CN214589688U - Linear light field laser - Google Patents
Linear light field laser Download PDFInfo
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- CN214589688U CN214589688U CN202121243942.4U CN202121243942U CN214589688U CN 214589688 U CN214589688 U CN 214589688U CN 202121243942 U CN202121243942 U CN 202121243942U CN 214589688 U CN214589688 U CN 214589688U
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Abstract
The utility model relates to a semiconductor laser and laser radar application discloses a device of linear laser of far field high aspect ratio obtains, include: placing a plurality of laser emission units which are closely arranged into a linear array, wherein the laser emission units are not placed in the middle area of the linear array; placing a lens in the light emitting direction of the linear array, wherein the distance between the main surface of the lens and the linear array is the focal length of the lens; and placing the cylindrical mirror array in the light emergent direction of the lens. The device provided by the utility model make the linear array of laser's light collimation back through the lens formation of image expand the line source of high aspect ratio with the light field through the post lens array.
Description
Technical Field
The utility model belongs to the technical field of the semiconductor laser, concretely relates to linear light field laser instrument.
Background
Semiconductor lasers have been developed rapidly in various fields as they are gradually replaced with other laser sources in recent years due to their small size, chip-type, and easy integration. Semiconductor laser can be selected from a plurality of wavelengths, and has mature laser from ultraviolet 350nm to 2000nm, especially in the field of laser radar, the semiconductor laser is an indispensable light source requirement.
However, in order to improve the scanning efficiency of the laser radar, obtaining a uniform and high-brightness line laser light source is an indispensable approach in various radar schemes, but due to the poor quality of the light beam of the semiconductor laser and the influence of the directionality of the laser, in the scheme of obtaining a linear light field, a light beam with a high uniformity and a large aspect ratio (the line width direction is less than 1 °, and the line length direction is greater than 120 °) cannot be effectively obtained, and in the currently applied laser radar scheme, the requirement for a light beam with a large aspect ratio is higher and higher, and a new laser light source scheme is urgently needed.
SUMMERY OF THE UTILITY MODEL
The to-be-solved technical problem of the utility model is: how can change into the linear light field of great aspect ratio at the high efficiency of assurance laser, evenly, for solving above-mentioned problem, the utility model provides a linear light field laser instrument, include:
the laser emission units are closely arranged into a linear array;
lens and post lens array, lens and post lens array set gradually and set up in the luminous direction of the linear array of laser emission unit, the array orientation of post lens array is unanimous with the array orientation of laser emission unit, the laser emission unit is located lens optical axis direction both sides, do not set up the laser emission unit on lens optical axis and the near 100 micron region of optical axis.
Preferably, the laser emitting unit is one or a combination of a plurality of laser bar array chips, surface emitting laser array chips, and single-tube laser chips.
In any of the above aspects, preferably, the lens is one of a spherical lens, an aspherical lens, a combined lens, or a fresnel lens.
In any of the above aspects, it is preferable that the lenticular lens array is one of a concave lenticular lens array, a convex lenticular lens array, a fresnel lenticular lens array, or a diffractive optical element-based lenticular lens array.
In any of the above solutions, it is preferable that the spatial period of the lenticular lens array is between 3mm and 1 μm.
The utility model has the advantages that: the utility model provides a pair of linear light field laser instrument, through the linear laser output that lens formation of image makes the linear array of laser's light collimation back expand light into high homogeneity, high aspect ratio through the post lens array.
Drawings
Fig. 1 is a schematic structural diagram of a linear optical field laser according to a first embodiment of the present invention;
fig. 2 is a structural diagram of a surface-emitting laser chip according to a first embodiment of the present invention;
fig. 3 is a complete structure diagram of a linear light field laser according to a first embodiment of the present invention;
fig. 4 is a complete structure diagram of a linear light field laser according to a second embodiment of the present invention;
fig. 5 is a structural diagram of a single-tube laser chip according to a second embodiment of the present invention;
fig. 6 is a complete structure diagram of a linear light field laser according to a third embodiment of the present invention;
fig. 7 is a laser bar array chip structure according to a third embodiment of the present invention.
Detailed Description
In order to further understand the present invention, the present invention will be described in detail with reference to the following embodiments.
