CN116659665B - Full spectrum signal acquisition device - Google Patents
Full spectrum signal acquisition device Download PDFInfo
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- CN116659665B CN116659665B CN202310597376.4A CN202310597376A CN116659665B CN 116659665 B CN116659665 B CN 116659665B CN 202310597376 A CN202310597376 A CN 202310597376A CN 116659665 B CN116659665 B CN 116659665B
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- lenses
- lens
- spectrum signal
- detectors
- detector
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- 238000001228 spectrum Methods 0.000 title claims abstract description 55
- 230000003595 spectral effect Effects 0.000 claims description 6
- 238000001514 detection method Methods 0.000 abstract description 10
- 238000010586 diagram Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/12—Generating the spectrum; Monochromators
- G01J3/18—Generating the spectrum; Monochromators using diffraction elements, e.g. grating
Abstract
The invention provides a full spectrum signal acquisition device, comprising: the device comprises a Roland circle body, a plurality of first lenses, a plurality of second lenses, a plurality of first detectors and a plurality of second detectors; each first lens faces a first detector, each second lens faces a second detector, and the first lenses and the second lenses are arranged in a crossing manner. The spectrum signal can be well ensured to be totally reflected to the first detector or the second detector, and when the spectrum signal irradiates between the first lens and the second lens, the spectrum signal can be well divided into two halves, one half of the signal can be upwardly reflected to the first detector by the first lens, and the other half of the signal can be downwardly reflected to the second detector by the second lens, so that the detection of the spectrum signal can be well ensured, and the condition of missing can not occur. Therefore, by adopting the full spectrum signal acquisition device, the acquisition and detection of signals can be well ensured, and the full spectrum line detection without missing of spectrum signals can be realized.
Description
Technical Field
The invention relates to the technical field of spectrum detection equipment, in particular to a full spectrum signal acquisition device.
Background
The incident spectrum signal reaches the grating after passing through the slit, and various spectral lines are separated after diffraction by the grating, and as different wavelength spectral lines of different elements are densely focused on different positions of the Roland circle, in order to detect all spectrum signals, all spectrum signal detectors are required to be arranged on the Roland circle, and the basic function of the spectrum signal detectors is to convert the received optical signals into electrical signals. The spectrum signal detector receives the spectrum signal, but since the effective detecting unit edge of the current common spectrum signal detector has a certain distance from the edge of the detector shell, an ineffective detecting space is formed, which results in that the spectrum signal detector is completely arranged on the Roland circle, but the ineffective detecting space of two sections exists between the former spectrum signal detector and the latter spectrum signal detector, so that full spectrum detection cannot be realized, and therefore, a full spectrum signal acquisition device is needed to solve the problem.
Disclosure of Invention
In order to solve the problems, the invention adopts the following technical scheme: a full spectrum signal acquisition device comprising: the device comprises a Roland circle body, a plurality of first lenses, a plurality of second lenses, a plurality of first detectors and a plurality of second detectors;
the first lenses, the second lenses, the first detectors and the second detectors are arranged on the Rowland circle body;
Each first lens faces one first detector, each second lens faces one second detector, and a plurality of first lenses and a plurality of second lenses are arranged in a crossing way.
Further, the rowland circle body is provided with a rowland circle plane, a slit and a grating are arranged on the rowland circle plane, an external light source passes through the slit and irradiates the grating, and a plurality of first lenses and a plurality of second lenses are arranged on the rowland circle plane.
Further, an included angle between each first lens and the rowland circle plane is 45 degrees.
Further, an included angle between each second lens and the Roland circle plane is-45 degrees.
Further, the first lenses and the second lenses are reflective lenses.
Further, the shapes of the first lenses and the second lenses are parallelograms.
Further, the hypotenuse of each first lens abuts against the hypotenuse of one second lens.
Further, the plurality of first detectors and the plurality of second detectors are each spectral signal detectors.
Further, each of the first detectors is disposed above one of the first lenses.
Further, each of the second detectors is disposed below one of the second lenses.
The beneficial effects of the invention are as follows: by using the full spectrum signal acquisition device, a plurality of first detectors and a plurality of second detectors are arranged on the Rowland circle body, the Rowland circle plane on the Rowland circle body is alternately provided with the first lenses and the second lenses, an external spectrum signal passes through the slit and irradiates the grating, various spectral lines are separated after diffraction of the grating, and finally, when the grating irradiates the first lenses and the second lenses, the spectrum signal can be well ensured to be totally reflected to the first detectors or the second detectors, the spectrum signal can be well divided into two halves, half of the signal can be upwardly reflected to the first detectors by the first lenses, and the other half of the signal can be downwardly reflected to the second detectors by the second lenses, so that the detection of the spectrum signal can be well ensured, and the condition of missing can not occur. Therefore, by adopting the full spectrum signal acquisition device, the acquisition and detection of signals can be well ensured, and the full spectrum line detection without missing of spectrum signals can be realized.
