[go: up one dir, main page]

CN116699741A - Optical element and optical module - Google Patents

Optical element and optical module Download PDF

Info

Publication number
CN116699741A
CN116699741A CN202310586724.8A CN202310586724A CN116699741A CN 116699741 A CN116699741 A CN 116699741A CN 202310586724 A CN202310586724 A CN 202310586724A CN 116699741 A CN116699741 A CN 116699741A
Authority
CN
China
Prior art keywords
optical element
angle
optical
light
included angle
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
CN202310586724.8A
Other languages
Chinese (zh)
Inventor
蔡磊
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.)
Focuslight Technologies Inc
Original Assignee
Focuslight Technologies Inc
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 Focuslight Technologies Inc filed Critical Focuslight Technologies Inc
Priority to CN202310586724.8A priority Critical patent/CN116699741A/en
Publication of CN116699741A publication Critical patent/CN116699741A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00Mountings, adjusting means, or light-tight connections, for optical elements

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lenses (AREA)

Abstract

一种光学元件及光学模组,涉及光学技术领域。该光学元件包括相对设置的第一表面、第二表面和第三表面,第一表面为平面且与光轴具有第一夹角,第二表面为凹面且与光轴具有第二夹角,第三表面为平面;入射至第一表面的光束经其折射后偏转入射至第二表面,经第二表面反射后光束自第三表面出射。该光学元件能够减少光学系统沿光轴方向的体积,解决光学系统在单一方向上尺寸受限的问题,提高了光学系统的兼容性。

An optical element and an optical module relate to the field of optical technology. The optical element includes a first surface, a second surface and a third surface oppositely arranged, the first surface is a plane and has a first angle with the optical axis, the second surface is concave and has a second angle with the optical axis, and the second surface is a concave surface with a second angle with the optical axis. The three surfaces are planes; the light beam incident on the first surface is deflected and incident on the second surface after being refracted by it, and the light beam emerges from the third surface after being reflected by the second surface. The optical element can reduce the volume of the optical system along the optical axis, solve the problem that the size of the optical system is limited in a single direction, and improve the compatibility of the optical system.

Description

光学元件及光学模组Optical components and optical modules

技术领域technical field

本发明涉及光学技术领域,具体而言,涉及一种光学元件及光学模组。The invention relates to the field of optical technology, in particular to an optical element and an optical module.

背景技术Background technique

半导体激光器具有体积小、重量轻、可靠性高、使用寿命长、功耗低等优点,目前已经广泛应用于国民经济的各个领域,比如泵浦以及工业加工等领域。Semiconductor lasers have the advantages of small size, light weight, high reliability, long service life, and low power consumption. They have been widely used in various fields of the national economy, such as pumping and industrial processing.

现有的半导体激光器的准直大多采取的是透射式准直,即光束的出光方向与激光器方向平行,这就使得存在以下几种问题,一是光学系统沿光轴方向体积过大;二是当光学系统在安装时存在一定夹角时,光学系统需要做相应角度的夹角设置矫正,极大地减小了系统的兼容性;三是存在灵活度差的问题,不能满足定向出光的需求。The collimation of existing semiconductor lasers mostly adopts transmissive collimation, that is, the light output direction of the beam is parallel to the direction of the laser, which causes the following problems. One is that the volume of the optical system along the optical axis is too large; the other is When the optical system has a certain angle during installation, the optical system needs to be corrected for the corresponding angle setting, which greatly reduces the compatibility of the system; third, there is a problem of poor flexibility, which cannot meet the needs of directional light output.

发明内容Contents of the invention

本发明的目的在于提供一种光学元件及光学模组,其能够减少光学系统沿光轴方向的体积,解决光学系统在单一方向上尺寸受限的问题,提高了光学系统的兼容性。The purpose of the present invention is to provide an optical element and an optical module, which can reduce the volume of the optical system along the optical axis, solve the problem of the limited size of the optical system in a single direction, and improve the compatibility of the optical system.

本发明的实施例是这样实现的:Embodiments of the present invention are achieved like this:

本发明的一方面,提供一种光学元件,该光学元件包括相对设置的第一表面、第二表面和第三表面,第一表面为平面且与光轴具有第一夹角,第二表面为凹面且与光轴具有第二夹角,第三表面为平面;入射至第一表面的光束经其折射后偏转入射至第二表面,经第二表面反射后光束自第三表面出射。该光学元件能够减少光学系统沿光轴方向的体积,解决光学系统在单一方向上尺寸受限的问题,提高了光学系统的兼容性。In one aspect of the present invention, an optical element is provided, the optical element includes a first surface, a second surface and a third surface oppositely arranged, the first surface is a plane and has a first angle with the optical axis, and the second surface is The concave surface has a second angle with the optical axis, and the third surface is a plane; the light beam incident on the first surface is deflected and incident on the second surface after being refracted by it, and the light beam emerges from the third surface after being reflected by the second surface. The optical element can reduce the volume of the optical system along the direction of the optical axis, solve the problem that the size of the optical system is limited in a single direction, and improve the compatibility of the optical system.

