JPS60242420A - Spatial frequency filter - Google Patents

Spatial frequency filter

Info

Publication number
JPS60242420A
JPS60242420A JP9961284A JP9961284A JPS60242420A JP S60242420 A JPS60242420 A JP S60242420A JP 9961284 A JP9961284 A JP 9961284A JP 9961284 A JP9961284 A JP 9961284A JP S60242420 A JPS60242420 A JP S60242420A
Authority
JP
Japan
Prior art keywords
luminous flux
plate
savart
spatial frequency
plates
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.)
Granted
Application number
JP9961284A
Other languages
Japanese (ja)
Other versions
JPH06100733B2 (en
Inventor
Yoshiyori Takizawa
義順 瀧澤
Takahiro Nakamura
隆広 中村
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.)
Toshiba Corp
Toshiba AVE Co Ltd
Original Assignee
Toshiba Corp
Toshiba Audio Video Engineering 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 Toshiba Corp, Toshiba Audio Video Engineering Co Ltd filed Critical Toshiba Corp
Priority to JP59099612A priority Critical patent/JPH06100733B2/en
Priority to DE19853515020 priority patent/DE3515020A1/en
Priority to US06/727,914 priority patent/US4807981A/en
Publication of JPS60242420A publication Critical patent/JPS60242420A/en
Publication of JPH06100733B2 publication Critical patent/JPH06100733B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To improve band limitation effect in a slanting direction by employing the basic constitution structured by stacking a birefringent plate which separates luminous flux at 45 deg. of a horizontal axis and birefringent plates which separate luminous flux horizontally and vertically. CONSTITUTION:The Savart plate S11 which separates the luminous flux at 45 deg. to the horizontal axis, Savart plate S12 which separates the luminous flux horizontally or vertically, and Savart plate S13 which separates the luminous flux at right angles to the luminous flux separation of the Savart plate S11. The angle between the luminous flux separation directions of the Savart plates S11 and S12 is 45 deg., so two pieces of luminous flux separated by the Savart plates S11 and S12 are separated in 1:1 light intensity proportion into four pieces of luminous flux, and the number of pieces of luminous flux passed through the Savart plate S13 is eight. Thus, sufficient band limitation effect is obtained even in the slanting direction, so components with low importance to the human eyes are removed, so that natural reproduced images are obtained when this filter is applied to a solid-state image pickup device, etc.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は水晶等の複屈折物質から成る平行平面板を結
像光学系に配設するシステムに用いられる空間周波数フ
ィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a spatial frequency filter used in a system in which a parallel plane plate made of a birefringent material such as quartz is arranged in an imaging optical system.

〔発明の技術的背景〕[Technical background of the invention]

近年、固体撮像素子、ファイバースコープ等のように、
空間情報を離散的にサンプリングするこ゛とによって画
像情報を得るシステムが開発されている。しかしこのシ
ステムにおいては、サンプリング処理に特有なナイキス
ト限界がある。そして、ナイキスト限界を越える情報の
うち、結像光学系と画素の開口配列によって決まる応答
特性の帯域内の情報が、低周波域に折シ返し、ナイキス
ト限界内の信号に対する正しい情報再生を妨害してしま
うという問題がある。
In recent years, solid-state imaging devices, fiberscopes, etc.
Systems have been developed that obtain image information by discretely sampling spatial information. However, this system has a Nyquist limit inherent to the sampling process. Of the information that exceeds the Nyquist limit, information within the response characteristic band determined by the imaging optical system and pixel aperture arrangement is reflected back into the low frequency range, interfering with correct information reproduction for signals within the Nyquist limit. There is a problem with this.

上記の問題を解決するために、水晶等の複屈折板を用い
、上記の折シ返しを越こす周波数域にいくつかの光学的
周波数トラ、プを持つ空間周波数フィルタを構成し、折
シ返しによる偽信号の発生を軽減するという方法がある
In order to solve the above problem, a birefringent plate such as quartz is used to construct a spatial frequency filter that has several optical frequency traps in the frequency range that exceeds the above-mentioned folding. There is a method to reduce the occurrence of false signals due to

第7図は上記空間周波数フィルタの一例であシ、S1〜
S3はサバール板、PI、PIは偏光解消板である。同
図(a)は、使用時の構成であシ、同図(b)は、各板
の分解図である。各板の矢印は、光束の分離方向上を示
している。
FIG. 7 is an example of the above-mentioned spatial frequency filter, S1~
S3 is a Savart plate, and PI and PI are depolarization plates. FIG. 4(a) shows the configuration when in use, and FIG. 2(b) is an exploded view of each plate. The arrows on each plate indicate the direction in which the luminous flux is separated.

