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JPS6053950B2 - television receiver - Google Patents
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JPS6053950B2 - television receiver - Google Patents

television receiver

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Publication number
JPS6053950B2
JPS6053950B2 JP6373177A JP6373177A JPS6053950B2 JP S6053950 B2 JPS6053950 B2 JP S6053950B2 JP 6373177 A JP6373177 A JP 6373177A JP 6373177 A JP6373177 A JP 6373177A JP S6053950 B2 JPS6053950 B2 JP S6053950B2
Authority
JP
Japan
Prior art keywords
signal
circuit
video signal
level
scanning speed
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
Application number
JP6373177A
Other languages
Japanese (ja)
Other versions
JPS53148325A (en
Inventor
進 吉田
良夫 石垣
欽也 真貝
尭央 土屋
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP6373177A priority Critical patent/JPS6053950B2/en
Publication of JPS53148325A publication Critical patent/JPS53148325A/en
Publication of JPS6053950B2 publication Critical patent/JPS6053950B2/en
Expired legal-status Critical Current

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  • Transforming Electric Information Into Light Information (AREA)
  • Details Of Television Scanning (AREA)

Description

【発明の詳細な説明】 テレビジョン受像機で画像を咲出させる場合、輝度の
高い部分では受像管のビーム電流が増加するためにビー
ムのスポットサイズが大きくなり鮮鋭度が低下してしま
う。
DETAILED DESCRIPTION OF THE INVENTION When displaying an image on a television receiver, the beam current of the picture tube increases in areas with high brightness, which increases the beam spot size and reduces sharpness.

特に第1図Aに示すように水平方向の輪部部分1や同図
Bに示すように線の部分2ては、本来の映像信号は第2
図Aに示すように黒レベルと白レベルの間で急峻に変化
するが、受像機の伝送係の周波数特性のため高域成分が
減衰するので、信号は同図Bに示すようになま つて水
平方向の鮮鋭度は一層低下してまう。 そこで、鮮鋭度
の低下を補償する方法として、第2図Bの映像信号50
から同図Cに示すような2次微分信号SBを得、これを
信号50に加えて同図Dに示すような立上り及び立下り
の急峻な映像信号Scを得、これを受像管に供給する方
法がある。 しカルながら、この方法では、信号のピー
クの部分でビーム電流がより増加するので、ビームのス
ポットサイズは一層大きくなり、そのため鮮鋭度はそれ
程改善されない。
In particular, in the horizontal ring part 1 as shown in Figure 1A and the line part 2 as shown in Figure 1B, the original video signal is
As shown in Figure A, there is a sharp change between the black level and the white level, but because the frequency characteristics of the receiver's transmission system attenuate the high-frequency components, the signal becomes distorted as shown in Figure B. Horizontal sharpness is further reduced. Therefore, as a method of compensating for the decrease in sharpness, the video signal 50 shown in FIG.
A second-order differential signal SB as shown in C in the same figure is obtained, and this is added to the signal 50 to obtain a video signal Sc with steep rises and falls as shown in D in the same figure, which is supplied to the picture tube. There is a way. However, in this method, the beam current increases more at the peak of the signal, so the beam spot size becomes larger, so the sharpness is not improved as much.

また、別な方法として、第3図Aの映像信号50をそ
のまま受像管に供給するとともに、この映像信号50を
微分して同図Bに示すような信号SAを得、これを例え
ば主偏向コイルとは別に設けた補助偏向コイルに供給し
て水平偏向磁界を同図Cに示すように補正し、これによ
りスクリーン上でのビームの走査速度を同図Dに示すよ
うに変調する方法がある。
As another method, the video signal 50 shown in FIG. 3A is supplied as is to the picture tube, and this video signal 50 is differentiated to obtain a signal SA shown in FIG. There is a method in which the horizontal deflection magnetic field is corrected as shown in Figure C by supplying it to a separately provided auxiliary deflection coil, thereby modulating the scanning speed of the beam on the screen as shown in Figure D.