可选地,第一夹角不等于90°。通过将第一夹角设置为不等于90°,这样,光学元件的第一表面则相对光轴呈锐角或者钝角设置,如此,最终得到的光学元件的出射光的通光口径能够通过调节第一夹角的具体角度实现相对增大或者相对缩小。Optionally, the first included angle is not equal to 90°. By setting the first included angle to be not equal to 90°, the first surface of the optical element is set at an acute angle or an obtuse angle relative to the optical axis, so that the light aperture of the exit light of the finally obtained optical element can be adjusted by adjusting the first The specific angle of the included angle realizes relative increase or relative reduction.

可选地,第一夹角在30°至150°之间。Optionally, the first included angle is between 30° and 150°.

可选地,当第一夹角为锐角时,由第三表面出射的出射光的通光口径与第一夹角的余角呈正相关;当第一夹角为钝角时,由第三表面出射的出射光的通光口径与第一夹角的补角呈正相关。如此,根据需要通过调整第一夹角便可以实现对该光学元件的出射光的通光口径进行调整。Optionally, when the first included angle is an acute angle, the aperture of the outgoing light emitted from the third surface is positively correlated with the complementary angle of the first included angle; when the first included angle is an obtuse angle, the light emitted from the third surface The aperture of the outgoing light is positively correlated with the supplementary angle of the first included angle. In this way, by adjusting the first included angle as required, the light aperture of the outgoing light of the optical element can be adjusted.

可选地,光学元件满足以下公式:α=2×(45°-θ),其中,α为由第三表面出射的出射光和第一方向之间的夹角,θ为第二夹角,第一方向与光轴垂直。这样,在实际应用时用户可以对第二表面的第二夹角进行调整便可以得到具有特定出光方向的出射光。Optionally, the optical element satisfies the following formula: α=2×(45°-θ), where α is the angle between the outgoing light emitted from the third surface and the first direction, and θ is the second angle, The first direction is perpendicular to the optical axis. In this way, in practical application, the user can adjust the second included angle of the second surface to obtain outgoing light with a specific light outgoing direction.

可选地,光学元件满足第一关系式时,光学元件用于对光源出射的光束进行汇聚,第一关系式为D>R×(n-1);光学元件满足第二关系式时,光学元件用于对光源出射的光束进行准直,第二关系式为D=R×(n-1);光学元件满足第三关系式时,光学元件用于对光源出射的光束进行发散,第三关系式为D<R×(n-1);其中,D为光源至第二表面的中心的距离,R为第二表面的曲率半径,n为光学元件的折射率。如此,通过对第二表面的曲率半径进行调整便可以实现出射光的调节,使得出射光根据需要调整为汇聚光、准直光或者发散光。Optionally, when the optical element satisfies the first relational expression, the optical element is used to converge the light beam emitted by the light source, and the first relational expression is D>R×(n-1); when the optical element satisfies the second relational expression, the optical The element is used to collimate the light beam emitted by the light source, and the second relational expression is D=R×(n-1); when the optical element satisfies the third relational expression, the optical element is used to diverge the light beam emitted by the light source, and the third The relationship is D<R×(n-1); wherein, D is the distance from the light source to the center of the second surface, R is the radius of curvature of the second surface, and n is the refractive index of the optical element. In this way, the adjustment of the outgoing light can be realized by adjusting the radius of curvature of the second surface, so that the outgoing light can be adjusted as converging light, collimated light or divergent light as required.

可选地,第二表面为球面、椭球面、抛物面或者双曲面。Optionally, the second surface is a sphere, an ellipsoid, a parabola or a hyperboloid.

可选地,第二表面上镀设有反射膜。本申请通过在第二表面上增设反射膜,这样,可以增加第二表面的反射率,进而提高光学元件的光利用率。Optionally, a reflective film is coated on the second surface. In the present application, by adding a reflective film on the second surface, the reflectivity of the second surface can be increased, thereby improving the light utilization rate of the optical element.

本发明的另一方面,提供一种光学模组,该光学模组包括光源和设于光源出光侧的上述的光学元件,光源出射的光束经光学元件的第一表面的折射后偏转入射至光学元件的第二表面,经第二表面反射后自第三表面出射。该光学模组能够减少光学系统沿光轴方向的体积,解决光学系统在单一方向上尺寸受限的问题,提高了光学系统的兼容性。Another aspect of the present invention provides an optical module, the optical module includes a light source and the above-mentioned optical element arranged on the light output side of the light source, the light beam emitted by the light source is deflected and incident on the optical The second surface of the element emits from the third surface after being reflected by the second surface. The optical module can reduce the volume of the optical system along the optical axis, solve the problem that the size of the optical system is limited in a single direction, and improve the compatibility of the optical system.

