JPH0627420A - Back light device - Google Patents

Back light device

Info

Publication number
JPH0627420A
JPH0627420A JP4184141A JP18414192A JPH0627420A JP H0627420 A JPH0627420 A JP H0627420A JP 4184141 A JP4184141 A JP 4184141A JP 18414192 A JP18414192 A JP 18414192A JP H0627420 A JPH0627420 A JP H0627420A
Authority
JP
Japan
Prior art keywords
light
polarized light
linearly polarized
liquid crystal
crystal display
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
JP4184141A
Other languages
Japanese (ja)
Inventor
Tooru Nakakusu
徹 中楠
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.)
Casio Computer Co Ltd
Original Assignee
Casio Computer 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 Casio Computer Co Ltd filed Critical Casio Computer Co Ltd
Priority to JP4184141A priority Critical patent/JPH0627420A/en
Publication of JPH0627420A publication Critical patent/JPH0627420A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide a back light device which projects the light from a light source on a liquid crystal panel by almost 100% and to increase the brightness of an image displayed on the liquid crystal panel. CONSTITUTION:The light source light from a parabolic mirror 14 is spectrally split to the P polarized light and the S polarized light by a polarized light beam splitter 15. Besides, the split S polarized light is changed to the P polarized light by a 1/2 wavelength plate 19. Then, the P polarized light transmitted through the plate 19 and the P polarized light transmitted through the splitter 15 are respectively condensed at an identical position by condenser lenses 20 and 22. Besides, the P polarized light condensed by the lenses 20 and 22 is reflected on the reflecting surface 24 of a concave mirror 23 and made incident on the liquid crystal panel 11.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、たとえば液晶プロジェ
クタや液晶表示装置などに使用されるバックライト装置
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a backlight device used in, for example, a liquid crystal projector or a liquid crystal display device.

【0002】[0002]

【従来の技術】従来、この種のバックライト装置は、図
2に示すように、メタルハライドランプ等の光源1と放
物面鏡2とからなり、光源1で発生した光源光を放物面
鏡2により液晶表示パネル3の光入射面に向けて反射す
るようになっている。
2. Description of the Related Art Conventionally, as shown in FIG. 2, a backlight device of this type conventionally includes a light source 1 such as a metal halide lamp and a parabolic mirror 2, and the source light generated by the light source 1 is a parabolic mirror. 2 reflects the light toward the light incident surface of the liquid crystal display panel 3.

【0003】[0003]

【発明が解決しようとする課題】ところで、このような
構成のバックライト装置では、光源1で発生する光源光
が液晶表示パネル3の光入射面に対しP偏光とS偏光の
両方を含んでいるため、液晶表示パネル3の光入射側に
偏光板を配置し、P偏光またはS偏光のいずれか一方を
偏光板で吸収する必要がある。しかしながら、P偏光ま
たはS偏光のいずれか一方を偏光板で吸収すると、液晶
表示パネル3に入射する光源光の光量が半分になってし
まい、偏光板で吸収される分が無駄となるばかりでなく
液晶表示パネル3の明るさも半減してしまうという問題
があった。
In the backlight device having such a configuration, the light source light generated by the light source 1 includes both P-polarized light and S-polarized light with respect to the light incident surface of the liquid crystal display panel 3. Therefore, it is necessary to dispose a polarizing plate on the light incident side of the liquid crystal display panel 3 and absorb either the P polarized light or the S polarized light by the polarizing plate. However, if either the P-polarized light or the S-polarized light is absorbed by the polarizing plate, the light amount of the light source light incident on the liquid crystal display panel 3 will be halved, and the amount absorbed by the polarizing plate will be wasted. There is a problem that the brightness of the liquid crystal display panel 3 is also halved.