この方法によれば、区間Taでは″ビームの走査速度が
早くなつてスクリーン上の対応する点の発光量は減少し
、区間’Lではビームの走査速度が遅くなつてスクリー
ン上の対応する点の発光量は増加するので、ビームのス
ポットサイズを考慮するとスクリーン上の水平方向の発
光i量は第3図Eに示すように変化し水平方向の鮮鋭度
が改善される。しかしながら、この方法によるときは、
図から明らかなように、スクリーン上の発光部分の幅が
映像信号S。
According to this method, in section Ta, the scanning speed of the beam becomes faster and the amount of light emitted at the corresponding point on the screen decreases, and in section 'L, the scanning speed of the beam becomes slower and the amount of light emitted at the corresponding point on the screen decreases. Since the amount of light emitted increases, taking into account the spot size of the beam, the amount of light emitted i in the horizontal direction on the screen changes as shown in Figure 3E, and the sharpness in the horizontal direction is improved.However, when using this method, teeth,
As is clear from the figure, the width of the light emitting part on the screen is the video signal S.

の時間幅に対応せず細くなつてしまうという欠点がある
。この点にかんがみ、映像信号の波形を補正することに
より、第3図に示すような方法の欠点をなくすようにし
た方法がある。これは、第4図に示すように、映像増幅
器11を通じて取り出されたものと映像信号SO(第5
図A)を微分信号発生回路として例えは微分回路12に
て微分して微分信号SA(同図B)を得、これを映像信
号の補正信号発生回路てある整流回路13にて両波整流
して信号SAのうち映像信号SOの立下り部に対応する
部分を極性反転した状態の信号SD(同図C)を得、合
成器14において、もとの映像信号SOに対してこの信
号SDを合成して、これより、もとの映像信号S。
It has the disadvantage that it does not correspond to the time width of , and becomes narrow. In view of this point, there is a method that eliminates the drawbacks of the method shown in FIG. 3 by correcting the waveform of the video signal. As shown in FIG. 4, the video signal SO (5th
For example, the differential signal SA (FIG. A) is differentiated by the differential signal generating circuit 12 to obtain the differential signal SA (FIG. B), which is then double-wave rectified by the rectifying circuit 13, which is a video signal correction signal generating circuit. The polarity of the portion of the signal SA corresponding to the falling edge of the video signal SO is inverted to obtain a signal SD (C in the same figure), and the synthesizer 14 combines this signal SD with respect to the original video signal SO. After combining, the original video signal S is obtained.

に比べて白信号の幅が広くされた映像出力信号Sp(同
図D)を得、この映像出力信号Spを受像管16の制御
電極である例えばカソード17に供給して電子ビームを
密度変調する。また、映像出力信号S2あるいはもとの
映像信号SOを走査速度変調回路として例えば微分回路
15にて微分して微分信号Sv(同図E)を得、これを
走査速度変調用信号として受像管16に例えば水平及び
垂直の偏向手段18とは別個に設けた走査速度変調用偏
向手段19に供給して、受像管16のスクリーン上にお
ける電子ビームの走査速度を変調する。なお、走査速度
変調用偏向手段19は、偏向手段18の手前側において
管16のネック部内に2枚の静電偏.向板を水平方向に
対向して配置して構成することができる。この方法によ
れば、スクリーン上での水平方向の発光分布は第5図F
の線5で示すようになり、発光部分の幅はもとの映像信
号SOの立上りの中.間点から立下りの中間点までの時
間に対応するものとなつて、第3図に示した方法のよう
に細くなつてしまうことはない。
A video output signal Sp (D in the same figure) in which the width of the white signal is made wider than that of the video output signal Sp is obtained, and this video output signal Sp is supplied to the control electrode of the picture tube 16, for example, the cathode 17, to density-modulate the electron beam. . Further, the video output signal S2 or the original video signal SO is differentiated by a differentiating circuit 15 using a scanning speed modulation circuit, for example, to obtain a differential signal Sv (E in the same figure), and this is used as a signal for scanning speed modulation to the picture tube 16. For example, the electron beam is supplied to a scanning speed modulating deflection means 19 provided separately from the horizontal and vertical deflection means 18 to modulate the scanning speed of the electron beam on the screen of the picture tube 16. The scanning speed modulation deflection means 19 includes two electrostatic deflection sheets in the neck of the tube 16 on the front side of the deflection means 18. The facing plates may be arranged to face each other in the horizontal direction. According to this method, the horizontal luminescence distribution on the screen is shown in Figure 5F.
As shown by line 5, the width of the light emitting part is within the rising edge of the original video signal SO. It corresponds to the time from the midpoint to the midpoint of the fall, and does not become narrow as in the method shown in FIG.

