JP2002100224A - Point-to-line light source converting light guide body - Google Patents

Point-to-line light source converting light guide body

Info

Publication number
JP2002100224A
JP2002100224A JP2000288567A JP2000288567A JP2002100224A JP 2002100224 A JP2002100224 A JP 2002100224A JP 2000288567 A JP2000288567 A JP 2000288567A JP 2000288567 A JP2000288567 A JP 2000288567A JP 2002100224 A JP2002100224 A JP 2002100224A
Authority
JP
Japan
Prior art keywords
light source
light
point
line
light guide
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
JP2000288567A
Other languages
Japanese (ja)
Inventor
Shinichiro Ochiai
真一郎 落合
Atsushi Togo
篤史 東後
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.)
SHIMADA PREC KK
SHIMADA PRECISION KK
Original Assignee
SHIMADA PREC KK
SHIMADA PRECISION KK
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 SHIMADA PREC KK, SHIMADA PRECISION KK filed Critical SHIMADA PREC KK
Priority to JP2000288567A priority Critical patent/JP2002100224A/en
Publication of JP2002100224A publication Critical patent/JP2002100224A/en
Pending legal-status Critical Current

Links

Landscapes

  • Planar Illumination Modules (AREA)
  • Light Guides In General And Applications Therefor (AREA)
  • Diffracting Gratings Or Hologram Optical Elements (AREA)
  • Liquid Crystal (AREA)
  • Non-Portable Lighting Devices Or Systems Thereof (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a point-to-line light source converting light guide body which can effectively convert a point light source to a line light source having an even brightness while realizing cost reduction and size reduction and which can be preferably used as a line light source for an end face of a light guide plate. SOLUTION: Light from point light sources 5a and 5b are introduced into a transparent rod-like body via both end faces 1c and 1d. A diffraction grating is provided on a side face 1b of a transparent rod-like body. The diffraction grating diffracts incident light I so that the light is emitted from another side face 1b. A grating part 3 and a non-grating part 4 comprise a unit width W and plural diffraction grating parts 3 are provided with certain spacing. The ratio between the width of the grating part and the width of the non-grating part within each unit width W is changed so that the brightness at the other side face 1b is high and uniform.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、液晶のバックライ
トやフロントライトなどに用いられる点−線光源変換導
光体、より詳しくは、点光源から高輝度で均一な線光源
を得るため表面に回折格子を設けた点−線光源変換導光
体に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a point-to-line light source conversion light guide used for a backlight or front light of a liquid crystal, and more particularly to a surface light source for obtaining a high-intensity and uniform line light source from a point light source. The present invention relates to a point-to-line light source conversion light guide provided with a diffraction grating.

【0002】[0002]

【従来の技術】従来、均一な輝度の面光源を得る発光装
置として、例えば図5に示すようなものが知られている
(特開平7−11771号公報)。この発光装置は、筐体
31内の両側に背面に反射ミラー32をもち、前面にレ
ンズフィルム33をもつ冷陰極管34からなる第1,第
2の光源ユニット35a,35bを図5の紙面に垂直な方
向に設け、両光源ユニット35a,35b間の後端、前端
を、逆V字状断面をもつ反射板36と反射シート37と
第1のプリズムアレイ板38、V字状断面をもつ第2の
プリズムアレイ板39で夫々覆う一方、第2のプリズム
アレイ板39の前面に、V字状断面をもつ第1のレンズ
フィルム40と、透明板41、拡散板42、第2のレンズ
フィルム43からなる光放射部材44とを順次設けてな
る。第1,第2のプリズムアレイ板38,39の対向する
表面の各プリズムは、夫々頂角90°,120°の三角形断
面を有して前者の稜線が紙面と平行に、後者の稜線が紙
面と垂直に延びている。
2. Description of the Related Art Conventionally, as a light emitting device for obtaining a surface light source having uniform luminance, for example, a light emitting device as shown in FIG. 5 is known.
(Japanese Unexamined Patent Publication No. 7-11771). In this light emitting device, first and second light source units 35a and 35b each having a reflection mirror 32 on the rear surface on both sides in the housing 31 and a cold cathode tube 34 having a lens film 33 on the front surface are shown in FIG. Provided in a vertical direction, the rear end and the front end between the two light source units 35a and 35b are provided with a reflecting plate 36 and a reflecting sheet 37 having an inverted V-shaped cross section, a first prism array plate 38, and a first having a V-shaped cross section. A first lens film 40 having a V-shaped cross section, a transparent plate 41, a diffusion plate 42, and a second lens film 43 on the front surface of the second prism array plate 39, respectively. And a light emitting member 44 composed of Each of the prisms on the opposing surfaces of the first and second prism array plates 38 and 39 has a triangular cross section with apex angles of 90 ° and 120 °, respectively, and the former ridge line is parallel to the paper surface and the latter ridge line is the paper surface. And extend vertically.

【0003】この発光装置では、光源ユニット35a,3
5bからレンズフィルム33を通って出た光が、図中の
矢印で示すように、第1のプリズムアレイ板38で反射
され、次いで第2のプリズムアレイ板39を通って略平
行光となって、第1のレンズフィルム40を経て光放射
部材44に入射し、この光放射部材の各層を通る間に多
方向へ分散され、第2のレンズフィルム43の全面から
均一に出射するので、均一な輝度の面光源が得られる。
In this light emitting device, the light source units 35a, 35
The light exiting from the lens 5b through the lens film 33 is reflected by the first prism array plate 38, and then becomes substantially parallel light through the second prism array plate 39, as shown by the arrow in the drawing. The light enters the light emitting member 44 via the first lens film 40, is dispersed in multiple directions while passing through each layer of the light emitting member, and is uniformly emitted from the entire surface of the second lens film 43. A bright surface light source is obtained.

