WO2018137312A1 - Fluorescent module and relevant light source - Google Patents

Fluorescent module and relevant light source Download PDF

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Publication number
WO2018137312A1
WO2018137312A1 PCT/CN2017/090332 CN2017090332W WO2018137312A1 WO 2018137312 A1 WO2018137312 A1 WO 2018137312A1 CN 2017090332 W CN2017090332 W CN 2017090332W WO 2018137312 A1 WO2018137312 A1 WO 2018137312A1
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Prior art keywords
light
wavelength conversion
conversion layer
fluorescent
substrate
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PCT/CN2017/090332
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French (fr)
Chinese (zh)
Inventor
胡飞
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深圳市绎立锐光科技开发有限公司
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Publication of WO2018137312A1 publication Critical patent/WO2018137312A1/en

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Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K2/00Non-electric light sources using luminescence; Light sources using electrochemiluminescence
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K9/00Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
    • F21K9/20Light sources comprising attachment means
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V17/00Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages
    • F21V17/10Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages characterised by specific fastening means or way of fastening
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V7/00Reflectors for light sources

Definitions

  • the utility model relates to the field of illumination and display, in particular to a fluorescent module and a related light source.
  • halogen lamps and gas discharge lamps reaches the bottleneck, the energy conversion efficiency is low, the life is short, a large amount of heat is generated during use, and the halogen lamps and gas discharge lamps are large in size, and are increasingly unsuitable for new lighting display application scenarios.
  • LED light sources have high energy conversion efficiency and long life, which is a cold light source, but the optical power density of a single LED is low.
  • High-brightness LED technology achieves high-power-density light by combining multiple LEDs by combining the illumination of multiple LEDs.
  • the combination of multiple LEDs causes an increase in the volume of the light source, and at the same time brings about a problem of an increase in the volume of the heat dissipating component, resulting in a low power density of the outgoing light per unit volume of the light source.
  • the thickness of the wavelength conversion layer is greater than the depth of the groove along a direction perpendicular to the light incident surface.
  • the excitation source is a laser source.
  • the utility model comprises the following beneficial effects: by arranging the wavelength conversion layer in the groove of the substrate, the maximum length of the wavelength conversion layer in a direction parallel to the light incident surface is greater than perpendicular to the light incident surface.
  • the maximum length of the direction, and the light reflecting layer is disposed on a surface other than the light incident surface of the wavelength conversion layer, on the one hand, the optical path of the light in the wavelength conversion layer is short, and the laser beam can be quickly emitted after being formed.
  • FIG. 3 is a schematic cross-sectional view showing another embodiment of the fluorescent module of the present invention.
  • the main design concept of the fluorescent module provided by the utility model is to reduce unnecessary optical loss, including loss caused by light reflection, light absorption, insufficient light utilization rate and thermal effect.
  • the utility model selects the wavelength conversion layer whose parallel length to the direction of the light incident surface is greater than the maximum length perpendicular to the direction of the light incident surface, so as to reduce the optical path of the light in the wavelength conversion layer and increase the heat dissipation area of the wavelength conversion layer.
  • the reflector surrounding the wavelength conversion layer directly reflects the laser light from the wavelength conversion layer back to the wavelength conversion layer, thereby avoiding the loss caused by multiple reflections.
  • FIG. 1 is a schematic cross-sectional view showing an embodiment of a fluorescent module of the present invention.
  • the fluorescent module 10 includes a substrate 120, a wavelength conversion layer 110, and a reflective cover 130.
  • the fluorescent ceramic may also be another composite ceramic layer which differs from the composite ceramic layer described above only in the ceramic matrix.
  • the ceramic substrate is a pure phase fluorescent ceramic, that is, the ceramic substrate itself has an activator capable of emitting a laser light under irradiation of excitation light.
  • the technical scheme combines the advantages of the luminescent ceramic particles of the above composite ceramic layer with high luminous efficiency and the above-mentioned pure phase fluorescent ceramics having the luminescent property, and simultaneously illuminating by using the luminescent ceramic particles and the ceramic matrix, thereby further improving the luminescent ceramic layer.
  • the luminous efficiency, and the ceramic matrix has a certain amount of activator doping, but the doping amount is low, and the ceramic substrate can ensure sufficient light transmittance.
  • the first surface 1201 of the substrate 120 is a light reflecting surface capable of reflecting light incident on the first surface 1201.
  • the first surface is The 1201 is set as a light reflecting surface to reduce the light loss caused thereby. This function can be achieved by plating a reflective film on the first surface 1201.
  • the first light-passing port 131 is positioned with a lens optical element capable of changing the angular distribution of the outgoing light. Further, the lens can be easily disassembled and replaced to meet the needs of different exit angle distributions.
  • the thickness of the wavelength conversion layer 110 of the fluorescent module in FIG. 1 is equal to the depth of the groove 1202.
  • the thickness of the wavelength conversion layer 310 is greater than that on the substrate 320.
  • the light reflecting layer is provided on the other surfaces of the wavelength conversion layer 310 except the light incident surface, that is, the laser light can still be emitted only through the light incident surface, which is the same as the principle of the above embodiments.
  • the excitation source is a laser source, including a laser diode source, a laser diode array source, a laser source, and the like.
  • the advantage of the laser light source is that the energy density is high, the divergence angle is small, and it is easy to be directly collected and guided onto the wavelength conversion layer, which is suitable for high-intensity illumination display.

Abstract

A fluorescent module (10), comprising: a substrate (120) which comprises a first surface (1201), the first surface (1201) being provided with a groove (1202); and a wavelength conversion layer (110) disposed in the groove (1202) and configured to convert an incident excitation light into an excited light having a wavelength range different from that of the excitation light and then emit same. The wavelength conversion layer (110) comprises a light incident surface (1101); the maximum length of the wavelength conversion layer (110) in a direction parallel to the light incident surface (1101) is greater than the maximum length in the direction perpendicular to the light incident surface (1101); and a light reflective layer is disposed on all surfaces of the wavelength conversion layer (110) except the light incident surface (1101). A reflective cover (130) connected to the substrate (120) covers the first surface (1201) from above and surrounds, together with the first surface (1201), the wavelength conversion layer (110); the reflective cover (130) comprises a second surface (1301) close to one side of the wavelength conversion layer (110), and is capable of reflecting the excited light incident on the second surface (1301) back to the wavelength conversion layer (110); and the reflective cover (130) further comprises a first light through opening ( 131) for transmission of the excited light.

Description

一种荧光模块及相关光源  Fluorescent module and related light source 技术领域Technical field
本实用新型涉及照明、显示领域,特别是涉及一种荧光模块及相关光源。The utility model relates to the field of illumination and display, in particular to a fluorescent module and a related light source.