【0004】本発明は、このような問題点に鑑みてなさ
れたもので、その目的は光源からの光を液晶表示パネル
にほぼ100%入射させることができ、かつ液晶表示パ
ネルの明るさを増大させることのできるバックライト装
置を提供しようとするものである。
The present invention has been made in view of the above problems, and an object thereof is to allow almost 100% of light from a light source to enter a liquid crystal display panel and to increase the brightness of the liquid crystal display panel. It is intended to provide a backlight device that can be operated.

【0005】[0005]

【課題を解決するための手段】上記課題を解決するため
に本発明は、光源と、この光源で発生した光源光を前方
に向けて平行に反射する放物面鏡と、この放物面鏡で反
射された光源光を偏光方向が互いに90度異なる2つの
直線偏光に分光する分光手段と、この分光手段で分光さ
れた2つの直線偏光のうち一方の直線偏光を他方の直線
偏光と同じ偏光方向にする偏光手段と、この偏光手段か
らの直線偏光を集光する第1の集光手段と、前記分光手
段で分光された2つの直線偏光のうち他方の直線偏光を
前記第1の集光手段と同じ位置に集光する第2の集光手
段と、これら第1の集光手段および第2の集光手段と同
一位置に焦点を有すると共に第1の集光手段および第2
の集光手段の焦点距離よりも曲率半径の小さい反射面を
有し前記第1の集光手段および第2の集光手段で集光さ
れた直線偏光を液晶表示パネルに向けて反射する凹面鏡
とを具備したものである。
In order to solve the above-mentioned problems, the present invention provides a light source, a parabolic mirror which reflects the light of the light source generated by the light source in a forward direction, and a parabolic mirror. The light source light reflected by the light source is split into two linearly polarized lights having polarization directions different from each other by 90 degrees, and one of the two linearly polarized lights split by this spectrally polarized light is the same as the other linearly polarized light. And a first condensing means for condensing the linearly polarized light from the polarizing means, and the other linearly polarized light of the two linearly polarized light dispersed by the spectroscopic means. Second condensing means for condensing at the same position as the means, and a first condensing means and a second condensing means having a focal point at the same position as the first condensing means and the second condensing means.
A concave mirror having a reflecting surface having a radius of curvature smaller than the focal length of the light collecting means and reflecting the linearly polarized light collected by the first light collecting means and the second light collecting means toward the liquid crystal display panel. It is equipped with.

【0006】[0006]

【作用】このような構成の本発明では、第1および第2
の集光手段で集光された直線偏光を凹面鏡の反射面に当
てて液晶表示パネルに入射させることにより、液晶表示
パネルに入射する光量が増大するので、液晶表示パネル
に表示される画像の明るさを高めることができる。
In the present invention having such a structure, the first and second
When the linearly polarized light collected by the light collecting means is applied to the liquid crystal display panel by applying it to the reflecting surface of the concave mirror, the amount of light entering the liquid crystal display panel increases, so that the brightness of the image displayed on the liquid crystal display panel is increased. The height can be increased.

【0007】[0007]

【実施例】以下、本発明の一実施例を図1を参照して説
明する。図1は液晶表示装置の概略構成を示す図で、こ
の液晶表示装置は、液晶表示パネル11と、この液晶表
示パネル11を背面側から照明するバックライト装置1
2とから構成されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT An embodiment of the present invention will be described below with reference to FIG. FIG. 1 is a diagram showing a schematic configuration of a liquid crystal display device. The liquid crystal display device includes a liquid crystal display panel 11 and a backlight device 1 for illuminating the liquid crystal display panel 11 from the back side.
2 and.

【0008】上記バックライト装置12は、メタルハラ
イドランプ等の光源13と、この光源13で発生した光
源光を前方に向けて平行に反射する放物面鏡14とを備
えており、放物面鏡14の前方には偏光ビームスプリッ
タ15が対向配置されている。
The backlight unit 12 includes a light source 13 such as a metal halide lamp, and a parabolic mirror 14 that reflects the light source light generated by the light source 13 in parallel to the front side. A polarization beam splitter 15 is arranged in front of 14 to face it.