第8図は第7図の空間周波数フィルタによる光束の分離
状態を示している。Vは垂直方向、Hは水平方向であシ
、各O印が光束の最小単位の分離位置を示し、○印部6
矢印は偏光方向を意味する。今、光は、サバール板S1
側から入射するものとする。サバール板S1に′よって
入射光は、偏光方向に従って、2光束に分離される。(
第8図(a))。サバール板S1からの射出光は、偏光
解消板P1を介してサバール板S2を通る。これによっ
て、テバール板Sノで分離された2光束がさらにそれぞ
れ分離され4光束(第8図(b))となる。この射出光
は、偏光解消板P2を介してサバール板S3に通され、
最終的には、第8図(e)に示すように8光束に分離さ
れる。サバール板は、櫛形フィルタとして作用すること
が知られているが、上記のフィルタでは、サバール板S
1〜S3の各櫛形フィルタとしての空間周波数特性をか
け合わせた特性の空間周波数フィルタとなる。第10図
に示したフィルタIOAも同様な特性となる。同図(a
)はフィルタ全体の構造、同図(b)は、使用される各
サバール板S1〜S4の光束分離方向を示している。ま
た、第11図に示す空間周波数フィルタ11にもある。
FIG. 8 shows a state in which the light beam is separated by the spatial frequency filter of FIG. V is vertical direction, H is horizontal direction, each O mark indicates the separation position of the minimum unit of luminous flux, ○ mark part 6
Arrows indicate polarization direction. Now, the light is Savart plate S1
Assume that the light is incident from the side. The incident light is separated into two beams by the Savart plate S1' according to the polarization direction. (
Figure 8(a)). The light emitted from the Savard plate S1 passes through the Savard plate S2 via the depolarization plate P1. As a result, the two light beams separated by the Tevar plate S are further separated into four light beams (FIG. 8(b)). This emitted light is passed through the Savart plate S3 via the depolarization plate P2,
Ultimately, the light beam is separated into eight beams as shown in FIG. 8(e). It is known that the Savart plate acts as a comb-shaped filter, but in the above filter, the Savart plate S
The spatial frequency filter has a characteristic obtained by multiplying the spatial frequency characteristics of each of the comb filters 1 to S3. The filter IOA shown in FIG. 10 also has similar characteristics. The same figure (a
) shows the structure of the entire filter, and FIG. 2(b) shows the beam separation direction of each of the Savart plates S1 to S4 used. It also exists in the spatial frequency filter 11 shown in FIG.

同図(1)はフィルタ全体の構造、同図(b)は使用さ
れるサバール板81.82の光束分離方向を示している
Figure (1) shows the overall structure of the filter, and Figure (b) shows the light beam separation direction of the Savart plates 81 and 82 used.

〔背景技術の問題点〕[Problems with background technology]

第7図及び第10図に示した空間周波数フィルタは、第
9図に破線で示す空間周波数にトラツノポイントを持つ
。UHは水平方向空間周波数軸、Uvは垂直方向空間周
波数軸である。また、破線で示すトラ、グポイントには
、対応するサバール板と同符号を付している。
The spatial frequency filters shown in FIGS. 7 and 10 have trigonal points at the spatial frequencies shown by broken lines in FIG. 9. UH is a horizontal spatial frequency axis, and Uv is a vertical spatial frequency axis. In addition, the trough and g points indicated by broken lines are given the same reference numerals as the corresponding Savard plates.

このような空間周波数フィルタをCODを用いた固体撮
像素子の光学系に設けた場合、人間の目にとって比較的
重要度の低い斜め方向の空間周波数情報が高い周波数の
ものまで透過する。
When such a spatial frequency filter is provided in the optical system of a solid-state image pickup device using COD, spatial frequency information in an oblique direction, which is relatively less important to the human eye, is transmitted up to high frequency information.