本发明的有益效果包括:The beneficial effects of the present invention include:

本申请提供的光学元件包括相对设置的第一表面、第二表面和第三表面,第一表面为平面且与光轴具有第一夹角,第二表面为凹面且与光轴具有第二夹角,第三表面为平面;入射至第一表面的光束经其折射后偏转入射至第二表面,经第二表面反射后光束自第三表面出射。本申请通过在光学元件上分别设置第一表面、第二表面和第三表面,且使得入射至第一表面的光束能够被偏转至第二表面,进而经过第二表面的反射后能够自第三表面出射,这样,本申请能够减少光学元件沿光轴方向的尺寸,能够解决光学系统在单一方向尺寸受限的问题。即,该光学元件对安装位置的单一方向的尺寸要求较低,其装配灵活度较高,能够提高光学系统的兼容性;另外,本申请通过如上设计,还能够减少元件数量、降低光学元件的成本和重量。The optical element provided by the present application includes a first surface, a second surface and a third surface oppositely arranged, the first surface is a plane and has a first included angle with the optical axis, and the second surface is concave and has a second included angle with the optical axis Angle, the third surface is a plane; the light beam incident on the first surface is deflected and incident on the second surface after being refracted by it, and the light beam emerges from the third surface after being reflected by the second surface. In the present application, the first surface, the second surface and the third surface are respectively arranged on the optical element, and the light beam incident on the first surface can be deflected to the second surface, and then can be reflected from the third surface after being reflected by the second surface. In this way, the present application can reduce the size of the optical element along the optical axis direction, and can solve the problem that the size of the optical system is limited in a single direction. That is, the optical element has lower requirements on the size of the installation position in a single direction, and its assembly flexibility is higher, which can improve the compatibility of the optical system; in addition, the application can also reduce the number of elements and reduce the cost of the optical element through the above design. cost and weight.

附图说明Description of drawings

为了更清楚地说明本发明实施例的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,应当理解,以下附图仅示出了本发明的某些实施例,因此不应被看作是对范围的限定,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他相关的附图。In order to illustrate the technical solutions of the embodiments of the present invention more clearly, the accompanying drawings used in the embodiments will be briefly introduced below. It should be understood that the following drawings only show some embodiments of the present invention, and thus It should be regarded as a limitation on the scope, and those skilled in the art can also obtain other related drawings based on these drawings without creative work.

图1为本发明实施例提供的光学元件的结构示意图之一;Fig. 1 is one of the structural schematic diagrams of the optical element provided by the embodiment of the present invention;

图2为本发明实施例提供的光学元件的结构示意图之二;Fig. 2 is the second structural schematic diagram of the optical element provided by the embodiment of the present invention;

图3为本发明实施例提供的光学元件的结构示意图之三;Fig. 3 is the third structural schematic diagram of the optical element provided by the embodiment of the present invention;

图4为本发明实施例提供的光学元件的结构示意图之四;Fig. 4 is the fourth schematic structural view of the optical element provided by the embodiment of the present invention;

图5为本发明实施例提供的光学元件的结构示意图之五;Fig. 5 is the fifth structural schematic diagram of the optical element provided by the embodiment of the present invention;

图6为本发明实施例提供的光学元件的结构示意图之六;Fig. 6 is the sixth schematic diagram of the structure of the optical element provided by the embodiment of the present invention;

图7为本发明实施例提供的光学元件的结构示意图之七。FIG. 7 is a seventh schematic diagram of the structure of the optical element provided by the embodiment of the present invention.

图标:10-光学元件;11-第一表面;12-第二表面;13-第三表面;20-光源。Icons: 10 - optical element; 11 - first surface; 12 - second surface; 13 - third surface; 20 - light source.

具体实施方式Detailed ways

为使本发明实施例的目的、技术方案和优点更加清楚,下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明一部分实施例,而不是全部的实施例。通常在此处附图中描述和示出的本发明实施例的组件可以以各种不同的配置来布置和设计。In order to make the purpose, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the drawings in the embodiments of the present invention. Obviously, the described embodiments It is a part of embodiments of the present invention, but not all embodiments. The components of the embodiments of the invention generally described and illustrated in the figures herein may be arranged and designed in a variety of different configurations.

因此,以下对在附图中提供的本发明的实施例的详细描述并非旨在限制要求保护的本发明的范围,而是仅仅表示本发明的选定实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。Accordingly, the following detailed description of the embodiments of the invention provided in the accompanying drawings is not intended to limit the scope of the claimed invention, but merely represents selected embodiments of the invention. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without creative efforts fall within the protection scope of the present invention.

应注意到:相似的标号和字母在下面的附图中表示类似项,因此,一旦某一项在一个附图中被定义,则在随后的附图中不需要对其进行进一步定义和解释。It should be noted that like numerals and letters denote similar items in the following figures, therefore, once an item is defined in one figure, it does not require further definition and explanation in subsequent figures.

在本发明的描述中,需要说明的是,术语“中心”、“上”、“下”、“左”、“右”、“竖直”、“水平”、“内”、“外”等指示的方位或位置关系为基于附图所示的方位或位置关系,或者是该发明产品使用时惯常摆放的方位或位置关系,仅是为了便于描述本发明和简化描述,而不是指示或暗示所指的装置或元件必须具有特定的方位、以特定的方位构造和操作,因此不能理解为对本发明的限制。此外,术语“第一”、“第二”、“第三”等仅用于区分描述,而不能理解为指示或暗示相对重要性。In the description of the present invention, it should be noted that the terms "center", "upper", "lower", "left", "right", "vertical", "horizontal", "inner", "outer" etc. The indicated orientation or positional relationship is based on the orientation or positional relationship shown in the drawings, or the orientation or positional relationship that is usually placed when the product of the invention is used, and is only for the convenience of describing the present invention and simplifying the description, rather than indicating or implying References to devices or elements must have a particular orientation, be constructed, and operate in a particular orientation and therefore should not be construed as limiting the invention. In addition, the terms "first", "second", "third", etc. are only used for distinguishing descriptions, and should not be construed as indicating or implying relative importance.