【0004】[0004]

【発明が解決しようとする課題】ところが、上記従来の
発光装置は、第1,第2のプリズムアレイ板38,39に
多数のプリズムがあるとはいえ、その一辺が例えば0.16
mmと光の波長に比べて相当大きいものであるうえ、各プ
リズムが協同することなく個別に光を純幾何光学的に全
反射または屈折するものであるため、出射面の輝度を全
体に高めようとすると、各プリズムの谷間にあたる箇所
で乱反射が起きて出射光量が減り、出射面である第2の
レンズフィルム43面に極端な明暗のコントラストが生
じるという問題がある。また、上記従来の発光装置は、
反射ミラー32、レンズフィルム33、冷陰極管34から
なる1対の光源ユニット35a,35b、2つのプリズム
アレイ板38,39、2つのレンズフィルム40,43、
透明板41、拡散板42、反射板36など多数の部材で
複雑に構成されているため、これら光媒体を通る間の光
損失も大きく、線光源の発生光量を高効率で面照明に変
換できないうえ、製造コストの低減および装置の軽量化
や薄型化が難しいという問題がある。ここで、装置を小
型化すべく線光源である冷陰極管34に代えて、点光源
である発光ダイオードなどを使おうとすると、上述の明
暗のコントラストや光路中の光損失が原因で、十分な輝
度の満足な均一線光源を得ることができない。
However, in the above-mentioned conventional light emitting device, although the first and second prism array plates 38 and 39 have a large number of prisms, one side thereof is, for example, 0.16.
mm, which is considerably larger than the wavelength of light, and since each prism individually reflects or totally reflects or refracts light in pure geometrical optics without cooperating, increase the brightness of the exit surface as a whole. In this case, there is a problem that irregular reflection occurs at a position corresponding to the valley of each prism and the amount of emitted light is reduced, resulting in an extremely bright and dark contrast on the surface of the second lens film 43 which is the exit surface. In addition, the above-mentioned conventional light emitting device,
A pair of light source units 35a and 35b including a reflection mirror 32, a lens film 33, and a cold cathode tube 34, two prism array plates 38 and 39, two lens films 40 and 43,
Since it is composed of a large number of members such as the transparent plate 41, the diffusion plate 42, and the reflection plate 36, a large amount of light is lost while passing through these optical media, and the amount of light generated by the linear light source cannot be converted to surface illumination with high efficiency. In addition, there is a problem that it is difficult to reduce the manufacturing cost and reduce the weight and thickness of the device. Here, if an attempt is made to use a light emitting diode or the like as a point light source in place of the cold cathode tube 34 as a line light source in order to reduce the size of the device, sufficient brightness due to the above-mentioned contrast between light and dark and light loss in the optical path will be caused. Cannot obtain a satisfactory uniform line light source.

【0005】そこで、本発明の目的は、光の幾何光学的
性質を利用した従来のプリズムによる全反射や屈折でな
く、微細加工の難しさなどから今まで用いられることが
なかった回折格子による光の波動的性質に基づく回折現
象を利用して、コストダウンと小型化を図りつつ、従来
より遥かに高効率に点光源を均一な輝度の線光源に変換
でき、さらには導光板の端面の線光源として利用すれば
好適な点−線光源変換導光体を提供することにある。
Accordingly, an object of the present invention is not to provide total reflection or refraction by a conventional prism utilizing the geometrical optical properties of light, but to use a diffraction grating which has not been used until now due to the difficulty of fine processing. By utilizing the diffraction phenomena based on the wave dynamics of a point light source, it is possible to convert a point light source into a line light source with uniform brightness at a much higher efficiency than before, while reducing costs and miniaturization. An object of the present invention is to provide a point-to-line light source conversion light guide suitable for use as a light source.

【0006】[0006]

【課題を解決するための手段】上記目的を達成するた
め、本発明の点光源を線光源に変換する点−線光源変換
導光体は、矩形断面をもつ透明な棒状体からなり、この
棒状体の一方の側面または少なくとも一端面から点光源
の光が入射するとともに、上記棒状体の一方の側面また
は他方の側面に、上記点光源から入射した光を上記他方
の側面から出射するように回折させる回折格子が設けら
れ、この回折格子の断面形状または単位幅における非格
子部幅に対する格子部幅の割合の少なくとも1つが、上
記他方の側面における輝度が増大し、かつ均一化される
ように変化せしめられていることを特徴とする。
To achieve the above object, a point-to-line light source conversion light guide for converting a point light source to a line light source according to the present invention comprises a transparent rod having a rectangular cross section. Light from a point light source enters from one side surface or at least one end surface of the body, and is diffracted onto one side surface or the other side surface of the rod-like body so that light incident from the point light source exits from the other side surface. A diffraction grating is provided, and at least one of the cross-sectional shape of the diffraction grating or the ratio of the grating portion width to the non-grating portion width in a unit width is changed so that the brightness on the other side surface is increased and uniformized. It is characterized by being hampered.

【0007】図1に例示するように、透明な棒状体から
なる導光板1の一方の側面1aに、一例として間隔dで
回折格子2(刻線溝)が加工されている場合、導光板1の
一端面1cから側面1aに向けて入射した点光源からの光
Iは、上記回折格子2によって矢印の如く他方の側面1
bに向かって回折されるが、入射光Iと回折光Dの間に
は、入射角をi、回折角をθ、光の波長をλ、mを整数と
して、次式(1)が成立する。 (sini−sinθ)=±m(λ/d) …(1) 図中のD1,D2,D3は、上式(1)中のmを夫々1,2,3と
したときの回折光の方向を示している。側面1aの回折
格子2に対する入射光Iの入射角は、臨界角φ(例えば
アクリル製導光板の場合,φ=42゜)よりも大きいので、
1次の回折光D1は入射角iに近い回折角θ1で、2次の
回折光D2はθ1よりも狭い回折角θ2で、3次の回折光
3はθ2よりも狭い回折角θ3で、側面1aにおいて夫々
反射型の回折をして他方の側面1bに向かう。他方の側
面1bに対する1,2次の回折光の入射角は臨界角φより
も大きいので、1,2次の回折光D1,D2は他方の側面1
bで全反射されて導光板1内を更に遠方へ導かれるが、
3次以上の高次の回折光D3,…は、その入射角よりも大
きい出射角で屈折して他方の側面1bから前方へ出てい
くので、高次の回折光D3,…によって他方の側面1bが
明るく照らされ、これによって線光源が得られる。
As shown in FIG. 1, when one side surface 1a of a light guide plate 1 made of a transparent rod is provided with diffraction gratings 2 (cut grooves) at an interval d, for example, the light guide plate 1 The light I from the point light source incident from one end face 1c toward the side face 1a of the
The incident light is diffracted toward b, and the following formula (1) is established between the incident light I and the diffracted light D, where i is the incident angle, θ is the diffraction angle, λ is the wavelength of light, and m is an integer. . (sini−sin θ) = ± m (λ / d) (1) D 1 , D 2 and D 3 in the figure are diffractions when m in the above equation (1) is 1 , 2 , and 3 , respectively. The direction of light is shown. Since the incident angle of the incident light I on the diffraction grating 2 on the side surface 1a is larger than the critical angle φ (for example, in the case of an acrylic light guide plate, φ = 42 °),
The first-order diffracted light D 1 is a diffraction angle θ 1 close to the incident angle i, the second-order diffracted light D 2 is a diffraction angle θ 2 narrower than θ 1 , and the third-order diffracted light D 3 is more than θ 2 At a narrow diffraction angle θ 3 , each of the side surfaces 1 a is subjected to reflection-type diffraction toward the other side surface 1 b. Since the angle of incidence of the first and second order diffracted lights on the other side 1b is larger than the critical angle φ, the first and second order diffracted lights D 1 and D 2 are
The light is totally reflected at b and guided further inside the light guide plate 1,
Since the higher-order diffracted lights D 3 ,... Are refracted at an emission angle larger than the incident angle and go forward from the other side surface 1 b, the higher-order diffracted lights D 3 ,. Is illuminated brightly, thereby obtaining a line light source.