【0009】上記偏光ビームスプリッタ15は放物面鏡
14からの入射光をP偏光とS偏光とに分光する分光面
16を有しており、この分光面16でP偏光と分光され
たS偏光は、偏光ビームスプリッタ15の側面17から
出射し、ミラー18を経て1/2波長板19に入射する
ようになっている。
The polarization beam splitter 15 has a spectral plane 16 for splitting the incident light from the parabolic mirror 14 into P-polarized light and S-polarized light. Is emitted from the side surface 17 of the polarization beam splitter 15, is incident on the half-wave plate 19 via the mirror 18.

【0010】上記1/2波長板19は入射光の偏光方向
を90度だけ変える偏光作用を有しており、この1/2
波長板19に入射したS偏光はP偏光となって1/2波
長板19から出射し、コンデンサレンズ20に入射する
ようになっている。このコンデンサレンズ20は入射光
をA点に集光する集光作用を有しており、コンデンサレ
ンズ20に入射した1/2波長板19からの入射光(P
偏光)はA点で集光した後、拡散光となって後述する凹
面鏡23の反射面に当たるようになっている。
The half-wave plate 19 has a polarization effect of changing the polarization direction of incident light by 90 degrees.
The S-polarized light that has entered the wave plate 19 becomes P-polarized light that is emitted from the half-wave plate 19 and enters the condenser lens 20. The condenser lens 20 has a condensing function of condensing the incident light at the point A, and the incident light (P
After being condensed at point A, the polarized light becomes diffused light and strikes the reflecting surface of the concave mirror 23 described later.

【0011】一方、前記分光面16でS偏光と分光され
たP偏光は、偏光ビームスプリッタ15の後面21から
出射し、コンデンサレンズ22に入射するようになって
いる。このコンデンサレンズ22は入射光をA点に集光
する集光作用を有しており、コンデンサレンズ22に入
射した偏光ビームスプリッタ15からの入射光(P偏
光)はA点で集光した後、拡散光となって凹面鏡23の
反射面24に当たるようになっている。
On the other hand, the P-polarized light split into the S-polarized light on the spectral surface 16 is emitted from the rear surface 21 of the polarization beam splitter 15 and is incident on the condenser lens 22. The condenser lens 22 has a condensing function of condensing the incident light at the point A, and the incident light (P-polarized light) incident on the condenser lens 22 from the polarization beam splitter 15 is condensed at the point A. It becomes diffused light and strikes the reflecting surface 24 of the concave mirror 23.

【0012】上記凹面鏡23は液晶表示パネル11の光
入射面に反射面24を対向させて配置されており、コン
デンサレンズ20および22と同じ位置に焦点を有して
いる。また、この凹面鏡23はコンデンサレンズ20お
よび22の焦点距離をそれぞれF1,F2とすると、そ
の曲率半径がR1,R2が焦点距離F1,F2のほぼ1
/2となっている。
The concave mirror 23 is arranged with the reflecting surface 24 facing the light incident surface of the liquid crystal display panel 11, and has a focal point at the same position as the condenser lenses 20 and 22. Further, assuming that the focal lengths of the condenser lenses 20 and 22 are F1 and F2, the concave mirror 23 has radiuses of curvature R1 and R2 of about 1 of the focal lengths F1 and F2.
/ 2.

【0013】このような構成の本実施例では、放物面鏡
14からの光源光を偏光ビームスプリッタ15でP偏光
とS偏光とに分光し、分光されたS偏光を1/2波長板
19でP偏光に変えることにより、液晶表示パネル11
にP偏光のみが入射させることができ、液晶表示パネル
11の光入射側に配置された偏光板でP偏光またはS偏
光のいずれか一方が吸収されることがないので、バック
ライト装置12からの光を液晶表示パネル11にほぼ1
00%入射させることができる。
In this embodiment having such a configuration, the light source light from the parabolic mirror 14 is split into P-polarized light and S-polarized light by the polarization beam splitter 15, and the split S-polarized light is divided into half wavelength plates 19 Liquid crystal display panel 11
Since only P-polarized light can be made incident on the liquid crystal display panel 11 and either the P-polarized light or the S-polarized light is not absorbed by the polarizing plate arranged on the light incident side of the liquid crystal display panel 11, Almost 1 light is transmitted to the liquid crystal display panel 11.
It can be made incident at 00%.

