CN209844202U - A semiconductor laser hollow laser light source emitting device - Google Patents
A semiconductor laser hollow laser light source emitting device Download PDFInfo
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- CN209844202U CN209844202U CN201921093937.2U CN201921093937U CN209844202U CN 209844202 U CN209844202 U CN 209844202U CN 201921093937 U CN201921093937 U CN 201921093937U CN 209844202 U CN209844202 U CN 209844202U
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 42
- 239000012788 optical film Substances 0.000 claims abstract description 9
- NTHWMYGWWRZVTN-UHFFFAOYSA-N sodium silicate Chemical compound [Na+].[Na+].[O-][Si]([O-])=O NTHWMYGWWRZVTN-UHFFFAOYSA-N 0.000 description 10
- 230000003287 optical effect Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 238000001093 holography Methods 0.000 description 2
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Abstract
本实用新型公开了一种半导体激光空心激光光源发射装置,属于半导体激光技术领域。本实用新型其特征在于,正八棱锥的锥面与底面所成的二面角角度为45度;正八棱锥的八个锥面为半导体激光厘米bar条出射光束的反射面;每个锥面蒸镀高反射光学膜,高反射光学膜的入射角为45度,高反射光学膜的中心波长为半导体激光厘米bar条输出波长;每个锥面对应一个半导体激光厘米bar条,半导体激光厘米bar条以正八棱锥的锥轴成轴对称分布;每个半导体激光厘米bar条输出光束经准直镜准直,形成平行光;平行光以45度角入射到正八棱锥的锥面,经正八棱锥的锥面反射,反射后的八个光束,围成正八边形,形成正八边形空心光源,空心光源以平行于锥轴方向射出。
The utility model discloses a semiconductor laser hollow laser light source emitting device, which belongs to the technical field of semiconductor lasers. The utility model is characterized in that the dihedral angle formed by the conical surface and the bottom surface of the regular octagonal pyramid is 45 degrees; the eight conical surfaces of the regular octagonal pyramid are the reflection surfaces of the semiconductor laser centimeter bar bar outgoing beam; each cone surface is evaporated High reflective optical film, the incident angle of high reflective optical film is 45 degrees, the central wavelength of high reflective optical film is the output wavelength of semiconductor laser centimeter bar; each cone corresponds to a semiconductor laser centimeter bar, semiconductor laser centimeter bar The cone axis of the regular octagonal pyramid is distributed axisymmetrically; the output beam of each semiconductor laser centimeter bar is collimated by a collimator to form parallel light; the parallel light is incident on the cone surface of the regular octagonal pyramid at an angle of 45 degrees, and passes through the cone of the regular octagonal pyramid Surface reflection, the reflected eight light beams are surrounded by a regular octagon to form a regular octagonal hollow light source, and the hollow light source is emitted in a direction parallel to the cone axis.
Description
技术领域technical field
本发明涉及一种半导体激光空心激光光源发射装置,属于半导体激光技术领域。The invention relates to a semiconductor laser hollow laser light source emitting device, which belongs to the technical field of semiconductor lasers.
背景技术Background technique
空心激光光源在激光光学、光信息处理、微粒波导、同位素分离、微电子学和材料科学、生物技术、医学以及原子学、分子学等领域中有着广泛的应用前景。人们已经利用光束整形,例如几何光学法、光学全息法和计算全息法等八种方法研制出了各种形式的空心激光光束。然而,这些方法获得的空心激光光束共同点是光强从光束内边缘到中心光强逐渐减弱,理论上只有光束中心上的一点光强才为零,因此无法获得高光强对比度的空心激光光束,而高光强对比度的空心激光光束在微观粒子的光学操控、光信息处理和材料科学等领域具有重要的应用。Hollow laser sources have broad application prospects in the fields of laser optics, optical information processing, particle waveguides, isotope separation, microelectronics and material science, biotechnology, medicine, atomics, and molecules. Various forms of hollow laser beams have been developed by using eight methods of beam shaping, such as geometric optics, optical holography, and computational holography. However, the common point of the hollow laser beams obtained by these methods is that the light intensity gradually weakens from the inner edge of the beam to the center. In theory, only the light intensity at the center of the beam is zero. Hollow laser beams with high light intensity contrast have important applications in the fields of optical manipulation of microscopic particles, optical information processing, and material science.
