TWI728110B - A projection screen - Google Patents

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TWI728110B
TWI728110B TW106115424A TW106115424A TWI728110B TW I728110 B TWI728110 B TW I728110B TW 106115424 A TW106115424 A TW 106115424A TW 106115424 A TW106115424 A TW 106115424A TW I728110 B TWI728110 B TW I728110B
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light
screen
incident
angle
light incident
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TW106115424A
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TW201740180A (en
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胡飛
周宇軒
李屹
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大陸商深圳光峰科技股份有限公司
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    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/54Accessories
    • G03B21/56Projection screens
    • G03B21/60Projection screens characterised by the nature of the surface
    • G03B21/602Lenticular screens
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B21/00Projectors or projection-type viewers; Accessories therefor
    • G03B21/54Accessories
    • G03B21/56Projection screens
    • G03B21/60Projection screens characterised by the nature of the surface

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  • General Physics & Mathematics (AREA)
  • Overhead Projectors And Projection Screens (AREA)
  • Optical Elements Other Than Lenses (AREA)

Abstract

The present invention provides a projection screen, which comprising a screen and a surface structure arranged on the projection surface of the screen. The surface structure comprises a matrix and a transparent microstructure array and a reflective layer arranged in a matrix. The transparent microstructure comprises a light incident surface and a light reflection surface. The light incident surface has a convergence and has a preset focal length in which the width in the first direction is a preset value; the light reflecting surface is a curved surface within a focal length range of the light incident surface for adjusting the exit light in the second direction and the plane of the screen In the direction of the first direction and the second direction parallel to the screen plane and perpendicular to each other. The projection screen surface structure can adjust the exit angle range of the screen exit light so that the maximum outgoing angle of the outgoing light can be greater than its incident angle and can control the incident light of a certain angle of incidence to be reflected by the screen after a predetermined angle range the effect of gain on the screen exit light within the preset angle range.

Description

一種投影螢幕 A projection screen

本發明涉及光學應用技術領域,特別是涉及一種投影螢幕。 The present invention relates to the field of optical application technology, in particular to a projection screen.

投影螢幕,應用於投影系統中用於放映投影圖像,投影螢幕與投影機的相對位置一般固定,發出的投射光近似為以一定角度的平行光入射到螢幕,入射光經螢幕發生反射,被反射的光線進入人眼,從而觀看者可觀看到圖像。 Projection screens are used in projection systems to project projected images. The relative position of the projection screen and the projector is generally fixed. The projected light is approximately incident on the screen at a certain angle of parallel light, and the incident light is reflected by the screen. The reflected light enters the human eye, so that the viewer can see the image.

在投影系統中,觀看者相對投影螢幕的位置往往是固定的。人們希望投影系統顯示在螢幕上圖像的反射光只反射到觀看區域,而減少其它無效區域的反射光,這樣可提高觀看螢幕圖像的亮度。 In the projection system, the position of the viewer relative to the projection screen is often fixed. People hope that the reflected light of the image displayed on the screen by the projection system is only reflected to the viewing area, and the reflected light of other invalid areas is reduced, so that the brightness of the viewing screen image can be improved.

因此,經由上述的說明,有鑑於此,本發明提供一種投影螢幕,能夠調整螢幕出射光的出射角度範圍,實現了對螢幕出射光在預設角度範圍內增益的效果。 Therefore, based on the above description, in view of this, the present invention provides a projection screen capable of adjusting the range of angles of light emitted from the screen, so as to achieve the effect of gaining the light emitted from the screen within a preset angle range.

本發明提供一種投影螢幕,能夠調整螢幕出射光的出射角度範圍,實現了對螢幕出射光在預設角度範圍內增益的效果。 The present invention provides a projection screen, which can adjust the angle range of the light emitted from the screen, and realizes the effect of gaining the light emitted from the screen within a preset angle range.

為實現以上目的,本發明提供一種投影螢幕,包括螢幕本體,還包括設置在該螢幕本體投射面上的表面結構;該表面結構包括矩陣式排布的透明微結構陣列以及反射層,其中該透明微結構包括:對入射光具有會聚作用且具有預設焦距的光入射面,該光入射面的沿第一方向的寬度為預設值,該光入射面用於調整出射光在第一方向與螢幕法線所形成的平面內的方向,使得出射光在該第一方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第一方向與螢幕法線所形成的平面內的入射角;位於該光入射面的焦距範圍內的、曲面形的光反射面,在該光反射面設置有該反射層,該光反射面用於調整出射光在第二方向與螢幕法線所形成的平面內的方向,使得出射光在該第二方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第二方向與螢幕法線所形成的平面內的入射角;該第一方向和該第二方向平行於螢幕平面且相互垂直。 In order to achieve the above objective, the present invention provides a projection screen, including a screen body, and a surface structure arranged on the projection surface of the screen body; the surface structure includes a matrix-arranged transparent microstructure array and a reflective layer, wherein the transparent The microstructure includes: a light incident surface that has a condensing effect on incident light and has a preset focal length, the width of the light incident surface along the first direction is a preset value, and the light incident surface is used to adjust the output light in the first direction and The direction in the plane formed by the screen normal is such that the maximum exit angle of the emitted light in the plane formed by the first direction and the screen normal is greater than that of the incident light in the plane formed by the first direction and the screen normal Incident angle; a curved light reflecting surface located within the focal range of the light incident surface, the reflecting layer is arranged on the light reflecting surface, and the light reflecting surface is used to adjust the emitted light in the second direction and the normal line of the screen. The direction in the formed plane is such that the maximum exit angle of the emitted light in the plane formed by the second direction and the screen normal is greater than the incident angle of the incident light in the plane formed by the second direction and the screen normal; the The first direction and the second direction are parallel to the screen plane and perpendicular to each other.

可選地,所述光入射面的焦距小於光入射面到光反射面距離的兩倍。 Optionally, the focal length of the light incident surface is less than twice the distance from the light incident surface to the light reflecting surface.

可選地,在第二方向與螢幕法線所形成的平面內,所述光反射面具有一焦點,且該焦點位於所述透明微結構內。 Optionally, in the plane formed by the second direction and the screen normal, the light reflecting mask has a focal point, and the focal point is located in the transparent microstructure.

可選地,所述光入射面為主軸與所述第二方向平行的圓柱面或拋物柱面。 Optionally, the light incident surface is a cylindrical surface or a parabolic surface with a main axis parallel to the second direction.

可選地,所述光反射面為主軸與所述第一方向平行的圓柱面或拋物柱面。 Optionally, the light reflection surface is a cylindrical surface or a parabolic surface with a main axis parallel to the first direction.

可選地,作為光入射面的圓柱面或拋物柱面的對稱中軸與螢幕法線不平行。 Optionally, the central axis of symmetry of the cylindrical surface or the parabolic cylinder as the light incident surface is not parallel to the screen normal.

可選地,作為光反射面的圓柱面或拋物柱面的對稱中軸與螢幕法線不平行。 Optionally, the central axis of symmetry of the cylindrical surface or the parabolic surface as the light reflecting surface is not parallel to the normal line of the screen.

可選地,所述光入射面為對入射光具有會聚作用且具有所述預設焦距的球面或者抛物面。 Optionally, the light incident surface is a spherical or parabolic surface that has a convergent effect on the incident light and has the preset focal length.

可選地,所述光反射面為球面或抛物面。 Optionally, the light reflecting surface is a spherical surface or a parabolic surface.

可選地,作為光入射面的球面或抛物面的對稱中軸與螢幕法線不平行。 Optionally, the central axis of symmetry of the spherical or parabolic surface as the light incident surface is not parallel to the screen normal.

可選地,作為光反射面的球面或抛物面的對稱中軸與螢幕法線不平行。 Optionally, the central axis of symmetry of the spherical or parabolic surface as the light reflecting surface is not parallel to the normal line of the screen.

可選地,所述透明微結構還包括連接所述光入射面和所述光反射面的側面,預設入射角度的入射光經所述光入射面端邊入射形成的折射光與所述側面平行,所述側面設置有光吸收體。 Optionally, the transparent microstructure further includes a side surface connecting the light incident surface and the light reflecting surface, and the refracted light formed by the incident light with a preset incident angle entering through the end of the light incident surface and the side surface Parallel, the side surface is provided with a light absorber.

可選地,對於所述透明微結構陣列中的一透明微結構,存在穿過該透明微結構且同時平行於第一方向和螢幕法線的第一平面,該透明微結構沿該第一平面的截面滿足以下關係式:當tan α

Figure 106115424-A0305-02-0005-4
-
Figure 106115424-A0305-02-0005-6
時,
Figure 106115424-A0305-02-0005-3
當tan α
Figure 106115424-A0305-02-0006-8
-
Figure 106115424-A0305-02-0006-9
時,
Figure 106115424-A0305-02-0006-12
當tan θ
Figure 106115424-A0305-02-0006-10
-tan α時,
Figure 106115424-A0305-02-0006-40
當tan θ
Figure 106115424-A0305-02-0006-13
-tan α時,
Figure 106115424-A0305-02-0006-14
其中,f為該透明微結構的光入射面的焦距,d為光入射面沿第一方向的寬度,h為光入射面到光反射面的距離,α為入射光在第一平面的入射角,θ為側面與螢幕法線的夾角,γ為入射光對應的出射光在第一平面的最大的第一出射角,β為入射光對應的出射光在第一平面的最大的第二出射角,第一出射角對應的出射光與第二出射角對應的出射光分別位於螢幕法線的兩側。 Optionally, for a transparent microstructure in the transparent microstructure array, there is a first plane passing through the transparent microstructure and parallel to the first direction and the normal line of the screen at the same time, and the transparent microstructure is along the first plane. The cross section satisfies the following relationship: when tan α
Figure 106115424-A0305-02-0005-4
-
Figure 106115424-A0305-02-0005-6
Time,
Figure 106115424-A0305-02-0005-3
When tan α
Figure 106115424-A0305-02-0006-8
-
Figure 106115424-A0305-02-0006-9
Time,
Figure 106115424-A0305-02-0006-12
When tan θ
Figure 106115424-A0305-02-0006-10
-tan α,
Figure 106115424-A0305-02-0006-40
When tan θ
Figure 106115424-A0305-02-0006-13
-tan α,
Figure 106115424-A0305-02-0006-14
Where f is the focal length of the light incident surface of the transparent microstructure, d is the width of the light incident surface in the first direction, h is the distance from the light incident surface to the light reflecting surface, and α is the incident angle of the incident light on the first plane , Θ is the angle between the side surface and the screen normal, γ is the largest first exit angle of the emitted light corresponding to the incident light in the first plane, β is the largest second exit angle of the exit light corresponding to the incident light in the first plane , The exit light corresponding to the first exit angle and the exit light corresponding to the second exit angle are respectively located on both sides of the normal line of the screen.

可選地,所述光吸收體填充在相鄰所述透明微結構的側面之間。 Optionally, the light absorber is filled between adjacent sides of the transparent microstructure.

可選地,所述表面結構至少包括第一區域和第二區域;所述第一區域的透明微結構的光入射面的主光軸與所述第二區域的透明微結構的光入射面的主光軸不平行。 Optionally, the surface structure at least includes a first area and a second area; the main optical axis of the light incident surface of the transparent microstructure in the first area is different from the light incident surface of the transparent microstructure in the second area. The main optical axis is not parallel.

由上述內容可知,與現有技術相比,本發明所提供的一種投影螢幕,包括螢幕本體和設置在螢幕本體投射面上的表面結構,該表面結構包括矩陣式排布的透明微結構陣列以及反射層。其中,透明微結構包括光入射面和光反射面,光入射面對入射光具有會聚作用,具有預設焦距;光反射面為曲面形,位於光入射面的焦距範圍內,在光反射面設置有反射層,使其對光具有反射作用。 It can be seen from the above content that, compared with the prior art, the projection screen provided by the present invention includes a screen body and a surface structure arranged on the projection surface of the screen body. The surface structure includes a matrix-arranged transparent microstructure array and a reflective surface. Floor. Among them, the transparent microstructure includes a light incident surface and a light reflecting surface. The light incident surface has a convergent effect on the incident light and has a preset focal length; the light reflecting surface is curved and located within the focal length range of the light incident surface, and the light reflecting surface is provided with The reflective layer makes it reflect light.

當投射光以一定入射角照射到投影螢幕,入射光經光入射面折射進入透明微結構,形成的折射光被會聚,並照射到位於焦平面之前的光反射面上,經反射後,光束再次經光入射面折射射出形成出射光,出射光的 反向延長線在透明微結構內形成一個點光源的像,出射光相當於從該點光源發出的光。通過光入射面調整出射光在第一方向與螢幕法線所形成平面內的方向,通過調整設計光入射面的焦距和沿第一方向的寬度、透明微結構的厚度(即光入射面與光反射面的距離)能夠控制透明微結構形成的點光源像的位置,進而來調整出射光在第一方向與螢幕法線所形成平面內的出射角度範圍。光反射面用於調整出射光在第二方向與螢幕法線所形成的平面內的方向,使得出射光在第二方向與螢幕法線所形成的平面內的最大出射角大於入射光在第二方向與螢幕法線所形成的平面內的入射角。 When the projected light is irradiated to the projection screen at a certain angle of incidence, the incident light is refracted by the light incident surface and enters the transparent microstructure. The resulting refracted light is condensed and irradiated on the light reflecting surface before the focal plane. After being reflected, the light beam is again It is refracted by the light incident surface to form outgoing light. The reverse extension line forms an image of a point light source in the transparent microstructure, and the emitted light is equivalent to the light emitted from the point light source. Adjust the direction of the emitted light in the plane formed by the first direction and the screen normal through the light incident surface, adjust the focal length of the designed light incident surface and the width along the first direction, and the thickness of the transparent microstructure (that is, the light incident surface and the light The distance of the reflective surface) can control the position of the point light source image formed by the transparent microstructure, and then adjust the exit angle range of the emitted light in the plane formed by the first direction and the normal line of the screen. The light reflecting surface is used to adjust the direction of the emitted light in the plane formed by the second direction and the screen normal, so that the maximum exit angle of the emitted light in the plane formed by the second direction and the screen normal is greater than that of the incident light in the second direction. The angle of incidence in the plane formed by the direction and the screen normal.

在實際應用中,根據入射光到達投影螢幕的入射角以及所要求的螢幕出射光的出射角度範圍,通過相應設計透明微結構光入射面的焦距和寬度、以及透明微結構的厚度,能夠控制以一定入射角的入射光在預設角度範圍內出射,從而實現對螢幕出射光在預設角度範圍內增益的效果,達到提高光利用率的效果。如果將螢幕出射光的出射角度範圍對應於觀看區域,則可將投影螢幕的出射光限定在觀看區域,可實現對對應於觀看區域的出射光增益的作用,能夠提高觀看者觀看到螢幕圖像的亮度。 In practical applications, according to the incident angle of the incident light reaching the projection screen and the required exit angle range of the light emitted from the screen, the focal length and width of the light incident surface of the transparent microstructure and the thickness of the transparent microstructure can be controlled accordingly by designing the focal length and width of the light incident surface of the transparent microstructure. The incident light with a certain incident angle is emitted within a preset angle range, so as to achieve the effect of gaining the light emitted from the screen within the preset angle range, and achieve the effect of improving the light utilization rate. If the output angle range of the light emitted from the screen corresponds to the viewing area, the light emitted from the projection screen can be limited to the viewing area, which can achieve the effect of gaining the output light corresponding to the viewing area, and can improve the viewer's viewing of the screen image The brightness.

<本發明> <The present invention>

α:入射角 α: incident angle

β:最大的第二出射角 β: The largest second exit angle

γ:最大的第一出射角 γ: The largest first exit angle

d:寬度 d: width

f:透明微結構的光入射面的焦距 f: the focal length of the light incident surface of the transparent microstructure

f’:光反射面的焦距 f’: Focal length of the light reflecting surface

h:距離 h: distance

100:透明微結構 100: Transparent microstructure

101:光入射面 101: Light incident surface

102:光反射面 102: light reflecting surface

103:反射層 103: reflective layer

104:側面 104: side

105:光吸收體 105: light absorber

106:焦平面 106: focal plane

107:投影螢幕 107: Projection screen

108:投影機 108: Projector

109:螢幕法線 109: Screen Normal

110:對稱中軸 110: Symmetrical Axis

圖1為本發明實施例提供的一種投影螢幕透明微結構的光路示意圖;圖2為投影螢幕懸掛後豎直方向的角度範圍示意圖;圖3為投影螢幕懸掛後水準方向的角度範圍示意圖;圖4為本發明實施例提供的一種投影螢幕表面結構的示意圖; 圖5A為本發明一種實施例中透明微結構沿第一方向和螢幕法線所成平面的截面圖;圖5B為圖5A所示透明微結構沿第二方向和螢幕法線所成平面的截面圖;圖6A為本發明又一種實施例中透明微結構沿第一方向和螢幕法線所成平面的截面圖;圖6B為圖6A所示透明微結構的光路示意圖;圖7為本發明又一種實施例中透明微結構沿第二方向和螢幕法線所成平面的截面圖;圖8為本發明又一實施例提供的一種投影螢幕表面結構的示意圖。 1 is a schematic diagram of the light path of a transparent microstructure of a projection screen provided by an embodiment of the present invention; FIG. 2 is a schematic diagram of the vertical angle range after the projection screen is suspended; FIG. 3 is a schematic diagram of the horizontal angle range after the projection screen is suspended; Is a schematic diagram of a surface structure of a projection screen provided by an embodiment of the present invention; 5A is a cross-sectional view of the transparent microstructure in an embodiment of the present invention along the first direction and the plane formed by the screen normal; FIG. 5B is a cross-sectional view of the transparent microstructure shown in FIG. 5A along the second direction and the plane formed by the screen normal Figure 6A is a cross-sectional view of the transparent microstructure along the first direction and the plane formed by the screen normal in another embodiment of the present invention; Figure 6B is a schematic diagram of the optical path of the transparent microstructure shown in Figure 6A; Figure 7 is another embodiment of the present invention A cross-sectional view of a plane formed by the transparent microstructure along the second direction and the normal line of the screen in an embodiment; FIG. 8 is a schematic diagram of a surface structure of a projection screen according to another embodiment of the present invention.

為了能夠更清楚地描述本發明所提出之一種投影螢幕,以下將配合圖式,詳盡說明本發明之較佳實施例。 In order to more clearly describe the projection screen proposed by the present invention, the preferred embodiments of the present invention will be described in detail below in conjunction with the drawings.

本發明提供一種投影螢幕,能夠調整螢幕出射光的出射角度範圍,實現了對螢幕出射光在預設角度範圍內增益的效果。 The present invention provides a projection screen, which can adjust the angle range of the light emitted from the screen, and realizes the effect of gaining the light emitted from the screen within a preset angle range.

本發明所提供的一種投影螢幕,包括螢幕本體,還包括設置在該螢幕本體投射面上的表面結構;表面結構包括矩陣式排布的透明微結構陣列以及反射層,其中透明微結構包括:光入射面,光入射面對入射光具有會聚作用,且具有預設焦距,光入射面的沿第一方向的寬度為預設值,光入射面利用其折射功能調整出射光在第一方向與螢幕法線所形成的平面內的方向,使得出射光在該第一方向與螢幕法線所形成的平面內的最大出射 角大於入射光在該第一方向與螢幕法線所形成的平面內的入射角;光反射面,光反射面位於光入射面的焦距範圍內,且為曲面形,在光反射面上設置有該反射層,光反射面利用其反射功能調整出射光在第二方向與螢幕法線所形成的平面內的方向,使得出射光在該第二方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第二方向與螢幕法線所形成的平面內的入射角;上述的第一方向和第二方向均平行於螢幕平面且兩者相互垂直。 The projection screen provided by the present invention includes a screen body and a surface structure arranged on the projection surface of the screen body; the surface structure includes a transparent microstructure array arranged in a matrix and a reflective layer, wherein the transparent microstructure includes: light The incident surface, the light incident surface has a convergent effect on the incident light, and has a preset focal length, the width of the light incident surface along the first direction is a preset value, and the light incident surface uses its refraction function to adjust the emitted light in the first direction and the screen The direction in the plane formed by the normal, so that the maximum output of the emitted light in the plane formed by the first direction and the screen normal The angle is greater than the incident angle of the incident light in the plane formed by the first direction and the normal line of the screen; the light reflecting surface, the light reflecting surface is located within the focal length range of the light incident surface, and is curved, and the light reflecting surface is provided with The reflective layer, the light reflecting surface uses its reflection function to adjust the direction of the emitted light in the plane formed by the second direction and the screen normal, so that the maximum emission of the emitted light in the plane formed by the second direction and the screen normal The angle is greater than the incident angle of the incident light in the plane formed by the second direction and the normal line of the screen; the above-mentioned first direction and the second direction are both parallel to the plane of the screen and both are perpendicular to each other.

由上述內容可知,本發明所提供的投影螢幕,包括螢幕本體和設置在螢幕本體投射面上的表面結構,該表面結構包括矩陣式排布的透明微結構陣列以及反射層。其中,透明微結構包括光入射面和光反射面,光入射面對入射光具有會聚作用,具有預設焦距;光反射面為曲面形,位於光入射面的焦距範圍內,在光反射面設置有反射層,使其對光具有反射作用。 It can be seen from the above content that the projection screen provided by the present invention includes a screen body and a surface structure arranged on the projection surface of the screen body. The surface structure includes a matrix-arranged transparent microstructure array and a reflective layer. Among them, the transparent microstructure includes a light incident surface and a light reflecting surface. The light incident surface has a convergent effect on the incident light and has a preset focal length; the light reflecting surface is curved and located within the focal length range of the light incident surface, and the light reflecting surface is provided with The reflective layer makes it reflect light.

於本發明中,所述透明微結構為折射率大於1的透明介質,可以為樹脂等有機成分,也可以為玻璃、石英等無機成分。 In the present invention, the transparent microstructure is a transparent medium with a refractive index greater than 1, which may be organic components such as resins, or inorganic components such as glass and quartz.

本發明中,所描述的出射角是指出射光與螢幕法線的夾角,光在某一平面內的方向為該束光在該平面上的投影的方向。 In the present invention, the described exit angle refers to the angle between the emitted light and the normal line of the screen, and the direction of the light in a certain plane is the direction of the projection of the beam of light on the plane.