【0014】また、本実施例では1/2波長板19を透
過したP偏光および偏光ビームスプリッタ15を透過し
たP偏光をそれぞれコンデンサレンズ20,22で同一
位置に集光し、これらコンデンサレンズ20,22の集
光点に焦点を有し且つコンデンサレンズ20,22の焦
点距離F1,F2に対して曲率半径R1,R2がほぼ1
/2の凹面鏡23でコンデンサレンズ20,22からの
P偏光を液晶表示パネル11の光入射面に向けて反射す
ることにより、液晶表示パネル11に入射する光源光の
光量がほぼ2倍となるので、液晶表示パネル11に表示
される画像の明るさを倍増させることができる。
Further, in this embodiment, the P-polarized light transmitted through the half-wave plate 19 and the P-polarized light transmitted through the polarization beam splitter 15 are condensed at the same positions by the condenser lenses 20 and 22, respectively. 22 has a focal point at the focal point and has radiuses of curvature R1 and R2 of approximately 1 with respect to focal lengths F1 and F2 of the condenser lenses 20 and 22
By reflecting the P-polarized light from the condenser lenses 20 and 22 toward the light incident surface of the liquid crystal display panel 11 by the / 2 concave mirror 23, the light amount of the light source light incident on the liquid crystal display panel 11 is almost doubled. The brightness of the image displayed on the liquid crystal display panel 11 can be doubled.

【0015】なお、上記実施例では放物面鏡14からの
光源光を偏光方向が互いに90度異なる2つの直線偏光
(P偏光とS偏光)に分光する手段として偏光ビームス
プリッタ15を用いたが、偏光プリズム等を用いても良
い。また、上記実施例では偏光ビームスプリッタ15で
分光されたP偏光およびS偏光のうちS偏光を1/2波
長板19でP偏光に変えるようにしたが、P偏光を1/
2波長板19でS偏光に変えるようにしても良い。
In the above embodiment, the polarization beam splitter 15 is used as a means for splitting the light source light from the parabolic mirror 14 into two linearly polarized lights (P-polarized light and S-polarized light) whose polarization directions are different from each other by 90 degrees. Alternatively, a polarizing prism or the like may be used. Further, in the above-described embodiment, the S-polarized light of the P-polarized light and the S-polarized light split by the polarization beam splitter 15 is changed to the P-polarized light by the ½ wavelength plate 19.
The two-wave plate 19 may be changed to S-polarized light.

【0016】さらに、上記実施例では1/2波長板19
を透過したP偏光および偏光ビームスプリッタ15を透
過したP偏光を集光する手段としてそれぞれコンデンサ
レンズ20,22を用いたが、凹面鏡等を用いても良
い。
Further, in the above embodiment, the half-wave plate 19 is used.
Although the condenser lenses 20 and 22 are used as means for condensing the P-polarized light that has passed through and the P-polarized light that has passed through the polarization beam splitter 15, a concave mirror or the like may be used.

【0017】また、上記実施例では本発明に係るバック
ライト装置を液晶表示装置に適用した場合について説明
したが、液晶プロジェクタ等にも適用できることは説明
するまでもない。
Further, in the above embodiment, the case where the backlight device according to the present invention is applied to the liquid crystal display device has been described, but it goes without saying that it can also be applied to a liquid crystal projector or the like.