ところで、この場合、走査速度変調用信号Svのレベル
は映像出力信号S,従つて映像信号S。
By the way, in this case, the level of the scanning speed modulation signal Sv is the video output signal S, and therefore the video signal S.

の・レベルに応じて変化し、映像信号SOのレベルが小
さいときは走査速度変調用信号Svのレベルも小さくな
る。従つて、映像信号SOのレベルが小さいときは、走
査速度の変調があまりかからず、即ち走査速度が大きく
変化せず、このようなときにも、上述のように映像出力
信号Spとしてもとの映像信号SOに比べて同じ量だけ
白信号の幅が広げられたものが得られると、逆に発光部
分の幅が大きくなりすぎてしまうという不都合がある。
これを防止するには、映像信号S。のレベルにかかわら
ず、走査速度変調用信号のレベルが一定になるようにす
ればよい。そのためには、一つの方法として、上述の微
分ノ回路15から得られる微分信号Svをりミッタに供
給する方法が考えられる。
When the level of the video signal SO is low, the level of the scanning speed modulation signal Sv also becomes low. Therefore, when the level of the video signal SO is low, the scanning speed is not modulated much, that is, the scanning speed does not change significantly, and even in such a case, the original video output signal Sp is used as the video output signal Sp, as described above. If a white signal whose width is widened by the same amount as the video signal SO is obtained, there is the problem that the width of the light-emitting portion becomes too large.
To prevent this, the video signal S. The level of the scanning speed modulation signal may be kept constant regardless of the level of the scanning speed modulation signal. One possible method for this purpose is to supply the differential signal Sv obtained from the differential circuit 15 described above to the limiter.

しかしながら、この場合、りミッタの出力信号は矩形波
状のものになつてしまい、これを再びフィルタなどに供
給して波形整形する必要があるので、構成が複雑になつ
・てしまう。別の方法として、第6図に示すように、微
分回路15から得られる微分信号SvをAGC回路21
に供給して一定レベルにする方法が考えられる。
However, in this case, the output signal of the limiter becomes a rectangular waveform, and it is necessary to supply this signal again to a filter or the like for waveform shaping, resulting in a complicated configuration. As another method, as shown in FIG.
One possible method is to supply it to a certain level.

しかしながらこの場合、微分信号Svのピークの”レベ
ルを検出してそのレベルに応じて利得を制御しても、そ
の制御には遅れが生じるので、そのときどきでピークの
レベルを一定にすることは実際上不可能である。この発
明は、この点にかんがみ、映像信号S。
However, in this case, even if the peak level of the differential signal Sv is detected and the gain is controlled according to that level, there will be a delay in the control, so it is not practical to keep the peak level constant from time to time. In view of this point, the present invention provides a video signal S.

のレベルが小さいときは、これに加えて白信号の幅を広
げるための補正用信号のレベルが、映像信号SOのレベ
ルに比例した値よりもより小さくなるようにする。この
ため、この発明では、第7図に示すように、上述の整流
回路13から得られる信号SDを非直線回路22に供給
し、合成器14において、もとの映像信号SOに対して
この非直線回路22から得られる信号SEを合成して映
像出力信号Spを得るようにする。
When the level of is small, in addition to this, the level of the correction signal for widening the width of the white signal is made smaller than the value proportional to the level of the video signal SO. For this reason, in the present invention, as shown in FIG. The signal SE obtained from the linear circuit 22 is synthesized to obtain the video output signal Sp.

ここで、非直線回路22は、第8図に示すように、入力
電圧に対する出力電圧の比が入力電圧が多きくなるほど
大きくなるような回路にする。
Here, as shown in FIG. 8, the nonlinear circuit 22 is a circuit in which the ratio of the output voltage to the input voltage increases as the input voltage increases.