従って、再生像が不自然にみえてしiつという問題があ
る。また、3板のサバール板(櫛形フィルタ)のかけ合
わせ特性を得るために、第7図の例では5板、第10図
の例では4板の複屈折板が必要となシ、板敷が多くなる
という欠点がある。さらに、第7図の例では、偏光解消
板が波長特性を持つため、入射光の波長域が広い場合に
は上述したような特性を持つが波長域が狭い場合には波
長によって特性が異なるという欠点がある。つiシ、偏
光解消板は、波長域の特定された光が入射すると、その
分離した光束の偏光状態が所望の状態とならず、周波数
帯域制限が不充分となることがある。
Therefore, there is a problem in that the reproduced image looks unnatural. In addition, in order to obtain the multiplication characteristics of three Savart plates (comb-shaped filters), five birefringent plates are required in the example shown in Figure 7, and four birefringent plates are required in the example shown in Figure 10. It has the disadvantage of becoming. Furthermore, in the example shown in Figure 7, the depolarizing plate has wavelength characteristics, so if the wavelength range of the incident light is wide, it will have the characteristics described above, but if the wavelength range is narrow, the characteristics will differ depending on the wavelength. There are drawbacks. However, when light with a specified wavelength range is incident on the depolarizing plate, the polarization state of the separated light beam may not be in the desired state, resulting in insufficient frequency band limitation.

さらに、カラー固体撮像装置においては、斜め方向に入
射光を空間変調する方式が多く用いられるが、このよう
な方式においては、上記変・調量波数と同一の斜め方向
の空間周波数の信号が入射光情報に含まれてしまうと、
色偽信号が再生されてしまうという問題があシ、上述し
た空間周波数フィルタでは色偽信号を充分に減少するこ
とができないという欠点がある。
Furthermore, in color solid-state imaging devices, a method is often used that spatially modulates incident light in an oblique direction. If it is included in optical information,
There is a problem that color artifacts are reproduced, and the above-mentioned spatial frequency filter has the disadvantage that color artifacts cannot be sufficiently reduced.

次に、第11図に示した空間周波数フィルタ2JAによ
ると、第12図に示すように4光束分離を得る。この分
離光束において、○印で示す空間周波数位置の光束は、
Δ印で示す位置の光束に比べて強くなる。このフィルタ
においては、斜め方向は、水平、垂直に比べ低い周波数
にトラップポイントを持つが、第13図に示すように、
水平方向に対してはトラップポイントを持たないフィル
タになってしまうという欠点がある。
Next, according to the spatial frequency filter 2JA shown in FIG. 11, four beam separation is obtained as shown in FIG. 12. In this separated luminous flux, the luminous flux at the spatial frequency position indicated by the circle is
The luminous flux is stronger than that at the position indicated by the Δ mark. In this filter, the diagonal direction has a trap point at a lower frequency than the horizontal and vertical directions, but as shown in Figure 13,
The drawback is that the filter does not have trap points in the horizontal direction.

〔発明の目的〕[Purpose of the invention]

この発明は上記の事情に対処すべくなされたもので、第
1に少ない板数の複屈折板で、高い帯域制限効果を発揮
し、また第2に人間の視覚にとって重要度の低い斜め方
向の帯域制限効果を向上した空間周波数フィルタを提供
することを目的とする。
This invention was made to address the above-mentioned circumstances. Firstly, a birefringent plate with a small number of plates can exhibit a high band-limiting effect, and secondly, it can be used in diagonal directions that are less important for human vision. An object of the present invention is to provide a spatial frequency filter with improved band-limiting effect.

〔発明の概要〕[Summary of the invention]

この発明は、水平軸に対して45°方向に光束分離を得
るサバール板811と、この第1の複屈折板のlIシに
配設され水平又は垂直方向に光束分離を得るサバール板
S12と、このサバール板812を前記サバール板81
1と共に挟み、前記サバール板1311の光束分離方向
とは直交する方向に光束分離を得るサバール板81Bと
で上記目的を達成するものである。
The present invention includes a Savart plate 811 that obtains luminous flux separation in a direction of 45° with respect to the horizontal axis, and a Savart plate S12 that obtains luminous flux separation in the horizontal or vertical direction, which is disposed on the lI side of this first birefringent plate. This Savard plate 812 is replaced by the Savard plate 81.
The above object is achieved by the Savart plate 81B which is sandwiched together with the Savard plate 1311 and separates the light beam in a direction perpendicular to the light beam separation direction of the Savard plate 1311.