此外,术语“水平”、“竖直”等术语并不表示要求部件绝对水平或悬垂,而是可以稍微倾斜。如“水平”仅仅是指其方向相对“竖直”而言更加水平,并不是表示该结构一定要完全水平,而是可以稍微倾斜。Furthermore, the terms "horizontal", "vertical" and the like do not imply that a component is absolutely level or overhanging, but may be slightly inclined. For example, "horizontal" only means that its direction is more horizontal than "vertical", and it does not mean that the structure must be completely horizontal, but can be slightly inclined.

在本发明的描述中,还需要说明的是,除非另有明确的规定和限定,术语“设置”、“安装”、“相连”、“连接”应做广义理解,例如,可以是固定连接,也可以是可拆卸连接,或一体地连接;可以是机械连接,也可以是电连接;可以是直接相连,也可以通过中间媒介间接相连,可以是两个元件内部的连通。对于本领域的普通技术人员而言,可以具体情况理解上述术语在本发明中的具体含义。In the description of the present invention, it should also be noted that, unless otherwise clearly specified and limited, the terms "installation", "installation", "connection" and "connection" should be understood in a broad sense, for example, it may be a fixed connection, It can also be a detachable connection or an integral connection; it can be a mechanical connection or an electrical connection; it can be a direct connection or an indirect connection through an intermediary, and it can be the internal communication of two components. Those of ordinary skill in the art can understand the specific meanings of the above terms in the present invention in specific situations.

请参照图1,本实施例提供一种光学元件10,该光学元件10包括相对设置的第一表面11、第二表面12和第三表面13,第一表面11为平面且与光轴具有第一夹角,第二表面12为凹面且与光轴具有第二夹角,第三表面13为平面;入射至第一表面11的光束经其折射后偏转入射至第二表面12,经第二表面12反射后光束自第三表面13出射。该光学元件10能够减少光学系统沿光轴方向的体积,解决光学系统在单一方向上尺寸受限的问题,提高了光学系统的兼容性。Please refer to FIG. 1 , the present embodiment provides an optical element 10, the optical element 10 includes a first surface 11, a second surface 12 and a third surface 13 oppositely arranged, the first surface 11 is a plane and has a distance from the optical axis An included angle, the second surface 12 is a concave surface and has a second included angle with the optical axis, and the third surface 13 is a plane; the light beam incident on the first surface 11 is deflected and incident on the second surface 12 after being refracted by it, and passed through the second The light beam is emitted from the third surface 13 after being reflected by the surface 12 . The optical element 10 can reduce the volume of the optical system along the optical axis, solve the problem that the size of the optical system is limited in a single direction, and improve the compatibility of the optical system.

需要说明的是,第一,上述第一表面11为该光学元件10的入光面,入射至该光学元件10的光束将从第一表面11入射。It should be noted that, firstly, the above-mentioned first surface 11 is a light-incident surface of the optical element 10 , and the light beam incident on the optical element 10 will be incident from the first surface 11 .

在本实施例中,第一表面11为平面,且第一表面11与光轴之间具有第一夹角。In this embodiment, the first surface 11 is a plane, and there is a first angle between the first surface 11 and the optical axis.

示例性地,上述第一夹角不等于90°。换言之,第一夹角为锐角或者钝角,也就是说,第一表面11相对光轴是呈倾斜设置的。通过将第一夹角设置为不等于90°,这样,光学元件10的第一表面11则相对光轴呈锐角或者钝角设置。当第一夹角为锐角时,自第一表面11入射的光束能够在第一表面11处发生折射偏转,然后入射至第二表面12,如此,最终得到的光学元件10的出射光的通光口径能够相对第一夹角为90°时增大;当第一夹角为钝角时,最终得到的光学元件10的出射光的通光口径能够相对第一夹角为90°时缩小。Exemplarily, the above-mentioned first included angle is not equal to 90°. In other words, the first included angle is an acute angle or an obtuse angle, that is, the first surface 11 is inclined relative to the optical axis. By setting the first angle not equal to 90°, the first surface 11 of the optical element 10 is set at an acute angle or an obtuse angle with respect to the optical axis. When the first included angle is an acute angle, the light beam incident from the first surface 11 can be refracted and deflected at the first surface 11, and then incident to the second surface 12, so that the finally obtained optical element 10 can pass through the light The caliber can be increased when the first included angle is 90°; when the first included angle is an obtuse angle, the finally obtained optical aperture of the outgoing light of the optical element 10 can be reduced when the first included angle is 90°.

在本实施例中,上述第一夹角在30°至150°之间。例如,第一夹角可以为30°、50°、100°、120°、150°等。第一夹角的具体角度值本申请不做限制,本领域技术人员可以根据需要自行选择合适角度。In this embodiment, the first included angle is between 30° and 150°. For example, the first included angle may be 30°, 50°, 100°, 120°, 150° and so on. The specific angle value of the first included angle is not limited in the present application, and those skilled in the art can select an appropriate angle according to needs.