背景技术Background technique
在照明、显示领域,高亮度一直是本领域技术人员追求的目标,同时,还要兼顾能量转换效率、光源寿命、光源体积等因素。In the field of illumination and display, high brightness has always been the goal pursued by those skilled in the art, and at the same time, factors such as energy conversion efficiency, light source life, and light source volume are also taken into consideration.
卤素灯、气体放电灯的亮度达到瓶颈,其能量转换效率低,寿命短,在使用时产生大量的热量,而且卤素灯、气体放电灯体积大,越来越不适于新型的照明显示应用场景。The brightness of halogen lamps and gas discharge lamps reaches the bottleneck, the energy conversion efficiency is low, the life is short, a large amount of heat is generated during use, and the halogen lamps and gas discharge lamps are large in size, and are increasingly unsuitable for new lighting display application scenarios.
LED光源具有较高的能量转换效率,而且寿命长,是冷光源,但是单颗LED的光功率密度较低。有高亮度LED技术通过将多颗LED组合起来,通过对多颗LED的发光进行合光来实现高功率密度的光。然而,该技术方案中,多颗LED组合导致光源体积增大,同时带来了散热部件体积增大的问题,导致该光源单位体积的出射光功率密度低。LED light sources have high energy conversion efficiency and long life, which is a cold light source, but the optical power density of a single LED is low. High-brightness LED technology achieves high-power-density light by combining multiple LEDs by combining the illumination of multiple LEDs. However, in this technical solution, the combination of multiple LEDs causes an increase in the volume of the light source, and at the same time brings about a problem of an increase in the volume of the heat dissipating component, resulting in a low power density of the outgoing light per unit volume of the light source.
LD(Laser Diode,激光二极管)光源与LED光源同为冷光源,但是单颗LD的光功率密度远高于LED的光功率密度。然而,LD的光谱具有局限性,绿光LD成本高,导致RGB的LD组合光源成本高,不适于大规模应用。因此,现有技术通常用蓝光LD激发黄色荧光粉的激光激发荧光粉技术获得白光。LD (Laser Diode, laser diode) The light source is the same as the LED light source, but the optical power density of a single LD is much higher than the optical power density of the LED. However, the spectrum of LD has limitations, and the cost of green LD is high, resulting in high cost of RGB LD combination light source, which is not suitable for large-scale applications. Therefore, the prior art generally obtains white light by a laser-excited phosphor technique in which a blue phosphor is excited by a blue LD.
技术问题technical problem
然而,荧光粉发出的光为朗伯分布的光,光发散角大,收集透镜只能收集光发散角约在150°(±75°)范围内的光,导致部分光未被利用。而且荧光粉存在散热问题,过高的温度将导致荧光材料的发光效率下降。因此,一般需要将LD光源与旋转的荧光色轮结构相结合以改善荧光粉的散热,又额外增加了马达等装置,导致光源体积增大,限制了该激光荧光粉光源在小尺寸、微型设备上的应用。此外,现有技术方案往往不考虑光在发光装置内传播时的光损耗问题。综上所述,现有的激光激发荧光粉技术的发光效率还不够高,削弱了其在高亮度照明显示领域的竞争力。However, the light emitted by the phosphor is a Lambertian-distributed light with a large light divergence angle, and the collecting lens can only collect light having a light divergence angle of about 150° (±75°), resulting in partial light being unused. Moreover, the phosphor has a heat dissipation problem, and an excessively high temperature causes a decrease in the luminous efficiency of the fluorescent material. Therefore, it is generally required to combine the LD light source with the rotating fluorescent color wheel structure to improve the heat dissipation of the phosphor, and additionally add a motor and the like, resulting in an increase in the volume of the light source, limiting the laser phosphor light source in a small size, miniature device. Application on. In addition, prior art solutions often do not consider the problem of optical loss when light propagates within the illumination device. In summary, the luminous efficiency of the existing laser-excited phosphor technology is not high enough, which weakens its competitiveness in the field of high-brightness illumination display.
技术解决方案Technical solution
针对上述现有技术的激光激发荧光粉技术发光效率低的缺陷,本实用新型提供一种高发光效率的荧光模块,包括:基板,包括第一表面,所述第一表面上设置有一凹槽;设置于所述凹槽内的波长转换层,用于将入射的激发光转换成波长范围不同于所述激发光的受激光而出射,所述波长转换层包括一光入射面,所述波长转换层沿平行于所述光入射面的方向的最大长度大于沿垂直于所述光入射面的方向的最大长度,所述波长转换层的除光入射面之外的面设置有光反射层;与所述基板相连接的反射罩,覆盖在所述第一表面上方,并与所述第一表面共同将所述波长转换层包围,所述反射罩包括靠近所述波长转换层一侧的第二表面,能够将入射到该第二表面的受激光反射回所述波长转换层,所述反射罩还包括第一通光口,用于透射所述受激光。In view of the above-mentioned prior art laser-excited phosphor technology, the luminous efficiency is low, and the present invention provides a fluorescent module with high luminous efficiency, comprising: a substrate comprising a first surface, wherein the first surface is provided with a groove; a wavelength conversion layer disposed in the recess for converting incident excitation light into a laser beam having a wavelength range different from the excitation light, the wavelength conversion layer including a light incident surface, the wavelength conversion a maximum length of the layer in a direction parallel to the light incident surface is greater than a maximum length in a direction perpendicular to the light incident surface, and a surface of the wavelength conversion layer other than the light incident surface is provided with a light reflecting layer; a reflective cover connected to the substrate, covering the first surface, and surrounding the wavelength conversion layer together with the first surface, the reflective cover including a second side adjacent to the wavelength conversion layer The surface is capable of reflecting the laser light incident on the second surface back to the wavelength conversion layer, and the reflection cover further includes a first light passage for transmitting the laser light.
在一个实施方式中,沿垂直于所述光入射面的方向且过所述波长转换层的中心的直线穿过所述第一通光口。In one embodiment, a straight line passing through a direction perpendicular to the light incident surface and passing through the center of the wavelength conversion layer passes through the first light passing opening.
在一个实施方式中,所述反射罩为半球形反射罩,所述波长转换层设置于所述反射罩的球心位置,球心与所述第一通光口围成的锥形的立体角为0.03π~0.586π。In one embodiment, the reflector is a hemispherical reflector, the wavelength conversion layer is disposed at a spherical center position of the reflector, and a solid angle of a cone surrounded by the center and the first light passage It is 0.03π~0.586π.