发明内容Contents of the invention
为了提高空心激光光强对比度,同时,提高暗斑尺寸,我们发明了一种半导体激光空心激光光源发射装置,同时,本发明还具有装调容易的优点。In order to improve the contrast of hollow laser light intensity and increase the size of dark spots, we have invented a semiconductor laser hollow laser light source emitting device. At the same time, the invention also has the advantage of easy installation and adjustment.
本发明之一种半导体激光空心激光光源发射装置其特征在于,如图 1 所示,包括:正八棱锥1、半导体激光厘米bar条2和准直镜3;正八棱锥1的每个锥面与底面所成的二面角角度都为45度;正八棱锥1的每个锥面蒸镀高反射光学膜,高反射光学膜的入射角为45度,高反射光学膜的中心波长为半导体激光厘米bar条2的输出波长;正八棱锥1每一个锥面对应一个半导体激光厘米bar条2,半导体激光厘米bar条2以正八棱锥1的锥轴成轴对称分布,每个半导体激光厘米bar条2输出波长相同。A kind of semiconductor laser hollow laser light source emitting device of the present invention is characterized in that, as shown in Figure 1, comprises: regular octagonal pyramid 1, semiconductor laser centimeter bar bar 2 and collimator mirror 3; Each taper surface and bottom surface of regular octagonal pyramid 1 The resulting dihedral angles are all 45 degrees; each cone surface of the regular octagonal pyramid 1 is evaporated with a high-reflection optical film, the incident angle of the high-reflection optical film is 45 degrees, and the central wavelength of the high-reflection optical film is semiconductor laser centimeter bar The output wavelength of bar 2; each cone surface of the regular octagonal pyramid 1 corresponds to a semiconductor laser centimeter bar bar 2, and the semiconductor laser centimeter bar bar 2 is distributed axisymmetrically with the cone axis of the regular octagonal pyramid 1, and each semiconductor laser centimeter bar bar 2 outputs same wavelength.
本发明之一种半导体激光空心激光光源发射装置在工作时,同现有半导体激光厘米bar条一样,每个半导体激光厘米bar条2的输出光均需要由准直镜3准直为一束平行光,如图2所示。在图2中每束平行光以45度角入射到正八棱锥1的锥面,锥面和平行光束相交线的尺寸不要大于半导体激光厘米bar条发光的尺寸,八个半导体激光厘米bar条的光束经正八棱锥的锥面反射,反射后的八个光束,围成正八边形,形成正八边形空心激光光源,空心激光光源以平行于锥轴方向射出,实现高光强对比度和大暗斑尺寸的空心激光光源。When a semiconductor laser hollow laser light source emitting device of the present invention is working, the same as the existing semiconductor laser centimeter bar, the output light of each semiconductor laser centimeter bar 2 needs to be collimated by a collimator 3 into a beam of parallel beams. light, as shown in Figure 2. In Figure 2, each beam of parallel light is incident on the conical surface of the regular octagonal pyramid 1 at an angle of 45 degrees. The size of the intersection line between the conical surface and the parallel beam should not be greater than the size of the semiconductor laser centimeter bar. The beams of eight semiconductor laser centimeter bars Reflected by the conical surface of the regular octagonal pyramid, the eight reflected beams form a regular octagon to form a regular octagonal hollow laser light source. The hollow laser light source is emitted parallel to the cone axis to achieve high light intensity contrast and large dark spot size. Laser light source.
可见,在本发明之一种半导体激光空心激光光源发射装置中,正八棱锥可以改换成其他的正棱锥,提高暗斑尺寸,另外可以根据需要,通过调整半导体激光厘米bar条的位置,如图 2所示,满足不同暗斑尺寸要求的半导体激光空心激光光源。It can be seen that in one semiconductor laser hollow laser light source emitting device of the present invention, the regular octagonal pyramid can be replaced with other regular pyramids to increase the size of the dark spot. In addition, the position of the centimeter bar of the semiconductor laser can be adjusted as required, as shown in the figure 2, semiconductor laser hollow laser light sources that meet the requirements of different dark spot sizes.
由于在本发明的构成中有八个半导体激光厘米bar条2,每个半导体激光厘米bar条2都水平放置,经过正八棱镜反射后输出的空心激光光束以垂直水平方向射出,因此,降低了半导体激光空心激光光源发射装置的装调难度。Since there are eight semiconductor laser centimeter bar bars 2 in the composition of the present invention, each semiconductor laser centimeter bar bar 2 is all placed horizontally, and the hollow laser beam output after being reflected by the regular octagonal prism emits with the vertical horizontal direction, therefore, reduces the semiconductor laser beam. Difficulty in the assembly and adjustment of the laser hollow laser light source emitting device.
附图说明Description of drawings
图 1 是本发明之一种半导体激光空心激光光源发射装置的结构示意图的俯视图,该图同时作为摘要附图。图 2 为沿图 1中的 A-A方向的剖视图,能清晰表示每个半导体激光厘米bar条光束行走路径情况。Fig. 1 is a top view of a structural schematic diagram of a semiconductor laser hollow laser light source emitting device of the present invention, which is also used as a summary drawing. Figure 2 is a cross-sectional view along the A-A direction in Figure 1, which can clearly show the beam path of each semiconductor laser centimeter bar.
具体实施方式Detailed ways
下面结合图1对本发明进一步详细说明。The present invention will be further described in detail below in conjunction with FIG. 1 .
本发明之一种半导体激光空心激光光源发射装置其具体方案如下所述,如图 1所示,正八棱锥1的每个锥面与底面的二面角为45度;将正八棱锥固定水平放置,八个锥面方向分别水平放置一个半导体激光厘米bar条2,半导体激光厘米bar条2出光方向指向对应着的锥面;每个半导体激光厘米bar条2都以正八棱锥1的锥轴成轴对称分布;从每个半导体激光厘米bar条2输出的光束经准直镜3进行准直,准直后光束成为一束平行光;每束平行光再以45度角入射到正八棱锥1的每个锥面,锥面和平行光束相交线的尺寸不要大于半导体激光厘米bar条发光的尺寸,每束平行光再经正八棱锥1的锥面反射,根据光在两种均匀介质界面发生反射时的反射定律,得出每束平行光在两界面反射时的反射角等于入射角,因此,反射后的八个光束,围成正八边形,形成正八边形空心激光光源,空心激光光源以平行于锥轴方向射出,最终实现高光强对比度和大暗斑尺寸的空心激光光源。Its specific scheme of a semiconductor laser hollow laser source emitting device of the present invention is as follows, as shown in Figure 1, the dihedral angle between each cone surface and the bottom surface of the regular octagonal pyramid 1 is 45 degrees; the regular octagonal pyramid is fixed and placed horizontally, A semiconductor laser centimeter bar 2 is placed horizontally in the eight cone directions, and the light emission direction of the semiconductor laser centimeter bar 2 points to the corresponding cone surface; each semiconductor laser centimeter bar 2 is axisymmetric with the cone axis of the regular octagonal pyramid 1 Distribution; the beam output from each semiconductor laser centimeter bar 2 is collimated by the collimator 3, and the beam becomes a beam of parallel light after collimation; each beam of parallel light is incident on each of the regular octagonal pyramid 1 at an angle of 45 degrees The size of the cone surface, the intersection line of the cone surface and the parallel beam should not be larger than the size of the semiconductor laser centimeter bar, and each beam of parallel light is reflected by the cone surface of the regular octagonal pyramid 1, according to the reflection when the light is reflected at the interface of two homogeneous media According to the law, the reflection angle of each beam of parallel light is equal to the incident angle when it is reflected on the two interfaces. Therefore, the eight reflected beams form a regular octagon to form a regular octagonal hollow laser light source. The hollow laser light source is parallel to the cone. It emits in the axial direction, and finally realizes a hollow laser light source with high light intensity contrast and large dark spot size.
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