【0008】本発明の回折格子による手法が、各プリズ
ムが協同することなく個別に光を全反射または屈折する
従来のプリズムアレイ板38,39(図5参照)と本質的
に異なる点は、格子間隔dがサブミクロンから数十ミク
ロン(0.1〜10μm)までと上記プリズムの一辺0.16mmに
比して1/100のオーダであり、多数の微細刻線溝間の隣
接する平滑面が協同、相乗して波動としての光を格段に
強く回折でき、格段に高輝度の照光面1bが得られるこ
とである。なお、このような回折格子をもつ導光板は、
例えば、刻線溝を内面に機械加工したり回折格子のホロ
グラム電鋳膜を内張りした金型による成形、あるいは導
光板の裏面に刻線溝を直接機械加工または印刷したり、
印刷やホログラムによる膜を張り付けて作ることができ
る。
The diffraction grating method of the present invention is essentially different from the conventional prism array plates 38, 39 (see FIG. 5) in which each prism totally reflects or refracts light individually without cooperation. The interval d is 1/100 of submicron to several tens of microns (0.1 to 10 μm) compared to 0.16 mm on one side of the above prism. Thus, light as a wave can be remarkably strongly diffracted, and the illuminated surface 1b with remarkably high brightness can be obtained. In addition, the light guide plate having such a diffraction grating,
For example, the engraved groove is machined on the inner surface or molded by a mold with a hologram electroformed film of a diffraction grating, or the engraved groove is directly machined or printed on the back surface of the light guide plate,
It can be made by attaching a film by printing or hologram.

【0009】請求項1の点−線光源変換導光体では、矩
形断面をもつ透明な棒状体の一方または他方の側面に設
けられた回折格子の断面形状または単位幅における非格
子部幅に対する格子部幅の割合の少なくとも1つが、上
記他方の側面1bにおける輝度が増大し、かつ均一化さ
れるように変化せしめられている。即ち、点−線光源変
換導光体1の回折格子2は、例えば、光源側の一端面1
cから離れる、つまり光源から届く光量が減じるにしたが
って、例えば、断面形状が正弦波から鋸歯状に、または
単位幅における非格子部幅に対する格子部幅の割合が次
第に大きくなっている。従って、光源からの光は、光量
の多い一端面1c側で弱く回折され、光量が少ない遠方
側になるほど強く回折されるので、導光体の他方の側面
1bは非常に均一な輝度で照らされる。つまり、上記点
−線光源変換導光体によって、点光源からの光が高輝度
で均一な線光源に変換されるのである。
In the point-to-line light source conversion light guide according to the first aspect of the present invention, the diffraction grating provided on one or the other side surface of the transparent bar having a rectangular cross section has a cross-sectional shape or a non-grating portion width in a unit width. At least one of the ratios of the widths of the portions is changed so that the brightness on the other side surface 1b is increased and uniformized. That is, the diffraction grating 2 of the point-line light source conversion light guide 1 is, for example, one end face 1 on the light source side.
As the distance from c increases, that is, as the amount of light reaching the light source decreases, for example, the cross-sectional shape changes from a sine wave to a saw-tooth shape, or the ratio of the grating portion width to the non-grating portion width in a unit width gradually increases. Therefore, the light from the light source is weakly diffracted on the one end face 1c side where the light quantity is large, and is strongly diffracted on the far side where the light quantity is small, so that the other side face 1b of the light guide is illuminated with very uniform luminance. . That is, the light from the point light source is converted into a high-intensity and uniform line light source by the point-to-line light source conversion light guide.

【0010】請求項2の点−線光源変換導光体は、点光
源の光が棒状体の両端面から入射し、上記回折格子は棒
状体の一方の側面に縦方向に回折溝が設けられ、上記棒
状体の他方の側面に縦方向または横方向にプリズムアレ
イが設けられていることを特徴とする。
According to a second aspect of the present invention, there is provided a point-to-line light source conversion light guide, wherein the light of the point light source enters from both end surfaces of the rod, and the diffraction grating is provided with a diffraction groove in a longitudinal direction on one side surface of the rod. A prism array is provided on the other side surface of the rod in a vertical or horizontal direction.

【0011】請求項2の点−線光源変換導光体では、棒
状体の両端面から入射した点光源の光が、棒状体の一方
の側面に縦方向に設けられた回折格子によって、請求項
1で述べたと同様に回折され、高輝度で均一な線光源と
なって他方の側面から出射するが、その際、大きい出射
角で出射しようとする低次の回折光は、他方の側面に縦
または横方向に設けられたプリズムアレイによって小さ
い出射角に収束される。点光源が棒状体の両側にあるこ
とと、低次の回折光がプリズムアレイによって収束され
ることによって、他方の側面は一層高輝度かつ均一に光
るので、一層効率的な線光源への変換が行なわれる。
In the point-to-line light source conversion light guide according to the second aspect, the light of the point light source incident from both end faces of the rod is provided by a diffraction grating provided on one side surface of the rod in a vertical direction. The light is diffracted in the same manner as described in 1, and becomes a high-intensity and uniform line light source, and is emitted from the other side. At this time, low-order diffracted light to be emitted at a large emission angle is vertically transmitted to the other side. Alternatively, the light is converged to a small emission angle by a prism array provided in the lateral direction. Since the point light source is on both sides of the rod and the low-order diffracted light is converged by the prism array, the other side is illuminated with higher brightness and uniformity. Done.

【0012】請求項3の点−線光源変換導光体は、直角
三角形断面をもつ透明な棒状体からなり、この棒状体の
水平な下面から点光源の光が入射するとともに、上記棒
状体の鉛直な側面に、上記点光源から入射し、棒状体の
斜面で全反射した光を、上記鉛直な側面から出射するよ
うに回折させる回折格子が設けられ、この回折格子の断
面形状または単位幅における非格子部幅に対する格子部
幅の割合の少なくとも1つが、上記鉛直な側面における
輝度が増大し、かつ均一化されるように変化せしめられ
ていることを特徴とする。
According to a third aspect of the present invention, the point-to-line light source conversion light guide is formed of a transparent rod having a right-angled triangular cross section. Light from the point light source enters from a horizontal lower surface of the rod. On the vertical side surface, a diffraction grating that is incident from the point light source and diffracts the light totally reflected on the inclined surface of the rod-shaped body so as to emit from the vertical side surface is provided. At least one of the ratios of the grid width to the non-grid width is changed so that the luminance on the vertical side surface is increased and is made uniform.