第二,第二表面12位于第一表面11的出光侧,该第二表面12为凹面,且其与光轴之间具有第二夹角。在本实施例中,第二表面12用于反射光束。具体地,第二表面12能够将第一表面11出射的光束反射至第三表面13。Second, the second surface 12 is located on the light emitting side of the first surface 11 , the second surface 12 is concave, and has a second included angle with the optical axis. In this embodiment, the second surface 12 is used to reflect light beams. Specifically, the second surface 12 can reflect the light beam emitted from the first surface 11 to the third surface 13 .

其中,第二表面12的第二夹角是第二表面12与光轴之间的夹角,如图1和图2所示,第二夹角为θ。Wherein, the second included angle of the second surface 12 is the included angle between the second surface 12 and the optical axis, as shown in FIG. 1 and FIG. 2 , the second included angle is θ.

在本实施例中,第二夹角θ的取值可以为锐角,例如,该第二夹角θ可以为30°、45°或者60°等。In this embodiment, the value of the second included angle θ may be an acute angle, for example, the second included angle θ may be 30°, 45°, or 60°.

第三,上述第三表面13为平面,该第三表面13位于第二表面12的出光侧,在本实施例中,第三表面13为该光学元件10的出光面。Thirdly, the above-mentioned third surface 13 is a plane, and the third surface 13 is located on the light emitting side of the second surface 12 . In this embodiment, the third surface 13 is the light emitting surface of the optical element 10 .

在本实施例中,第一表面11、第二表面12和第三表面13均为该光学元件10的表面,即第一表面11、第二表面12和第三表面13为同一材质所连接的一体结构。这样,一个光学元件10便可以实现光束的角度偏转,能够缩小元件体积。In this embodiment, the first surface 11, the second surface 12 and the third surface 13 are all surfaces of the optical element 10, that is, the first surface 11, the second surface 12 and the third surface 13 are connected by the same material One structure. In this way, an optical element 10 can realize the angular deflection of the light beam, and the volume of the element can be reduced.

在本实施例中,如图1所示,三个表面依次连接以形成一体式的光学元件10。在本实施例中,出光面(即第三表面13)与光轴平行,也就是说,本申请的光学元件10的出光方向和入射至第一表面11的入射光的方向垂直。In this embodiment, as shown in FIG. 1 , the three surfaces are sequentially connected to form an integrated optical element 10 . In this embodiment, the light emitting surface (ie, the third surface 13 ) is parallel to the optical axis, that is, the light emitting direction of the optical element 10 of the present application is perpendicular to the direction of the incident light incident on the first surface 11 .

综上所述,本申请提供的光学元件10包括相对设置的第一表面11、第二表面12和第三表面13,第一表面11为平面且与光轴具有第一夹角,第二表面12为凹面且与光轴具有第二夹角,第三表面13为平面;入射至第一表面11的光束经其折射后偏转入射至第二表面12,经第二表面12反射后光束自第三表面13出射。本申请通过在光学元件10上分别设置第一表面11、第二表面12和第三表面13,且使得入射至第一表面11的光束能够被偏转至第二表面12,进而经过第二表面12的反射后能够自第三表面13出射,这样,本申请能够减少光学元件10沿光轴方向的尺寸,能够解决光学系统在单一方向尺寸受限的问题。即,该光学元件10对安装位置的单一方向的尺寸要求较低,其装配灵活度较高,能够提高光学系统的兼容性;另外,本申请通过如上设计,还能够减少元件数量、降低光学元件10的成本和重量。In summary, the optical element 10 provided by the present application includes a first surface 11, a second surface 12 and a third surface 13 oppositely arranged, the first surface 11 is a plane and has a first angle with the optical axis, and the second surface 12 is a concave surface and has a second angle with the optical axis, and the third surface 13 is a plane; the light beam incident on the first surface 11 is deflected and incident on the second surface 12 after being refracted by it, and the light beam is reflected from the second surface 12 from the second surface 12 Three surfaces 13 emerge. In the present application, the first surface 11, the second surface 12, and the third surface 13 are respectively arranged on the optical element 10, and the light beam incident on the first surface 11 can be deflected to the second surface 12, and then passes through the second surface 12 After reflection, the light can emerge from the third surface 13. In this way, the present application can reduce the size of the optical element 10 along the optical axis direction, and can solve the problem that the size of the optical system is limited in a single direction. That is to say, the optical element 10 has low requirements on the size of the installation position in a single direction, and its assembly flexibility is high, which can improve the compatibility of the optical system; in addition, the application can also reduce the number of components and reduce the number of optical components through the above design. 10 for cost and weight.

请参照图3和图4,可选地,当第一夹角为锐角时,由第三表面13出射的出射光的通光口径与第一夹角的余角呈正相关;当第一夹角为钝角时,由第三表面13出射的出射光的通光口径与第一夹角的补角呈正相关。Please refer to Fig. 3 and Fig. 4, optionally, when the first included angle is an acute angle, the aperture of the outgoing light emitted by the third surface 13 is positively correlated with the complementary angle of the first included angle; when the first included angle When the angle is an obtuse angle, the aperture of the light emitted from the third surface 13 is positively correlated with the supplementary angle of the first included angle.