The utility model provides a linear light field laser instrument, include: the laser emitting units 1 are arranged in a linear array at a short distance; the laser emitting device comprises a lens 2 and a cylindrical lens array 3, wherein the lens 2 and the cylindrical lens array 3 are sequentially arranged and arranged in the light emitting direction of the linear array of the laser emitting unit 1, the arrangement direction of the cylindrical lens array 3 is consistent with that of the laser emitting unit 1, the laser emitting unit 1 is positioned at two sides of the optical axis direction of the lens 2, the laser emitting unit 1 is not arranged on the 100 micron area near the optical axis and the optical axis of the lens 2, the laser emitting unit 1 is one or combination of a laser batten array chip, a surface emitting laser array chip and a plurality of single tube laser chips, the lens 2 is one of a ball lens, a non-ball lens, a combined lens or a Fresnel lens, the cylindrical lens array 3 is one of a concave cylindrical lens array, a convex cylindrical lens array, a Fresnel cylindrical lens array or a cylindrical lens array based on a diffraction optical element, the spatial period of the cylindrical lens array 3 is between 3mm and 1 μm.
Example one
The present embodiment provides a linear optical field laser, including:
the surface-emitting laser chip 1 is shown in fig. 2, wherein 1a is 16 active emitting regions, the active emitting regions 1a are arranged in a linear array, 1b is a positive electrode, 1c is a negative electrode, the outline of the active emitting region is a circular region with a diameter of 10 micrometers, and the central region of the surface-emitting chip 1 is free of the active emitting regions 1 a. When the positive and negative electrodes are connected to an external power source, the active emission region 1a emits laser light in the normal direction thereof.
The structure of the linear light field laser is shown in fig. 3, and the surface emitting laser chip 1 is welded and fixed on the metal shell 4; the lens 2 is fixed above the surface-emitting laser chip 1 through the metal shell 5, the distance between the lens 2 and the surface-emitting laser chip 1 is the focal length of the lens 2, and the intersection point of the optical axis 2a opposite to the lens 2 and the surface of the laser chip is free of the active emitting area 1 a; the cylindrical lens array 3 is fixed above the lens 2 through a metal tube shell 6.
The cylindrical lens array 3 is a convex lens array, and the array period of the cylindrical lens array is 0.2 mm.
The positive electrode 1b of the chip is connected and conducted with the positive electrode pin 8a of the metal tube shell through a gold thread, and the negative electrode 1c of the chip is connected and conducted with the negative electrode pin 8b of the metal tube shell through a gold thread.
Through the combination of the surface-emitting laser chip, the lens and the cylindrical lens array in the embodiment, as in the structure shown in fig. 3, the device can emit linear laser with high uniformity and large length-width ratio only by connecting the device pin with a power supply.
Example two
The present embodiment provides a linear optical field laser, including:
the single-tube laser chip 1 'is shown in fig. 5, wherein 1' a is an active emitting region, 1 'b is a positive electrode, 1' c is a negative electrode, and the outline of the active emitting region is a square region of 100 micrometers × 10 micrometers. When the positive and negative electrodes are connected to an external power source, the active emission region 1' a emits laser light in a normal direction thereof.
The structure of the linear light field laser is shown in fig. 4, the two single-tube laser chips 1' are welded and fixed on the metal shell 4 and are respectively positioned at two sides of the optical axis of the lens 2, and the two single-tube laser chips are combined into a linear array; the lens 2 is fixed above the surface emission laser chip 1 'through the metal shell 5, and the distance between the lens 2 and the single-tube laser chip 1' is the focal length of the lens 2; the cylindrical lens array 3 is fixed above the lens 2 through a metal tube shell 6.
The cylindrical lens array 3' is a concave lens array, and the array period of the concave lens array is 1.2 mm.
The positive electrode 1 'b of the chip is connected and conducted with the positive electrode pin 8a of the metal tube shell through a gold thread, and the negative electrode 1' c of the chip is connected and conducted with the negative electrode pin 8b of the metal tube shell through a gold thread.
Through the combination of the surface-emitting laser chip, the lens and the cylindrical lens array in the embodiment, as in the structure shown in fig. 3, the device can emit linear laser with high uniformity and large length-width ratio only by connecting the device pin with a power supply.
EXAMPLE III
The present embodiment provides a linear optical field laser, including:
the laser bar array chip 1 "is shown in fig. 2, wherein 1" a is 8 active emitting regions, the 8 active emitting regions are arranged in a linear array, 1 "b is a positive electrode, 1" c is a negative electrode, the outline of the active emitting region is a square region with a diameter of 100 micrometers × 10 micrometers, and the central region of the laser bar array chip 1 is free of the active emitting region 1 "a. When the positive electrode and the negative electrode are connected with an external power supply, the active emission region 1' a emits laser light in the normal direction thereof.
The structure of the linear light field laser is shown in fig. 3, and the laser bar array chip 1 is welded and fixed on the metal shell 4; the lens 2 is fixed above the laser bar array chip 1 through the metal shell 5, the distance between the lens 2 and the surface emitting laser chip 1 is the focal length of the lens 2, and the intersection point of the optical axis 2a opposite to the lens 2 and the surface of the laser chip is free of the active emitting area 1 a; the cylindrical lens array 3 is fixed above the lens 2 through a metal tube shell 6.
The cylindrical lens array 3 is a convex lens array, and the array period of the cylindrical lens array is 0.2 mm.
The positive electrode 1b of the chip is connected and conducted with the positive electrode pin 8a of the metal tube shell through a gold thread, and the negative electrode 1c of the chip is connected and conducted with the negative electrode pin 8b of the metal tube shell through a gold thread.
Through the combination of the surface-emitting laser chip, the lens and the cylindrical lens array in the embodiment, as in the structure shown in fig. 3, the device can emit linear laser with high uniformity and large length-width ratio only by connecting the device pin with a power supply.
To sum up, the utility model provides a linear light field laser. The laser emission units are arranged in a linear array at a short distance, and the laser emission units are not arranged in the middle area of the linear array; placing a lens in the light emitting direction of the linear array, wherein the distance between the main surface of the lens and the linear array is the focal length of the lens; and placing the cylindrical mirror array in the light emergent direction of the lens. The device provided by the utility model make the linear array of laser's light collimation back through the lens formation of image and expand into high homogeneity, high aspect ratio's line laser output through the cylindrical lens array.
It will be understood by those skilled in the art that a linear optical field laser according to the present invention includes any combination of the above-mentioned embodiments and embodiments of the present invention and the various parts shown in the drawings, which are not described in detail and are not intended to simplify the present description. Any modification, equivalent replacement, or improvement made within the spirit and principle of the present invention should be included in the protection scope of the present invention.
Claims (5)
1. A linear optical field laser, comprising:
the laser emission units are closely arranged into a linear array;
lens and post lens array, lens and post lens array set gradually and set up in the luminous direction of the linear array of laser emission unit, the array orientation of post lens array is unanimous with the array orientation of laser emission unit, the laser emission unit is located lens optical axis direction both sides, do not set up the laser emission unit on lens optical axis and the near 100 micron region of optical axis.
2. The linear light field laser as claimed in claim 1, wherein the laser emitting unit is one or more of a laser bar array chip, a surface emitting laser array chip, and a plurality of single-tube laser chips.
3. The linear light field laser as defined in claim 1, wherein the lens is one of a spherical lens, an aspherical lens, a combined lens or a fresnel lens.
4. The linear optical field laser as claimed in claim 1, wherein the cylindrical lens array is one of a concave cylindrical lens array, a convex cylindrical lens array, a fresnel cylindrical lens array or a cylindrical lens array based on diffractive optical elements.
5. A linear light field laser as claimed in claim 1 wherein the spatial period of the cylindrical lens array is between 3mm and 1 μm.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202121243942.4U CN214589688U (en) | 2021-06-04 | 2021-06-04 | Linear light field laser |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202121243942.4U CN214589688U (en) | 2021-06-04 | 2021-06-04 | Linear light field laser |
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| CN214589688U true CN214589688U (en) | 2021-11-02 |
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Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113224644A (en) * | 2021-06-04 | 2021-08-06 | 河北派科艾知光电科技有限公司 | Linear light field laser |
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Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113224644A (en) * | 2021-06-04 | 2021-08-06 | 河北派科艾知光电科技有限公司 | Linear light field laser |
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Address after: Room 302, Building B, 226 Guangtian Road, Tangxiayong Community, Yanluo Street, Bao'an District, Shenzhen City, Guangdong Province, 518000 Patentee after: Paco Optoelectronic Technology (Shenzhen) Co.,Ltd. Address before: 065000 Room 501, unit 2, building 3, Xiangtai garden, economic and Technological Development Zone, Langfang City, Hebei Province Patentee before: Hebei PAIKE Aizhi Photoelectric Technology Co.,Ltd. |
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