【0013】請求項3の点−線光源変換導光体では、直
角三角形断面をもつ透明な棒状体の鉛直な側面に設けら
れた回折格子の断面形状または単位幅における非格子部
幅に対する格子部幅の割合の少なくとも1つが、上記鉛
直な側面における輝度が増大し、かつ均一化されるよう
に変化せしめられていて、棒状体の水平な下面から入射
した点光源の光が、棒状体の斜面で全反射して、鉛直な
側面の回折格子に入射する。この回折格子は、点光源に
対する相対位置によって決まる入射光量に基づいて入射
光量が減じるにしたがって、例えば、断面形状が正弦波
から鋸歯状に、または単位幅における非格子部幅に対す
る格子部幅の割合が変化し、輝度が均一化するようにな
っている。従って、点光源からの光は、回折格子の入射
光量の多い部分で弱く回折され、入射光量が少ない部分
になるほど強く回折されるので、導光体の鉛直の側面
は、非常に均一な輝度で照らされる。つまり、上記点−
線光源変換導光体によって、点光源からの光が高輝度で
均一な線光源に変換されるのである。
According to a third aspect of the present invention, there is provided a light guide for converting light into a point-to-line light source. At least one of the width ratios is changed so that the brightness on the vertical side surface is increased and uniformized, and the light of the point light source incident from the horizontal lower surface of the rod-shaped body is inclined. , And is incident on the diffraction grating on the vertical side surface. As the incident light amount is reduced based on the incident light amount determined by the relative position with respect to the point light source, for example, the diffraction grating has a cross-sectional shape from a sine wave to a sawtooth shape, or a ratio of the grating portion width to the non-grating portion width in a unit width. Is changed, and the luminance is made uniform. Therefore, the light from the point light source is weakly diffracted at the portion where the amount of incident light on the diffraction grating is large, and is strongly diffracted at the portion where the amount of incident light is small, so that the vertical side surface of the light guide has very uniform brightness. Illuminated. That is, the above point-
The light from the point light source is converted into a high-intensity and uniform line light source by the line light source conversion light guide.

【0014】[0014]

【発明の実施の形態】以下、本発明を図示の実施の形態
により詳細に説明する。図2(A),(B)は、本発明の請
求項1に記載の点−線光源変換導光体の一実施形態を示
す夫々斜視図、平面図である。この点−線光源変換導光
体1は、図2(A)に示すように、正方形断面をもつ透明
樹脂製の棒状体からなり、この棒状体の両端面1c,1d
から点光源5a,5b(図2(B)参照)の光Iが入射すると
ともに、棒状体の一方の側面1aに入射した光Iを他方
の側面1bから出射するように回折させる反射型の回折
格子2が設けられている。回折格子2は、図2(A)では
図1と同様に一定格子間隔dで設けられているように描
かれているが、実際には、図2(B)に示す単位幅Wにお
ける非格子部幅に対する格子部幅の割合が、両端面1c,
1dからの到達光量の減少に応じて回折光量が増加する
ように、中央部に近づくに従って次第に大きくなるよう
に設定されている。ここで、単位幅Wとは、1つの格子
部幅3と1つの非格子部幅4との和であり、単位区間の
幅である。図2(B)の導光板1の側面1aには、模式的
に示された単位幅Wを有する14個の区間が設けられ、
格子部幅は各区間の太線部分3、非格子部幅は各区間の
細線部分4で夫々示されており、中央部に近づくほど各
区間での太線部分3の割合、つまり格子部幅が増えてい
ることから、回折光量が増えることが理解できる。な
お、上記区間の数は、説明の便宜上14個としたが、実
際には遥かに多い数で、例えば1例では1000個程度であ
る。また、回折格子2の断面形状および格子間隔dは、
光源の波長λに対して側面1bの照明に寄与する高次の
回折光の全回折光に占める割合が多くなるように設定さ
れている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below in detail with reference to the illustrated embodiments. 2A and 2B are a perspective view and a plan view, respectively, showing one embodiment of the point-to-line light source conversion light guide according to claim 1 of the present invention. As shown in FIG. 2A, the point-to-line light source conversion light guide 1 is made of a transparent resin rod having a square cross section, and both end faces 1c and 1d of the rod.
The light I of the point light sources 5a and 5b (see FIG. 2B) is incident on the rod, and the light I incident on one side 1a of the rod is diffracted so as to be emitted from the other side 1b. A grid 2 is provided. Although the diffraction grating 2 is depicted in FIG. 2A as being provided at a constant grating interval d as in FIG. 1, actually, the non-grating in the unit width W shown in FIG. The ratio of the grid width to the width of the edge is equal to both end faces 1c,
The amount of diffracted light is set to increase as the amount of diffracted light increases as the amount of light reaching from 1d decreases. Here, the unit width W is the sum of one lattice portion width 3 and one non-lattice portion width 4, and is the width of a unit section. On the side surface 1a of the light guide plate 1 in FIG. 2B, 14 sections each having a unit width W schematically shown are provided,
The grid portion width is indicated by the thick line portion 3 of each section, and the non-grid portion width is indicated by the thin line portion 4 of each section. Therefore, it can be understood that the amount of diffracted light increases. Although the number of the sections is set to 14 for convenience of explanation, the number is actually much larger, for example, about 1000 in one example. Further, the cross-sectional shape and the grating interval d of the diffraction grating 2 are
It is set so that the ratio of higher-order diffracted light that contributes to the illumination of the side surface 1b to the total diffracted light with respect to the wavelength λ of the light source increases.