在一个实施方式中,所述第一通光口为所述激发光的光入射口。In one embodiment, the first light passing port is a light incident port of the excitation light.
在一个实施方式中,所述反射罩还包括第二通光口,所述第二通光口为所述激发光的光入射口,所述第一通光口能够反射所述激发光,所述第二通光口能够反射所述受激光。In one embodiment, the reflector further includes a second light passing port, wherein the second light passing port is a light incident port of the excitation light, and the first light passing port is capable of reflecting the excitation light. The second light passing port is capable of reflecting the received laser light.
在一个实施方式中,在平行于所述光入射面的平面上,所述波长转换层的最大长度小于所述基板的最大长度的1/5。In one embodiment, the maximum length of the wavelength conversion layer is less than 1/5 of the maximum length of the substrate on a plane parallel to the light incident surface.
在一个实施方式中,沿垂直于所述光入射面方向,所述波长转换层的厚度大于所述凹槽的深度。In one embodiment, the thickness of the wavelength conversion layer is greater than the depth of the groove along a direction perpendicular to the light incident surface.
在一个实施方式中,所述第一通光口位置设置有一光学元件,所述光学元件为二向色片或透镜。In one embodiment, the first light-passing port is provided with an optical element, which is a dichroic color film or a lens.
在一个实施方式中,所述波长转换层为荧光陶瓷。荧光陶瓷具有自吸式少的特点,即荧光陶瓷发出的受激光不容易被荧光陶瓷吸收。In one embodiment, the wavelength conversion layer is a fluorescent ceramic. Fluorescent ceramics have the characteristics of less self-priming, that is, the laser light emitted by the fluorescent ceramic is not easily absorbed by the fluorescent ceramic.
在一个实施方式中,所述基板为金属基板、硅基板或氮化铝基板。该类基板的导热性能好,而且容易加工。In one embodiment, the substrate is a metal substrate, a silicon substrate, or an aluminum nitride substrate. This type of substrate has good thermal conductivity and is easy to process.
在一个实施方式中,所述第一表面为光反射面。进一步减少了光在荧光模块中的吸收损耗,使得入射到第一表面的非凹槽位置的光也能够被收集。In one embodiment, the first surface is a light reflecting surface. The absorption loss of light in the fluorescent module is further reduced so that light incident at the non-groove position of the first surface can also be collected.
本实用新型还提供了一种光源,包括上述任一荧光模块,还包括用于出射激发光的激发光源,所述波长转换层设置在所述激发光的光路上。The present invention also provides a light source comprising any of the above fluorescent modules, further comprising an excitation light source for emitting excitation light, the wavelength conversion layer being disposed on the optical path of the excitation light.
在一个实施方式中,所述激发光源为激光光源。In one embodiment, the excitation source is a laser source.
有益效果Beneficial effect
与现有技术相比,本实用新型包括如下有益效果:通过将波长转换层设置于基板的凹槽内,使波长转换层沿平行于光入射面的方向的最大长度大于沿垂直于光入射面的方向的最大长度,并在波长转换层的除光入射面之外的面设置光反射层,一方面使得光在波长转换层内的光程较短,形成受激光后能够很快的出射,减少了光在波长转换层内传播而导致的损失,另一方面使波长转换层较薄,热量主要从波长转换层底部发散,缩短了热传导距离,减小了基板厚度;还通过包围波长转换层的反射罩反射入射到反射罩第二表面的受激光,使得所有受激光都从反射罩的第一通过口出射,减小了荧光模块出射的受激光发散角范围,使其更容易被光收集元件收集。在以上各个部件协同作用下,荧光模块减少了光损耗,改善了散热,实现了更高的发光效率。Compared with the prior art, the utility model comprises the following beneficial effects: by arranging the wavelength conversion layer in the groove of the substrate, the maximum length of the wavelength conversion layer in a direction parallel to the light incident surface is greater than perpendicular to the light incident surface. The maximum length of the direction, and the light reflecting layer is disposed on a surface other than the light incident surface of the wavelength conversion layer, on the one hand, the optical path of the light in the wavelength conversion layer is short, and the laser beam can be quickly emitted after being formed. The loss caused by the propagation of light in the wavelength conversion layer is reduced, and on the other hand, the wavelength conversion layer is thinner, the heat is mainly dispersed from the bottom of the wavelength conversion layer, the heat conduction distance is shortened, the thickness of the substrate is reduced, and the wavelength conversion layer is also surrounded. The reflector reflects the laser light incident on the second surface of the reflector, so that all the laser light is emitted from the first passage of the reflector, which reduces the range of the laser divergence angle emitted by the fluorescent module, making it easier to be collected by the light. Component collection. Under the synergy of the above components, the fluorescent module reduces light loss, improves heat dissipation, and achieves higher luminous efficiency.
附图说明DRAWINGS
图1为本实用新型的荧光模块的一个实施例的截面示意图。1 is a schematic cross-sectional view of one embodiment of a fluorescent module of the present invention.
图2为本实用新型的荧光模块的另一个实施例的截面示意图。2 is a schematic cross-sectional view showing another embodiment of the fluorescent module of the present invention.
图3为本实用新型的荧光模块的另一个实施例的截面示意图。3 is a schematic cross-sectional view showing another embodiment of the fluorescent module of the present invention.
本发明的最佳实施方式BEST MODE FOR CARRYING OUT THE INVENTION
在一些激光激发荧光粉的光源中,通过使激发光在波长转换层中来回不断反射,将其全部转换为受激光,然后通过一个开口将受激光引导出射。该些技术方案错误的将“所有光经若干次反射后都能够出射”作为假设条件,忽略了光在每一次反射中的损耗。事实上,假若每一次反射的反射率为99%,则反射20次将损失约20%的光,这不符合照明显示中高亮度低功耗的技术要求。In some sources of laser-excited phosphors, by exciting the excitation light back and forth in the wavelength conversion layer, all of them are converted into laser light, and then guided by the laser through an opening. These technical solutions incorrectly assume that "all light can be emitted after several reflections" as a hypothesis, ignoring the loss of light in each reflection. In fact, if the reflectance of each reflection is 99%, then 20 times of reflection will lose about 20% of the light, which does not meet the technical requirements of high brightness and low power consumption in the illumination display.