このような非直線回路22は、第9図に示すように、ダ
イオード23と抵抗24で簡単に構成することができる
。即ち、入力電圧が大きいほど、ダイオード23のイン
ピーダンスが小さくなるので、抵抗24とダイオード2
3で決まる分圧比は大きくなり、入力電圧に対する出力
電圧の比は大きくなる。このようにすれば、映像信号S
。のレベルが小さく、従つて走査速度変調用信号Svの
レベルも小さく走査速度の変調が強くかからないときは
、映像出力信号Spにおいて白信号の幅はそれ程広げら
れないから、発光部分の幅が大きくなりすぎてしまうよ
うなことはない。即ち、第14図及び第15図は、映像
信号SOのレベルが大きいときと小さいときを示すもの
で、微分回路12から得られる微分信号SAのレベル従
つて整流回路13から得られる信号SDのレベルは映像
信号S。
Such a non-linear circuit 22 can be easily constructed from a diode 23 and a resistor 24, as shown in FIG. That is, the larger the input voltage, the smaller the impedance of the diode 23, so the resistance 24 and the diode 2
The voltage division ratio determined by 3 becomes large, and the ratio of the output voltage to the input voltage becomes large. In this way, the video signal S
. When the level of the scanning speed modulation signal Sv is small, and therefore the scanning speed modulation signal Sv is also small and the scanning speed is not strongly modulated, the width of the white signal in the video output signal Sp is not widened that much, so the width of the light emitting part becomes large. There's no such thing as too much. That is, FIGS. 14 and 15 show when the level of the video signal SO is large and when it is small, and the level of the differential signal SA obtained from the differentiating circuit 12 and the level of the signal SD obtained from the rectifier circuit 13 are shown in FIGS. is the video signal S.

のレベルに対してほぼ比例したものとなる。しかしなが
ら、非直線回路22から得られる信号SEのレベルは、
映像信号SOのレベルに比例せず、映像信号SOのレベ
ルに対する信号SEのレベルの比は、第15図のように
映像信号SOのレベルが小さいときほど小さくなる。従
つて、合成器14から得られる映像出力信号Spの幅は
、映像信号SOのレベルが小さいときはあまり大きくな
らない。第15図で鎖線S″Pで示すものは、信号S。
が非直線回路22を通じることなく直接映像信号SOに
合成されたときの映像出力信号である。そして、走査速
度変調用信号Svのレベルが小さいときは、このように
映像出力信号Spにおいて白信号の幅はそれ程広げられ
ないから、発光部分の幅が大きくなりすぎることはない
。第9図のように、非直線回路22は、ダイオードと抵
抗で構成できるから、整流回路13と非直線回路22を
一つの回路で兼ねさせることもできる。
It is approximately proportional to the level of However, the level of the signal SE obtained from the nonlinear circuit 22 is
It is not proportional to the level of the video signal SO, and the ratio of the level of the signal SE to the level of the video signal SO becomes smaller as the level of the video signal SO becomes smaller, as shown in FIG. Therefore, the width of the video output signal Sp obtained from the synthesizer 14 does not become very large when the level of the video signal SO is low. What is indicated by a chain line S''P in FIG. 15 is a signal S.
This is the video output signal when the signal is directly combined with the video signal SO without passing through the non-linear circuit 22. When the level of the scanning speed modulation signal Sv is low, the width of the white signal in the video output signal Sp is not widened as much, so the width of the light emitting portion does not become too large. As shown in FIG. 9, since the non-linear circuit 22 can be composed of a diode and a resistor, one circuit can serve as both the rectifier circuit 13 and the non-linear circuit 22.

第10図は、この場合の例で、25は両者を兼用した同
極性化回路で、極性反転回路26と、ダイオード27及
び28と、抵抗29で構成されている。
FIG. 10 shows an example of this case. Reference numeral 25 denotes a polarization circuit that serves both functions, and is composed of a polarity inversion circuit 26, diodes 27 and 28, and a resistor 29.

第11図の例のように、さらに、微分回路15から得ら
れる微分信号Svを非直線回路31に供給し、これより
得られる信号Svcを走査速度変調用信号として走査速
度変調用偏向手段19に供給するようにしてもよい。
As in the example of FIG. 11, the differential signal Sv obtained from the differentiating circuit 15 is further supplied to the non-linear circuit 31, and the signal Svc obtained thereby is sent to the scanning speed modulation deflection means 19 as a scanning speed modulation signal. It may also be supplied.