【0015】この実施形態では、格子部3と非格子部4
を各単位幅Wの左右に2分して設けたが、両者を1つの
単位幅中に交互に設けてその単位幅に特定の非格子部幅
に対する格子部幅の割合が得られるようにしてもよい。
また、非格子部幅に対する格子部幅の割合は、必ずしも
図2(B)のように中央部に近づくにつれて漸増させる必
要はなく、他方の側面1bで高くかつ均一な輝度が得ら
れる限り、任意に変化させることができる。この実施形
態では、回折格子2は、格子間隔dが数μmで、内面に
刻線溝を機械加工した金型を用いて導光体と同時に成形
されるが、本発明の回折格子は、間隔dが0.1〜10μ
m、回折格子のホログラム膜を内挿したインモールド成
形、導光板裏面への刻線溝の機械加工、または導光板裏
面への印刷やホログラムによる回折格子膜の張付けによ
っても作成することができる。
In this embodiment, the lattice 3 and the non-grid 4
Are provided on the left and right sides of each unit width W, but they are alternately provided in one unit width so that the unit width can obtain the ratio of the lattice width to the specific non-grid width. Is also good.
Also, the ratio of the grid width to the non-grid width need not be gradually increased as approaching the central portion as shown in FIG. 2B, but may be any value as long as high and uniform brightness can be obtained on the other side surface 1b. Can be changed to In this embodiment, the diffraction grating 2 is formed at the same time as the light guide using a mold having a grating interval d of several μm and a machined groove on the inner surface. d is 0.1 to 10μ
m, it can also be formed by in-mold molding in which a hologram film of a diffraction grating is inserted, machining of a groove on the back surface of the light guide plate, printing on the back surface of the light guide plate, or pasting the diffraction grating film by a hologram.

【0016】上記構成の点−線光源変換導光体1は、次
のように点光源を線光源に変換する。両側の点光源5a,
5bからの光は、両端面1c,1dを経て側面1aに入射
し、側面1aの各単位幅W内の格子部3に設けられた回
折格子に当たると、格子間隔dで隣接する多数の刻線溝
間の鏡面の協同によって回折され、高次の回折光が図2
(B)の矢印で示すように他方の側面1bから外部へ出射
され、低次の回折光が図1の矢印D1の方向へ向かって
他方の側面1bで内部へ全反射する。
The point-to-line light source conversion light guide 1 configured as described above converts a point light source to a line light source as follows. Point light sources 5a on both sides,
The light from 5b is incident on the side surface 1a via both end surfaces 1c and 1d, and hits the diffraction grating provided on the grating portion 3 within each unit width W of the side surface 1a. The diffracted light is diffracted by the cooperation of the mirror surface between the grooves, and the higher-order diffracted light is shown in FIG.
Is emitted from the other side 1b, as shown by arrows in (B) to the outside, the low-order diffracted light is totally reflected into the interior on the other side surface 1b toward the direction of the arrow D 1 of the Figure 1.

【0017】回折格子は、図5の従来例で述べた一辺が
0.16mm程度で光を個別に幾何光学的に全反射する従来の
プリズムアレイに比して、寸法が1/100のオーダで多数
の刻線溝が協同、相乗して波動としての光を特定方向へ
集中的に回折するので、従来例に比して格段に高強度の
回折光が得られる。しかも、回折格子の断面形状および
格子間隔dは、他方の側面1bの照明に寄与する高次の
回折光の全回折光に占める割合が多くなるように設定さ
れるとともに、各単位幅Wにおける非格子部4の幅に対
する格子部3の幅の割合が、両端面1c,1dから中央部
に近づくに従って次第に大きくなるように設定されてい
る。従って、点光源5a,5bからの光を回折によって高
効率に他方の側面1bの照明に利用できるうえ、点光源
から離れるに伴なう光量の減少を回折格子の密度増加で
補償でき、棒状体の他方の側面1bは非常に高くかつ均
一な輝度で照らされる。つまり、点−線光源変換導光体
1によって、点光源5a,5bからの光が高くかつ均一な
輝度の線光源に変換されることになる。また、片側のみ
に点光源がある場合に比して、倍の輝度が得られる。
The diffraction grating has one side described in the conventional example of FIG.
Compared to the conventional prism array, which is about 0.16 mm and totally reflects light individually and geometrically, a large number of grooved grooves cooperate with each other in the order of 1/100, synergistically, and act as a wave in a specific direction. Since the light is diffracted intensively, diffracted light of much higher intensity than in the conventional example can be obtained. In addition, the cross-sectional shape and the grating interval d of the diffraction grating are set so that the ratio of higher-order diffracted light that contributes to the illumination of the other side surface 1b in the total diffracted light increases, and the non- The ratio of the width of the grating portion 3 to the width of the grating portion 4 is set so as to gradually increase from the end surfaces 1c and 1d toward the center. Therefore, the light from the point light sources 5a and 5b can be efficiently used for illuminating the other side surface 1b by diffraction, and the decrease in the amount of light accompanying the separation from the point light source can be compensated for by increasing the density of the diffraction grating. Is illuminated with a very high and uniform brightness. That is, the light from the point light sources 5a and 5b is converted by the point-to-line light source conversion light guide 1 into a line light source having high and uniform luminance. In addition, double brightness can be obtained as compared with a case where a point light source is provided on only one side.

【0018】なお、上記実施形態を含む本発明の点−線
光源変換導光体は、出願人が最近出願した同じく回折格
子を用いたフロントライト導光板(特願2000−27
8456号)の一端面に線光源として用いれば、フロン
トライトユニットひいてはこれによって照明される液晶
ディスプレイの製造コストの低減および軽量化と薄型化
を図りつつ、高くかつ均一な輝度の面光源を提供するこ
とができる。また、回折格子の単位幅Wにおける非格子
部幅に対する格子部幅の割合を増加せずに、回折格子の
断面形状を正弦波から鋸歯状に変化させることによって
も、回折光の強度を高めることができる。
The point-to-line light source conversion light guide of the present invention including the above-described embodiment is a front light light guide plate (Japanese Patent Application No. 2000-27) using a diffraction grating recently applied by the applicant.
No. 8456) as a line light source, it provides a surface light source with high and uniform brightness while reducing the manufacturing cost and reducing the weight and thickness of the front light unit and hence the liquid crystal display illuminated thereby. be able to. It is also possible to increase the intensity of the diffracted light by changing the cross-sectional shape of the diffraction grating from a sine wave to a sawtooth shape without increasing the ratio of the grating portion width to the non-grating portion width in the unit width W of the diffraction grating. Can be.