本实用新型提供的荧光模块,主要的设计构思是减少不必要的光损耗,包括由光反射、光吸收、光利用率不足和热效应带来的损耗。本实用新型选择平行于光入射面方向的最大长度大于垂直于光入射面方向的最大长度的波长转换层,以减少光在波长转换层中的光程,增大波长转换层的散热面积,同时,包围波长转换层的反射罩直接将来自波长转换层的受激光反射回波长转换层,避免了多次反射带来的损耗。The main design concept of the fluorescent module provided by the utility model is to reduce unnecessary optical loss, including loss caused by light reflection, light absorption, insufficient light utilization rate and thermal effect. The utility model selects the wavelength conversion layer whose parallel length to the direction of the light incident surface is greater than the maximum length perpendicular to the direction of the light incident surface, so as to reduce the optical path of the light in the wavelength conversion layer and increase the heat dissipation area of the wavelength conversion layer. The reflector surrounding the wavelength conversion layer directly reflects the laser light from the wavelength conversion layer back to the wavelength conversion layer, thereby avoiding the loss caused by multiple reflections.
在本实用新型中如涉及“第一”、“第二”等的描述仅用于描述目的,以便于描述方便,而不能理解为指示或暗示其相对重要性或者隐含指明所指示的技术特征的数量。由此,限定有“第一”、“第二”的特征可以明示或者隐含地包括至少一个该特征。The descriptions of the "first", "second" and the like in the present invention are used for descriptive purposes only, for convenience of description, and are not to be construed as indicating or implying their relative importance or implicitly indicating the indicated technical features. quantity. Thus, features defining "first" or "second" may include at least one of the features, either explicitly or implicitly.
下面结合附图和实施方式对本实用新型实施例进行详细说明。The embodiments of the present invention are described in detail below with reference to the accompanying drawings and embodiments.
请参见图1,图1为本实用新型的荧光模块的一个实施例的截面示意图。荧光模块10包括基板120、波长转换层110和反射罩130。Please refer to FIG. 1. FIG. 1 is a schematic cross-sectional view showing an embodiment of a fluorescent module of the present invention. The fluorescent module 10 includes a substrate 120, a wavelength conversion layer 110, and a reflective cover 130.
基板120包括第一表面1201,第一表面1201上设置有一凹槽1202。The substrate 120 includes a first surface 1201, and a groove 1202 is disposed on the first surface 1201.
波长转换层110设置在凹槽1202内,用于将入射的激发光转换成波长范围不同于激发光的受激光而出射。波长转换层110包括一光入射面1101,波长转换层110沿平行于该光入射面1101的方向的最大长度大于沿垂直于光入射面1101的方向的最大长度,且波长转换层的除光入射面1101之外的其他面均设置有光反射层。The wavelength conversion layer 110 is disposed in the recess 1202 for converting the incident excitation light into a laser light having a wavelength range different from the excitation light. The wavelength conversion layer 110 includes a light incident surface 1101. The maximum length of the wavelength conversion layer 110 in a direction parallel to the light incident surface 1101 is greater than a maximum length in a direction perpendicular to the light incident surface 1101, and the wavelength of the wavelength conversion layer is incident on the light. The other faces other than the face 1101 are provided with a light reflecting layer.
反射罩130与基板120相连接,并覆盖在第一表面1201上方,使得反射罩130与第一表面1201共同将波长转换层110包围。反射罩130包括靠近波长转换层一侧的第二表面1301,能够将入射到该第二表面1301的受激光反射回波长转换层110。反射罩130还包括第一通光口131,用于透射受激光。The reflector 130 is coupled to the substrate 120 and overlies the first surface 1201 such that the reflector 130 and the first surface 1201 together surround the wavelength conversion layer 110. The reflector 130 includes a second surface 1301 adjacent to one side of the wavelength conversion layer, and is capable of reflecting the laser light incident on the second surface 1301 back to the wavelength conversion layer 110. The reflector 130 further includes a first light passage 131 for transmitting the laser light.
在本实施例中,激发光通过反射罩130的第一通光口131入射到波长转换层110的光入射面1101,波长转换层110吸收激发光并出射受激光,受激光呈近似朗伯分布的光从波长转换层110中出射。由于波长转换层110的除光入射面1101之外的面设置有光反射层,因此受激光只能从光入射面1101出射,出射光的角度范围为180°(±90°)。入射到反射罩130的第一通光口131的受激光直接出射,而入射到反射罩130的第二表面1301的光被反射回到波长转换层110,该部分回到波长转换层110的光被波长转换层散射后,重新以近似朗伯分布的光从波长转换层110出射。重复上述过程,最终受激光从第一通光口131出射,从第一通光口131出射的出射光发散角相对于光入射面1101的出射光发散角大大减小,有利于后续光学元件的收集利用。In the present embodiment, the excitation light is incident on the light incident surface 1101 of the wavelength conversion layer 110 through the first light-passing port 131 of the reflection cover 130, and the wavelength conversion layer 110 absorbs the excitation light and emits the laser light, and the laser is approximately Lambertian. The light exits from the wavelength conversion layer 110. Since the light reflecting layer is provided on the surface other than the light incident surface 1101 of the wavelength conversion layer 110, the laser light can be emitted only from the light incident surface 1101, and the angle of the emitted light is 180° (±90°). The laser light incident on the first light-passing port 131 of the reflection cover 130 is directly emitted, and the light incident on the second surface 1301 of the reflection cover 130 is reflected back to the wavelength conversion layer 110, and the portion returns to the light of the wavelength conversion layer 110. After being scattered by the wavelength conversion layer, light having an approximately Lambertian distribution is again emitted from the wavelength conversion layer 110. The above process is repeated, and finally the laser light is emitted from the first light-passing port 131, and the divergence angle of the outgoing light emitted from the first light-passing port 131 is greatly reduced with respect to the light-emitting angle of the light-incident surface 1101, which is favorable for the subsequent optical components. Collect and use.
本实用新型中,波长转换层的除了光入射面之外的其他各面均设置有光反射层,避免了光从波长转换层侧面出射。假若没有侧面的光反射层,则从侧面出射的光经反射罩反射后难以直接返回波长转换层,难以被收集利用,从而导致光损耗。In the present invention, each of the wavelength conversion layers except the light incident surface is provided with a light reflecting layer to prevent light from exiting from the side of the wavelength conversion layer. If there is no light reflection layer on the side, the light emitted from the side surface is reflected by the reflector and is difficult to directly return to the wavelength conversion layer, which is difficult to collect and utilize, resulting in light loss.