この場合の非直線回路31は、非直線回路22とは逆に
、第12図に示すように、入力電圧に対する出力電圧の
比が入力電圧が小さくなるほど大きくなるような回路に
する。
In this case, the nonlinear circuit 31 is a circuit in which the ratio of the output voltage to the input voltage increases as the input voltage decreases, as shown in FIG. 12, contrary to the nonlinear circuit 22.

このようにすれば、第14図及び第15図に示すように
、映像信号SOのレベルの違いほど走査速度変調用信号
SvOのレベルは違わず、即ち映像信号SOのレベルが
小さいときでも走査速度変調用信号SvOのレベルはそ
れ程小さくならず、走査速度の変調はそれ程弱められな
いから、非直線回路22による白信号の幅の拡大の度合
の違いとの共働により、映像信号S。
In this way, as shown in FIGS. 14 and 15, the level of the scanning speed modulation signal SvO does not differ as much as the level of the video signal SO, that is, even when the level of the video signal SO is small, the scanning speed Since the level of the modulation signal SvO is not so reduced and the modulation of the scanning speed is not weakened so much, the video signal S.

のレベルが大きいときでも小さいときでも同一の発光分
布を得ることができる。なお、走査速度変調用偏向手段
19は、第13図に示すように受像管16の電子銃の例
えば集束電極を特殊に形成することにより構成すること
もできる。
The same luminescence distribution can be obtained whether the level of is large or small. The scanning speed modulation deflection means 19 can also be constructed by specially forming, for example, a focusing electrode of the electron gun of the picture tube 16, as shown in FIG.

即ち、第13図は管16のネック部内の電子銃を示すも
ので、カソード40、制御電極41、加速電極42、第
1陽極43、集束電極44及び第2陽極45が順次同じ
軸心上に配列されている。
That is, FIG. 13 shows the electron gun inside the neck of the tube 16, in which a cathode 40, a control electrode 41, an accelerating electrode 42, a first anode 43, a focusing electrode 44 and a second anode 45 are sequentially arranged on the same axis. Arranged.

そして、集束電極44を、1つの円筒体をその中間部に
おいて水平面と直交するも管軸と斜めに交わる平面によ
つて切断したような形状を有するように分割された2個
の電極部44A及び44Bにて構成し、電極部44A及
び44Bにはそれぞれ零Vないし数KVの集束電圧を供
給するとともに、これに重畳して両電極部44A及び4
4B間に上述の走査速度変調用信号SvないしSvcを
供給する。従つて、集束電極44の位置で信号Svない
しSvOによつて水平方向の電界が発生し、これにより
ビーム46が水平方向に偏向されてスクリーン上におい
てビーム46の走査速度が変調さLれる。また、水平偏
向コイルを走査速度変調用偏向手段に兼用させ、水平偏
向信号に対して上述の走査速度変調用信号を合成したも
のをこれに供給してもよい。
The focusing electrode 44 is divided into two electrode parts 44A and 44A, each having a shape similar to that of a single cylindrical body cut by a plane that is orthogonal to the horizontal plane at the middle part and diagonal to the tube axis. 44B, and a focused voltage of zero V to several KV is supplied to each of the electrode parts 44A and 44B, and superimposed on this, both electrode parts 44A and 4
The above-mentioned scanning speed modulation signals Sv to Svc are supplied between 4B and 4B. Therefore, a horizontal electric field is generated by the signals Sv to SvO at the location of the focusing electrode 44, which deflects the beam 46 horizontally and modulates the scanning speed of the beam 46 on the screen. Alternatively, the horizontal deflection coil may also be used as the deflection means for scanning speed modulation, and a combination of the above-mentioned scanning speed modulation signal and the horizontal deflection signal may be supplied thereto.

上述のように、この発明によれば、映像信号のレベルの
いかんにかかわらず、発光部分の幅を適切に規制して鮮
鋭度を改善することができる。
As described above, according to the present invention, the width of the light emitting portion can be appropriately regulated to improve sharpness regardless of the level of the video signal.

なお、この発明はカラーテレビジョン受像機にも適用で
きるもので、この場合には輝度信号を上)述の映像信号
として扱えばよい。
Note that the present invention can also be applied to a color television receiver, and in this case, the luminance signal may be treated as the above-mentioned video signal.