【0019】図2の点−線光源変換導光体1は、他方の
側面1bに、請求項2に記載されたように縦方向に図示
しないプリズムアレイを設けることもできる。このプリ
ズムアレイは、頂角が鋭角の二等辺三角形が図2(B)の
側面1bに沿って連続的に並んだもので、プリズムアレ
イの稜線は、図2(B)の紙面に垂直な方向、つまり縦方
向に延びる。一方の側面1aの回折格子で回折された低
次の回折光は、既述の如く全反射するような大きな入射
角で他方の側面1bに入射するが、他方の側面1bに上記
プリズムアレイが設けられている場合は、上記大きな入
射角で入射する光束がプリズムアレイによって捕らえら
れて、前方に法線方向へ収束するように出射される。従
って、この点−線光源変換導光体によれば、他方の側面
1bは、一層高輝度かつ均一に光るので、一層効率的な
点光源から線光源への変換を行なうことができる。な
お、プリズムアレイをその稜線が横(水平)方向に延びる
ように設けることもでき、これによっても同様の作用効
果を奏することができる。
In the point-to-line light source conversion light guide 1 shown in FIG. 2, a prism array (not shown) may be provided in the vertical direction on the other side surface 1b. In this prism array, an isosceles triangle having an acute vertex angle is continuously arranged along the side surface 1b in FIG. 2B, and the ridge line of the prism array is in a direction perpendicular to the plane of FIG. 2B. That is, it extends in the vertical direction. The low-order diffracted light diffracted by the diffraction grating on one side 1a is incident on the other side 1b at such a large incident angle as to be totally reflected as described above, but the prism array is provided on the other side 1b. In this case, the light beam incident at the large incident angle is caught by the prism array and emitted forward so as to converge in the normal direction. Therefore, according to this point-to-line light source conversion light guide, the other side surface 1b emits light with higher luminance and more uniformly, so that a more efficient conversion from a point light source to a line light source can be performed. In addition, the prism array can be provided so that the ridge line extends in the horizontal (horizontal) direction, so that the same operation and effect can be obtained.

【0020】図3は、請求項1に記載の点−線光源変換
導光体の他の実施形態を示す斜視図である。この点−線
光源変換導光体11は、図2の両端面にある点光源5a,
5bを一方の側面11aの後方に置き換えて4個にすると
ともに、一方の側面11aの回折格子を透過型にした点
が図2の実施形態と異なる。反射型と透過型の回折格子
のレリーフ形状は、Maxwell の方程式から導かれる回折
の理論式に基づいて、所望の回折を起こさせるような計
算をコンピュータを用いて行なうことにより求めること
ができ、その際、反射率を変化させることができる。ま
た、側面1aの各単位幅Wにおける非格子部幅に対する
格子部幅の割合は、4つの点光源5に対する各単位幅W
の相対位置によって決まる点光源からの受光量が減じる
にしたがって、次第に大きくなっている。
FIG. 3 is a perspective view showing another embodiment of the point-to-line light source conversion light guide according to the first aspect. The point-to-line light source conversion light guide 11 includes point light sources 5a,
This embodiment differs from the embodiment shown in FIG. 2 in that 5b is replaced behind one side surface 11a to make four, and the diffraction grating on one side surface 11a is of a transmission type. The relief shapes of the reflection type and transmission type diffraction gratings can be obtained by performing calculations using a computer to cause desired diffraction based on the theoretical equations of diffraction derived from Maxwell's equation. In this case, the reflectance can be changed. The ratio of the grid width to the non-grid width in each unit width W of the side surface 1a is expressed by the unit width W for the four point light sources 5.
Are gradually increased as the amount of light received from the point light source, which is determined by the relative position of the light source, decreases.

【0021】この実施形態によれば、点光源5からの光
は、側面11aの受光量の多い単位幅部で弱く、受光量
の少ない単位幅部で強く夫々回折されるので、他方の側
面1bは非常に均一な輝度で照らされるから、点光源5,
5,…からの光を高輝度で均一な線光源に変換すること
ができる。なお、この実施形態の他方の側面11bに
も、既に述べたと同様に縦方向または横方向にプリズム
アレイを設けることができ、これによって一層効率的な
点光源から線光源への変換を行なうことができる。
According to this embodiment, the light from the point light source 5 is weakly diffracted at the unit width portion of the side surface 11a where the amount of received light is large and strongly diffracted at the unit width portion where the amount of received light is small. Is illuminated with very uniform brightness, so point light sources 5,
, Can be converted into a high-intensity and uniform line light source. The other side surface 11b of this embodiment can be provided with a prism array in the vertical or horizontal direction in the same manner as described above, thereby making it possible to perform more efficient conversion from a point light source to a line light source. it can.

【0022】図4は、請求項3に記載の点−線光源変換
導光体の一実施形態を示す斜視図である。この点−線光
源変換導光体21は、直角三角形断面をもつ透明な棒状
体からなり、この棒状体の水平な下面21aから3個の
点光源5の光が入射するとともに、上記棒状体の鉛直な
側面21cに、点光源5から入射し、棒状体の斜面21b
で全反射した光を、鉛直な側面21cから出射するよう
に回折させる透過型の回折格子が設けられている。この
回折格子も、図3の実施形態と同様、簡略化して描かれ
ているが、側面21cの各単位幅Wにおける非格子部幅
に対する格子部幅の割合が、3つの点光源5に対する各
単位幅Wの相対位置によって決まる点光源からの受光量
が減じるにしたがって、それを補償するように設定され
ている。
FIG. 4 is a perspective view showing an embodiment of the point-to-line light source conversion light guide according to the third aspect. The point-to-line light source conversion light guide 21 is formed of a transparent rod having a right-angled triangular cross section. Light from the three point light sources 5 is incident from a horizontal lower surface 21a of the rod, and the rod-shaped light is converted to a light. The incident light from the point light source 5 is incident on the vertical side surface 21c, and the inclined surface 21b
There is provided a transmission type diffraction grating for diffracting the light totally reflected by the light source so as to exit from the vertical side surface 21c. This diffraction grating is also illustrated in a simplified manner as in the embodiment of FIG. 3, but the ratio of the grating portion width to the non-grating portion width in each unit width W of the side surface 21c is different for each unit for the three point light sources 5. As the amount of light received from the point light source, which is determined by the relative position of the width W, decreases, the amount is compensated for.

【0023】この実施形態は、点光源5からの光が棒状
体に入射し、次いで全反射された後に前面の回折格子に
入る点が、図3の点光源5からの光が直接背面の回折格
子に入る実施形態と相違する。しかし、回折格子が同じ
透過型であるので、その回折作用自体は何ら異ならな
い。従って、この実施形態でも、点光源5,5,…からの
光を高輝度で均一な線光源に変換することができるとと
もに、点−線光源変換導光体の背部に空間的余裕がない
フロントライトユニットなどの導光装置に、好適に組み
込むことができる。
In this embodiment, the point at which light from the point light source 5 enters the rod-shaped body and then enters the front diffraction grating after being totally reflected is that light from the point light source 5 in FIG. Differs from the embodiment in which a grid is entered. However, since the diffraction gratings are of the same transmission type, the diffraction action itself does not differ at all. Therefore, also in this embodiment, the light from the point light sources 5, 5,... Can be converted into a high-intensity and uniform line light source, and the front light source has no space at the back of the point-line light source conversion light guide. It can be suitably incorporated in a light guide device such as a light unit.

