor C9 of the coupling river, is changed by changing the DC voltage applied to the emitter of the transistor Q2.
The output can be increased by one step from zero to the maximum value -.
ぞL2て、コンデンサC9は増幅回路2の入力1311
1に接続するとともに、この出力側は電力増幅回路3側
に接続1〜、発振回路1の出力は所望の大きさに増幅さ
れて電力増幅回路3に供給されることになる。Now L2, capacitor C9 is connected to input 1311 of amplifier circuit 2.
1, and this output side is connected to the power amplifier circuit 3 side.The output of the oscillation circuit 1 is amplified to a desired magnitude and supplied to the power amplifier circuit 3.
当該電圧増幅回路3は反転用人カドランスT35!:経
て人力した高周波電圧を特性の揃った電力用MO3FE
T Qsと04の並列、及び同じ< MOSi2”ET
Q、とO6の並列を更にプノ7ユプル接続し、′1(
L力芥)1ニーを犬にするとともに、低歪率特性を得る
ようにA 13級動作を行わせしめ出カド・ランスT5
及びr3.に増幅された高周波電力を得ている。The voltage amplifying circuit 3 is an inverting quadrant T35! : MO3FE for power use with uniform characteristics using high-frequency voltage generated manually
Parallel of T Qs and 04, and same < MOSi2”ET
Q, and O6 are connected in parallel, and '1(
L force) In addition to making the 1st knee a dog, it is made to perform A13 class operation to obtain low distortion characteristics.
and r3. It obtains high frequency power that is amplified.
この出力電力は更にコンデンサC1o及びC1□、−そ
才1にコイルL1にてπ形構成したマツチング回路4を
経るとともに電力検出回路5を経て出力端子dに至る。This output power further passes through a matching circuit 4 which is configured in a π-shape with capacitors C1o and C1□, and a coil L1, and also passes through a power detection circuit 5 to an output terminal d.
なお、」二記出力端子dには負荷として前段でオートチ
ューニング回路を備えた前述したエツチング用の反応器
を接続する。Incidentally, the above-mentioned etching reactor equipped with an auto-tuning circuit at the front stage is connected as a load to the second output terminal d.
捷だ、特に説明を省略した上ら1 it、o+ R11
及びR1□は入力抵抗、C13I CJ41 CJ5及
びC,、CJ、カップリング用コンテンサ、T7 及び
°r8(l−1、バイアス用トランスを示し、これら各
回路素子は設計上イ11意に設定される。コンデンサC
1□及びC18、可変抵抗器R13はバイアス調整回路
である。It's a good thing, especially if you omit the explanation, it, o+ R11
and R1□ are input resistances, C13I CJ41 CJ5 and C,, CJ, coupling capacitors, T7 and °r8 (l-1, bias transformers, and each of these circuit elements is set uniquely in the design. .Capacitor C
1□, C18, and variable resistor R13 are bias adjustment circuits.
一方、−に配電力検出回路5は帰還用増幅回路6に接続
し、出力電力の大きさに比例した例えば直流化信号SI
を当該回路6に供給するとともに、該回路6に於ては予
め設定された基準信号と当該直流化信号を比較し、その
偏差に基づいた直流制御信号S2を得る。On the other hand, the power distribution detection circuit 5 is connected to the feedback amplifier circuit 6 and outputs a direct current signal SI proportional to the magnitude of the output power.
is supplied to the circuit 6, and the circuit 6 compares the DC signal with a preset reference signal to obtain a DC control signal S2 based on the deviation.
そして、増幅回路6の出)J側は制御用FETΩ7のべ
〜スに接続し当該制御信号S2を供給する。The output (J) side of the amplifier circuit 6 is connected to the base of the control FET Ω7 to supply the control signal S2.
制御用FET O7は第2図に示すように入力端子(ベ
ース電圧)対出力電圧(アノ−1・電圧)特性が極めて
直線性に優れたものを用いている。As shown in FIG. 2, the control FET O7 has extremely excellent linearity in the input terminal (base voltage) versus output voltage (ano-1/voltage) characteristic.
PET O7のカソードは直接接地するとともに、アノ
−ドはカノプリングコンデンザC1□を介して前記した
発振回路1の増幅段、即ちトランジスタQ2のエミッタ
に接続される。発振回路1の増幅段のバイアスは当該ア
ノ−ドの電圧の大きさに比例して可変せしめられるよう
になし、具体的にばFETO7のゲート、カソード間電
圧を零から増加させた場合、前述した如く発振回路1の
出力電圧が零から比例的に増加し最大慎重で可変できる
ように設定する。なお、C18はコンデンサを示す。The cathode of the PET O7 is directly grounded, and the anode is connected to the amplification stage of the oscillation circuit 1, ie, the emitter of the transistor Q2, via the canopling capacitor C1□. The bias of the amplification stage of the oscillation circuit 1 is made to be variable in proportion to the magnitude of the voltage at the anode. Specifically, when the voltage between the gate and cathode of the FETO 7 is increased from zero, the bias as described above is changed. The output voltage of the oscillation circuit 1 is set so that it increases proportionally from zero and can be varied with maximum care. Note that C18 indicates a capacitor.
よって、以上の構成によりクローズトループによるノイ
ードバソク制御を行うことができ出力電力は常に一定に
制狽]することかできる。Therefore, with the above configuration, it is possible to perform closed-loop noise control, and the output power can be always kept constant.