Drawings
The invention is further illustrated by the accompanying drawings, which are not to be construed as limiting the invention in any way.
Fig. 1 is a schematic diagram of the overall structure of a full spectrum signal acquisition device according to an embodiment;
Fig. 2 is a schematic diagram of a direction of a full spectrum signal acquisition device according to an embodiment.
Detailed Description
The technical solution of the present invention will be further described below with reference to the accompanying drawings of the embodiments of the present invention, and the present invention is not limited to the following specific embodiments. It should be noted that, without conflict, the embodiments of the present invention and features of the embodiments may be combined with each other.
As shown in fig. 1 to 2, a full spectrum signal acquisition device includes: a rowland circle body, a plurality of first lenses 200, a plurality of second lenses 300, a plurality of first detectors 400, and a plurality of second detectors 500; the first lenses 200, the second lenses 300, the first detectors 400 and the second detectors 500 are all arranged on the rowland circle body; each of the first lenses 200 faces one of the first detectors 400, each of the second lenses 300 faces one of the second detectors 500, and a plurality of the first lenses 200 are disposed to intersect a plurality of the second lenses 300. Further, the rowland circle body has a rowland circle plane 100, a slit 600 and a grating 700 are disposed on the rowland circle plane, an external light source passes through the slit 600 and irradiates the grating 700, and a plurality of first lenses 200 and a plurality of second lenses 300 are disposed on the rowland circle plane.
In one embodiment, by disposing the first detectors 400 and the second detectors 500 on the rowland circle body, the positions where the first detectors 400 and the second detectors 500 are disposed are positions irradiated by an external light source. That is, by providing a plurality of first detectors 400 and a plurality of second detectors 500, the range which can be irradiated by the external light source is fully arranged, so that the light source can be well received. That is, the specific number of the first detector 400 and the second detector 500 may be adjusted according to the irradiation range of the external light source, it is worth mentioning that, in order to ensure that the first lens 200 is matched with the first detector 400, the second lens 300 is matched with the second detector 500, and thus, the number of the first lens 200 is consistent with the number of the first detector 400, and the number of the second lens 300 is consistent with the number of the second detector 500, that is, the numbers of the first detector 400, the second detector 500, the first lens 200 and the second lens 300 may be specifically adjusted according to the irradiation range of the external light source, which is not cumbersome in this embodiment.
In one embodiment, each of the first lenses 200 is disposed at an angle of 45 ° to the rowland circle plane 100. Each of the second lenses 300 has an angle of-45 ° with respect to the rowland circle plane 100. Further, the first lenses 200 and the second lenses 300 are reflective lenses. It should be noted that the shapes of the first lenses 200 and the second lenses 300 are parallelograms. The hypotenuse of each first lens 200 abuts against the hypotenuse of one second lens 300. It is further noted that each of the first detectors 400 is disposed above one of the first lenses 200. Each of the second detectors 500 is disposed under one of the second lenses 300. That is, when an external light source, that is, an incident light is irradiated onto the grating 700 through the slit 600, a diffraction spectrum is formed by diffraction of the grating 700, an emitted spectrum signal is upwardly reflected to the first detector 400 through the first lens 200, when an external light source, that is, an incident light is irradiated onto the grating 700 through the slit 600, a diffraction spectrum is formed by diffraction of the grating 700, an emitted spectrum signal is downwardly reflected to the second detector 500 through the second lens 300, a plurality of first lenses 200 and a plurality of second lenses 300 are closely spaced apart from each other, and since the first lens 200 and the second lens 300 are in a parallelogram shape, a gap between them is a slant line when the first lens 200 and the second lens 300 are close together, and since the first lens 200 is 45 ° to the rowland plane 100, the second lens 300 is-45 ° to the rowland plane 100, even if the spectrum signal is irradiated onto the second lens 300, the spectrum signal is well reflected to the second detector 500 by the second lens 300, and the first lens 200 is well reflected to the second lens 300, and the second half of the spectrum signal is well detected by the first lens 300, and the second half of the spectrum signal is well reflected to the second lens 300. Therefore, by adopting the full spectrum signal acquisition device, the acquisition and detection of signals can be well ensured, and the full spectrum line detection without missing of spectrum signals can be realized.
