JPS5927507B2 - Contour enhancement circuit - Google Patents

Contour enhancement circuit

Info

Publication number
JPS5927507B2
JPS5927507B2 JP275677A JP275677A JPS5927507B2 JP S5927507 B2 JPS5927507 B2 JP S5927507B2 JP 275677 A JP275677 A JP 275677A JP 275677 A JP275677 A JP 275677A JP S5927507 B2 JPS5927507 B2 JP S5927507B2
Authority
JP
Japan
Prior art keywords
signal
crt
waveform
scanning speed
gamma
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
JP275677A
Other languages
Japanese (ja)
Other versions
JPS5387621A (en
Inventor
実 竹田
克彦 山本
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP275677A priority Critical patent/JPS5927507B2/en
Publication of JPS5387621A publication Critical patent/JPS5387621A/en
Publication of JPS5927507B2 publication Critical patent/JPS5927507B2/en
Expired legal-status Critical Current

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  • Details Of Television Scanning (AREA)
  • Video Image Reproduction Devices For Color Tv Systems (AREA)

Description

【発明の詳細な説明】 本発明はビデオ信号の輪郭部分に相当する信号で、CR
Tのような表示素子の走査速度を変調して、表示画面上
での輪郭部を強調することにより、画質の改善をはかれ
るような輪郭強調回路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides a signal corresponding to the contour part of a video signal,
The present invention relates to an edge enhancement circuit that improves image quality by modulating the scanning speed of a display element such as T and emphasizing an edge on a display screen.

従来、テレビ受像機などで表示画面の輪郭部分を強調し
て画質の改善をするために、ビデオ信号の高周波部分を
強調する方法や、走査速度を信号に応じて変調して輪郭
部分を強調して画質の改善する方法などがある。
Conventionally, in order to improve the image quality by emphasizing the outlines of the display screen on television receivers, etc., methods have been used to emphasize the high frequency parts of the video signal, or to emphasize the outlines by modulating the scanning speed according to the signal. There are ways to improve image quality.

このうち走査速度変調方式について、内容を説明する。Among these, the details of the scanning speed modulation method will be explained.

第1図で受像機のビデオ信号の波形をaとすると、この
微分波形はbとなり、この微分波形をCRTの偏向電流
に重畳すると、cのような波形となる。CRTのグリッ
ドなどにaの信号を加え、電子ビームの偏向をcの信号
で行うと、通常の偏向速度に比してbの微分波形のbl
の期間では偏向速度が速くなり、b2の期間では偏向速
度が遅くなる。したがつて、CRT面上での輝度分布は
blに相当する部分では、走査速度変調のない場合より
も暗くなり、b2に相当する部分では明るくなり、理想
的にはdのような輝度分布となるはずである。しかし、
実際のCRTでは電子ビームのビームスポット径はビー
ム量が増加すればすなわち高輝度部分(明るい場面)で
は大きくなり、輪郭部分の特性が劣化し、実際のCRT
画面上での輝度分布はeのようになる。このため、走査
速度変調を行つても高輝度部分の輪郭強調効果は十分に
達成されないという欠点がある。この第1図のような動
作を行わせる実際の回路構成を第2図に示す。第2図で
0はビデオ信号入力端であり、ビデオ増幅器1で増幅し
、ビデオ出力段2を経て、CRTTに加えており、1の
出力信号を微分回路5で微分して、第1図のbの波形を
つくり増幅器6で増幅する。偏向および高圧回路につい
ては、同期分離回路3で、同期信号を分離し、偏向・高
圧回路4で、偏向コイルヘ加える信号および高圧をつく
つて、偏向コイル9、CRT7へ加えている。6で得た
走査速度変調信号は走査速度変調用コイル8に加えて走
査速度変調を行う。
In FIG. 1, if the waveform of the video signal from the receiver is a, the differential waveform is b, and when this differential waveform is superimposed on the deflection current of the CRT, it becomes a waveform like c. When a signal a is applied to a CRT grid, etc., and the electron beam is deflected using a signal c, the differential waveform bl of b becomes smaller than the normal deflection speed.
In the period b2, the deflection speed becomes faster, and in the period b2, the deflection speed becomes slower. Therefore, the brightness distribution on the CRT screen will be darker in the part corresponding to bl than in the case without scanning speed modulation, and brighter in the part corresponding to b2, and ideally the brightness distribution will be like d. It should be. but,
In an actual CRT, the beam spot diameter of the electron beam increases as the beam amount increases, that is, in high-brightness areas (bright scenes), and the characteristics of the outline area deteriorate, causing the beam spot diameter of the electron beam to increase.
The brightness distribution on the screen is as shown in e. For this reason, there is a drawback that even if scanning speed modulation is performed, the effect of contour enhancement in high-brightness portions cannot be sufficiently achieved. FIG. 2 shows an actual circuit configuration for performing the operation shown in FIG. 1. In Fig. 2, 0 is the video signal input terminal, which is amplified by the video amplifier 1, passed through the video output stage 2, and applied to the CRTT, and the output signal of 1 is differentiated by the differentiating circuit 5. A waveform b is created and amplified by an amplifier 6. Regarding the deflection and high voltage circuits, a synchronization separation circuit 3 separates the synchronization signal, and a deflection/high voltage circuit 4 generates a signal and high voltage to be applied to the deflection coil and applies them to the deflection coil 9 and CRT 7. The scanning speed modulation signal obtained in step 6 is added to the scanning speed modulation coil 8 to perform scanning speed modulation.

前述したように、CRTは高輝度部分でビームスポット
径が大きくなり、特性が劣化する。この様子を第3図で
示す。第3図は、カラーCRTの電子ビーム電流を10
0pA、500μA、1000μA、1500μAとし
たときに、空間周波数レスポンスがどのように変化して
行くかを示したものであり、大電流域(高輝度部分)で
特性が劣化しており、第1図aのようなビデオ信号に、
走査速度変調をしてCRTに表示しても、eのような画
面になつて高輝度部分での輪郭部の強調が不十分となる
ことがよくわかる。本発明は上記従来技術に鑑み、CR
Tの高輝度部分での特性の劣化をも補償して、高輝度部
分でも十分な輪郭強調効果を得られるようにするもので
ある。
As mentioned above, in a CRT, the beam spot diameter becomes large in the high-brightness portion, and the characteristics deteriorate. This situation is shown in FIG. Figure 3 shows the color CRT electron beam current of 10
This shows how the spatial frequency response changes when the voltage is 0 pA, 500 μA, 1000 μA, and 1500 μA. The characteristics deteriorate in the large current area (high brightness area), and Figure 1 For a video signal like a,
It can be clearly seen that even if the image is displayed on a CRT with scanning speed modulation, the screen will look like e, and the contours in the high-brightness areas will not be sufficiently emphasized. In view of the above-mentioned prior art, the present invention provides CR
This also compensates for the deterioration of the characteristics in the high-brightness portion of T, so that a sufficient edge enhancement effect can be obtained even in the high-brightness portion.

以下本発明の詳細について説明する。The details of the present invention will be explained below.

第4図は本発明の一実施例を示すものである。第4図に
おいてaは入力ビデオ信号であり、これをガソマ補正し
て、ビデオ信号の波形を整形してbのような波形をつく
り、即ち1より大なる補正値でガンマ補正された波形を
つくりこれを微分してcのような波形とする。このcの
波形を走査速度変調信号として、偏向電流に重畳すると
その波形はdのようになる。CRTのグリツドなどにa
の信号を加え、cの信号で走査速度変調するとCRT画
面上での輝度分布は理想的(即ちCRT自身の特性が理
想的)な場合にはeのようになるが、実際のCRTは、
前述のように高輝度部でのビームスポツト径は、低輝度
のときよりも大きくなるため、実際の場面ではfのよう
な輝度分布となる。この波形かられかるように、輪郭強
調効果は理想的であり、従来例の第1図eのように高輝
度部での特性の劣化はない。このように入力ビデオ信号
をガンマ補正し、これを微分して走査速度変調信号とす
ることによつて、輪郭強調効果を改善することができる
。次にこのガンマ補正を行う簡易な手段およびこの信号
を用いて輪郭強調する手段を具体的に説明する。第5図
にその一実施例を示す。
FIG. 4 shows an embodiment of the present invention. In Fig. 4, a is the input video signal, which is subjected to gasoma correction and the waveform of the video signal is shaped to create a waveform like b, that is, a waveform that has been gamma-corrected with a correction value greater than 1. This is differentiated to give a waveform like c. When this waveform c is superimposed on the deflection current as a scanning speed modulation signal, the waveform becomes as shown in d. a for CRT grids, etc.
When the signal of is added and the scanning speed is modulated by the signal of c, the brightness distribution on the CRT screen becomes e if it is ideal (that is, the characteristics of the CRT itself are ideal), but in an actual CRT,
As mentioned above, the beam spot diameter in a high brightness area is larger than that in a low brightness area, so in an actual scene, the brightness distribution will be as shown in f. As can be seen from this waveform, the edge enhancement effect is ideal, and there is no deterioration of characteristics in high brightness areas as in the conventional example shown in FIG. 1e. By gamma-correcting the input video signal and differentiating it to obtain a scanning speed modulation signal in this manner, the edge enhancement effect can be improved. Next, a simple means for performing this gamma correction and a means for enhancing contours using this signal will be specifically explained. FIG. 5 shows an example of this.

なお第5図で第2図と同じものは同一の番号を付してあ
る。ビデオ信号出力をCRT7のグリツドに加えると、
CRT7は第6図に示すように、一般にガンマ特性(γ
+2.2)があり、入力のビデオ信号aに対してビーム
電流はbのような波形となるため、このビーム電流の波
形を何らかの手段で検出すれば、第4図の入力信号aの
ガンマ補正波形である波形bを得ることができる。この
ため、CRT7のカソードに抵抗10を付加し、この低
抗に流れるビーム電流量を電圧として取出すようにする
。この抵抗10の両端に表われる信号は第4図のbのよ
うなガンマ補正された信号となる。この信号を第5図の
5で微分することにより、第4図のcのような波形を得
ることができる。この信号を第5図の6で増幅して走査
速度変調コイル8で変調することにより、CRTの画面
上では高輝度部分でのCRTの特性劣化を補償した第4
図fのような理想的に輪郭強調された画像を表示するこ
とができる。次に他の実施例を第7図に示す。
Note that the same parts in FIG. 5 as in FIG. 2 are given the same numbers. When the video signal output is added to the CRT7 grid,
As shown in Figure 6, CRT7 generally has gamma characteristics (γ
+2.2), and the beam current has a waveform like b for the input video signal a, so if this beam current waveform is detected by some means, gamma correction of the input signal a shown in Figure 4 can be performed. A waveform b can be obtained. For this reason, a resistor 10 is added to the cathode of the CRT 7, and the amount of beam current flowing through this resistor is extracted as a voltage. The signal appearing at both ends of this resistor 10 becomes a gamma-corrected signal as shown in FIG. 4b. By differentiating this signal by 5 in FIG. 5, a waveform as shown in c in FIG. 4 can be obtained. By amplifying this signal at 6 in FIG. 5 and modulating it at the scanning speed modulation coil 8, a fourth
An ideally edge-enhanced image as shown in FIG. f can be displayed. Next, another embodiment is shown in FIG.

第7図でも、第2図と共通のものには同一の番号を附し
てある。ビデオ信号は、1で増幅されてビデオ出力トラ
ンジスタ11に加えられ、その出力は負荷抵抗12、の
両端に表われる。この出力電圧でCRT7を1駆動する
のであるが、トランジスタ11からCRTのカソート−
接続する間に信号取出用のトランス13を附加すること
により、CRT7のビーム電流量を検出することができ
る。このトランス13で検出した信号は、入力ビデオ信
号をCRTに加えたときのCRTのビーム電流量を示す
から、第4図のbのような波形となる。この信号を前述
の実施例のようにして処理し、走査速度変調用コイル8
に加えると、CRTの画面上で得られる輝度分布は第4
図fのようになり、CRTの高輝度部分での特性の劣化
を補償した性能のものとなる。なおこのトランス13は
ビデオ信号の高周波部分を強調するピーキングコイルと
しても利用することができることは白明である。このよ
うに走査速度変調して、画面上の輪郭部分を強調して画
質の改善をはかる場合に、CRTの特性が高輝度部で劣
化するのを補償するために入力ビデオ信号をガンマ補正
し、これを微分して、この微分信号を走査速度変調信号
として利用する。
In FIG. 7, the same numbers are given to the same parts as in FIG. 2. The video signal is amplified by 1 and applied to a video output transistor 11, the output of which appears across a load resistor 12. This output voltage drives the CRT 7 by 1, and the cathode voltage of the CRT is output from the transistor 11.
By adding a transformer 13 for signal extraction during connection, the amount of beam current of the CRT 7 can be detected. The signal detected by this transformer 13 indicates the amount of beam current of the CRT when an input video signal is applied to the CRT, and therefore has a waveform as shown in b in FIG. This signal is processed as in the previous embodiment, and the scanning speed modulation coil 8
In addition, the brightness distribution obtained on the CRT screen is the fourth
As shown in Figure f, the performance compensates for the deterioration of the characteristics in the high brightness portion of the CRT. It is obvious that this transformer 13 can also be used as a peaking coil for emphasizing the high frequency portion of the video signal. When the scanning speed is modulated in this way to emphasize outlines on the screen to improve image quality, the input video signal is gamma-corrected to compensate for the deterioration of CRT characteristics in high-brightness areas. This is differentiated and this differentiated signal is used as a scanning speed modulation signal.

すなわちビデオ信号をガンマ補正するためにCRTのガ
ンマ特性を有効に利用して、CRTにビデオ信号を加え
、そのCRTに流れるビーム電流、即ちガンマ補正され
た信号を取出して利用する。この信号を微分して、この
微分信号を走査速度変調信号とする。なお、上記実施例
はテレビジヨン受像機以外にも各種の画像表示、文字表
示、図形表示などを行うCRT表示装置などの各種の表
示装置に用いることもできる。
That is, in order to gamma-correct the video signal, the gamma characteristics of the CRT are effectively used, the video signal is applied to the CRT, and the beam current flowing through the CRT, that is, the gamma-corrected signal, is extracted and used. This signal is differentiated and the differentiated signal is used as a scanning speed modulation signal. In addition to television receivers, the above embodiments can also be used in various display devices such as CRT display devices that display various images, characters, graphics, and the like.

以上のように本発明はビデオ信号のガンマ補正をされた
走査速度変調に用いるための信号を得るために複雑かつ
高価な回路を付加することなく、非常に簡易な方法でC
RTの高輝度部での特性の劣化をも補償した輪郭強調効
果をあげることができる。
As described above, the present invention provides a very simple method for obtaining a signal for use in gamma-corrected scanning velocity modulation of a video signal without adding any complicated and expensive circuitry.
It is possible to achieve an edge enhancement effect that compensates for the deterioration of characteristics in the high brightness portion of RT.

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

第1図は従来の走査速度変調方式による輪郭強調効果を
説明する波形図、第2図は第1図の走査速度変調方式を
具体化する回路構成図、第3図はCRTのビームスポツ
ト径の変化による空間周波数レスポンスを示す図、第4
図はCRTの特性をも考慮した走査速度変調を行なうこ
めの波形図およびその効果を示す波形図、第5図は本発
明の一実施例の回路構成図、第6図はCRTのガンマ特
性を示す図、第7図は本発明の他の実施例を示す回路構
成図である。 1・・・・・・ビデオ増幅器、2・・・・・・ビデオ出
力段、3・・・・・・同期分離回路、4・・・・・・偏
向・高圧回路、5・・・・・・微分回路、6・・・・・
・増幅器、7・・・・・・CRTl8・・・・・・走査
速度変調用コイル、9・・・・・・偏向コイル、10・
・・・・・抵抗、11・・・・・・トランジスタ、12
・・・・・・抵抗、13・・・・・・トランス。
Fig. 1 is a waveform diagram explaining the edge enhancement effect of the conventional scanning speed modulation method, Fig. 2 is a circuit diagram embodying the scanning speed modulation method of Fig. 1, and Fig. 3 shows the beam spot diameter of a CRT. Diagram showing spatial frequency response due to change, 4th
The figure shows a waveform diagram for performing scanning speed modulation that also takes into account the characteristics of a CRT, and a waveform diagram showing its effect. Figure 5 is a circuit configuration diagram of an embodiment of the present invention. Figure 6 shows the gamma characteristics of a CRT. FIG. 7 is a circuit configuration diagram showing another embodiment of the present invention. 1...Video amplifier, 2...Video output stage, 3...Synchronization separation circuit, 4...Deflection/high voltage circuit, 5...・Differential circuit, 6...
・Amplifier, 7...CRTl8...Scanning speed modulation coil, 9...Deflection coil, 10...
...Resistor, 11...Transistor, 12
...Resistor, 13...Transformer.

Claims (1)

【特許請求の範囲】[Claims] 1 入力画像信号を補正値が1より大なる値でガンマ補
正するためのガンマ補正回路と、前記ガンマ補正された
画像信号を微分するための微分回路と、前記微分された
信号で陰極線管の走査速度を変調する走査速度変調回路
とを備えたことを特徴とする輪郭強調回路。
1: a gamma correction circuit for gamma-correcting an input image signal with a correction value greater than 1; a differentiation circuit for differentiating the gamma-corrected image signal; and scanning of a cathode ray tube using the differentiated signal. 1. A contour enhancement circuit comprising: a scanning speed modulation circuit that modulates speed.
JP275677A 1977-01-12 1977-01-12 Contour enhancement circuit Expired JPS5927507B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP275677A JPS5927507B2 (en) 1977-01-12 1977-01-12 Contour enhancement circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP275677A JPS5927507B2 (en) 1977-01-12 1977-01-12 Contour enhancement circuit

Publications (2)

Publication Number Publication Date
JPS5387621A JPS5387621A (en) 1978-08-02
JPS5927507B2 true JPS5927507B2 (en) 1984-07-06

Family

ID=11538179

Family Applications (1)

Application Number Title Priority Date Filing Date
JP275677A Expired JPS5927507B2 (en) 1977-01-12 1977-01-12 Contour enhancement circuit

Country Status (1)

Country Link
JP (1) JPS5927507B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6074772A (en) * 1983-09-29 1985-04-27 Matsushita Electric Ind Co Ltd Quantizing method of multi-value picture information

Also Published As

Publication number Publication date
JPS5387621A (en) 1978-08-02

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