【0024】[0024]

【発明の効果】以上の説明で明らかなように、本発明の
請求項1に記載の点−線光源変換導光体は、一方の側面
または少なくとも一端面から点光源の光が入射する矩形
断面をもつ透明な棒状体の一方または他方の側面に、入
射光を回折して他方の側面から出射させる回折格子を設
け、その回折格子の断面形状または単位幅における非格
子部幅に対する格子部幅の割合の少なくとも1つを、他
方の側面における輝度が増大し、かつ均一化されるよう
に変化させているので、点光源から遠方の光量不足が回
折格子の密度増大で補償され、指向性の強い強度な回折
光の出射によって、他方の側面において高輝度で均一な
線光源が得られ、小型・軽量化と製造コストの低減を図
りつつ、フロントライトユニットなどの導光装置に都合
好く適用することができる。
As is apparent from the above description, the point-to-line light source conversion light guide according to claim 1 of the present invention has a rectangular cross section on which light from the point light source enters from one side surface or at least one end surface. A diffraction grating that diffracts incident light and emits it from the other side surface is provided on one or the other side surface of the transparent rod-shaped body having a cross-sectional shape or a non-grating portion width in a unit width. Since at least one of the ratios is changed so that the brightness on the other side is increased and made uniform, the lack of light amount far from the point light source is compensated by the increase in the density of the diffraction grating, and the directivity is high. By emitting high-intensity diffracted light, a high-intensity and uniform line light source can be obtained on the other side, and can be conveniently applied to a light guide device such as a front light unit while reducing the size, weight, and manufacturing cost. thing It can be.

【0025】本発明の請求項2に記載の点−線光源変換
導光体は、点光源の光が棒状体の両端面から入射し、回
折格子は棒状体の一方の側面に縦方向に設けられ、棒状
体の他方の側面に縦方向または横方向にプリズムアレイ
(稜線)が設けられているので、請求項1の上記作用効果
に加えて、プリズムアレイが大きい出射角で出射しよう
とする低次の回折光を小さい出射角に収束するから、他
方の側面が一層高輝度かつ均一に照らされて、一層効率
的な線光源への変換を行なうことができる。
According to a second aspect of the present invention, there is provided a point-to-line light source conversion light guide, wherein the light of the point light source is incident from both end faces of the rod, and the diffraction grating is provided on one side surface of the rod in a vertical direction. Vertical or horizontal prism array on the other side of the rod
Since the (ridge line) is provided, the prism array converges a low-order diffracted light that is to be emitted at a large exit angle to a small exit angle in addition to the above-described function and effect of claim 1, so that the other side surface is A more efficient conversion to a linear light source can be performed with higher luminance and uniform illumination.

【0026】本発明の請求項3に記載の点−線光源変換
導光体は、水平な下面から点光源の光が入射する直角三
角形断面をもつ透明な棒状体の鉛直な側面に、斜面で全
反射された入射光を回折して鉛直な側面から出射させる
回折格子を設け、その回折格子の断面形状または単位幅
における非格子部幅に対する格子部幅の割合の少なくと
も1つを、他方の側面における輝度が増大し、かつ均一
化されるように変化させているので、点光源から遠方の
光量不足が回折格子の密度増大で補償され、指向性の強
い強度な回折光の出射によって、鉛直な側面において高
輝度で均一な線光源が得られ、小型・軽量化と製造コス
トの低減を図りつつ、フロントライトユニットなどの導
光装置に都合好く適用することができる。
According to a third aspect of the present invention, there is provided a point-to-line light source conversion light guide, wherein a transparent rod-like body having a right-angled triangular cross section on which light from the point light source enters from a horizontal lower surface is formed by a slope. A diffraction grating for diffracting the totally reflected incident light and emitting the diffracted light from a vertical side surface, wherein at least one of the sectional shape of the diffraction grating or the ratio of the grating portion width to the non-grating portion width in a unit width is set to the other side surface; Is increased so as to be uniform, so that the shortage of the light amount far from the point light source is compensated by the increase in the density of the diffraction grating, and by the emission of the diffracted light having strong directivity, the vertical A high-intensity and uniform line light source can be obtained on the side surface, and it can be conveniently applied to a light guide device such as a front light unit while reducing the size and weight and reducing the manufacturing cost.

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

【図1】 点−線光源変換導光体の側面に設けられた回
折格子による光の回折を原理的に示す模式図である。
FIG. 1 is a schematic view showing the principle of light diffraction by a diffraction grating provided on a side surface of a point-to-line light source conversion light guide.

【図2】 本発明の請求項1に記載の点−線光源変換導
光体の一実施形態を示す斜視図および平面図である。
FIG. 2 is a perspective view and a plan view showing an embodiment of a point-to-line light source conversion light guide according to claim 1 of the present invention.

【図3】 本発明の請求項1に記載の点−線光源変換導
光体の他の実施形態を示す斜視図である。
FIG. 3 is a perspective view showing another embodiment of the point-to-line light source conversion light guide according to claim 1 of the present invention.

【図4】 本発明の請求項3に記載の点−線光源変換導
光体の一実施形態を示す斜視図である。
FIG. 4 is a perspective view showing an embodiment of a point-to-line light source conversion light guide according to claim 3 of the present invention.

【図5】 従来の発光装置を示す断面図である。FIG. 5 is a cross-sectional view showing a conventional light emitting device.

【符号の説明】[Explanation of symbols]

1,11,21 点−線光源変換導光体 1a,11a 一方の側面 1b,11b 他方の側面 1c,11c 一端面 1d,11d 他端面 2 回折格子 W 単位幅 3 格子部 4 非格子部 5,5a,5b 点光源 21a 水平な下面 21b 斜面 21c 鉛直な側面 I 点光源からの光 1,11,21 Point-to-line light source conversion light guide 1a, 11a One side 1b, 11b The other side 1c, 11c One end 1d, 11d The other end 2 Diffraction grating W Unit width 3 Grating portion 4 Non-grating portion 5, 5a, 5b Point light source 21a Horizontal lower surface 21b Slope 21c Vertical side light from I point light source