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

以下この発明の実施例を図面を参照して説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図はこの発明の一実施例であシ、S11〜sisの
3板のサバール板が貼シ合わせられて構成されている。
FIG. 1 shows an embodiment of the present invention, which is constructed by laminating three Savard plates S11 to sis.

各サバール板811〜813は、同図(b)に矢印で示
す方向に光束分離方向を持つ。
Each of the Savart plates 811 to 813 has a light beam separation direction in the direction shown by an arrow in FIG.

第2図は、第1図の空間周波数フィルタの光束分離の様
子を示している。1板のサバール板を透過した光束が更
にもう1板のサバール板を透過する場合、第2のサバー
ル板の入射光量と、その分離された光束の光量との比は
、2板のサバール板の光束分離方向を0とした場合、5
iI12θ:傷2θとなる。本実施例においては、サバ
ール板811と812の光束分離方向のなす角度は45
°となっている。このため、サバール板S11によって
分離された2光束(第2図(a))は、それぞれ光強度
1:1に分離されて4光束(第2図(b))になる。サ
バール板812pS1:I間でも光束分離方向は45’
となっているため、サバール板813を透過した光束は
、8光束(第2図(C))となる。
FIG. 2 shows how the spatial frequency filter shown in FIG. 1 separates the light beam. When a light beam transmitted through one Savard plate is further transmitted through another Savard plate, the ratio of the amount of light incident on the second Savard plate to the amount of the separated light beam is as follows: If the beam separation direction is 0, then 5
iI12θ: Injury 2θ. In this embodiment, the angle formed by the light beam separation directions of the Savart plates 811 and 812 is 45
°. Therefore, the two light beams separated by the Savart plate S11 (FIG. 2(a)) are separated into four light beams (FIG. 2(b)) with a light intensity of 1:1. Even between Savart plate 812pS1:I, the beam separation direction is 45'
Therefore, the number of light beams transmitted through the Savart plate 813 is eight light beams (FIG. 2(C)).

上記した空間周波数フィルタによると、サバール板81
1,812,813のそれぞれの櫛形フィルタとしての
特性をかけ合わせた総合特性となる。そして、この総合
特性は、第3図に示すように、破線で示した空間周波数
にドラッグポイントを持つ特性となる。
According to the above-described spatial frequency filter, the Savart plate 81
The total characteristic is obtained by multiplying the characteristics of 1, 812, and 813 comb filters. As shown in FIG. 3, this comprehensive characteristic has a drag point at the spatial frequency indicated by the broken line.

Uvは、垂直方向空間周波数軸、UHは垂直方向空間周
波数軸である。また、破線で示すトラップ特性線3*、
3b、4m、4b、5*。
Uv is the vertical spatial frequency axis, and UH is the vertical spatial frequency axis. In addition, the trap characteristic line 3* shown by the broken line,
3b, 4m, 4b, 5*.

5bと軸の交点は、サバール板の厚さによって決まる。The intersection of 5b and the axis is determined by the thickness of the Savart plate.

上記のように、本発明によると、特性線J a。As mentioned above, according to the present invention, the characteristic line Ja.

3bと、特性線4m、4bと、特性線5a。3b, characteristic lines 4m, 4b, and characteristic line 5a.

5bの3組による総合特性3枚のサバール板811.8
12,813で得ることができる。
Comprehensive characteristics of 3 sets of 5b 3 Sabal boards 811.8
12,813.

しかも、本フィルタによると、人間の目の解像度のよい
水平方向に対しては、帯域制限を行なうことなく、人間
の目にとって重要でない斜め方向にトラップポイントを
持つ特性を作っているO この発明では、水平軸に対して光束の分離方向が45°
の方向をなす第1のサバール板と、この第1のサバール
板の光束分離方向とは直交する光束分離方向を有した第
2のサバール板と、この第1.第2のサバール板の間に
垂直又は水平方向へ光束分離方向を有した第3のサバー
ル板とを設け、上記の特性を得ている。
Moreover, according to this filter, in the horizontal direction, where the resolution of the human eye is good, there is no band limitation, and a characteristic is created that has trap points in the diagonal direction, which is not important to the human eye. , the separation direction of the luminous flux is 45° with respect to the horizontal axis
, a second Savard plate having a light beam separation direction perpendicular to the light beam separation direction of the first Savard plate, and a second Savard plate having a light beam separation direction perpendicular to the light beam separation direction of the first Savard plate. A third Savard plate having a light beam separation direction in the vertical or horizontal direction is provided between the second Savard plate to obtain the above characteristics.