他方、帰還用増幅回路6には出力可変信号発生回路7を
接続し、任意に或いはプログラム化された出力可変信号
S7.を当該増幅1回路6に供給し、FETO7のベー
ス、カソード間電圧を所望値に可変できるJ、うに構成
し、前述した如くこの種発振器の出力電力をオープンル
ープで安定、正確、且つ容易に可変せしめることができ
るようにする。On the other hand, a variable output signal generation circuit 7 is connected to the feedback amplifier circuit 6, and outputs an arbitrary or programmed variable output signal S7. is supplied to the amplifier 1 circuit 6, and the voltage between the base and cathode of the FETO 7 can be varied to a desired value.As mentioned above, the output power of this type of oscillator can be stably, accurately, and easily varied in an open loop. To be able to coerce people.
なお、符号す、c及びdは直流電源の入力端子である。Note that symbols S, C, and D are input terminals of the DC power supply.
(効果)
以上の説明から明らかなように、本発明に係る高周波発
振器は発振回路の増幅素子に接続U7、アノード電圧に
より当該増幅素子のバイアスを可変せしめるFETを備
え、このFETのベースに印加する各種制御用直流信号
により発振器の出力電力の大きさを制御するようにした
だめ容易、叶つ正確で大幅な出力電力制御が可能となる
とともに、安定な動作を期待でき、しかもMOS FE
Tを電力増幅段に使用することにより従、来プラズマエ
ツチングの分野における発振器の短寿命という障害を排
することができる等技術価値の高い高周波発振器として
提供することができる。(Effects) As is clear from the above description, the high frequency oscillator according to the present invention includes an FET connected to the amplification element of the oscillation circuit and an FET that changes the bias of the amplification element by an anode voltage. By controlling the magnitude of the output power of the oscillator using various control DC signals, it is possible to easily and accurately control the output power to a large extent, and stable operation can be expected.
By using T in the power amplification stage, it is possible to provide a high-frequency oscillator with high technical value, which can eliminate the problem of short life of oscillators in the field of plasma etching.
第1図は本発明に係る高周波発振器の電気回路図、第2
図は第1図中制御用F E ’I’の入力電圧対出力電
圧特性図である。
1は発振回路、3は電力増幅回路、Q+ + 02は高
周波用npn)77ジスタ、Q3.Q4.Q5.Q 6
は電υ用MO8型電界効果トランジスタ、Ω7は制イ1
j]1川電界効果トランジスタである。
特許出願人 東京電f化学株式会肚Fig. 1 is an electric circuit diagram of a high frequency oscillator according to the present invention, Fig. 2 is an electric circuit diagram of a high frequency oscillator according to the present invention;
The figure is an input voltage versus output voltage characteristic diagram of the control F E 'I' in FIG. 1. 1 is an oscillation circuit, 3 is a power amplifier circuit, Q+ + 02 is a high frequency npn) 77 transistor, Q3. Q4. Q5. Q 6
is MO8 type field effect transistor for electric υ, Ω7 is control 1
j] is a single field effect transistor. Patent applicant Tokyo Denf Chemical Co., Ltd.
Claims (1)
J、・いて、AiJ記発振回路の増幅素子に接続し、ア
ノード電圧により前記増幅素子のバイアスを1−iJ変
せしめる制御用電界効果トランジスタを備え、該電界効
果l・ランジスタのベースに印加する制御用直流信4づ
により発振器の出力電力の大きさを制側1することを特
徴とする高周波発振器0(2) nil記電力増幅回路
は高電力用電界効果トランジスタにより構成したことを
特徴とする特許請求の範囲第1項記載の高周波発振器○(+) A control field effect transistor is provided in a high frequency oscillator including an oscillation circuit and a power amplification circuit, is connected to an amplification element of the AiJ oscillation circuit, and changes the bias of the amplification element by 1-iJ by an anode voltage. A high frequency oscillator 0(2) nil power amplifier circuit is characterized in that the magnitude of the output power of the oscillator is controlled by a control DC signal 4 applied to the base of the field effect transistor. A high-frequency oscillator according to claim 1, characterized in that it is constituted by a power field effect transistor.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58028195A JPS59153303A (en) | 1983-02-22 | 1983-02-22 | High frequency oscillator |
US06/580,853 US4577165A (en) | 1983-02-22 | 1984-02-16 | High-frequency oscillator with power amplifier and automatic power control |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58028195A JPS59153303A (en) | 1983-02-22 | 1983-02-22 | High frequency oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59153303A true JPS59153303A (en) | 1984-09-01 |
Family
ID=12241889
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58028195A Pending JPS59153303A (en) | 1983-02-22 | 1983-02-22 | High frequency oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59153303A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6467897A (en) * | 1987-09-07 | 1989-03-14 | Fujitsu Ltd | High-frequency amplifier for semiconductor manufacturing device |
JPH06325897A (en) * | 1993-05-17 | 1994-11-25 | Adtec:Kk | Impedance matching device for high frequency plasma |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS50140842A (en) * | 1974-04-30 | 1975-11-12 |
-
1983
- 1983-02-22 JP JP58028195A patent/JPS59153303A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS50140842A (en) * | 1974-04-30 | 1975-11-12 |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6467897A (en) * | 1987-09-07 | 1989-03-14 | Fujitsu Ltd | High-frequency amplifier for semiconductor manufacturing device |
JPH06325897A (en) * | 1993-05-17 | 1994-11-25 | Adtec:Kk | Impedance matching device for high frequency plasma |
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