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

第1図〜第3図はこの発明の説明のための図、第4図は
この発明の説明のための一方法を示す系統図、第5図は
その説明のための波形図、第6図はこの発明の説明のた
めの他の方法を示す系統図、第7図はこの発明の一例の
系統図、第8図はその非直線回路の特性を示す図、第9
図は非直線回路の一例の接続図、第10図はこの発明の
具体例の接続図、第11図はこの発明の他の例の系統図
、第12図はその別の非直線回路の特性を示す図、第1
3図は走査速度変調用偏向手段の一例の断面図、第14
図及び第15図はこの発明の説明のための波形図である
。 11は映像増幅器、12及び15は微分回路、13は整
流回路、16は受像管、22及び31は非直線回路であ
る。
Figures 1 to 3 are diagrams for explaining the present invention, Figure 4 is a system diagram showing one method for explaining the invention, Figure 5 is a waveform diagram for explaining the invention, and Figure 6 is a diagram for explaining the invention. is a system diagram showing another method for explaining this invention, FIG. 7 is a system diagram of an example of this invention, FIG. 8 is a diagram showing the characteristics of the nonlinear circuit, and FIG.
The figure is a connection diagram of an example of a non-linear circuit, Figure 10 is a connection diagram of a specific example of this invention, Figure 11 is a system diagram of another example of this invention, and Figure 12 is a characteristic of another non-linear circuit. Figure 1 showing
Figure 3 is a cross-sectional view of an example of a deflection means for scanning speed modulation;
15 and 15 are waveform diagrams for explaining the present invention. 11 is a video amplifier, 12 and 15 are differentiating circuits, 13 is a rectifier circuit, 16 is a picture tube, and 22 and 31 are nonlinear circuits.

Claims (1)

【特許請求の範囲】[Claims] 1 もとの映像信号からこの微分成分を取出す微分信号
発生回路と、この出力の負極性成分を反転してこの正極
性成分と加算して、映像信号の立上り部及び立下り部で
同極性の補正信号を得る補正信号発生回路と、この出力
を非直線性回路を介してもとの映像信号に加算して白信
号の幅を拡大した信号を得る信号加算器と、該加算器の
出力を受像管の制御電極及び走査速度変調回路の入力端
子に供給する信号供給路と、上記走査速度変調回路の出
力で駆動され受像管のスクリーン上における電子ビーム
の走査速度を変調する走査速度変調用偏向手段の夫々を
設け、上記非直線性回路は入力電圧に対する出力電圧の
比が入力電圧が大きくなるほど大に選定したことを特徴
とするテレビジョン受像機。
1 A differential signal generation circuit extracts this differential component from the original video signal, inverts the negative polarity component of this output and adds it to this positive polarity component, and generates the same polarity at the rising and falling parts of the video signal. a correction signal generation circuit for obtaining a correction signal; a signal adder for adding this output to the original video signal via a non-linearity circuit to obtain a signal with an expanded white signal; A signal supply path for supplying the control electrode of the picture tube and the input terminal of the scanning velocity modulation circuit, and a scanning velocity modulation deflection that is driven by the output of the scanning velocity modulation circuit and modulates the scanning velocity of the electron beam on the screen of the picture tube. 2. A television receiver, characterized in that the non-linearity circuit is selected such that the ratio of the output voltage to the input voltage increases as the input voltage increases.
JP6373177A 1977-05-31 1977-05-31 television receiver Expired JPS6053950B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6373177A JPS6053950B2 (en) 1977-05-31 1977-05-31 television receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6373177A JPS6053950B2 (en) 1977-05-31 1977-05-31 television receiver

Publications (2)

Publication Number Publication Date
JPS53148325A JPS53148325A (en) 1978-12-23
JPS6053950B2 true JPS6053950B2 (en) 1985-11-28

Family

ID=13237832

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6373177A Expired JPS6053950B2 (en) 1977-05-31 1977-05-31 television receiver

Country Status (1)

Country Link
JP (1) JPS6053950B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6373432U (en) * 1986-10-30 1988-05-16

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6373432U (en) * 1986-10-30 1988-05-16

Also Published As

Publication number Publication date
JPS53148325A (en) 1978-12-23

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