在本实用新型中,波长转换层110的作用在于接收激发光的照射,并将激发光转换为波长不同的受激光。这里的激发光可以为固态光源发出的光,如LED光、激光二极管光、激光器光,也可以为其他任何本实用新型申请前公开的光源光。波长转换层可以为硅胶/树脂的有机封装荧光粉层,也可以为玻璃封装荧光粉层,还可以为荧光陶瓷。由于荧光陶瓷为陶瓷结构,其热稳定性及导热性能远远优于以玻璃或硅胶为封装基质的荧光粉层,能够承受大功率激发光的照射,可以适用于高亮度激光荧光照明/显示领域。In the present invention, the wavelength conversion layer 110 functions to receive the excitation light and convert the excitation light into laser light of different wavelengths. The excitation light here may be light emitted by a solid-state light source, such as LED light, laser diode light, laser light, or any other source light as disclosed in the present application. The wavelength conversion layer may be a silicone/resin organic package phosphor layer, a glass package phosphor layer, or a fluorescent ceramic. Because the fluorescent ceramic is a ceramic structure, its thermal stability and thermal conductivity are far superior to those of glass or silica gel as the package matrix, which can withstand high-power excitation light, and can be applied to high-brightness laser fluorescent illumination/display field. .
荧光陶瓷可以是纯相的荧光陶瓷,具体可以是各种氧化物陶瓷、氮化物陶瓷或氮氧化物陶瓷,通过在陶瓷制备过程中掺入微量的激活剂元素(如镧系元素),形成发光中心。由于一般激活剂元素的掺杂量较小(一般小于1%),该类荧光陶瓷通常是透明或半透明发光陶瓷,激发光容易直接穿过该发光陶瓷层后出射,因此该发光陶瓷层的发光效率不高,更适于较低功率的激发光应用场景。例如,荧光陶瓷可以是Ce掺杂YAG陶瓷或Ce掺杂LuAG陶瓷。The fluorescent ceramics may be pure phase fluorescent ceramics, specifically various oxide ceramics, nitride ceramics or oxynitride ceramics, and formed by incorporating a trace amount of activator elements (such as lanthanides) into the ceramic preparation process. center. Since the doping amount of the general activator element is small (generally less than 1%), the fluorescent ceramic is usually a transparent or translucent luminescent ceramic, and the excitation light is easily emitted directly after passing through the luminescent ceramic layer, so that the luminescent ceramic layer is The luminous efficiency is not high, and it is more suitable for the lower power excitation light application scene. For example, the fluorescent ceramic may be a Ce doped YAG ceramic or a Ce doped LuAG ceramic.
荧光陶瓷还可以是复合陶瓷层,其以透明/半透明陶瓷作为基质,在陶瓷基质内分布着发光陶瓷颗粒(如荧光粉颗粒)。透明/半透明陶瓷基质可以是各种氧化物陶瓷(如氧化铝陶瓷、Y3Al5O12陶瓷)、氮化物陶瓷(如氮化铝陶瓷)或氮氧化物陶瓷,陶瓷基质的作用在于对光和热进行传导,使得激发光能够入射到发光陶瓷颗粒上,并使受激光能够从发光陶瓷层中出射;发光陶瓷颗粒承担发光陶瓷层的主要发光功能,用于吸收激发光并将其转换为受激光。发光陶瓷颗粒的晶粒粒径较大,而且激活剂元素的掺杂量较大(如1~5%),使得其发光效率高;而且发光陶瓷颗粒分散于陶瓷基质中,避免了位于荧光陶瓷较深位置的发光陶瓷颗粒无法被激发光照射到的情况,还避免了纯相荧光陶瓷整体掺杂量较大而导致的激活剂元素浓度中毒的情况,从而提高了发光陶瓷层的发光效率。进一步的,上述荧光陶瓷中还可以增加散射颗粒,使散射颗粒分布于陶瓷基质中。散射颗粒可以是散射粒子,如氧化铝,氧化钇,氧化锆,氧化镧,氧化钛,氧化锌,硫酸钡等,既可以是单一材料的散射颗粒,也可以是两种或两种以上的组合,其特点为表观白色,能够对可见光进行散射,而且材料稳定,能够承受高温,粒径与激发光波长处于同一数量级或低一个数量级。The fluorescent ceramic may also be a composite ceramic layer having a transparent/translucent ceramic as a matrix in which luminescent ceramic particles (such as phosphor particles) are distributed. The transparent/translucent ceramic substrate may be various oxide ceramics (such as alumina ceramics, Y3Al5O12 ceramics), nitride ceramics (such as aluminum nitride ceramics) or oxynitride ceramics, and the ceramic matrix functions to conduct light and heat. The excitation light can be incident on the luminescent ceramic particles and the laser light can be emitted from the luminescent ceramic layer; the luminescent ceramic particles bear the main illuminating function of the luminescent ceramic layer for absorbing the excitation light and converting it into a laser. The granules of the luminescent ceramic particles have a large grain size, and the doping amount of the activator element is large (for example, 1 to 5%), so that the luminescence efficiency is high; and the luminescent ceramic particles are dispersed in the ceramic matrix, thereby avoiding the presence of the fluorescent ceramics. The luminescent ceramic particles in the deep position cannot be irradiated by the excitation light, and the poisoning of the activator element concentration caused by the large doping amount of the pure phase fluorescent ceramic is avoided, thereby improving the luminous efficiency of the luminescent ceramic layer. Further, in the above fluorescent ceramic, scattering particles may be added to distribute the scattering particles in the ceramic matrix. The scattering particles may be scattering particles such as alumina, cerium oxide, zirconium oxide, cerium oxide, titanium oxide, zinc oxide, barium sulfate, etc., either as scattering particles of a single material or as a combination of two or more kinds. It is characterized by an apparent white color, which is capable of scattering visible light, and is stable in material and capable of withstanding high temperatures. The particle size is of the same order of magnitude or an order of magnitude lower than the wavelength of the excitation light.
荧光陶瓷还可以是另外一种复合陶瓷层,该复合陶瓷层与上述复合陶瓷层的区别仅在于陶瓷基质不同。在本实施方式中,陶瓷基质是纯相的荧光陶瓷,即陶瓷基质本身具有激活剂,能够在激发光的照射下发出受激光。该技术方案综合了上述复合陶瓷层的发光陶瓷颗粒具有高发光效率的优势以及上述纯相的荧光陶瓷具有发光性能的优势,同时利用发光陶瓷颗粒与陶瓷基质进行发光,进一步提高了发光陶瓷层的发光效率,而且该陶瓷基质虽然具有一定的激活剂掺杂量,但是掺杂量较低,能够保证该陶瓷基质具有足够的透光性。在该发光陶瓷层中,同样可以增加散射颗粒增强发光陶瓷层的内部散射。The fluorescent ceramic may also be another composite ceramic layer which differs from the composite ceramic layer described above only in the ceramic matrix. In the present embodiment, the ceramic substrate is a pure phase fluorescent ceramic, that is, the ceramic substrate itself has an activator capable of emitting a laser light under irradiation of excitation light. The technical scheme combines the advantages of the luminescent ceramic particles of the above composite ceramic layer with high luminous efficiency and the above-mentioned pure phase fluorescent ceramics having the luminescent property, and simultaneously illuminating by using the luminescent ceramic particles and the ceramic matrix, thereby further improving the luminescent ceramic layer. The luminous efficiency, and the ceramic matrix has a certain amount of activator doping, but the doping amount is low, and the ceramic substrate can ensure sufficient light transmittance. In the luminescent ceramic layer, it is also possible to increase the internal scattering of the luminescent ceramic layer by the scattering particles.