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.7 識別記号 FI テーマコート゛(参考) // F21S 2/00 F21Y 101:02 G02F 1/13357 F21S 1/00 D F21Y 101:02 G02F 1/1335 530 Fターム(参考) 2H038 AA54 BA01 2H049 AA07 AA13 AA25 AA31 AA43 AA55 AA65 AA66 CA05 CA08 CA09 CA15 2H091 FA19Z FA21Z FA23Z FA29Z FA41Z FD03 LA12 LA18──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. 7 Identification symbol FI Theme coat ゛ (reference) // F21S 2/00 F21Y 101: 02 G02F 1/13357 F21S 1/00 D F21Y 101: 02 G02F 1/1335 530 F term (reference) 2H038 AA54 BA01 2H049 AA07 AA13 AA25 AA31 AA43 AA55 AA65 AA66 CA05 CA08 CA09 CA15 2H091 FA19Z FA21Z FA23Z FA29Z FA41Z FD03 LA12 LA18

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 点光源を線光源に変換する点−線光源変
換導光体において、 上記点−線光源変換導光体は、矩形断面をもつ透明な棒
状体からなり、この棒状体の一方の側面または少なくと
も一端面から点光源の光が入射するとともに、上記棒状
体の一方の側面または他方の側面に、上記点光源から入
射した光を上記他方の側面から出射するように回折させ
る回折格子が設けられ、この回折格子の断面形状または
単位幅における非格子部幅に対する格子部幅の割合の少
なくとも1つが、上記他方の側面における輝度が増大
し、かつ均一化されるように変化せしめられていること
を特徴とする点−線光源変換導光体。
1. A point-to-line light source conversion light guide for converting a point light source to a line light source, wherein the point-to-line light source conversion light guide comprises a transparent rod having a rectangular cross section. And a diffraction grating that diffracts the light incident from the point light source on one side or the other side of the rod-shaped body so that the light is emitted from the other side. At least one of the cross-sectional shape of the diffraction grating or the ratio of the grating portion width to the non-grating portion width in the unit width is changed so that the brightness on the other side surface is increased and uniformized. A point-to-line light source conversion light guide.
【請求項2】 請求項1に記載の点−線光源変換導光体
において、上記点光源の光は棒状体の両端面から入射
し、上記回折格子は棒状体の一方の側面に縦方向に回折
溝が設けられ、上記棒状体の他方の側面に縦方向または
横方向にプリズムアレイが設けられていることを特徴と
する点−線光源変換導光体。
2. The point-to-line light source conversion light guide according to claim 1, wherein the light of the point light source is incident from both end faces of the rod, and the diffraction grating is vertically arranged on one side surface of the rod. A point-to-line light source conversion light guide, wherein a diffraction groove is provided, and a prism array is provided in the vertical or horizontal direction on the other side surface of the rod-shaped body.
【請求項3】 点光源を線光源に変換する点−線光源変
換導光体において、 上記点−線光源変換導光体は、直角三角形断面をもつ透
明な棒状体からなり、この棒状体の水平な下面から点光
源の光が入射するとともに、上記棒状体の鉛直な側面
に、上記点光源から入射し、棒状体の斜面で全反射した
光を、上記鉛直な側面から出射するように回折させる回
折格子が設けられ、この回折格子の断面形状または単位
幅における非格子部幅に対する格子部幅の割合の少なく
とも1つが、上記鉛直な側面における輝度が増大し、か
つ均一化されるように変化せしめられていることを特徴
とする点−線光源変換導光体。
3. A point-to-line light source conversion light guide for converting a point light source to a line light source, wherein the point-to-line light source conversion light guide comprises a transparent rod having a right-angled triangular cross section. While the light of the point light source is incident from the horizontal lower surface, the light incident from the point light source on the vertical side surface of the rod is diffracted so that the light totally reflected on the inclined surface of the rod is emitted from the vertical side surface. A diffraction grating is provided, and at least one of the cross-sectional shape of the diffraction grating or the ratio of the grating portion width to the non-grating portion width in a unit width is changed so that the luminance on the vertical side surface is increased and uniformized. A point-to-line light source conversion light guide, comprising: a light source;
JP2000288567A 2000-09-22 2000-09-22 Point-to-line light source converting light guide body Pending JP2002100224A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000288567A JP2002100224A (en) 2000-09-22 2000-09-22 Point-to-line light source converting light guide body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000288567A JP2002100224A (en) 2000-09-22 2000-09-22 Point-to-line light source converting light guide body

Publications (1)

Publication Number Publication Date
JP2002100224A true JP2002100224A (en) 2002-04-05

Family

ID=18772140

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000288567A Pending JP2002100224A (en) 2000-09-22 2000-09-22 Point-to-line light source converting light guide body

Country Status (1)

Country Link
JP (1) JP2002100224A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004008023A1 (en) * 2002-07-11 2004-01-22 Sharp Kabushiki Kaisha Light guide device and display device
JP2011099972A (en) * 2009-11-05 2011-05-19 Toppan Printing Co Ltd Optical member, and el display device and el lighting system using the same
JP2013205512A (en) * 2012-03-27 2013-10-07 Dainippon Printing Co Ltd Light diffusion film, polarization plate, image forming apparatus, and display device

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04322204A (en) * 1991-04-23 1992-11-12 Sumitomo Chem Co Ltd Plane lighting device
JPH09325218A (en) * 1996-05-31 1997-12-16 Shimada Precision Kk Light guide plate and light guide assembly
JPH1064321A (en) * 1996-08-22 1998-03-06 Omron Corp Light guide device, liquid crystal display device, and electronic device
JPH1114835A (en) * 1997-06-20 1999-01-22 Shimada Precision Kk Light emission display plate
JPH11287993A (en) * 1998-04-01 1999-10-19 Shimada Precision Kk Light guide plate for spot light source
JP2000011723A (en) * 1998-06-29 2000-01-14 Minebea Co Ltd Sheet-like lighting system

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04322204A (en) * 1991-04-23 1992-11-12 Sumitomo Chem Co Ltd Plane lighting device
JPH09325218A (en) * 1996-05-31 1997-12-16 Shimada Precision Kk Light guide plate and light guide assembly
JPH1064321A (en) * 1996-08-22 1998-03-06 Omron Corp Light guide device, liquid crystal display device, and electronic device
JPH1114835A (en) * 1997-06-20 1999-01-22 Shimada Precision Kk Light emission display plate
JPH11287993A (en) * 1998-04-01 1999-10-19 Shimada Precision Kk Light guide plate for spot light source
JP2000011723A (en) * 1998-06-29 2000-01-14 Minebea Co Ltd Sheet-like lighting system

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004008023A1 (en) * 2002-07-11 2004-01-22 Sharp Kabushiki Kaisha Light guide device and display device
JP2011099972A (en) * 2009-11-05 2011-05-19 Toppan Printing Co Ltd Optical member, and el display device and el lighting system using the same
JP2013205512A (en) * 2012-03-27 2013-10-07 Dainippon Printing Co Ltd Light diffusion film, polarization plate, image forming apparatus, and display device

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