在图3和图4中,图3是以第一夹角为锐角为例,B表示通光口径,β为第一夹角的余角,θ0/2为1/2的光源20的发散角。In Fig. 3 and Fig. 4, Fig. 3 is an example where the first included angle is an acute angle, B represents the aperture of the light, β is the complementary angle of the first included angle, and θ 0 /2 is the divergence of the light source 20 of 1/2 horn.

通过对比图3和图4可以发现,在光源20的发散角不变的情况下,调整第一夹角的余角β,第一表面11的偏转角度会发生改变,对应地,自第二表面12反射后,从第三表面13出射的出射光的通光口径B也会发生变化。具体地,第三表面13出射的出射光的通光口径与第一夹角的余角呈正相关。即,第一夹角的余角β增大时,相应地,第三表面13出射的出射光的通光口径B也会增大。因此,用户可以根据光学元件10所需的出射光的通光口径去调整第一表面11的第一夹角的余角的大小(或者调整第一表面11的第一夹角的大小)。当然,当第一夹角为钝角时,也可以通过调整第一夹角的补角来实现由第三表面13出射的出射光的通光口径的大小的调节。由于当第一夹角为钝角时,由第三表面13出射的出射光的通光口径与第一夹角的补角也呈正相关,故调节方式本申请不再赘述。By comparing Fig. 3 and Fig. 4, it can be found that, under the condition that the divergence angle of the light source 20 remains unchanged, adjusting the complementary angle β of the first included angle, the deflection angle of the first surface 11 will change, correspondingly, from the second surface After reflection by 12 , the aperture B of the outgoing light emitted from the third surface 13 will also change. Specifically, the aperture of the light emitted from the third surface 13 is positively correlated with the complementary angle of the first included angle. That is, when the complementary angle β of the first included angle increases, correspondingly, the aperture B of the outgoing light emitted from the third surface 13 will also increase. Therefore, the user can adjust the size of the complementary angle of the first included angle of the first surface 11 (or adjust the size of the first included angle of the first surface 11 ) according to the required aperture of the outgoing light of the optical element 10 . Of course, when the first included angle is an obtuse angle, the size of the aperture of the light emitted from the third surface 13 can also be adjusted by adjusting the supplementary angle of the first included angle. Since when the first included angle is an obtuse angle, the aperture of the outgoing light emitted from the third surface 13 is also positively correlated with the supplementary angle of the first included angle, so the adjustment method will not be repeated in this application.

请参照图1和图2,可选地,光学元件10满足以下公式:α=2×(45°-θ),其中,α为由第三表面13出射的出射光和第一方向之间的夹角,θ为第二夹角,第一方向与光轴垂直。1 and 2, optionally, the optical element 10 satisfies the following formula: α=2×(45°-θ), where α is the distance between the outgoing light emitted by the third surface 13 and the first direction included angle, θ is the second included angle, and the first direction is perpendicular to the optical axis.

即,请参考图1,图1示出的第二夹角θ等于45°,当θ等于45°时,对应的,由第三表面13出射的出射光和第一方向之间的夹角α为0°,即由第三表面13出射的出射光和第一方向无夹角,这样,由第三表面13出射的出射光将垂直出射,如图1所示。That is, please refer to FIG. 1. The second included angle θ shown in FIG. 1 is equal to 45°. When θ is equal to 45°, correspondingly, the included angle α between the outgoing light emitted by the third surface 13 and the first direction is 0°, that is, there is no included angle between the outgoing light emitted from the third surface 13 and the first direction, so that the emitted light emitted from the third surface 13 will exit vertically, as shown in FIG. 1 .

请参考图2,图2示出的第二夹角θ大于45°,当θ大于45°时,对应的,由第三表面13出射的出射光和第一方向之间的夹角α与第一方向有夹角,但是该夹角向第二象限偏转,这样,通过调整第二夹角θ的角度值便可以实现光学元件10的出射光朝向指定方向出射。Please refer to FIG. 2. The second included angle θ shown in FIG. 2 is greater than 45°. When θ is greater than 45°, correspondingly, the angle α between the outgoing light emitted by the third surface 13 and the first direction is different from the first direction. There is an included angle in one direction, but the included angle is deflected toward the second quadrant. In this way, by adjusting the angle value of the second included angle θ, the outgoing light of the optical element 10 can be realized to exit in a specified direction.

应理解,当需要光学元件10的出射光朝向第一象限出射时,则对应的,上述第二夹角θ应当小于45°。It should be understood that when the outgoing light of the optical element 10 needs to exit toward the first quadrant, correspondingly, the above-mentioned second included angle θ should be smaller than 45°.