【0018】[0018]

【発明の効果】以上説明したように本発明によれば、光
源からの光を液晶表示パネルにほぼ100%入射させる
ことができ、かつ液晶表示パネルに表示される画像の明
るさを高めることのできるバックライト装置を提供でき
る。
As described above, according to the present invention, almost 100% of the light from the light source can be incident on the liquid crystal display panel, and the brightness of the image displayed on the liquid crystal display panel can be increased. It is possible to provide a back light device that can do so.

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

【図1】本発明の一実施例に係るバックライト装置の概
略構成を示す図。
FIG. 1 is a diagram showing a schematic configuration of a backlight device according to an embodiment of the present invention.

【図2】従来のバックライト装置の概略構成を示す図。FIG. 2 is a diagram showing a schematic configuration of a conventional backlight device.

【符号の説明】[Explanation of symbols]

11…液晶表示パネル、12…バックライト装置、13
…光源、14…放物面鏡、15…偏光ビームスプリッ
タ、18…ミラー、19…1/2波長板、20,22…
コンデンサレンズ、23…凹面鏡。
11 ... Liquid crystal display panel, 12 ... Backlight device, 13
... light source, 14 ... parabolic mirror, 15 ... polarization beam splitter, 18 ... mirror, 19 ... 1/2 wave plate, 20, 22 ...
Condenser lens, 23 ... concave mirror.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 光源と、この光源で発生した光源光を前
方に向けて平行に反射する放物面鏡と、この放物面鏡で
反射された光源光を偏光方向が互いに90度異なる2つ
の直線偏光に分光する分光手段と、この分光手段で分光
された2つの直線偏光のうち一方の直線偏光を他方の直
線偏光と同じ偏光方向にする偏光手段と、この偏光手段
からの直線偏光を集光する第1の集光手段と、前記分光
手段で分光された2つの直線偏光のうち他方の直線偏光
を前記第1の集光手段と同じ位置に集光する第2の集光
手段と、これら第1の集光手段および第2の集光手段と
同一位置に焦点を有すると共に第1の集光手段および第
2の集光手段の焦点距離よりも曲率半径の小さい反射面
を有し前記第1の集光手段および第2の集光手段で集光
された直線偏光を液晶表示パネルに向けて反射する凹面
鏡とを具備したことを特徴とするバックライト装置。
1. A light source, a parabolic mirror that reflects the light source light generated by the light source toward the front in parallel, and a light source light reflected by the parabolic mirror whose polarization directions differ from each other by 90 degrees. A linearly polarized light from the linearly polarized light from the linearly polarized light from the linearly polarized light from the linearly polarized light from the linearly polarized light First condensing means for condensing, and second condensing means for condensing the other linearly polarized light of the two linearly polarized light separated by the spectroscopic means at the same position as the first condensing means. Has a focal point at the same position as the first light converging means and the second light converging means, and has a reflecting surface having a radius of curvature smaller than the focal lengths of the first light converging means and the second light converging means. The linearly polarized light collected by the first light collecting means and the second light collecting means is And a concave mirror that reflects toward the crystal display panel.
JP4184141A 1992-07-10 1992-07-10 Back light device Pending JPH0627420A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4184141A JPH0627420A (en) 1992-07-10 1992-07-10 Back light device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4184141A JPH0627420A (en) 1992-07-10 1992-07-10 Back light device

Publications (1)

Publication Number Publication Date
JPH0627420A true JPH0627420A (en) 1994-02-04

Family

ID=16148090

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4184141A Pending JPH0627420A (en) 1992-07-10 1992-07-10 Back light device

Country Status (1)

Country Link
JP (1) JPH0627420A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6239851B1 (en) 1995-10-12 2001-05-29 Ibm Corporation Planar light source device having polarization separator formed of two sheets with mating triangular prisms and different indices of refraction

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6239851B1 (en) 1995-10-12 2001-05-29 Ibm Corporation Planar light source device having polarization separator formed of two sheets with mating triangular prisms and different indices of refraction

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