In one embodiment, the plurality of first detectors 400 and the plurality of second detectors 500 are each spectral signal detectors. That is, the first detector 400 and the second detector 500 may be detectors capable of detecting an optical signal, for example, the first detector 400 and the second detector 500 may be CCD detectors. That is, the first detector 400 and the second detector 500 may be other spectrum signal detectors, which is not described in detail in this embodiment.
In summary, the above-described embodiments are not intended to be limiting embodiments of the present invention, and modifications and equivalent variations, which are within the spirit and scope of the present invention, will be within the technical scope of the present invention.
Claims (7)
1. A full spectrum signal acquisition device, comprising: the device comprises a Roland circle body, a plurality of first lenses, a plurality of second lenses, a plurality of first detectors and a plurality of second detectors;
the first lenses, the second lenses, the first detectors and the second detectors are arranged on the Rowland circle body;
each first lens faces one first detector, each second lens faces one second detector, and a plurality of first lenses and a plurality of second lenses are arranged in a crossing way;
The shapes of the first lenses and the second lenses are parallelograms;
the first lenses and the second lenses are reflective lenses;
the hypotenuse of each first lens is abutted with the hypotenuse of one second lens.
2. The full spectrum signal acquisition device of claim 1, wherein: the Rowland round body is provided with a Rowland round plane, the Rowland round plane is provided with a slit and a grating, an external light source passes through the slit and irradiates onto the grating, and a plurality of first lenses and a plurality of second lenses are arranged on the Rowland round plane.
3. The full spectrum signal acquisition device of claim 2, wherein: and an included angle between each first lens and the Roland round plane is 45 degrees.
4. A full spectrum signal acquisition device according to claim 3, wherein: and the included angle between each second lens and the Roland round plane is-45 degrees.
5. The full spectrum signal acquisition device of claim 4, wherein: the plurality of first detectors and the plurality of second detectors are spectral signal detectors.
6. The full spectrum signal acquisition device of claim 5, wherein: each first detector is arranged above one first lens.
7. The full spectrum signal acquisition device of claim 6, wherein: each second detector is arranged below one second lens.
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CN116659665B true CN116659665B (en) | 2024-05-03 |
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Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2005095910A1 (en) * | 2004-04-01 | 2005-10-13 | Alexandr Markovich Livshits | Spectrometer |
DE19861479B4 (en) * | 1998-11-21 | 2016-02-25 | Spectro Analytical Instruments Gmbh | Simultaneous double grating spectrometer with semiconductor line sensors or photomultipliers |
CN205958106U (en) * | 2016-08-10 | 2017-02-15 | 无锡创想分析仪器有限公司 | Beam -splitting structure of spectrum appearance |
CN107490435A (en) * | 2017-07-27 | 2017-12-19 | 江苏天瑞仪器股份有限公司 | Full spectrum sweep type spark photo-electric direct reading spectrometer |
CN217638695U (en) * | 2022-06-13 | 2022-10-21 | 北京北分瑞利分析仪器(集团)有限责任公司 | Oil emission spectrometer light splitting system and device covering ultraviolet visible near-infrared band |
CN115931129A (en) * | 2022-12-09 | 2023-04-07 | 北方工业大学 | High-sensitivity high-resolution full-spectrum optical system |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
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JP7395775B2 (en) * | 2020-05-18 | 2023-12-11 | シグレイ、インコーポレイテッド | Systems and methods for X-ray absorption spectroscopy using a crystal analyzer and multiple detector elements |
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- 2023-05-24 CN CN202310597376.4A patent/CN116659665B/en active Active
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19861479B4 (en) * | 1998-11-21 | 2016-02-25 | Spectro Analytical Instruments Gmbh | Simultaneous double grating spectrometer with semiconductor line sensors or photomultipliers |
WO2005095910A1 (en) * | 2004-04-01 | 2005-10-13 | Alexandr Markovich Livshits | Spectrometer |
CN205958106U (en) * | 2016-08-10 | 2017-02-15 | 无锡创想分析仪器有限公司 | Beam -splitting structure of spectrum appearance |
CN107490435A (en) * | 2017-07-27 | 2017-12-19 | 江苏天瑞仪器股份有限公司 | Full spectrum sweep type spark photo-electric direct reading spectrometer |
CN217638695U (en) * | 2022-06-13 | 2022-10-21 | 北京北分瑞利分析仪器(集团)有限责任公司 | Oil emission spectrometer light splitting system and device covering ultraviolet visible near-infrared band |
CN115931129A (en) * | 2022-12-09 | 2023-04-07 | 北方工业大学 | High-sensitivity high-resolution full-spectrum optical system |
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