本实用新型中,波长转换层的除了光入射面之外的其他面上的光反射层,可以通过在波长转换层表面镀制反射膜实现,然后将波长转换层与基板通过焊接或粘结的方式相连。在一个实施方式中,还可以在基板的第一表面或仅在凹槽的表面位置镀制/涂覆反射膜层,然后将波长转换层设置于凹槽内。In the present invention, the light reflecting layer of the wavelength conversion layer other than the light incident surface can be realized by plating a reflective film on the surface of the wavelength conversion layer, and then the wavelength conversion layer and the substrate are welded or bonded. The way is connected. In one embodiment, the reflective film layer may also be plated/coated on the first surface of the substrate or only at the surface location of the recess, and then the wavelength converting layer is disposed within the recess.
在本实用新型中,基板120的主要作用为承载波长转换层110,并充当波长转换层110的散热导体。基板120可以为金属基板、硅基板或氮化铝基板,这些基板的特点是导热性能良好且易加工。In the present invention, the main function of the substrate 120 is to carry the wavelength conversion layer 110 and serve as a heat dissipation conductor of the wavelength conversion layer 110. The substrate 120 may be a metal substrate, a silicon substrate or an aluminum nitride substrate, and these substrates are characterized by good thermal conductivity and easy processing.
在本实施例的一个实施方式中,基板120的第一表面1201为光反射面,能够对入射到第一表面1201的光进行反射。当受激光从波长转换层110中出射,并在反射罩130与波长转换层110之间进行反射时,有可能有小部分光未能从反射罩130回到波长转换层110,将第一表面1201设置为光反射面能够减少因此带来的光损失。可以通过在第一表面1201上镀制反射膜来实现该功能。In an embodiment of the embodiment, the first surface 1201 of the substrate 120 is a light reflecting surface capable of reflecting light incident on the first surface 1201. When the laser light is emitted from the wavelength conversion layer 110 and reflected between the reflection cover 130 and the wavelength conversion layer 110, there is a possibility that a small portion of the light fails to return from the reflection cover 130 to the wavelength conversion layer 110, and the first surface is The 1201 is set as a light reflecting surface to reduce the light loss caused thereby. This function can be achieved by plating a reflective film on the first surface 1201.
在本实施例的一个实施方式中,如图所示,沿垂直于所述光入射面1101的方向且过所述波长转换层110的中心的直线穿过所述第一通光口。具体地,从波长转换层110的光入射面1101垂直出射的光能够直接穿过第一通光口131而出射。第一通光口131设置在该位置有利于提高光出射效率。可以理解,在其他实施方式中,第一通光口也可以设置在其他位置,使得从波长转换层斜出射的光才能直接通过第一通光口出射。In one embodiment of the present embodiment, as shown, a straight line passing through a direction perpendicular to the light incident surface 1101 and passing through the center of the wavelength conversion layer 110 passes through the first light passing opening. Specifically, light that is perpendicularly emitted from the light incident surface 1101 of the wavelength conversion layer 110 can be directly emitted through the first light passing opening 131. Setting the first light passing port 131 at this position is advantageous for improving light emission efficiency. It can be understood that in other embodiments, the first light-passing port can also be disposed at other positions, so that the light obliquely emitted from the wavelength conversion layer can be directly emitted through the first light-passing port.
在本实施例的一个实施方式中,反射罩130为半球形反射罩,波长转换层110设置于反射罩130的球心位置,这样可以使被第二表面1301反射的受激光原路返回到波长转换层110,避免光路偏移而无法直接回到波长转换层110。In one embodiment of the embodiment, the reflector 130 is a hemispherical reflector, and the wavelength conversion layer 110 is disposed at a center of the reflector 130 such that the laser-received path reflected by the second surface 1301 returns to the wavelength. The conversion layer 110 avoids the optical path offset and cannot directly return to the wavelength conversion layer 110.
第一通光口131不能太大,否则出射的受激光的发散角太大,在进入后续光学元件时有可能导致部分光无法被利用。第一通光口131也不能太小,否则被第二表面1301反射的光远远多于经第一通光口131出射的光,导致受激光要增加被波长转换层110散射的次数和被第二表面1301反射的次数,这将导致产生大量的光散射损耗和光反射损耗,不利于发光效率的提高。在如图1所示的截面示意图中,从第一通光口131出射的受激光的发散角(即最左侧光线与最右侧光线的夹角)应控制在20°~90°之间。设第一通光口131为圆形,则可算出反射罩的球心与第一通光口围成的锥形的立体角约为0.03π~0.586π。当第一通光口为其他形状,如矩形等时,只要满足球心与第一通光口围成的锥形的立体角在0.03π~0.586π的范围内,即可使得出射的受激光既不会发散角过大,又不会存在过多的散射和反射光损耗。The first light passing port 131 cannot be too large, otherwise the divergence angle of the emitted laser light is too large, and some light may not be utilized when entering the subsequent optical element. The first light-passing port 131 is also not too small, otherwise the light reflected by the second surface 1301 is much more than the light emitted through the first light-passing port 131, resulting in the number of times the laser light is increased by the wavelength conversion layer 110 and is The number of times the second surface 1301 is reflected, which will result in a large amount of light scattering loss and light reflection loss, which is disadvantageous for the improvement of luminous efficiency. In the schematic cross-sectional view shown in FIG. 1, the divergence angle of the laser light emitted from the first light-passing port 131 (ie, the angle between the leftmost light and the rightmost light) should be controlled between 20° and 90°. . When the first light-passing port 131 is circular, the solid angle of the cone surrounded by the center of the reflector and the first light-passing opening can be calculated to be about 0.03π to 0.586π. When the first light-passing port has other shapes, such as a rectangle or the like, as long as the solid angle of the cone surrounded by the center of the ball and the first light-passing opening is in the range of 0.03π to 0.586π, the laser light to be emitted can be made. Neither the divergence angle is too large nor the excessive scattering and reflected light loss.