请参照图5至图7,光学元件10满足第一关系式时,光学元件10用于对光源20出射的光束进行汇聚,第一关系式为D>R×(n-1);光学元件10满足第二关系式时,光学元件10用于对光源20出射的光束进行准直,第二关系式为D=R×(n-1);光学元件10满足第三关系式时,光学元件10用于对光源20出射的光束进行发散,第三关系式为D<R×(n-1);Please refer to FIG. 5 to FIG. 7, when the optical element 10 satisfies the first relational expression, the optical element 10 is used to converge the light beam emitted by the light source 20, and the first relational expression is D>R×(n-1); the optical element 10 When the second relational expression is satisfied, the optical element 10 is used to collimate the light beam emitted by the light source 20, and the second relational expression is D=R×(n-1); when the optical element 10 satisfies the third relational expression, the optical element 10 For diverging the light beam emitted by the light source 20, the third relational expression is D<R×(n-1);

其中,D为光源20至第二表面12的中心的距离,R为第二表面12的曲率半径,n为光学元件10的折射率。Wherein, D is the distance from the light source 20 to the center of the second surface 12 , R is the radius of curvature of the second surface 12 , and n is the refractive index of the optical element 10 .

示例地,请参照图5所示,当需要自第三表面13出射的出射光为汇聚光时,则对应地,光源20至第二表面12的中心的距离D和第二表面12的曲率半径R需要满足该关系式D>R×(n-1)。For example, please refer to FIG. 5 , when the outgoing light from the third surface 13 needs to be converging light, then correspondingly, the distance D from the light source 20 to the center of the second surface 12 and the radius of curvature of the second surface 12 R needs to satisfy the relationship D>R×(n−1).

请参照图6所示,当需要自第三表面13出射的出射光为准直光时,则对应地,光源20至第二表面12的中心的距离D和第二表面12的曲率半径R需要满足该关系式D=R×(n-1)。Please refer to FIG. 6, when the outgoing light from the third surface 13 needs to be collimated light, correspondingly, the distance D from the light source 20 to the center of the second surface 12 and the radius of curvature R of the second surface 12 need This relational expression D=R×(n−1) is satisfied.

请参照图7所示,当需要自第三表面13出射的出射光为发散光时,则对应地,光源20至第二表面12的中心的距离D和第二表面12的曲率半径R需要满足该关系式D<R×(n-1)。Please refer to FIG. 7, when the outgoing light from the third surface 13 needs to be divergent light, correspondingly, the distance D from the light source 20 to the center of the second surface 12 and the radius of curvature R of the second surface 12 need to satisfy This relational expression D<R×(n-1).

这样,用户可以根据光学元件10所需的出射光的类型,只需要对光源20至第二表面12的中心的距离D和第二表面12的曲率半径R进行适当调整即可实现,其操作方式简单。In this way, the user can adjust the distance D from the light source 20 to the center of the second surface 12 and the radius of curvature R of the second surface 12 according to the type of outgoing light required by the optical element 10. Simple.

本申请提供的光学元件10通过设置第一表面11、第二表面12和第三表面13,且将三个表面的相关光学参数进行关联设置,这样,只需要对相应表面的光学参数进行适当调整便可以实现光学元件10的出射光的高灵活度输出和高自由度以及兼容性的输出,该光学元件10结构简单、体积小,且对光学元件10的单一方向的尺寸要求低,能够应用于多种场合,具有较佳的应用场景和实用价值。The optical element 10 provided by the present application sets the first surface 11, the second surface 12 and the third surface 13, and correlates the relevant optical parameters of the three surfaces, so that only the optical parameters of the corresponding surfaces need to be adjusted appropriately The output of high flexibility, high degree of freedom and compatibility of the outgoing light of the optical element 10 can be realized. The optical element 10 is simple in structure, small in size, and has low requirements on the size of the optical element 10 in a single direction, and can be used in It has better application scenarios and practical value in various occasions.

在本实施例中,可选地,上述第二表面12为球面、椭球面、抛物面或者双曲面。其中,第二表面12的面型的具体选用本申请不做限制,本领域技术人员可以自行选择确定。In this embodiment, optionally, the above-mentioned second surface 12 is a spherical surface, an ellipsoid, a paraboloid or a hyperboloid. Wherein, the specific selection of the surface shape of the second surface 12 is not limited in this application, and those skilled in the art can choose and determine it by themselves.

为进一步提高第二表面12的反射率,从而有效提高光学元件10的光利用率,可选地,第二表面12上镀设有反射膜。In order to further increase the reflectivity of the second surface 12 , thereby effectively improving the light utilization efficiency of the optical element 10 , optionally, a reflective film is coated on the second surface 12 .

本发明的另一方面,提供一种光学模组,该光学模组包括光源20和设于光源20出光侧的上述的光学元件10,光源20出射的光束经光学元件10的第一表面11的折射后偏转入射至光学元件10的第二表面12,经第二表面12反射后自第三表面13出射。Another aspect of the present invention provides an optical module, the optical module includes a light source 20 and the above-mentioned optical element 10 disposed on the light output side of the light source 20, the light beam emitted by the light source 20 passes through the first surface 11 of the optical element 10 After refraction, the incident light is deflected to the second surface 12 of the optical element 10 , and is emitted from the third surface 13 after being reflected by the second surface 12 .

由于该光学元件10的具体结构、光路原理及其有益效果均已在前文中进行了详细阐述与说明,故本申请在此不再赘述。Since the specific structure, optical path principle and beneficial effects of the optical element 10 have been described and illustrated in detail above, the present application will not repeat them here.