當投射光以一定入射角照射到投影螢幕,入射光經光入射面折射進入透明微結構,形成的折射光被會聚,並照射到位於焦平面之前的光反射面上,經反射後,光束再次經光入射面折射射出形成出射光,出射光的反向延長線在透明微結構內形成一個點光源的像,出射光相當於由該點光源發出的光。通過光入射面能夠調整出射光在第一方向與螢幕法線所形成的平面內的方向,能夠使得出射光在該第一方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第一方向與螢幕法線所形成的平面內的入 射角,通過調整設計光入射面的焦距和沿第一方向的寬度、透明微結構的厚度(即光入射面與光反射面的距離)能夠控制透明微結構形成的點光源像的位置,進而來調整出射光在第一方向與螢幕法線所形成平面內的出射角度範圍。光反射面用於調整出射光在第二方向與螢幕法線所形成的平面內的方向,能使得出射光在該第二方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第二方向與螢幕法線所形成的平面內的入射角。 When the projected light is irradiated to the projection screen at a certain angle of incidence, the incident light is refracted by the light incident surface and enters the transparent microstructure. The resulting refracted light is condensed and irradiated on the light reflecting surface before the focal plane. After being reflected, the light beam is again It is refracted and emitted by the light incident surface to form outgoing light, and the reverse extension line of the outgoing light forms an image of a point light source in the transparent microstructure, and the outgoing light is equivalent to the light emitted by the point light source. Through the light incident surface, the direction of the emitted light in the plane formed by the first direction and the screen normal can be adjusted, so that the maximum exit angle of the emitted light in the plane formed by the first direction and the screen normal can be greater than that of the incident light. The entrance in the plane formed by the first direction and the screen normal The angle of incidence, by adjusting the focal length and width along the first direction of the designed light incident surface, and the thickness of the transparent microstructure (that is, the distance between the light incident surface and the light reflecting surface), the position of the point light source image formed by the transparent microstructure can be controlled, and then To adjust the angle range of the emitted light in the plane formed by the first direction and the screen normal. The light reflecting surface is used to adjust the direction of the emitted light in the plane formed by the second direction and the screen normal, so that the maximum exit angle of the emitted light in the plane formed by the second direction and the screen normal is greater than that of the incident light. The incident angle in the plane formed by the second direction and the screen normal.

在實際應用中,根據入射光到達投影螢幕的入射角以及所要求的螢幕出射光的出射角度範圍,通過相應設計透明微結構光入射面的焦距和寬度、以及透明微結構的厚度,能夠控制以一定入射角的入射光在預設角度範圍內出射,從而實現對螢幕出射光在預設角度範圍內增益的效果。如果將螢幕出射光的出射角度範圍對應於觀看區域,則可將投影螢幕的出射光限定在觀看區域,可實現對對應於觀看區域的出射光增益的作用,能夠提高觀看者觀看到螢幕圖像的亮度。 In practical applications, according to the incident angle of the incident light reaching the projection screen and the required exit angle range of the light emitted from the screen, the focal length and width of the light incident surface of the transparent microstructure and the thickness of the transparent microstructure can be controlled accordingly by designing the focal length and width of the light incident surface of the transparent microstructure. The incident light with a certain incident angle is emitted within a preset angle range, so as to achieve the effect of gaining the light emitted from the screen within the preset angle range. If the output angle range of the light emitted from the screen corresponds to the viewing area, the light emitted from the projection screen can be limited to the viewing area, which can achieve the effect of gaining the output light corresponding to the viewing area, and can improve the viewer's viewing of the screen image The brightness.

本發明中,要求光反射面位於光入射面的焦距範圍內,即是要求光入射面與光反射面的距離小於光入射面的焦距。首先,要求光反射面不能位於光入射面的焦平面上:假若光反射面在該焦平面上,則入射光會聚在光反射面的一點上。考慮最簡單的入射光沿螢幕法線入射的情況(入射角為0°),則光線被光反射面反射後,經光入射面出射,出射光還是沿螢幕法線方向平行出射,根本沒有改變光的角度。其次,假若光反射面到光入射面的距離大於光入射面的焦距,則在透明微結構中,光在到達光反射面之前就會聚了,會聚後的光以發散光的形式入射到光反射面,被反射後進一步發散,使得許多光無法到達光入射面;而且此種情況,意味著要麼 光入射面的曲率大(加工難、光學設計難、容易脫離近軸光學範疇),要麼光入射面到光反射面的距離大(意味著螢幕加厚)。本發明將光反射面設置在光入射面的焦距範圍內,目的是實現這樣的模型──點光源的物距小於凸透鏡的焦距,從而存在一個點光源的像,光相當於從該點光源像發出,必然是發散的。 In the present invention, the light reflecting surface is required to be within the focal length range of the light incident surface, that is, the distance between the light incident surface and the light reflecting surface is required to be smaller than the focal length of the light incident surface. First, it is required that the light reflecting surface cannot be located on the focal plane of the light incident surface: if the light reflecting surface is on the focal plane, the incident light will converge on a point on the light reflecting surface. Consider the simplest case where the incident light is incident along the normal line of the screen (incidence angle is 0°), then after the light is reflected by the light reflecting surface, it exits through the light incident surface, and the emitted light still exits in parallel along the normal direction of the screen without any change at all. The angle of light. Secondly, if the distance between the light reflecting surface and the light incident surface is greater than the focal length of the light incident surface, then in the transparent microstructure, the light will converge before reaching the light reflecting surface, and the condensed light will be incident on the light reflecting surface in the form of divergent light. After being reflected, it diverges further, making it impossible for a lot of light to reach the light incident surface; and in this case, it means either The curvature of the light incident surface is large (difficult to process, difficult to design, and easy to deviate from the paraxial optics category), or the distance from the light incident surface to the light reflecting surface is large (meaning the screen is thickened). The present invention sets the light reflecting surface within the focal length range of the light incident surface, and aims to realize such a model—the object distance of the point light source is smaller than the focal length of the convex lens, so that there is an image of a point light source, and the light is equivalent to the image from the point light source. Issued must be divergent.

以上是本發明的核心思想,為使本發明的上述目的、特徵和優點能夠更加明顯易懂,下面結合附圖對本發明的原理以及具體實施方式做詳細的說明。 The above is the core idea of the present invention. In order to make the above objectives, features and advantages of the present invention more obvious and understandable, the principles and specific implementations of the present invention will be described in detail below with reference to the accompanying drawings.

在下面的描述中闡述了很多具體細節以便於充分理解本發明,但是本發明還可以採用其他不同於在此描述的其它方式來實施,本領域技術人員可以在不違背本發明內涵的情況下做類似推廣,因此本發明不受下面公開的具體實施例的限制。 In the following description, many specific details are set forth in order to fully understand the present invention, but the present invention can also be implemented in other ways different from those described here, and those skilled in the art can do so without departing from the connotation of the present invention. Similar promotion, therefore, the present invention is not limited by the specific embodiments disclosed below.

其次,本發明結合示意圖進行詳細描述,在詳述本發明實施例時,為便於說明,表示結構的剖面圖會不依一般比例作局部放大,而且所述示意圖只是示例,其在此不應限制本發明保護的範圍。此外,在實際製作中應包含長度、寬度及深度的三維空間尺寸。 Secondly, the present invention will be described in detail in combination with schematic diagrams. When describing the embodiments of the present invention in detail, the cross-sectional view showing the structure will not be partially enlarged according to the general scale, and the schematic diagram is only an example, which should not limit the present invention. The scope of invention protection. In addition, the three-dimensional dimensions of length, width and depth should be included in the actual production.

下面結合本發明實施例中透明微結構的一種示意圖對本發明投影螢幕對出射光的出射角度範圍進行調整的原理進行詳細描述。 In the following, the principle of adjusting the output angle range of the emitted light by the projection screen of the present invention will be described in detail with reference to a schematic diagram of the transparent microstructure in the embodiment of the present invention.

對於本發明所述透明微結構陣列中的一透明微結構,存在穿過該透明微結構且同時平行於第一方向和螢幕法線的平面,請參考圖1,圖1為本發明實施例提供的一種投影螢幕透明微結構的光路示意圖,如圖1所示,透明微結構包括一光入射面101、一光反射面102,其中,該光入射面101 具有透明微結構的光入射面的焦距f,其寬度為d,該光反射面102到焦平面106的距離h。 For a transparent microstructure in the transparent microstructure array of the present invention, there is a plane passing through the transparent microstructure and parallel to the first direction and the screen normal. Please refer to FIG. 1, which is an embodiment of the present invention. A schematic diagram of the light path of a transparent microstructure of a projection screen. As shown in FIG. 1, the transparent microstructure includes a light incident surface 101 and a light reflecting surface 102, wherein the light incident surface 101 The focal length f of the light incident surface with a transparent microstructure has a width d, and the distance h from the light reflecting surface 102 to the focal plane 106.

假設入射光在第一方向與螢幕法線109所成的第一平面內的入射角為α(入射角指入射光與投影螢幕法線的夾角,入射光在該第一平面內的入射角指入射光束在該第一平面內的投影與螢幕法線的夾角),在該第一平面內,入射光經透明微結構後形成的出射光,包括分別位於螢幕法線兩側的第一出射光和第二出射光,第一出射光對應以第一出射角射出,第二出射光對應為第二出射角,螢幕出射光的出射角度範圍對應為最大的第一出射角γ和最大的第二出射角β之間的角度範圍,因此由最大的第一出射角γ和最大的第二出射角β描述投影螢幕的出射光的出射角度範圍。 Assume that the incident angle of the incident light in the first plane formed by the first direction and the screen normal 109 is α (the incident angle refers to the angle between the incident light and the projection screen normal, and the incident angle of the incident light in the first plane refers to the angle between the incident light and the normal line of the projection screen. The angle between the projection of the incident light beam in the first plane and the normal line of the screen). In the first plane, the emitted light formed after the incident light passes through the transparent microstructure includes the first emitted light located on both sides of the normal line of the screen. Compared with the second exit light, the first exit light corresponds to the first exit angle, the second exit light corresponds to the second exit angle, and the exit angle range of the screen exit light corresponds to the largest first exit angle γ and the largest second exit angle. The angle range between the exit angles β, so the largest first exit angle γ and the largest second exit angle β describe the exit angle range of the exit light of the projection screen.

基於光學反射理論,根據入射光的入射角α,通過相應設計透明微結構的光入射面的焦距f,光入射面的寬度d,光反射面到光入射面的焦平面106的距離h,可以控制投影螢幕出射光的第一出射角和第二出射角的範圍,從而控制和調整投影螢幕形成的出射光在第一方向與螢幕法線109所形成的第一平面內的出射角度範圍。 Based on the optical reflection theory, according to the incident angle α of the incident light, by correspondingly designing the focal length f of the light incident surface of the transparent microstructure, the width d of the light incident surface, and the distance h from the light reflecting surface to the focal plane 106 of the light incident surface, The range of the first exit angle and the second exit angle of the light emitted by the projection screen is controlled, so as to control and adjust the exit angle range of the light formed by the projection screen in the first plane formed by the first direction and the screen normal 109.

請參考圖2,圖2為投影螢幕懸掛後豎直方向的角度範圍示意圖。如圖2所示,在實際應用中,該第一方向可以是投影螢幕懸掛後的豎直方向,在投影螢幕107懸掛後豎直範圍內,螢幕出射光對應於觀看區域具有一定角度範圍,通過投影螢幕107表面結構可控制螢幕出射光在豎直範圍的出射角度範圍,使在螢幕豎直範圍內螢幕的出射光對應於觀看區域。 Please refer to FIG. 2, which is a schematic diagram of the vertical angle range of the projection screen after it is hung. As shown in Figure 2, in practical applications, the first direction may be the vertical direction after the projection screen is suspended. Within the vertical range after the projection screen 107 is suspended, the light emitted from the screen has a certain angular range corresponding to the viewing area. The surface structure of the projection screen 107 can control the emission angle range of the light emitted from the screen in the vertical range, so that the light emitted from the screen in the vertical range of the screen corresponds to the viewing area.

請繼續參考圖3,圖3為投影螢幕懸掛後水準方向的角度範圍示意圖。如圖3所示,第一方向也可以是投影螢幕懸掛後的水準方向, 通過投影螢幕表面結構可實現控制螢幕出射光在水準範圍內的出射角度範圍,使在水準範圍內螢幕出射光對應於觀看區域。 Please continue to refer to Figure 3, which is a schematic diagram of the angular range of the horizontal direction after the projection screen is hung. As shown in Figure 3, the first direction can also be the horizontal direction after the projection screen is hung. Through the surface structure of the projection screen, it is possible to control the emission angle range of the light emitted from the screen within the level range, so that the light emitted from the screen within the level range corresponds to the viewing area.

在本發明的一種具體實施例中,可參考圖1,該光入射面101的焦距小於光入射面101到光反射面102距離的兩倍,這樣,保證折射光經該光反射光面102形成的透明微結構的光入射面的焦距f,點光源的像也必然在透明微結構內(即螢幕內部),是一個虛像,從而可以利用點光源的虛像與光入射面邊緣的位置關係控制出射光在第一方向的角度範圍。假若光入射面101的焦距大於光入射面101到光反射面102距離的兩倍,則必然導致出射光在螢幕與觀眾之間形成點光源的實像,這樣會造成

Figure 106115424-A0305-02-0013-41
出射光角度過大、難以控制角度範圍;
Figure 106115424-A0305-02-0013-42
在該點光源的實像位置附近,灰塵等空氣中的顆粒物可能會對該集中的光線造成極大的影響,嚴重影響觀影體驗。 In a specific embodiment of the present invention, referring to FIG. 1, the focal length of the light incident surface 101 is less than twice the distance from the light incident surface 101 to the light reflecting surface 102, so as to ensure that the refracted light is formed by the light reflecting surface 102. The focal length f of the light incident surface of the transparent microstructure, the image of the point light source must also be in the transparent microstructure (that is, the inside of the screen), which is a virtual image, which can be controlled by the positional relationship between the virtual image of the point light source and the edge of the light incident surface The angular range of the emitted light in the first direction. If the focal length of the light incident surface 101 is greater than twice the distance between the light incident surface 101 and the light reflecting surface 102, it will inevitably cause the emitted light to form a real image of a point light source between the screen and the audience.
Figure 106115424-A0305-02-0013-41
The angle of the emitted light is too large and it is difficult to control the angle range;
Figure 106115424-A0305-02-0013-42
Near the real image position of the point light source, airborne particles such as dust may have a great impact on the concentrated light and seriously affect the viewing experience.

本發明投影螢幕,其投射面設置有矩陣式排布的透明微結構陣列,基於透明微結構具有特定尺寸設計的光入射面和光反射面,能夠調整螢幕出射光在第一方向與螢幕法線所形成平面內的出射角度範圍,並保證在第二方向與螢幕法線所形成第二平面內螢幕出射光的出射範圍,實現對螢幕出射光在預設角度範圍內增益的效果。如果將出射角度範圍對應於觀看區域,則實現了對對應於觀看區域的出射光增益的作用,能夠提高觀看者觀看到螢幕圖像的亮度。 The projection screen of the present invention is provided with a matrix-arranged transparent microstructure array on the projection surface. Based on the transparent microstructure, the light incident surface and the light reflecting surface are designed with specific dimensions, and the light emitted from the screen can be adjusted in the first direction and the normal line of the screen. A range of exit angles in the plane is formed, and the exit range of the light emitted from the screen in the second plane formed by the second direction and the normal line of the screen is ensured, so as to achieve the effect of gaining the light emitted from the screen within the preset angle range. If the output angle range corresponds to the viewing area, the effect of gaining the output light corresponding to the viewing area is realized, and the brightness of the screen image viewed by the viewer can be improved.

下面結合附圖詳細描述本發明投影螢幕的幾種具體實施例。 Several specific embodiments of the projection screen of the present invention will be described in detail below with reference to the accompanying drawings.

請參考圖4,圖4為本發明實施例提供的一種投影螢幕表面結構的示意圖。如圖4所示,在本發明投影螢幕的一種具體實施例中, 該表面結構包括矩陣式排布的透明微結構100陣列以及反射層103,其中透明微結構100包括光入射面101和光反射面102。 Please refer to FIG. 4, which is a schematic diagram of a surface structure of a projection screen according to an embodiment of the present invention. As shown in FIG. 4, in a specific embodiment of the projection screen of the present invention, The surface structure includes an array of transparent microstructures 100 arranged in a matrix and a reflective layer 103, wherein the transparent microstructure 100 includes a light incident surface 101 and a light reflecting surface 102.

所述光入射面101為主軸與第二方向平行的圓柱面,對入射光具有會聚作用,具有預設透明微結構的光入射面的焦距f,沿第一方向的寬度d。光反射面102位於光入射面101的焦距範圍內,光反射面102為曲面形,設置有反射層103。圓柱面的主軸即為該圓柱面對應的圓柱體的軸線,也即平行於圓柱面的線。這裡的透明微結構的光入射面的焦距f認為是近軸光學下圓柱面上的圓弧的焦距,不限於嚴格意義上的作為“點”的焦點。 The light incident surface 101 is a cylindrical surface whose main axis is parallel to the second direction and has a condensing effect on incident light. The focal length f of the light incident surface with a preset transparent microstructure is the width d along the first direction. The light reflecting surface 102 is located within the focal length range of the light incident surface 101, and the light reflecting surface 102 is curved and is provided with a reflecting layer 103. The main axis of the cylindrical surface is the axis of the cylinder corresponding to the cylindrical surface, that is, the line parallel to the cylindrical surface. The focal length f of the light incident surface of the transparent microstructure here is considered to be the focal length of the arc on the cylindrical surface under paraxial optics, and is not limited to the focal point as a "point" in the strict sense.

在本發明的另一種實施例中,光入射面101也可以替換為主軸與第二方向平行的拋物柱面,拋物柱面的主軸即為平行於拋物柱面的線。 In another embodiment of the present invention, the light incident surface 101 can also be replaced with a parabolic cylinder whose main axis is parallel to the second direction, and the main axis of the parabolic cylinder is a line parallel to the parabolic cylinder.

當入射光經圓柱面或者拋物柱面的光入射面101折射進入透明微結構,被聚焦並經反射後再次由光入射面101折射出形成出射光,所形成出射光的反向延長線在透明微結構內會聚為一個點光源的虛像,出射光可看作是由該點光源發出的光經光入射面射出,因此通過調整光入射面的焦距和沿第一方向的寬度、透明微結構的厚度可以調整螢幕出射光在第一方向與螢幕法線109所形成第一平面內的出射角度範圍。 When the incident light is refracted by the cylindrical or parabolic light incident surface 101 into the transparent microstructure, it is focused and reflected and then refracted again by the light incident surface 101 to form the emergent light, and the reverse extension of the formed emergent light is in the transparent The microstructure converges into a virtual image of a point light source. The emitted light can be regarded as the light emitted by the point light source through the light incident surface. Therefore, by adjusting the focal length of the light incident surface and the width along the first direction, the transparent microstructure The thickness can adjust the emission angle range of the light emitted from the screen in the first plane formed by the first direction and the normal line 109 of the screen.

基於曲面形的光反射面102能擴大出射光在第二方向與螢幕法線109所形成的第二平面內的出射角度範圍。 The curved light reflecting surface 102 can expand the range of the exit angle of the exiting light in the second plane formed by the second direction and the normal line 109 of the screen.

請繼續參閱圖5A與圖5B,其中,圖5A為本發明一種實施例中透明微結構沿第一方向和螢幕法線所成平面的截面圖,該圖5B為圖5A所示透明微結構沿第二方向和螢幕法線所成平面的截面圖。如圖所示,在本實施例透明微結構的一種結構設計中,該光反射面102為主軸與第一方向平行的圓 柱面,或者,該光反射面102也可以是主軸與第一方向平行的拋物柱面。光反射面102的焦點位於透明微結構內,這樣在第二方向與螢幕法線所形成的平面內,折射光被會聚,再次經光入射面101折射出,形成的出射光的最大出射角大於入射角,保證了在第二方向與螢幕法線109所形成的第二平面的出射角度範圍。 Please continue to refer to FIGS. 5A and 5B, in which, FIG. 5A is a cross-sectional view of the transparent microstructure along the first direction and the screen normal in an embodiment of the present invention. The FIG. 5B is the transparent microstructure shown in FIG. 5A along the plane. A cross-sectional view of the plane formed by the second direction and the screen normal. As shown in the figure, in a structural design of the transparent microstructure of this embodiment, the light reflecting surface 102 is a circle whose main axis is parallel to the first direction. The cylindrical surface, or the light reflecting surface 102 may also be a parabolic cylindrical surface whose main axis is parallel to the first direction. The focal point of the light reflecting surface 102 is located in the transparent microstructure, so that in the plane formed by the second direction and the screen normal, the refracted light is converged and refracted again by the light incident surface 101. The maximum exit angle of the formed light is greater than The incident angle guarantees the scope of the exit angle of the second plane formed by the second direction and the screen normal 109.

在實際應用中,根據投射光到達投影螢幕的入射角,相應設計透明微結構的光入射面的焦距f,光入射面沿第一方向的寬度d,光反射面到光入射面的焦平面106的距離h,以及光反射面的焦距f’,可以控制調整螢幕出射光在第一方向與螢幕法線108所形成的第一平面內的出射角度範圍,同時保證螢幕出射光在第二方向與螢幕法線109所形成的第二平面內的出射角度範圍,實現以一定入射角的入射光經螢幕反射後在預設角度範圍內出射,實現對螢幕出射光在預設角度範圍內增益的效果。 In practical applications, according to the incident angle of the projected light to the projection screen, the focal length f of the light incident surface of the transparent microstructure is correspondingly designed, the width d of the light incident surface along the first direction, and the focal plane 106 from the light reflecting surface to the light incident surface. The distance h of the light reflecting surface and the focal length f'of the light reflecting surface can be controlled to adjust the angle range of the light emitted from the screen in the first plane formed by the first direction and the screen normal 108, while ensuring that the light emitted from the screen is in the second direction and The exit angle range in the second plane formed by the screen normal 109, realizes that the incident light with a certain incident angle is reflected by the screen and then exits within the preset angle range, which achieves the effect of gaining the screen's emergent light within the preset angle range .

在上述實施例中,透明微結構為對稱設計,即圓柱面形或拋物柱面形的光入射面101的對稱中軸與螢幕法線平行,圓柱面形或拋物柱面形的光反射面102的對稱中軸與螢幕法線平行。這種結構設計,參考圖1所示,由於入射光為傾斜入射,即具有一定的入射角,因此在第一方向與螢幕法線109所形成的第一平面內,入射光經投影螢幕透明微結構後形成的出射光,形成的位於螢幕法線一側的第一出射光的出射角γ的角度範圍,總大於位於螢幕法線另一側的第二出射光的出射角β的角度範圍,但在實際應用中,有時需要最大第二出射角β的範圍大於最大第一出射角γ的範圍。基於此,在本發明投影螢幕的另一種具體實施例中,為更靈活適應出射角度範圍需求,透明微結構可採用非對稱設計。 In the above embodiment, the transparent microstructure is a symmetrical design, that is, the central axis of symmetry of the cylindrical or parabolic light incident surface 101 is parallel to the screen normal, and the cylindrical or parabolic light reflecting surface 102 The axis of symmetry is parallel to the screen normal. This structure design, as shown in Figure 1, because the incident light is obliquely incident, that is, has a certain angle of incidence, so in the first plane formed by the first direction and the screen normal 109, the incident light is transparent through the projection screen. The angle range of the emergence angle γ of the first emergent light on the normal side of the screen formed by the emergent light formed after the structure is always greater than the angle range of the emergence angle β of the second emergent light on the other side of the screen normal. However, in practical applications, sometimes the range of the maximum second exit angle β is required to be greater than the range of the maximum first exit angle γ. Based on this, in another specific embodiment of the projection screen of the present invention, in order to more flexibly adapt to the requirements of the output angle range, the transparent microstructure may adopt an asymmetrical design.

請繼續參閱圖6A,圖6A為本發明又一種實施例中透明微結構沿第一方向和螢幕法線所成平面的截面圖。如圖6A所示,具體的,作為光入射面101的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行;或者,可參考圖7,圖7為本發明又一種實施例中透明微結構沿第二方向和螢幕法線所成平面的截面圖。如圖7所示,作為光反射面102的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行。或者,作為光入射面101的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行,同時作為光反射面102的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行。 Please continue to refer to FIG. 6A. FIG. 6A is a cross-sectional view of a plane formed by the transparent microstructure along the first direction and the normal line of the screen in another embodiment of the present invention. As shown in FIG. 6A, specifically, the central axis of symmetry 110 of the cylindrical or parabolic surface as the light incident surface 101 is not parallel to the screen normal 109; or, refer to FIG. 7, which is another embodiment of the present invention A cross-sectional view of the plane formed by the transparent microstructure along the second direction and the normal line of the screen. As shown in FIG. 7, the central axis of symmetry 110 of the cylindrical or parabolic surface as the light reflecting surface 102 is not parallel to the normal line 109 of the screen. Alternatively, the central axis of symmetry 110 of the cylindrical or parabolic surface as the light incident surface 101 is not parallel to the screen normal 109, and the central axis of symmetry 110 of the cylindrical or parabolic surface as the light reflecting surface 102 is not parallel to the screen normal 109 .

請參考圖6B,圖6B為圖6A所示透明微結構的光路示意圖,如圖6B所示,對於作為光入射面101的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行的實施例,即為在穿過該透明微結構且同時平行於第一方向和螢幕法線109的平面內的光路示意圖。光入射面101的對稱中軸110與螢幕法線109不平行,具有一定夾角,在第一方向與螢幕法線所形成的第一平面內,光入射面的焦點位置會隨之移動,相應的,所形成的出射光的反向延長線會聚形成的點光源的像的位置,也相應移動,因此通過調整光入射面101的對稱中軸110與螢幕法線109的夾角,改變點光源的像與光入射面的位置關係,可靈活控制所形成的第一出射光和第二出射光的角度範圍,例如,可以實現最大第二出射角β的範圍大於最大第一出射角γ的角度範圍。 Please refer to FIG. 6B. FIG. 6B is a schematic diagram of the optical path of the transparent microstructure shown in FIG. 6A. As shown in FIG. 6B, the center axis of symmetry 110 of the cylindrical or parabolic surface as the light incident surface 101 is not parallel to the screen normal 109 The embodiment is a schematic diagram of the light path in a plane passing through the transparent microstructure and parallel to the first direction and the normal line 109 of the screen. The central axis 110 of symmetry of the light incident surface 101 is not parallel to the screen normal 109 and has a certain included angle. In the first plane formed by the first direction and the screen normal, the focal position of the light incident surface will move accordingly, correspondingly, The position of the image of the point light source formed by the reverse extension of the emergent light is also moved accordingly. Therefore, by adjusting the angle between the symmetrical central axis 110 of the light incident surface 101 and the screen normal 109, the image and light of the point light source are changed. The positional relationship of the incident surface can flexibly control the angle range of the formed first and second emergent light. For example, it can be realized that the range of the maximum second emergence angle β is greater than the angular range of the maximum first emergence angle γ.

對於作為光反射面102的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行的實施例,在第二方向與螢幕法線109所形成的第二平面內,通過調整光反射面102的對稱中軸110與螢幕法線109的夾角,改變光反 射面的焦點在透明微結構內的位置,可控制和調整出射光在第二方向與螢幕法線109所形成的第二平面內的發散角範圍。 For the embodiment where the central axis of symmetry 110 of the cylindrical or parabolic surface as the light reflecting surface 102 is not parallel to the screen normal 109, the light reflecting surface is adjusted in the second plane formed by the second direction and the screen normal 109 The angle between the symmetrical axis 110 of 102 and the normal line 109 of the screen changes the light reflection The position of the focal point of the emitting surface in the transparent microstructure can control and adjust the divergence angle range of the emitted light in the second plane formed by the second direction and the screen normal 109.

對於作為光入射面101的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行,同時作為光反射面102的圓柱面或拋物柱面的對稱中軸110與螢幕法線109不平行的實施例,通過改變光入射面101的對稱中軸110與螢幕法線109的夾角,改變點光源的像與光入射面的位置關係,可控制所形成的第一出射光和第二出射光的角度範圍,同時通過調整光反射面102的對稱中軸110與螢幕法線109的夾角,可改變光反射面的焦點位置,可相應調整出射光在第二方向與螢幕法線109所形成的第二平面內的出射角度範圍。 The central axis of symmetry 110 of the cylindrical or parabolic surface as the light incident surface 101 is not parallel to the normal line 109 of the screen, and the central axis of symmetry 110 of the cylindrical or parabolic surface as the light reflecting surface 102 is not parallel to the normal line 109 of the screen. In an embodiment, by changing the angle between the central axis 110 of symmetry of the light incident surface 101 and the screen normal 109, the positional relationship between the image of the point light source and the light incident surface can be changed to control the angles of the first and second emergent lights formed At the same time, by adjusting the angle between the symmetry axis 110 of the light reflecting surface 102 and the screen normal 109, the focal position of the light reflecting surface can be changed, and the second plane formed by the second direction of the emitted light and the screen normal 109 can be adjusted accordingly The range of exit angles within.

進一步的,在本發明的另一種具體實施例中,對稱中軸110與入射光方向的夾角小於螢幕法線109與入射光方向的夾角,該技術方案可以使出射光的出射角沿螢幕法線109兩側的兩個方向分佈更為大小平均。 Further, in another specific embodiment of the present invention, the angle between the central axis of symmetry 110 and the incident light direction is smaller than the angle between the screen normal 109 and the incident light direction. This technical solution can make the exit angle of the emitted light follow the screen normal 109 The two directions on both sides are more evenly distributed.

這裡較好理解的是,圓柱面的對稱中軸110,即為在垂直於上述圓柱面主軸的平面內,平分圓柱面在該平面內的圓弧且過圓心的線;而拋物柱面的對稱中軸110,即為在垂直於上述拋物柱面主軸的平面內,過拋物柱面在該平面內的抛物線頂點和焦點的線。 It is better understood here that the central axis of symmetry 110 of the cylindrical surface is the line that bisects the arc of the cylindrical surface in the plane and passes through the center in the plane perpendicular to the main axis of the cylindrical surface; and the symmetry central axis of the parabolic surface 110 is a line that passes through the vertex and focus of the parabola in the plane perpendicular to the main axis of the parabolic cylinder.

這種不對稱設計便於更自由地結合入射角調整出射光的出射範圍,可以擴展設計的自由度,可以設計出適宜更多入射角和出射角要求的情況。 This asymmetric design facilitates more freely adjusting the emission range of the emitted light in combination with the incident angle, can expand the degree of freedom of design, and can be designed to meet the requirements of more incident angles and emission angles.

請參閱圖8,圖8為本發明又一實施例提供的一種投影螢幕表面結構的示意圖。如圖8所示,在本發明投影螢幕的其它具體實施例中,在上述各具體實施例的基礎上,該透明微結構還包括連接該光入射面101和該光反 射面102的一側面104,該側面104與預設入射角度的入射光經該光入射面101端邊折射形成的折射光平行,該側面104設置有一光吸收體105。 Please refer to FIG. 8, which is a schematic diagram of a surface structure of a projection screen according to another embodiment of the present invention. As shown in FIG. 8, in other specific embodiments of the projection screen of the present invention, on the basis of the above specific embodiments, the transparent microstructure further includes connecting the light incident surface 101 and the light reflecting surface. A side surface 104 of the emitting surface 102 is parallel to the refracted light formed by the incident light with a predetermined incident angle being refracted by the end of the light incident surface 101, and the side surface 104 is provided with a light absorber 105.

一個透明微結構可以具有一個或多個呈曲面或平面的側面,存在一平行入射光,該平行入射光在光入射面101與任一側面連接的邊形成的折射光都平行於該側面。 A transparent microstructure may have one or more curved or flat side surfaces, and there is a parallel incident light, and the refracted light formed by the parallel incident light on the side connecting the light incident surface 101 and any side surface is parallel to the side surface.

本實施例中,光吸收體105填充在相鄰該透明微結構100的側面104之間。 In this embodiment, the light absorber 105 is filled between the side surfaces 104 adjacent to the transparent microstructure 100.

當入射角為其它角度的雜散光照射到透明微結構內,尤其是大角度雜散光,其折射光線會偏折射到側面,會被側面的光吸收體吸收。 When the stray light with other angles of incidence is irradiated into the transparent microstructure, especially the large-angle stray light, the refracted light will be deflected to the side and be absorbed by the light absorber on the side.

因此,該透明微結構具有側面,側面設置有光吸收體,能夠將雜散光吸收,使雜散光不會出射到要求的出射角度範圍內,若出射光的出射角度範圍對應於觀看區域,可以使出射到觀看區域的雜散光減少,從而可增強觀看者觀看到螢幕圖像的對比度。 Therefore, the transparent microstructure has a side surface, and a light absorber is provided on the side surface, which can absorb stray light so that the stray light will not be emitted within the required output angle range. If the output angle range of the emitted light corresponds to the viewing area, the The stray light emitted to the viewing area is reduced, thereby enhancing the contrast of the screen image viewed by the viewer.

對於本實施例透明微結構陣列中的一透明微結構,在穿過該透明微結構且同時平行於第一方向和螢幕法線109的第一平面上,根據光學反射理論推導,沿該第一平面的截面滿足以下關係式,當tan α

Figure 106115424-A0305-02-0018-15
-
Figure 106115424-A0305-02-0018-20
時,
Figure 106115424-A0305-02-0018-24
當tan α
Figure 106115424-A0305-02-0018-16
-
Figure 106115424-A0305-02-0018-22
時,
Figure 106115424-A0305-02-0018-26
當tan θ
Figure 106115424-A0305-02-0018-17
-tan α時,
Figure 106115424-A0305-02-0018-27
當tan θ
Figure 106115424-A0305-02-0018-18
-tan α時,
Figure 106115424-A0305-02-0018-29
其中,f為該透明微結構的光入射面的焦距,d為光入射面沿第一方向的寬度,h為光入射面到光反射面的距離,α為入射光在第一平面的入射角,θ 為側面與螢幕法線109的夾角,γ為入射光對應的出射光在第一平面的最大的第一出射角,β為入射光對應的出射光在第一平面的最大的第二出射角,第一出射角對應的出射光與第二出射角對應的出射光分別位於螢幕法線109的兩側。 For a transparent microstructure in the transparent microstructure array of this embodiment, on a first plane passing through the transparent microstructure and parallel to the first direction and the screen normal 109, according to the optical reflection theory, along the first plane The cross-section of the plane satisfies the following relationship, when tan α
Figure 106115424-A0305-02-0018-15
-
Figure 106115424-A0305-02-0018-20
Time,
Figure 106115424-A0305-02-0018-24
When tan α
Figure 106115424-A0305-02-0018-16
-
Figure 106115424-A0305-02-0018-22
Time,
Figure 106115424-A0305-02-0018-26
When tan θ
Figure 106115424-A0305-02-0018-17
-tan α,
Figure 106115424-A0305-02-0018-27
When tan θ
Figure 106115424-A0305-02-0018-18
-tan α,
Figure 106115424-A0305-02-0018-29
Where f is the focal length of the light incident surface of the transparent microstructure, d is the width of the light incident surface in the first direction, h is the distance from the light incident surface to the light reflecting surface, and α is the incident angle of the incident light on the first plane , Θ is the angle between the side surface and the screen normal 109, γ is the largest first exit angle of the emitted light corresponding to the incident light in the first plane, β is the largest second exit angle of the emitted light corresponding to the incident light in the first plane The output light corresponding to the first output angle and the output light corresponding to the second output angle are respectively located on both sides of the normal line 109 of the screen.

因此,通過設計透明微結構的光入射面的焦距f、光入射面沿第一方向的寬度d、光反射面到焦平面106的距離h以及側面與螢幕法線109的夾角θ可以相應控制螢幕出射光在第二方向與螢幕法線109所形成的第二平面內的第一出射角和第二出射角,以控制和調整投影螢幕形成的出射光在第二平面內的出射角度範圍。 Therefore, by designing the focal length f of the light incident surface of the transparent microstructure, the width d of the light incident surface along the first direction, the distance h from the light reflecting surface to the focal plane 106, and the angle θ between the side surface and the screen normal 109, the screen can be controlled accordingly. The first exit angle and the second exit angle of the exit light in the second plane formed by the second direction and the screen normal 109 are used to control and adjust the exit angle range of the exit light formed by the projection screen in the second plane.

本發明所述投影螢幕,其透明微結構的光入射面也可採用球面形或抛物面形設計,使得光入射面可以同時調節第一方向和第二方向的出射角範圍。具體的,在本發明投影螢幕的又一種具體實施例中,投影螢幕包括螢幕本體和設置在螢幕本體投射面上的表面結構,該表面結構包括矩陣式排布的透明微結構陣列和反射層。其中,透明微結構包括光入射面和光反射面。 In the projection screen of the present invention, the light incident surface of the transparent microstructure can also adopt a spherical or parabolic design, so that the light incident surface can simultaneously adjust the output angle range of the first direction and the second direction. Specifically, in another specific embodiment of the projection screen of the present invention, the projection screen includes a screen body and a surface structure arranged on the projection surface of the screen body, and the surface structure includes a matrix-arranged transparent microstructure array and a reflective layer. Among them, the transparent microstructure includes a light incident surface and a light reflecting surface.

所述光入射面為對入射光具有會聚作用的、具有預設焦距的球面或者抛物面,其沿第一方向和第二方向的寬度為預設值。光反射面為位於光入射面的焦距範圍內的曲面,在光反射面設置有反射層。其中,該第一方向和第二方向平行於螢幕平面且相互垂直。本發明的球面的焦點和焦距為近軸光學意義上的焦點和焦距。 The light incident surface is a spherical or parabolic surface with a preset focal length that has a convergent effect on the incident light, and its width along the first direction and the second direction is a preset value. The light reflection surface is a curved surface located within the focal length range of the light incident surface, and a reflection layer is provided on the light reflection surface. Wherein, the first direction and the second direction are parallel to the plane of the screen and perpendicular to each other. The focal point and focal length of the spherical surface of the present invention are the focal point and focal length in the sense of paraxial optics.

在任意平行於螢幕法線的平面範圍內,當入射光經光入射面折射進入透明微結構,被聚焦並經光反射面反射後再次由光入射面折射出形成 出射光,所形成出射光的反向延長線在透明微結構內會聚為一個點光源的虛像,出射光可看作是由該點光源發出的光經光入射面射出,因此利用點光源的虛像與光入射面邊緣的位置關係控制出射光在任意平行於螢幕法線的平面內的角度範圍,通過調整光入射面的焦距和寬度、透明微結構的厚度調整螢幕出射光的出射角度範圍。 In any plane range parallel to the normal line of the screen, when the incident light is refracted by the light incident surface into the transparent microstructure, it is focused and reflected by the light reflecting surface and then refracted by the light incident surface again. Outgoing light, the reverse extension of the outgoing light formed is condensed into a virtual image of a point light source in the transparent microstructure. The outgoing light can be regarded as the light emitted by the point light source emitted from the light incident surface, so the virtual image of the point light source is used The positional relationship with the edge of the light incident surface controls the angle range of the emitted light in any plane parallel to the normal line of the screen. The angle range of the emitted light from the screen is adjusted by adjusting the focal length and width of the light incident surface and the thickness of the transparent microstructure.

在本實施例中的球面和抛物面實際與上述實施例中的圓柱面和拋物柱面對出射光角度的調節原理是相同的,所不同的是球面和抛物面調節兩個方向的出射角,而圓柱面和拋物柱面只調節一個方向的出射角。球面和抛物面為圓弧和抛物線的旋轉體,而圓柱面和拋物柱面為圓弧和抛物線的柱面。因此,本發明中的球面和抛物面在任意切面上的圓弧和抛物線及其對應的透明微結構其他部分,都可以參照上述實施例中圓柱面和拋物柱面中沿垂直於柱面方向的切面的設計規則。 The spherical and parabolic surfaces in this embodiment are actually the same as the cylindrical and parabolic surfaces in the above embodiments. The principle of adjusting the angle of the emitted light is the same. The difference is that the spherical and parabolic surfaces adjust the angle of emission in two directions. The surface and the parabolic cylinder only adjust the exit angle in one direction. The spherical surface and the parabola are the rotating bodies of the arc and the parabola, while the cylindrical surface and the parabola are the cylinder of the arc and the parabola. Therefore, in the present invention, the arc and parabola on any tangent surface of the sphere and parabola and other parts of the corresponding transparent microstructure can refer to the tangent surface perpendicular to the cylindrical surface in the cylindrical surface and the parabolic surface in the above embodiment. Design rules.

在本實施例透明微結構的一種實施方式中,光入射面的焦距小於光入射面到光反射面距離的兩倍。具體原理與上述描述相似,此處不再贅述。 In an implementation of the transparent microstructure of this embodiment, the focal length of the light incident surface is less than twice the distance from the light incident surface to the light reflecting surface. The specific principle is similar to the above description, and will not be repeated here.

在本實施例透明微結構的一種結構設計中,光反射面同樣為球面或者抛物面,球面形或者抛物面形的光反射面的焦點位於透明微結構內。在任意平行於螢幕法線的平面內,折射光經光反射面反射被會聚,再次經光入射面折射出,形成的出射光的最大出射角會大於入射角,擴大了出射光在第二方向與螢幕法線所形成的平面內的發散角,保證了出射光的出射範圍。 In a structural design of the transparent microstructure of this embodiment, the light reflecting surface is also spherical or parabolic, and the focal point of the spherical or parabolic light reflecting surface is located in the transparent microstructure. In any plane parallel to the normal line of the screen, the refracted light is converged by the reflection of the light reflecting surface, and then refracted by the light incident surface again. The maximum emergence angle of the formed emergent light will be greater than the incident angle, which expands the emergence of the light in the second direction. The divergence angle in the plane formed by the normal line of the screen ensures the emission range of the emitted light.

在本實施例中,光入射面和光反射面都同時調節了相互垂直的第一方向和第二方向上的出射光角度範圍。其中光反射面對兩個方向的出射光角度調節作為光入射面調節的補充,加強了微結構對出射角的放大功能。假若只用球面或抛物面形的光入射面進行調節,而光反射面採用平面反射面設計,則達到相同的效果需要加大光入射面的曲率,這將可能導致光學設計不符合近軸光學的設計或者導致單個微結構在螢幕上的面積減小、數量增多,使得螢幕製造複雜化。當然,在一些應用場景下,也可以採用光入射面為球面或抛物面,而光反射面為平面的設計方案;同理,上述實施例中光入射面為圓柱面或拋物柱面的情況,也可以將光反射面設計為平面,這樣在製作螢幕時不需要對光反射面進行形狀加工。 In this embodiment, both the light incident surface and the light reflecting surface simultaneously adjust the angle ranges of the emitted light in the first direction and the second direction that are perpendicular to each other. The adjustment of the exit light angle of the light reflecting surface in two directions is used as a supplement to the adjustment of the light incident surface, which strengthens the function of the microstructure to enlarge the exit angle. If only a spherical or parabolic light incident surface is used for adjustment, and the light reflecting surface adopts a flat reflecting surface design, the curvature of the light incident surface needs to be increased to achieve the same effect, which may lead to an optical design that does not conform to the paraxial optics The design may lead to a reduction in the area of a single microstructure on the screen and an increase in the number, which complicates the manufacture of the screen. Of course, in some application scenarios, a design scheme in which the light incident surface is a spherical or parabolic surface and the light reflecting surface is a flat surface can also be adopted; similarly, the case where the light incident surface is a cylindrical surface or a parabolic cylinder in the above embodiment is also applicable. The light-reflecting surface can be designed as a flat surface, so that the shape of the light-reflecting surface does not need to be processed when making the screen.

在實際應用中,根據投射光到達投影螢幕的入射角,相應設計光入射面的焦距,光入射面的寬度,光反射面到光入射面的焦平面的距離,以及光反射面的焦距,來控制螢幕出射光的出射角度範圍,實現以一定入射角的入射光經螢幕反射後以預設角度範圍出射,實現對螢幕出射光在預設角度範圍內增益的效果。 In practical applications, according to the incident angle of the projected light to the projection screen, the focal length of the light incident surface, the width of the light incident surface, the distance from the light reflecting surface to the focal plane of the light incident surface, and the focal length of the light reflecting surface are designed accordingly. Control the exit angle range of the light emitted from the screen, realize that the incident light with a certain incident angle is reflected by the screen and then exit at a preset angle range, so as to achieve the effect of gaining the light emitted from the screen within the preset angle range.

在上述具體實施例中,透明微結構為對稱設計,即球面形或抛物面形的光入射面的對稱中軸與螢幕法線平行,球面形或抛物面形的光反射面的對稱中軸與螢幕法線平行。球面或抛物面的對稱中軸,即為其旋轉對稱軸。這種結構設計,正如上述描述中分析,入射光經投影螢幕透明微結構後形成的出射光,形成的位於螢幕法線一側的第一出射光的出射角γ的角度範圍總大於位於螢幕法線另一側的第二出射光的出射角β的角度範 圍,會對螢幕出射光的出射角度範圍的調整受到限制,不能滿足實際應用中的一些需求。 In the above specific embodiment, the transparent microstructure is a symmetrical design, that is, the symmetry center axis of the spherical or parabolic light incident surface is parallel to the screen normal, and the symmetry center axis of the spherical or parabolic light reflecting surface is parallel to the screen normal . The central axis of symmetry of a spherical or parabolic surface is its rotational symmetry axis. This structure design, just like the analysis in the above description, the incident light formed after the transparent microstructure of the projection screen, the first outgoing light formed on the normal side of the screen, the angle range of the first outgoing light γ is always greater than that of the screen. The angle range of the exit angle β of the second exit light on the other side of the line The adjustment of the angle range of the light emitted by the screen is limited, which cannot meet some requirements in practical applications.

為解決這一問題,在本發明的另一種具體實施例中,作為光入射面的球面或抛物面的對稱中軸與螢幕法線不平行;或者作為光反射面的球面或者抛物面的對稱中軸與螢幕法線不平行;或者作為光入射面的球面或者抛物面的對稱中軸與螢幕法線不平行,同時,作為光反射面的球面或者抛物面的對稱中軸與螢幕法線不平行。採用這種不對稱設計便於更自由地結合入射角調整出射光的出射範圍,可以擴展設計的自由度,可以設計出適宜更多入射角和出射角要求的情況。 To solve this problem, in another specific embodiment of the present invention, the symmetry center axis of the sphere or paraboloid as the light incident surface is not parallel to the screen normal; or the symmetry center axis of the sphere or paraboloid as the light reflecting surface is in line with the screen method. The lines are not parallel; or the symmetry center axis of the sphere or paraboloid as the light incident surface is not parallel to the screen normal, and at the same time, the symmetry center axis of the sphere or paraboloid as the light reflecting surface is not parallel to the screen normal. The use of this asymmetric design facilitates more freely adjusting the emission range of the emitted light in combination with the angle of incidence, can expand the degree of freedom of design, and can be designed to meet the requirements of more incident angles and emission angles.

進一步的,在本發明的一個實施例中,對稱中軸與入射光方向的夾角小於螢幕法線與入射光方向的夾角,該技術方案可以使出射光的出射角沿各個方向分佈更為大小平均。 Further, in an embodiment of the present invention, the angle between the central axis of symmetry and the direction of the incident light is smaller than the angle between the normal of the screen and the direction of the incident light, and this technical solution can make the distribution of the emergence angle of the emergent light more even in all directions.

在本發明投影螢幕的其他實施例中,也可以將上述實施例相結合,得到光入射面為調節第一方向和第二方向兩個方向出射角的球面或抛物面,而光反射面為調節第二方向光出射角的圓柱面或拋物柱面的技術方案;與之類似,還包括光入射面和光反射面各自為圓柱面、拋物柱面、球面或抛物面中的任一個的自由組合。 In other embodiments of the projection screen of the present invention, the above-mentioned embodiments can also be combined to obtain the light incident surface as a spherical or parabolic surface that adjusts the exit angles in the first direction and the second direction, and the light reflecting surface is the adjustable first direction. The technical solution of a cylindrical surface or a parabolic cylindrical surface with two-direction light exit angles; similarly, it also includes a free combination of any one of a cylindrical surface, a parabolic cylindrical surface, a spherical surface, or a parabolic surface on the light incident surface and the light reflecting surface.

在本發明投影螢幕的其他實施例中,光入射面和光反射面中的至少一個為自由曲面,根據具體情況設計該自由曲面的形狀,這樣進一步增加了設計自由度,對任意入射角和出射角的要求都可以設計滿足,可以廣泛滿足各種應用情況。 In other embodiments of the projection screen of the present invention, at least one of the light incident surface and the light reflecting surface is a free-form surface, and the shape of the free-form surface is designed according to the specific situation, which further increases the design freedom. The requirements can be designed to meet, and can be widely used in various applications.

在本發明投影螢幕的其它具體實施例中,在上述各具體實施例的基礎上,該透明微結構還包括連接該光入射面和該光反射面的側面,該側面與預設入射角度的入射光經該光入射面端邊入射形成的折射光平行,該側面設置有光吸收體。 In other specific embodiments of the projection screen of the present invention, on the basis of the above specific embodiments, the transparent microstructure further includes a side surface connecting the light incident surface and the light reflecting surface, and the side surface is opposite to the predetermined incident angle. The refracted light formed by the light incident through the end of the light incident surface is parallel, and the side surface is provided with a light absorber.

一個透明微結構可以具有一個或多個呈曲面或平面的側面,存在一平行入射光,該平行入射光在光入射面與任一側面連接的邊形成的折射光都平行於該側面。其中,光吸收體可以是填充在相鄰該透明微結構的側面之間。 A transparent microstructure may have one or more curved or flat side surfaces, and there is a parallel incident light, and the refracted light formed by the parallel incident light on the side connecting the light incident surface and any side surface is parallel to the side surface. Wherein, the light absorber can be filled between adjacent sides of the transparent microstructure.

這樣,當入射角為其它角度的雜散光照射到透明微結構內,其折射光線會偏折射到側面,會被側面的光吸收體吸收。因此,該透明微結構具有側面,側面設置有光吸收體,能夠將雜散光吸收,使雜散光不會出射到要求的出射角度範圍內,若出射光的出射角度範圍對應於觀看區域,可以使出射到觀看區域的雜散光減少,從而可增強觀看者觀看到螢幕圖像的對比度。 In this way, when the stray light whose incident angle is other angles is irradiated into the transparent microstructure, its refracted light will be deflected to the side surface and will be absorbed by the light absorber on the side surface. Therefore, the transparent microstructure has a side surface, and a light absorber is provided on the side surface, which can absorb stray light so that the stray light will not be emitted within the required output angle range. If the output angle range of the emitted light corresponds to the viewing area, the The stray light emitted to the viewing area is reduced, thereby enhancing the contrast of the screen image viewed by the viewer.

從螢幕的製造成本和製造難易度方面考慮,可以選擇採用螢幕上的透明微結構完全一致的技術方案,這種設計也能夠滿足一定的觀影要求。然而,對於投影螢幕,其平面面積一般比較大,而投影機108放置位置相對螢幕固定,因此投影機108照射到螢幕表面的入射光,照射在螢幕表面不同區域的入射角度會不同,相對觀看區域的出射角度範圍也不同。 Considering the manufacturing cost and difficulty of the screen, a technical solution with the same transparent microstructure on the screen can be selected. This design can also meet certain viewing requirements. However, for projection screens, the plane area is generally relatively large, and the projector 108 is placed at a fixed position relative to the screen. Therefore, the incident light irradiated by the projector 108 on the screen surface will have different incident angles on different areas of the screen surface, relative to the viewing area. The range of exit angles is also different.

基於此,在本發明投影螢幕的另一種具體實施例中,設置在螢幕本體投射面的表面結構至少包括第一區域和第二區域,該第一區域的透明微結構的光入射面的主光軸與該第二區域的透明微結構的光入射面的主光 軸不平行。這裡的光入射面的主光軸過光入射面的焦點,且沿主光軸入射的光不發生折射。 Based on this, in another specific embodiment of the projection screen of the present invention, the surface structure provided on the projection surface of the screen body includes at least a first area and a second area. The main light of the light incident surface of the transparent microstructure of the first area is Axis and the main light of the light incident surface of the transparent microstructure of the second area The axes are not parallel. Here, the main optical axis of the light incident surface passes through the focal point of the light incident surface, and the light incident along the main optical axis is not refracted.

對於投影螢幕的第一區域和第二區域,入射光以不同入射角入射,位於第一區域的透明微結構和位於第二區域的透明微結構的尺寸設計不同,第一區域的透明微結構的光入射面的主光軸與第二區域的透明微結構的光入射面的主光軸不平行,使第一區域和第二區域的透明微結構對入射光可達到不同的出射角度調整效果,所形成出射光對應不同的出射範圍,以滿足對投影螢幕不同區域出射光的出射角度範圍的要求。 For the first area and the second area of the projection screen, the incident light is incident at different incident angles. The size of the transparent microstructure in the first area is different from that of the transparent microstructure in the second area. The size of the transparent microstructure in the first area is different. The main optical axis of the light incident surface is not parallel to the main optical axis of the light incident surface of the transparent microstructure in the second area, so that the transparent microstructures in the first area and the second area can achieve different exit angle adjustment effects for incident light. The formed outgoing light corresponds to different outgoing ranges to meet the requirements for the outgoing angle range of the outgoing light from different areas of the projection screen.

具體到上述實施例中,光入射面為圓柱面、拋物柱面、球面或抛物面,和/或光反射面為圓柱面、拋物柱面、球面或抛物面的情況,可以根據具體影院、投影場景的佈置,進一步細化第一區域和第二區域的光入射面和/或光反射面的區別設計。例如,使第一區域和第二區域的光入射面的主光軸和/或對稱中軸分別沿不同方向設置。 Specifically, in the foregoing embodiment, the light incident surface is cylindrical, parabolic, spherical, or parabolic, and/or the light reflecting surface is cylindrical, parabolic, spherical, or parabolic, depending on the specific theater or projection scene. The arrangement further refines the different design of the light incident surface and/or the light reflecting surface of the first area and the second area. For example, the main optical axis and/or the central axis of symmetry of the light incident surfaces of the first region and the second region are respectively arranged in different directions.

例如,第一區域可對應於投影螢幕的中部區域,第二區域對應於投影螢幕的邊緣區域,根據照射在螢幕中部區域和邊緣區域的投射光不同的入射角度以及對應要求的出射角度範圍,來分別設計不同區域透明微結構的尺寸。 For example, the first area may correspond to the middle area of the projection screen, and the second area may correspond to the edge area of the projection screen. According to the different incident angles of the projection light illuminating the middle area and the edge area of the screen and the corresponding required output angle range, Design the size of the transparent microstructure in different areas respectively.

可以理解的是,在實際應用中,為適應更多應用需求,可對投影螢幕的表面結構劃分更多區域,根據投射光在投影螢幕不同區域以不同的入射角入射,對應不同區域分別設計透明微結構,來分別對應調整螢幕出射光的出射範圍。 It is understandable that in practical applications, in order to meet the needs of more applications, the surface structure of the projection screen can be divided into more areas. According to the projection light incident on different areas of the projection screen at different incident angles, the corresponding areas are designed to be transparent. Microstructure to adjust the emission range of the light emitted from the screen respectively.