在一个实施方式中,第一通光口131位置设置有一透镜光学元件,该光学元件能够改变出射光的角分布。进一步地,该透镜可以方便的拆卸更换,以适应不同的出射光角分布的需求。In one embodiment, the first light-passing port 131 is positioned with a lens optical element capable of changing the angular distribution of the outgoing light. Further, the lens can be easily disassembled and replaced to meet the needs of different exit angle distributions.
在一个实施方式中,第一通光口131位置还设置有一二向色片光学元件,该二向色片可以为角度选择滤光片,对不同入射角的光具有不同的透射/反射性能,从而控制荧光模块的出射光角分布。In one embodiment, the first light-passing port 131 is further provided with a dichroic color optical element, and the dichroic color piece may be an angle selective filter having different transmission/reflection properties for light of different incident angles. , thereby controlling the angular distribution of the exiting light of the fluorescent module.
由于在本实用新型中,波长转换层内的每一点都可能是发光点,若波长转换层的尺寸太大,将可能导致较多的受激光多次反射后发生位置偏移,导致受激光不能被反射罩直接反射回波长转换层而导致光损耗,因此需对波长转换层的尺寸进行限制。在一个实施方式中,在平行于光入射面1101的平面上,波长转换层的最大长度小于基板的最大长度的1/5。以圆盘型的波长转换层和基板为例,即两者的直径至少相差5倍。除了减少光损耗,本技术方案还能够提高单位体积波长转换层的发光效率。In the present invention, each point in the wavelength conversion layer may be a light-emitting point. If the size of the wavelength conversion layer is too large, it may cause more positional shift after multiple reflections by the laser, resulting in failure of the laser. The reflector is directly reflected back to the wavelength conversion layer to cause optical loss, so the size of the wavelength conversion layer needs to be limited. In one embodiment, the maximum length of the wavelength conversion layer is less than 1/5 of the maximum length of the substrate on a plane parallel to the light incident surface 1101. Taking a disk-type wavelength conversion layer and a substrate as an example, the diameters of the two are at least 5 times different. In addition to reducing optical loss, the present technical solution is also capable of improving the luminous efficiency per unit volume of the wavelength conversion layer.
请参见图2,图2为本实用新型的荧光模块的另一个实施例的截面示意图。荧光模块20包括波长转换层210、基板220和反射罩230。Please refer to FIG. 2. FIG. 2 is a schematic cross-sectional view showing another embodiment of the fluorescent module of the present invention. The fluorescent module 20 includes a wavelength conversion layer 210, a substrate 220, and a reflective cover 230.
与图1所示的实施例不同之处在于,图1所示的荧光模块的第一通光口既作为受激光的出光口,又作为激发光的光入射口,而本实施例中,激发光的光入射口与受激光的出光口不同。本实施例中,反射罩230包括第一通光口231和第二通光口232。其中,第二通光口232为激发光的光入射口,第一通光口231为受激光的出光口。第一通光口231能够反射激发光,第二通光口232能够反射受激光。该技术方案下,可以更加灵活的设计光路。The difference from the embodiment shown in FIG. 1 is that the first light-passing port of the fluorescent module shown in FIG. 1 serves both as a light-emitting port for receiving the laser light and as a light incident port for exciting light, and in this embodiment, the excitation is performed. The light entrance of the light is different from the light exit of the laser. In this embodiment, the reflective cover 230 includes a first light passing opening 231 and a second light passing opening 232. The second light-passing port 232 is a light incident port for exciting light, and the first light-passing port 231 is a light-emitting port for receiving laser light. The first light passing port 231 can reflect the excitation light, and the second light passing port 232 can reflect the laser light. Under this technical solution, the optical path can be designed more flexibly.
在一个实施方式中,可以通过在通光口设置光学元件的方式实现对激发光和/或受激光的透射或反射功能。由于激发光和受激光的波长范围不同,因此可以选择二向色片作为一种设置在通光口的光学元件。In one embodiment, the transmission or reflection function of the excitation light and/or the laser light can be achieved by providing optical elements in the light-passing opening. Since the excitation light and the laser are different in wavelength range, the dichroic film can be selected as an optical element disposed at the light passage.
请参见图3,图3为本实用新型的荧光模块的另一个实施例的截面示意图。荧光模块30包括波长转换层310、基板320和反射罩330。Please refer to FIG. 3. FIG. 3 is a schematic cross-sectional view showing another embodiment of the fluorescent module of the present invention. The fluorescent module 30 includes a wavelength conversion layer 310, a substrate 320, and a reflective cover 330.
与图1所示的实施例不同之处在于,图1中的荧光模块的波长转换层110的厚度与凹槽1202深度相等,而本实施例中,波长转换层310的厚度大于基板320上的凹槽3202的深度。本实施例中,波长转换层310的除了光入射面的其他各面均设置有光反射层,即受激光仍然只能通过光入射面出射,与上述各实施方式的原理相同。The difference from the embodiment shown in FIG. 1 is that the thickness of the wavelength conversion layer 110 of the fluorescent module in FIG. 1 is equal to the depth of the groove 1202. In this embodiment, the thickness of the wavelength conversion layer 310 is greater than that on the substrate 320. The depth of the groove 3202. In the present embodiment, the light reflecting layer is provided on the other surfaces of the wavelength conversion layer 310 except the light incident surface, that is, the laser light can still be emitted only through the light incident surface, which is the same as the principle of the above embodiments.
本使用新型还提供了一种光源,包括上述各实施方式所述的荧光模块,还包括用于出射激发光的激发光源。波长转换层设置在激发光的光路上,激发光源发出的激发光通过图1/图3中的第一通光口或者图2中的第二通光口入射到波长转换层,从而进行激发发光。由于激发光与受激光的波长不同,可以在图1及图3对应的各实施方式中,在激发光源与上述荧光模块之间设置一二向色分光片,使其对激发光和受激光有不同的透射反射性能,从而对激发光和受激光进行分光。The present invention also provides a light source, including the fluorescent module described in each of the above embodiments, and an excitation light source for emitting excitation light. The wavelength conversion layer is disposed on the optical path of the excitation light, and the excitation light emitted by the excitation light source is incident on the wavelength conversion layer through the first light passing port in FIG. 1/FIG. 3 or the second light passing port in FIG. 2, thereby performing excitation light emission. . Since the wavelengths of the excitation light and the laser light are different, in each of the embodiments corresponding to FIG. 1 and FIG. 3, a dichroic beam splitter is disposed between the excitation light source and the fluorescent module to provide excitation light and laser light. Different transflective properties to split the excitation and laser.