需要说明的是,该光学模组可以应用于激光雷达、工业加工等领域。本申请对该光学模组的应用领域不做具体限制。It should be noted that this optical module can be used in lidar, industrial processing and other fields. The present application does not specifically limit the application field of the optical module.

以上所述仅为本发明的可选实施例而已,并不用于限制本发明,对于本领域的技术人员来说,本发明可以有各种更改和变化。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above descriptions are only optional embodiments of the present invention, and are not intended to limit the present invention. For those skilled in the art, the present invention may have various modifications and changes. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.

另外需要说明的是,在上述具体实施方式中所描述的各个具体技术特征,在不矛盾的情况下,可以通过任何合适的方式进行组合,为了避免不必要的重复,本发明对各种可能的组合方式不再另行说明。In addition, it should be noted that the various specific technical features described in the above specific embodiments can be combined in any suitable way if there is no contradiction. The combination method will not be described separately.

Claims (9)

1. An optical element is characterized by comprising a first surface, a second surface and a third surface which are oppositely arranged, wherein the first surface is a plane and has a first included angle with an optical axis, the second surface is a concave surface and has a second included angle with the optical axis, and the third surface is a plane;
the light beam incident on the first surface is deflected to be incident on the second surface after being refracted, and the light beam is emitted from the third surface after being reflected by the second surface.
2. An optical element as claimed in claim 1, wherein the first included angle is not equal to 90 °.
3. The optical element of claim 2, wherein the first included angle is between 30 ° and 150 °.
4. An optical element according to any one of claims 1 to 3, wherein when the first included angle is an acute angle, the light passing aperture of the outgoing light outgoing from the third surface is positively correlated with the complementary angle of the first included angle; when the first included angle is an obtuse angle, the light passing caliber of the emergent light emitted from the third surface is positively correlated with the complementary angle of the first included angle.
5. The optical element of claim 1, wherein the optical element satisfies the following formula: α=2× (45 ° - θ), where α is an angle between the outgoing light outgoing from the third surface and a first direction, θ is the second angle, and the first direction is perpendicular to the optical axis.
6. The optical element according to claim 1 or 5, wherein when the optical element satisfies a first relation, the optical element is configured to converge a light beam emitted from a light source, and the first relation is D > r× (n-1); when the optical element meets a second relation, the optical element is used for collimating the light beam emitted by the light source, and the second relation is D=R× (n-1); when the optical element meets a third relation, the optical element is used for diverging the light beam emitted by the light source, and the third relation is D < R× (n-1);
wherein D is a distance from the light source to a center of the second surface, R is a radius of curvature of the second surface, and n is a refractive index of the optical element.
7. The optical element of claim 1, wherein the second surface is spherical, ellipsoidal, parabolic, or hyperbolic.
8. The optical element of claim 1, wherein the second surface is coated with a reflective film.
9. An optical module, comprising a light source and the optical element according to any one of claims 1 to 8 disposed on a light emitting side of the light source, wherein a light beam emitted from the light source is deflected by refraction of a first surface of the optical element and then enters a second surface of the optical element, and is reflected by the second surface and then exits from the third surface.
CN202310586724.8A 2023-05-23 2023-05-23 Optical element and optical module Pending CN116699741A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202310586724.8A CN116699741A (en) 2023-05-23 2023-05-23 Optical element and optical module

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202310586724.8A CN116699741A (en) 2023-05-23 2023-05-23 Optical element and optical module

Publications (1)

Publication Number Publication Date
CN116699741A true CN116699741A (en) 2023-09-05

Family

ID=87826910

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202310586724.8A Pending CN116699741A (en) 2023-05-23 2023-05-23 Optical element and optical module

Country Status (1)

Country Link
CN (1) CN116699741A (en)

Similar Documents

Publication Publication Date Title
CN103471036B (en) Lighting effect theoretically nondestructive LED (Light Emitting Diode) light total reflection collimation system
CN114172015B (en) Focusing coupling light path of semiconductor laser
CN101943369B (en) a lens
EP4170229A1 (en) Vehicle lamp optical component, vehicle lamp module, and vehicle
WO2021129501A1 (en) Package structure for improving light spot shape
US11675144B2 (en) Laser module
CN211786401U (en) Packaging structure for improving shape of light spot
CN209801374U (en) Polarizing lens with large deflection angle and lamp
CN116699741A (en) Optical element and optical module
CN114814792A (en) A laser radar optical transmitter
CN220323631U (en) Refractive optical unit
US9110224B2 (en) Reflector with focused output
CN216958847U (en) Optical path system of laser and laser
CN217036313U (en) A dual-fiber semiconductor laser
CN112769038A (en) Slow axis collimation and space beam combination prism and semiconductor laser
CN206280919U (en) light emitting device
CN116699861A (en) Beam collimation assembly and laser emission device
CN116697296A (en) Light source coupling structure
TWI547667B (en) Light-emitting module and light-emitting device
CN212009268U (en) Low-cost high-power projection illumination dodging system
CN210511509U (en) Lens and optical system
CN110703450A (en) Beam Shaping Components, Modules and Laser Modules
CN219498481U (en) Laser module
CN219302659U (en) Transmitting module and laser radar
US20140098518A1 (en) Device for the beam shaping of light

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination