JPS58108889A - Frequency separating type single bulb color camera - Google Patents

Frequency separating type single bulb color camera

Info

Publication number
JPS58108889A
JPS58108889A JP56208585A JP20858581A JPS58108889A JP S58108889 A JPS58108889 A JP S58108889A JP 56208585 A JP56208585 A JP 56208585A JP 20858581 A JP20858581 A JP 20858581A JP S58108889 A JPS58108889 A JP S58108889A
Authority
JP
Japan
Prior art keywords
magnetic field
focusing
signal output
color camera
image pickup
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
JP56208585A
Other languages
Japanese (ja)
Inventor
Tokuzo Kadota
門田 徳三
Takashi Tsukada
敬 塚田
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 JP56208585A priority Critical patent/JPS58108889A/en
Publication of JPS58108889A publication Critical patent/JPS58108889A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J31/00Cathode ray tubes; Electron beam tubes
    • H01J31/08Cathode ray tubes; Electron beam tubes having a screen on or from which an image or pattern is formed, picked up, converted, or stored
    • H01J31/26Image pick-up tubes having an input of visible light and electric output
    • H01J31/46Tubes in which electrical output represents both intensity and colour of image

Landscapes

  • Color Television Image Signal Generators (AREA)

Abstract

PURPOSE:To obtain a frequency separating single-bulb color camera which has improved balance between an R signal and a B signal output after color separation, by combining an image pickup tube with a focusing coil which generates a focusing magnetic field directed from an electron gun side to a target side. CONSTITUTION:The focusing magnetic field 6' is applied at right angle to a scanning surface, so an electron beam running in the orthogonal field of this electric field is applied with vertical force. Namely, the electron beam is applied with force to right when the magnetic field faces as shown by 6 in a figure, or to left when the magnetic field faces as shown by 6'. Consequently, the beam lands at a target in a right declining ellipse ink the former case or in a left decliing ellipse in the latter case. Therefore, the R signal output and B signal output are held at nearly the same level. Thus, an error in color separation is reduced and the color S/N ratio is improved.

Description

【発明の詳細な説明】 本発明は交差型ストライプフィルターを内臓した周波数
分離型単管カラーカメラに関するものであり、特に色分
離後のR信号出力とB信号出力のバランス向上を計った
周波数分離単管カラーカメラを提供することを目的とす
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a frequency-separated single-tube color camera incorporating a cross-type stripe filter, and in particular to a frequency-separated single-tube color camera that improves the balance between R signal output and B signal output after color separation. The purpose is to provide a tube color camera.

周波数分離型単管カラーカメラにおいて、分光感度特性
が等しい場合、同じ明るさの赤色光および青色光を与え
た場合にR出力信号およびB出力信号のレベルが等しく
かつ高いことが色分離およびカラーS/Nの点で望まし
い。ところがビーム形状は真円状からセルフシャープニ
ング効果およびビームベンディング効果により歪んだ形
に変形する。従って交差したストライプフィルターを使
う周波数分離型単管カラーカメラにおいては、R出力信
号とB出力信号のレベルが異なるという欠点があった。
In a frequency-separated single-tube color camera, if the spectral sensitivity characteristics are equal, the levels of the R output signal and B output signal are equal and high when red light and blue light of the same brightness are applied. /N is desirable. However, the beam shape changes from a perfect circle to a distorted shape due to self-sharpening effects and beam bending effects. Therefore, a frequency-separated single-tube color camera using crossed stripe filters has a drawback in that the levels of the R output signal and the B output signal are different.

そこで、本発明は上記欠点を除去し、R信号出力とB信
号出力のバランスを向上させた周波数分離型単管カラー
カメラを提供しようとするものであり、電磁集束−電磁
偏向型撮像管(以後MM型撮像管と呼ぶ)と電磁集束−
静電偏向型撮像管(以後MS型撮像管と呼ぶ)の両方に
適用できるものである。本発明のMM型撮像管もしくは
MS型撮像管と電子銃側からターゲット側へ向かう集束
磁界を発生する集束コイルとを組み合わせたところに特
徴がある。かかる構成にすることにより交差型ストライ
プフィルターを内蔵した周波数分離型単管カラーカメラ
のR信号出力とB信号出力のバランス向上を計ることが
できる。以下MS型撮像管における実施例で本発明の詳
細な説明する。
Therefore, the present invention aims to eliminate the above-mentioned drawbacks and provide a frequency-separated single-tube color camera that improves the balance between R signal output and B signal output. MM type image pickup tube) and electromagnetic focusing
It can be applied to both electrostatic deflection type image pickup tubes (hereinafter referred to as MS type image pickup tubes). The feature is that the MM type image pickup tube or MS type image pickup tube of the present invention is combined with a focusing coil that generates a focused magnetic field directed from the electron gun side to the target side. By adopting such a configuration, it is possible to improve the balance between the R signal output and the B signal output of a frequency-separated single-tube color camera with a built-in cross-type stripe filter. The present invention will be explained in detail below using an example of an MS type image pickup tube.

MS型撮像管のビーム形状を調べた結果、次の様な事実
が判明した。即ちMS型撮像管において集束磁界の向き
をターゲット側から電子銃側にした時と、その逆の電子
銃側からターゲット側にした時とでビーム形状が異なる
ことが判明した。もちろん集束磁界を逆にした場合、偏
向方向が逆になるため偏向電界も逆にしている。MS型
撮像管と集束コイルの概略図を第1図に、集束磁界の向
きを変えた時のビーム形状の測定結果を第2図に示す。
As a result of investigating the beam shape of the MS type image pickup tube, the following facts were found. That is, it has been found that the beam shape is different when the direction of the focused magnetic field is changed from the target side to the electron gun side in the MS type image pickup tube, and when the direction is changed from the electron gun side to the target side. Of course, when the focusing magnetic field is reversed, the deflection direction is reversed, so the deflection electric field is also reversed. Fig. 1 shows a schematic diagram of the MS type image pickup tube and the focusing coil, and Fig. 2 shows the measurement results of the beam shape when changing the direction of the focusing magnetic field.

尚、ビーム形状の測定にはRCAのp3o。In addition, RCA p3o is used to measure the beam shape.

チャートを使用した。第1図において、1はカソード電
極、G1電極、G2電極からなる電子銃部、2は静電偏
向電界を発生する偏向電極、3はメソシー電極、4は光
電膜、透明電極、ストライプフィルター等から成るター
ゲット部、6は集束コイルであり、6,6′は集束磁界
である。第2図において、体)は集束磁界の向きが第1
図6の場合のビーム形状であり、伽)は集束磁界の向き
が同図e′の場合のビーム形状である。ビーム形状が集
束磁界の向きにより第2図の様に変化する理由は次の様
に考えられる。
I used a chart. In Figure 1, 1 is an electron gun section consisting of a cathode electrode, a G1 electrode, and a G2 electrode, 2 is a deflection electrode that generates an electrostatic deflection electric field, 3 is a mesocye electrode, and 4 is a photoelectric film, a transparent electrode, a stripe filter, etc. 6 is a focusing coil, and 6 and 6' are focusing magnetic fields. In Figure 2, the direction of the focused magnetic field is the first
The beam shape in the case of FIG. 6 is the beam shape when the direction of the focusing magnetic field is e' in the figure. The reason why the beam shape changes as shown in FIG. 2 depending on the direction of the focused magnetic field is considered to be as follows.

ターゲット上のビームはビームベンディングが無い場合
、セルフシャープニング効果により前縁のみ電流が流れ
る。今うスクが左上から右下に走査する場合を考えると
ビーム形状は見掛上左下りの三日月状になることが知ら
れている。次にビームヘンティア り効果に考える。セ
ルフシャープニング効果が無い場合、ビームの走査にょ
シ走査後の面電位と走査前の面電位は異なるためその電
位差により垂直方向に電界が生ずる。磁界が無い場合に
はこの電界によシミ子ビームは下方に曲げられランディ
ングする。従って上下方向に伸びた楕円形にビーム形状
は変形する。MS型撮像管(又はMM型撮像管)の場合
には集束磁界が走査面に対し垂直に加わっている為、こ
の電界の直交場を通る電子ビームはそれぞれに垂直な方
向のカを受ける。即ち第1図の6の様な磁界の向きでは
右側に、6′の様な磁界の向きでは左側にカを受ける。
When there is no beam bending in the beam on the target, current flows only at the leading edge due to the self-sharpening effect. If we consider the case where the beam scans from the upper left to the lower right, it is known that the beam shape will appear to be crescent-shaped, descending to the left. Next, consider the beam hentir effect. If there is no self-sharpening effect, the surface potential after scanning of the beam and the surface potential before scanning are different, and an electric field is generated in the vertical direction due to the potential difference. In the absence of a magnetic field, the electric field bends the shimiko beam downward and causes it to land. Therefore, the beam shape is deformed into an ellipse extending in the vertical direction. In the case of an MS type image pickup tube (or MM type image pickup tube), since a focusing magnetic field is applied perpendicularly to the scanning plane, electron beams passing through a field perpendicular to this electric field are subjected to forces in directions perpendicular to each other. That is, when the magnetic field is oriented as 6 in FIG. 1, the force is applied to the right side, and when the magnetic field is oriented 6' in FIG. 1, the force is applied to the left side.

この結果6の磁界の場合には右下りの楕円に、6′の磁
界の場合には左下りの楕円状になってターゲットにラン
ディングする。従ってセルフシャープニング効果とビー
ムベンディング効果とが合わさっている場合には第2図
の様なビーム形状がそれぞれ得られる。
As a result, in the case of a magnetic field of 6, it lands on the target in an elliptical shape descending to the right, and in the case of a magnetic field of 6', it lands in an elliptical shape descending to the left. Therefore, when the self-sharpening effect and the beam bending effect are combined, beam shapes as shown in FIG. 2 are obtained.

この様なビーム形状の場合について、ストライプフィル
ターで得られる出力信号のレベルを求めてみたのが第3
図である。横軸はy軸からの角度を、縦軸は変調度を表
わしている。第3図(a)が第2図(−)のビーム形状
の場合、第3図(b)が第2図(b)のビーム形状の場
合である。図においてAは右下りのストライプフィルタ
ーの実際の角度、Bは左下りのストライプフィルターの
角度である。この図から第2図(−)のビーム形状の方
がはゾ同一レベルのR信号出力とB信号出力が得られる
ことがわかる。この第2図(−)のビーム形状は集束磁
界が電子銃側からターゲット側へと向いている時得られ
る。
In the third part, we tried to find the level of the output signal obtained by the stripe filter in the case of such a beam shape.
It is a diagram. The horizontal axis represents the angle from the y-axis, and the vertical axis represents the degree of modulation. 3(a) is the case where the beam shape is as shown in FIG. 2(-), and FIG. 3(b) is the case where the beam shape is as shown in FIG. 2(b). In the figure, A is the actual angle of the stripe filter on the lower right, and B is the angle of the stripe filter on the lower left. It can be seen from this figure that the beam shape shown in FIG. 2 (-) provides R and B signal outputs of the same level. The beam shape shown in FIG. 2 (-) is obtained when the focusing magnetic field is directed from the electron gun side to the target side.

以上述べたように本発明は交差型ストライプフィルター
を用いる周波数分離型単管カラーカメラにおいて、MM
型撮像管もしくはMS型撮像管に電子銃側からターゲッ
ト側へと向かう集束磁界を発生する集束コイルを用いた
ことを特徴とするもので、その結果R信号出力とB信号
出力のレベルをはy同一レベルにすることができるとい
う効果を有するものである。その結果、色分離誤差が少
く、かつカラーS/Nを向上させることができるという
効果を有するものである。
As described above, the present invention provides a frequency-separated single-tube color camera using a crossed stripe filter.
It is characterized by using a focusing coil that generates a focusing magnetic field from the electron gun side to the target side in the type image pickup tube or MS type image pickup tube, and as a result, the level of the R signal output and the B signal output is This has the effect of making it possible to maintain the same level. As a result, it is possible to reduce color separation errors and improve color S/N.

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

第1図は本発明の一実施例における周波数分離型単管カ
ラーカメラの原理図、第2図はビーム形状の測定例を示
す図、第3図はy軸からのストライプフィルターの角度
と信号出力との関係を示す図である。 1・・・・・・電子銃部、2・・・・・・偏向電極、3
・・・・・・メツシー電極、5・・・・・集束コイル、
6,6′・・・・・集束磁界。
Figure 1 is a diagram showing the principle of a frequency-separated single-tube color camera according to an embodiment of the present invention, Figure 2 is a diagram showing an example of beam shape measurement, and Figure 3 is the angle of the stripe filter from the y-axis and the signal output. FIG. 1... Electron gun section, 2... Deflection electrode, 3
...Metshi electrode, 5...Focusing coil,
6,6'...Focusing magnetic field.

Claims (1)

【特許請求の範囲】[Claims] 交差型ストライプフィルターを内臓する周波数分離型撮
像管を備え、この撮像管を電磁集束−電磁偏向型もしく
は電磁集束・静電偏向型に構成し、集束磁界の向きが電
子銃側からターゲット側へ向かう集束磁界を発生する集
束コイルを用いたことを特徴とする周波数分離型単管カ
ラーカメラ。
Equipped with a frequency-separated image pickup tube that incorporates a cross-type stripe filter, this image pickup tube is configured as an electromagnetic focusing-electromagnetic deflection type or an electromagnetic focusing/electrostatic deflection type, and the direction of the focused magnetic field is directed from the electron gun side to the target side. A frequency-separated single-tube color camera characterized by the use of a focusing coil that generates a focusing magnetic field.
JP56208585A 1981-12-22 1981-12-22 Frequency separating type single bulb color camera Pending JPS58108889A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56208585A JPS58108889A (en) 1981-12-22 1981-12-22 Frequency separating type single bulb color camera

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56208585A JPS58108889A (en) 1981-12-22 1981-12-22 Frequency separating type single bulb color camera

Publications (1)

Publication Number Publication Date
JPS58108889A true JPS58108889A (en) 1983-06-29

Family

ID=16558619

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56208585A Pending JPS58108889A (en) 1981-12-22 1981-12-22 Frequency separating type single bulb color camera

Country Status (1)

Country Link
JP (1) JPS58108889A (en)

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