在一个实施方式中,激发光源为激光光源,包括激光二极管光源、激光二极管阵列光源、激光器光源等。激光光源的优势在于能量密度高、发散角小,易于直接被收集并引导入射到波长转换层上,适于高亮度照明显示。In one embodiment, the excitation source is a laser source, including a laser diode source, a laser diode array source, a laser source, and the like. The advantage of the laser light source is that the energy density is high, the divergence angle is small, and it is easy to be directly collected and guided onto the wavelength conversion layer, which is suitable for high-intensity illumination display.
本说明书中各个实施例采用递进的方式描述,每个实施例重点说明的都是与其他实施例的不同之处,各个实施例之间相同相似部分互相参见即可。The various embodiments in the present specification are described in a progressive manner, and each embodiment focuses on differences from other embodiments, and the same similar parts between the various embodiments may be referred to each other.
以上所述仅为本实用新型的实施方式,并非因此限制本实用新型的专利范围,凡是利用本实用新型说明书及附图内容所作的等效结构或等效流程变换,或直接或间接运用在其他相关的技术领域,均同理包括在本实用新型的专利保护范围内。The above is only the embodiment of the present invention, and thus does not limit the scope of the patent of the present invention. Any equivalent structure or equivalent process transformation made by using the description of the utility model and the drawings, or directly or indirectly applied to other The related technical fields are all included in the scope of patent protection of the present invention.

Claims (13)

1、一种荧光模块,其特征在于,包括A fluorescent module characterized by comprising
基板,包括第一表面,所述第一表面上设置有一凹槽;The substrate includes a first surface, and the first surface is provided with a groove;
设置于所述凹槽内的波长转换层,用于将入射的激发光转换成波长范围不同于所述激发光的受激光而出射,所述波长转换层包括一光入射面,所述波长转换层沿平行于所述光入射面的方向的最大长度大于沿垂直于所述光入射面的方向的最大长度,所述波长转换层的除光入射面之外的面设置有光反射层;a wavelength conversion layer disposed in the recess for converting incident excitation light into a laser beam having a wavelength range different from the excitation light, the wavelength conversion layer including a light incident surface, the wavelength conversion a maximum length of the layer in a direction parallel to the light incident surface is greater than a maximum length in a direction perpendicular to the light incident surface, and a surface of the wavelength conversion layer other than the light incident surface is provided with a light reflecting layer;
与所述基板相连接的反射罩,覆盖在所述第一表面上方,并与所述第一表面共同将所述波长转换层包围,所述反射罩包括靠近所述波长转换层一侧的第二表面,能够将入射到该第二表面的受激光反射回所述波长转换层,所述反射罩还包括第一通光口,用于透射所述受激光。a reflective cover connected to the substrate, covering the first surface, and surrounding the wavelength conversion layer together with the first surface, the reflective cover including a side close to the wavelength conversion layer The two surfaces are capable of reflecting the laser light incident on the second surface back to the wavelength conversion layer, and the reflector further includes a first light passage for transmitting the laser light.
2、根据权利要求1所述的荧光模块,其特征在于,沿垂直于所述光入射面的方向且过所述波长转换层的中心的直线穿过所述第一通光口。2. The fluorescent module according to claim 1, wherein a straight line passing through a direction perpendicular to a direction of the light incident surface and passing through a center of the wavelength conversion layer passes through the first light passing opening.
3、根据权利要求1或2所述的荧光模块,其特征在于,所述反射罩为半球形反射罩,所述波长转换层设置于所述反射罩的球心位置,球心与所述第一通光口围成的锥形的立体角为0.03π~0.586π。The fluorescent module according to claim 1 or 2, wherein the reflector is a hemispherical reflector, and the wavelength conversion layer is disposed at a center of the reflector, the center of the sphere and the first The solid angle of the cone enclosed by a light passage is 0.03π~0.586π.
4、根据权利要求1所述的荧光模块,其特征在于,所述第一通光口为所述激发光的光入射口。The fluorescent module according to claim 1, wherein the first light passing port is a light incident port of the excitation light.
5、根据权利要求1所述的荧光模块,其特征在于,所述反射罩还包括第二通光口,所述第二通光口为所述激发光的光入射口,所述第一通光口能够反射所述激发光,所述第二通光口能够反射所述受激光。The fluorescent module according to claim 1, wherein the reflective cover further comprises a second light passing port, wherein the second light passing port is a light incident port of the excitation light, the first pass The optical port is capable of reflecting the excitation light, and the second light passing port is capable of reflecting the received laser light.
6、根据权利要求1、2、4或5所述的荧光模块,其特征在于,在平行于所述光入射面的平面上,所述波长转换层的最大长度小于所述基板的最大长度的1/5。The fluorescent module according to claim 1, 2, 4 or 5, wherein a maximum length of the wavelength conversion layer is smaller than a maximum length of the substrate on a plane parallel to the light incident surface 1/5.
7、根据权利要求1所述的荧光模块,其特征在于,沿垂直于所述光入射面方向,所述波长转换层的厚度大于所述凹槽的深度。7. The fluorescent module according to claim 1, wherein a thickness of the wavelength conversion layer is greater than a depth of the groove in a direction perpendicular to the light incident surface.
8、根据权利要求1所述的荧光模块,其特征在于,所述第一通光口位置设置有一光学元件,所述光学元件为二向色片或透镜。The fluorescent module according to claim 1, wherein the first light-passing port is provided with an optical element, and the optical element is a dichroic color film or a lens.
9、根据权利要求1所述的荧光模块,其特征在于,所述波长转换层为荧光陶瓷。9. The fluorescent module of claim 1 wherein the wavelength converting layer is a fluorescent ceramic.
10、根据权利要求1所述的荧光模块,其特征在于,所述基板为金属基板、硅基板或氮化铝基板。The fluorescent module according to claim 1, wherein the substrate is a metal substrate, a silicon substrate or an aluminum nitride substrate.
11、根据权利要求1所述的荧光模块,其特征在于,所述第一表面为光反射面。The fluorescent module according to claim 1, wherein the first surface is a light reflecting surface.
12、一种光源,包括如权利要求1至11中任一项所述的荧光模块,还包括用于出射激发光的激发光源,所述波长转换层设置在所述激发光的光路上。A light source comprising the fluorescent module according to any one of claims 1 to 11, further comprising an excitation light source for emitting excitation light, the wavelength conversion layer being disposed on an optical path of the excitation light.
13、根据权利要求12所述的光源,其特征在于,所述激发光源为激光光源。13. A light source according to claim 12 wherein the excitation source is a laser source.
PCT/CN2017/090332 2017-01-25 2017-06-27 Fluorescent module and relevant light source WO2018137312A1 (en)

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