この基本原理によって、第4図(a) (b)に示す組
み合わせであっても、同様な目的、効果を達成すること
ができる。即ち第4図(a)のサバール板8211B2
2,823を順番に貼り合わせても良く、また第4図(
b)のサバール板s31゜832.833を順番に貼シ
合わせても良い。
Based on this basic principle, similar objectives and effects can be achieved even with the combinations shown in FIGS. 4(a) and 4(b). That is, the Savart plate 8211B2 in FIG. 4(a)
2,823 may be pasted together in order, or as shown in Figure 4 (
The Savart plates s31°832.833 of b) may be pasted together in order.

もちろんこの場合も、斜め方向に光束分離方向を有した
サバール板の厚みは、第3図の軸Uv。
Of course, in this case as well, the thickness of the Savart plate with the light beam separation direction diagonally corresponds to the axis Uv in FIG.

UH上での特性線のクロス点を一致させるため互いに等
しいことが必要である。
In order to match the crossing points of the characteristic lines on the UH, they must be equal to each other.

第5図は、第1図の実施例のものに更に、垂直方向に光
束分離方向を有したサバール板840を追加し、巣6図
のようにトラップ特性線6a。
In FIG. 5, a Savart plate 840 having a beam separation direction in the vertical direction is added to the embodiment shown in FIG. 1, and a trap characteristic line 6a is formed as shown in FIG.

6bを増加させたフィルタを示している。更に多くのサ
バール板を用い多くのトラップポイントを持ったフィル
タを構成してもよいが、本発明では、基本的には、水平
方向に対して45°方向に光束分離方向を持った第1の
サバール板、この第1のサバール板の光分離方向とは直
交する方向へ光束分離方向を持った第2のサバール板、
この第1.第2のサバール板の間に配置され水平又は垂
直方向に光束分離方向を持った第3のサバール板を重ね
合わせる構造に変シはない。
6b is shown. Although it is possible to configure a filter with many trap points using more Savart plates, the present invention basically uses a first filter having a beam separation direction in the direction of 45 degrees with respect to the horizontal direction. a Savard plate, a second Savard plate having a light beam separation direction in a direction perpendicular to the light separation direction of the first Savard plate;
This first. There is no change in the structure in which the third Savard plate is placed between the second Savard plates and has a beam separation direction in the horizontal or vertical direction.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、複屈折板(サバ
ール板)の1枚、1枚の櫛形フィルタとしての特性をか
け合わせた総合特性を得るが、特に、小ない枚数の複屈
折板で、良好な周波数ドラッグポイントを得ることがで
きる。しかも、本発明では、斜め方向にも十分な帯域制
限効果を有するため、人間の目にとっては重要度の低い
成分が除去され、固体撮像装置等に用いた場合、自然な
再生像を得るのに寄与できる。
As explained above, according to the present invention, a comprehensive characteristic is obtained by multiplying the characteristics of one birefringent plate (Savart plate) and one comb-shaped filter, but in particular, a small number of birefringent plates , you can get a good frequency drag point. Moreover, since the present invention has a sufficient band-limiting effect even in oblique directions, components of low importance to the human eye are removed, and when used in solid-state imaging devices, etc., it is difficult to obtain natural reproduced images. I can contribute.

また、第5図、第6図で説明したフィルタであれば、水
平方向、垂直方向を同等な特性にすることができ、はぼ
等方向な空間周波数特性を得ることも可能である。さら
に、斜め方向に入射光を空間変調するカラー撮像装置、
つま)市松状の色フィルタを有する装置の光学系では、
45°あるいは1350の方向に光束分離を得る櫛形フ
ィルタと、水平方向に光束分離を得る櫛形フィルタが共
に、前記斜め方向の空間変調周波数に対する応答を零と
するように板厚を選定すれば、色偽信号の軽減効果を大
幅に向上することができる。
Furthermore, with the filters described in FIGS. 5 and 6, it is possible to have equivalent characteristics in the horizontal and vertical directions, and it is also possible to obtain spatial frequency characteristics that are approximately equidirectional. Furthermore, a color imaging device that spatially modulates incident light in an oblique direction;
In the optical system of a device with a checkered color filter,
If the plate thicknesses of both the comb-shaped filter that obtains luminous flux separation in the 45° or 1350° direction and the comb-shaped filter that obtains luminous flux separation in the horizontal direction are zero in response to the spatial modulation frequency in the diagonal direction, the color The effect of reducing false signals can be greatly improved.

【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を示す構成説明図、第2図
は第1図の空間周波数フィルタの光束分離の説明図、第
3図は第1図の空間周波数フィルタの空間周波数特性説
明図、第4図はこの発明の他の実施例を示す説明図、第
5図は更に他の実施例を示す構成説明図、第6図は第5
図の空間周波数フィルタの空間周波数特性説明図、第7
図は従来の空間周波数フィルタの構成説明図、第8図は
第7図の空間周波数フィルタの光束分離の説明図、第9
図は第7図の空間同第12図は第11図の空間周波数フ
ィルタの光束分離の説明図、第13図は、第11図の空
間周波数フィルタの応答特性図である。 811〜813,821〜823.8B1〜S33.S
40・・・サバール板。 出願人代理人 弁理士 鈴 江 武 彦第1図 第2図 第3図 第4図 (a) (b) (C) 第11図 第12図 第13図 9間用沢畝 手続補正書 昭和 i9・1q29日 特許庁長官 志 賀 学 殿 1、事件の表示 特願昭59−99612号 2゜発明の名称 空間周波数フィルタ 3、補正をする者 事件との関係 特許出願人 (307) 株式会社 東芝 (ほか1名) 4、代理人 5、自発補正 6 補正のヌ・]象 明細書 7、補正の内容 (1) 明細書第2頁第10行目に「折り返しを越こす
」とあるのを「折り返しを起こす」と訂正する。 (2) 明細書第8頁第12行目乃至第13行目に「U
Hは垂直方向」とあるのf 「UHは水平方向」と訂正
する。 (3) 明細書第11貞第1行目に「小ない枚数の」と
あるのを「少ない枚数の」と訂正する。
Fig. 1 is an explanatory diagram of a configuration showing an embodiment of the present invention, Fig. 2 is an explanatory diagram of luminous flux separation of the spatial frequency filter of Fig. 1, and Fig. 3 is an explanatory diagram of spatial frequency characteristics of the spatial frequency filter of Fig. 1. 4 is an explanatory diagram showing another embodiment of the present invention, FIG. 5 is a configuration explanatory diagram showing still another embodiment, and FIG.
Spatial frequency characteristics explanatory diagram of the spatial frequency filter shown in Fig. 7.
The figure is an explanatory diagram of the configuration of a conventional spatial frequency filter, FIG. 8 is an explanatory diagram of the beam separation of the spatial frequency filter of FIG. 7, and FIG.
12 is an explanatory diagram of the beam separation of the spatial frequency filter of FIG. 11, and FIG. 13 is a response characteristic diagram of the spatial frequency filter of FIG. 11. 811-813, 821-823.8B1-S33. S
40...Savar board. Applicant's Representative Patent Attorney Takehiko Suzue Figure 1 Figure 2 Figure 3 Figure 4 (a) (b) (C) Figure 11 Figure 12 Figure 13 Figure 9 Amended Book of Proceedings Showa i9・1q 29th Manabu Shiga, Commissioner of the Japan Patent Office 1, Indication of the case, Patent Application No. 59-99612 2゜Name of the invention Spatial frequency filter 3, Person making the correction Relationship with the case Patent applicant (307) Toshiba Corporation ( (and 1 other person) 4. Agent 5, Voluntary amendment 6. Amendment 7. Contents of amendment (1) On page 2, line 10 of the specification, the phrase "beyond the fold" was changed to "``I'm going to make a comeback,'' he corrected. (2) “U
``H is vertical direction'' is corrected to ``UH is horizontal direction''. (3) In the first line of No. 11 of the specification, the phrase "of a small number of sheets" is corrected to "of a small number of sheets."

Claims (1)

【特許請求の範囲】[Claims] 水平軸に対して45’方向に光束分離を得る第1の複屈
折板と、この第1の複屈折板と厚みが同じで前記光束分
離の方向とは直交する方向へ光束分離を得る第2の複屈
折板と、前記第1゜第2の複屈折板の間に配設され水平
又は垂直方向に光束分離を得る第3の複屈折板とを重ね
た構造を基本構成として成シ、光学系に配設されること
を特徴とする空間周波数フィルタ。
a first birefringent plate that obtains beam separation in the 45' direction with respect to the horizontal axis; and a second birefringent plate that has the same thickness as the first birefringent plate and obtains beam separation in a direction perpendicular to the direction of the beam separation. The basic structure consists of a birefringent plate and a third birefringent plate disposed between the first and second birefringent plates to obtain luminous flux separation in the horizontal or vertical direction. A spatial frequency filter characterized in that:
JP59099612A 1984-04-28 1984-05-17 Spatial frequency filter Expired - Lifetime JPH06100733B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP59099612A JPH06100733B2 (en) 1984-05-17 1984-05-17 Spatial frequency filter
DE19853515020 DE3515020A1 (en) 1984-04-28 1985-04-25 LOCAL FREQUENCY FILTER
US06/727,914 US4807981A (en) 1984-04-28 1985-04-26 Spatial frequency filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59099612A JPH06100733B2 (en) 1984-05-17 1984-05-17 Spatial frequency filter

Publications (2)

Publication Number Publication Date
JPS60242420A true JPS60242420A (en) 1985-12-02
JPH06100733B2 JPH06100733B2 (en) 1994-12-12

Family

ID=14251915

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59099612A Expired - Lifetime JPH06100733B2 (en) 1984-04-28 1984-05-17 Spatial frequency filter

Country Status (1)

Country Link
JP (1) JPH06100733B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02204715A (en) * 1989-02-02 1990-08-14 Canon Inc Image pickup device having optical low pass filter
WO2001065306A1 (en) * 2000-02-29 2001-09-07 Daishinku Corporation Optical device
JP2001272632A (en) * 2000-01-21 2001-10-05 Daishinku Corp Depolarizing member, depolarizing member for optical low pass filter and optical low pass filter using the depolarizing member
JP2019035946A (en) * 2017-08-10 2019-03-07 キヤノン株式会社 Optical low-pass filter and imaging device

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51127746A (en) * 1975-04-29 1976-11-08 Sony Corp Optical filter
JPS5266449A (en) * 1975-11-28 1977-06-01 Sony Corp Optical filter
JPS59279A (en) * 1982-06-26 1984-01-05 Sony Corp Image pickup device
JPS5975222A (en) * 1982-10-22 1984-04-27 Victor Co Of Japan Ltd Optical filter
JPS60164719A (en) * 1984-02-07 1985-08-27 Sony Corp Optical low-pass filter
JPS60230116A (en) * 1984-04-28 1985-11-15 Toshiba Corp Color solid-state image pickup device

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51127746A (en) * 1975-04-29 1976-11-08 Sony Corp Optical filter
JPS5266449A (en) * 1975-11-28 1977-06-01 Sony Corp Optical filter
JPS59279A (en) * 1982-06-26 1984-01-05 Sony Corp Image pickup device
JPS5975222A (en) * 1982-10-22 1984-04-27 Victor Co Of Japan Ltd Optical filter
JPS60164719A (en) * 1984-02-07 1985-08-27 Sony Corp Optical low-pass filter
JPS60230116A (en) * 1984-04-28 1985-11-15 Toshiba Corp Color solid-state image pickup device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02204715A (en) * 1989-02-02 1990-08-14 Canon Inc Image pickup device having optical low pass filter
JP2001272632A (en) * 2000-01-21 2001-10-05 Daishinku Corp Depolarizing member, depolarizing member for optical low pass filter and optical low pass filter using the depolarizing member
WO2001065306A1 (en) * 2000-02-29 2001-09-07 Daishinku Corporation Optical device
US7123412B2 (en) 2000-02-29 2006-10-17 Daishinku Corporation Optical device
JP2019035946A (en) * 2017-08-10 2019-03-07 キヤノン株式会社 Optical low-pass filter and imaging device

Also Published As

Publication number Publication date
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