必須加以強調的是,以上對本發明所提供的一種投影螢幕進行了詳細介紹。本文中應用了具體個例對本發明的原理及實施方式進行了闡述,以上實施例的說明只是用於幫助理解本發明的方法及其核心思想。應當指出,對於本技術領域的普通技術人員來說,在不脫離本發明原理的前提下,還可以對本發明進行若干改進和修飾,這些改進和修飾也落入本發明權利要求的保護範圍內。 It must be emphasized that a projection screen provided by the present invention has been introduced in detail above. Specific examples are used in this article to illustrate the principle and implementation of the present invention. The description of the above examples is only used to help understand the method and core idea of the present invention. It should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, several improvements and modifications can be made to the present invention, and these improvements and modifications also fall within the protection scope of the claims of the present invention.

100:透明微結構 100: Transparent microstructure

101:光入射面 101: Light incident surface

102:光反射面 102: light reflecting surface

103:反射層 103: reflective layer

Claims (14)

一種投影螢幕,包括一螢幕本體,其中,還包括設置在該螢幕本體投射面上的表面結構;該表面結構包括矩陣式排布的透明微結構陣列以及反射層,其中,該透明微結構包括:對入射光具有會聚作用且具有預設焦距的光入射面,該光入射面的沿第一方向的寬度為預設值,該光入射面用於調整出射光在第一方向與螢幕法線所形成的平面內的方向,使得出射光在該第一方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第一方向與螢幕法線所形成的平面內的入射角;位於該光入射面的焦距範圍內的、曲面形的光反射面,在該光反射面設置有該反射層,該光反射面用於調整出射光在第二方向與螢幕法線所形成的平面內的方向,使得出射光在該第二方向與螢幕法線所形成的平面內的最大出射角大於入射光在該第二方向與螢幕法線所形成的平面內的入射角;該第一方向和該第二方向平行於螢幕平面且相互垂直;在該第二方向與螢幕法線所形成的平面內,所述光反射面具有一焦點,且該焦點位於所述透明微結構內。 A projection screen includes a screen body, which further includes a surface structure arranged on the projection surface of the screen body; the surface structure includes a matrix-arranged transparent microstructure array and a reflective layer, wherein the transparent microstructure includes: A light incident surface that has a convergent effect on the incident light and has a preset focal length. The width of the light incident surface along the first direction is a preset value. The light incident surface is used to adjust the direction of the emitted light in the first direction and the normal line of the screen. The direction in the formed plane is such that the maximum exit angle of the emitted light in the plane formed by the first direction and the screen normal is greater than the incident angle of the incident light in the plane formed by the first direction and the screen normal; A curved light reflection surface within the focal length range of the light incident surface, the reflection layer is provided on the light reflection surface, and the light reflection surface is used to adjust the emitted light in a plane formed by the second direction and the normal line of the screen Direction, so that the maximum exit angle of the emitted light in the plane formed by the second direction and the screen normal is greater than the incident angle of the incident light in the plane formed by the second direction and the screen normal; the first direction and The second direction is parallel to the screen plane and perpendicular to each other; in the plane formed by the second direction and the screen normal, the light reflecting mask has a focal point, and the focal point is located in the transparent microstructure. 如申請專利範圍第1項所述的投影螢幕,其中,該光入射面的焦距小於光入射面到光反射面距離的兩倍。 The projection screen described in item 1 of the scope of patent application, wherein the focal length of the light incident surface is less than twice the distance from the light incident surface to the light reflecting surface. 如申請專利範圍第1項所述之投影螢幕,其中,該光入射面為主軸與該第二方向平行的圓柱面或拋物柱面。 According to the projection screen described in item 1 of the scope of patent application, the light incident surface is a cylindrical surface or a parabolic surface whose main axis is parallel to the second direction. 如申請專利範圍第3項所述之投影螢幕,其中,該光反射面為主軸與該第一方向平行的圓柱面或拋物柱面。 The projection screen described in item 3 of the scope of patent application, wherein the light reflecting surface is a cylindrical surface or a parabolic surface with a main axis parallel to the first direction. 如申請專利範圍第4項所述的投影螢幕,其中,作為光入射面的圓柱面或拋物柱面的對稱中軸與螢幕法線不平行。 The projection screen described in item 4 of the scope of patent application, wherein the central axis of symmetry of the cylindrical or parabolic surface as the light incident surface is not parallel to the screen normal. 如申請專利範圍第4項所述的投影螢幕,其中,作為光反射面的圓柱面或拋物柱面的對稱中軸與螢幕法線不平行。 The projection screen described in item 4 of the scope of patent application, wherein the central axis of symmetry of the cylindrical or parabolic surface as the light reflecting surface is not parallel to the screen normal. 如申請專利範圍第1項所述的投影螢幕,其中,該光入射面為對入射光具有會聚作用且具有該預設焦距的球面或者抛物面。 According to the projection screen described in item 1 of the scope of patent application, the light incident surface is a spherical or parabolic surface that has a convergent effect on the incident light and has the preset focal length. 如申請專利範圍第7項所述的投影螢幕,其中,該光反射面為球面或抛物面。 The projection screen described in item 7 of the scope of patent application, wherein the light reflecting surface is a spherical surface or a parabolic surface. 如申請專利範圍第8項所述的投影螢幕,其中,作為光入射面的球面或抛物面的對稱中軸與螢幕法線不平行。 The projection screen described in item 8 of the scope of patent application, wherein the center axis of symmetry of the spherical or parabolic surface as the light incident surface is not parallel to the normal line of the screen. 如申請專利範圍第8項所述的投影螢幕,其中,作為光反射面的球面或抛物面的對稱中軸與螢幕法線不平行。 The projection screen described in item 8 of the scope of patent application, wherein the center axis of symmetry of the spherical or parabolic surface as the light reflecting surface is not parallel to the normal line of the screen. 如申請專利範圍第1-10項中的任一項所述的投影螢幕,其中,該透明微結構還包括連接該光入射面和該光反射面的側面,該側面與預設入射角度的入射光經該光入射面端邊入射形成的折射光平行,該側面設置有光吸收體。 The projection screen according to any one of items 1-10 in the scope of patent application, wherein the transparent microstructure further includes a side surface connecting the light incident surface and the light reflecting surface, and the side surface is opposite to the predetermined incident angle. The refracted light formed by the light incident through the end of the light incident surface is parallel, and the side surface is provided with a light absorber. 如申請專利範圍第11項所述的投影螢幕,其中,對於所述透明微結構陣列中的一透明微結構,存在穿過該透明微結構且同時平行於第一方向和螢幕法線的第一平面,該透明微結構沿該第一平面的截面滿足以下關係式:當tan α
Figure 106115424-A0305-02-0029-30
-
Figure 106115424-A0305-02-0029-34
時,
Figure 106115424-A0305-02-0029-36
當tan α
Figure 106115424-A0305-02-0029-31
-
Figure 106115424-A0305-02-0029-35
時,
Figure 106115424-A0305-02-0029-37
當tan θ
Figure 106115424-A0305-02-0029-32
-tan α時,
Figure 106115424-A0305-02-0029-38
當tan θ
Figure 106115424-A0305-02-0029-33
-tan α時,
Figure 106115424-A0305-02-0029-39
其中,f為該透明微結構的光入射面的焦距,d為光入射面沿第一方向的寬度,h為光入射面到光反射面的距離,α為入射光在第一平面的入射角,θ為側面與螢幕法線的夾角,γ為入射光對應的出射光在第一平面的最大的第一出射角,β為入射光對應的出射光在第一平面的最大的第二出射角,第一出射角對應的出射光與第二出射角對應的出射光分別位於螢幕法線的兩側。
The projection screen according to claim 11, wherein, for a transparent microstructure in the transparent microstructure array, there is a first transparent microstructure that passes through the transparent microstructure and is parallel to the first direction and the screen normal at the same time. Plane, the cross section of the transparent microstructure along the first plane satisfies the following relationship: when tan α
Figure 106115424-A0305-02-0029-30
-
Figure 106115424-A0305-02-0029-34
Time,
Figure 106115424-A0305-02-0029-36
When tan α
Figure 106115424-A0305-02-0029-31
-
Figure 106115424-A0305-02-0029-35
Time,
Figure 106115424-A0305-02-0029-37
When tan θ
Figure 106115424-A0305-02-0029-32
-tan α,
Figure 106115424-A0305-02-0029-38
When tan θ
Figure 106115424-A0305-02-0029-33
-tan α,
Figure 106115424-A0305-02-0029-39
Where f is the focal length of the light incident surface of the transparent microstructure, d is the width of the light incident surface in the first direction, h is the distance from the light incident surface to the light reflecting surface, and α is the incident angle of the incident light on the first plane , Θ is the angle between the side surface and the screen normal, γ is the largest first exit angle of the emitted light corresponding to the incident light in the first plane, β is the largest second exit angle of the exit light corresponding to the incident light in the first plane , The exit light corresponding to the first exit angle and the exit light corresponding to the second exit angle are respectively located on both sides of the normal line of the screen.
如專利申請範圍第11項所述的投影螢幕,其中,該光吸收體填充在相鄰該透明微結構的側面之間。 The projection screen according to item 11 of the scope of patent application, wherein the light absorber is filled between adjacent sides of the transparent microstructure. 如專利申請範圍第1項所述的投影螢幕,其中,該表面結構至少包括一第一區域和一第二區域,該第一區域和該第二區域分別對應於所述投影螢幕的中部區域和邊緣區域,使得位於該第一區域的該透明微結構的光入射面的主光軸與位於該第二區域的該透明微結構的光入射面的主光軸不平行。 The projection screen according to claim 1, wherein the surface structure at least includes a first area and a second area, and the first area and the second area respectively correspond to the central area and the second area of the projection screen. The edge area makes the main optical axis of the light incident surface of the transparent microstructure located in the first area not parallel to the main optical axis of the light incident surface of the transparent microstructure located in the second area.
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Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002103454A1 (en) 2001-06-18 2002-12-27 Toppan Printing Co., Ltd. Double-sided lens sheet and projection screen
TW200304579A (en) * 2002-03-29 2003-10-01 Toppan Printing Co Ltd Micro-lens sheet and projection screen
CN1837946A (en) * 2005-03-22 2006-09-27 株式会社东芝 Projection type screen and image projection system
CN104111580A (en) * 2013-04-16 2014-10-22 吴小平 Horizontal back family black gate or fresnel back family stripe reflection projection screen

Family Cites Families (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11142975A (en) * 1997-11-13 1999-05-28 Matsushita Electric Ind Co Ltd Reflection type and its manufacture
CN1779560A (en) * 2004-11-26 2006-05-31 精碟科技股份有限公司 Rear-projection screen and optical device thereof
JP5034533B2 (en) * 2006-02-07 2012-09-26 大日本印刷株式会社 Reflective screen
JP2008275971A (en) * 2007-05-01 2008-11-13 Seiko Epson Corp Screen and projection system
JP2009169007A (en) * 2008-01-15 2009-07-30 Kuraray Co Ltd Reflective screen
CN104597707B (en) * 2014-12-24 2016-09-14 深圳雅图数字视频技术有限公司 Optical projection system and screen thereof

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002103454A1 (en) 2001-06-18 2002-12-27 Toppan Printing Co., Ltd. Double-sided lens sheet and projection screen
TW200304579A (en) * 2002-03-29 2003-10-01 Toppan Printing Co Ltd Micro-lens sheet and projection screen
CN1837946A (en) * 2005-03-22 2006-09-27 株式会社东芝 Projection type screen and image projection system
CN104111580A (en) * 2013-04-16 2014-10-22 吴小平 Horizontal back family black gate or fresnel back family stripe reflection projection screen

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