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CN207816830U - Become wavelength excitation and the adjustable Raman spectrometer of spectral region - Google Patents

Become wavelength excitation and the adjustable Raman spectrometer of spectral region Download PDF

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Publication number
CN207816830U
CN207816830U CN201820297839.XU CN201820297839U CN207816830U CN 207816830 U CN207816830 U CN 207816830U CN 201820297839 U CN201820297839 U CN 201820297839U CN 207816830 U CN207816830 U CN 207816830U
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laser
plane
raman
raman spectrometer
blazed grating
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田兆硕
毕宗杰
王玲
张珊珊
张延超
李沫霖
付石友
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Shandong Marine Technology Research Institute
Harbin Institute of Technology Weihai
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Shandong Marine Technology Research Institute
Harbin Institute of Technology Weihai
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Abstract

本实用新型提出一种变波长激发及光谱范围可调的拉曼光谱仪,包括激光器,激光器发射的激光束激发样品所产生的拉曼光散射到入射狭缝,上述拉曼光依次经过第一平面反射镜、第一凹面反射镜反射后转变为平行光束入射到平面闪耀光栅表面,平面闪耀光栅固定在旋转平台上,通过旋转平台可使平面闪耀光栅旋转;经平面闪耀光栅分光后的反射光依次经过第二凹面反射镜以及第二平面反射镜后聚焦在探测器的表面,探测器与信号处理系统相连接,信号处理系统还与显示器相连接。上述拉曼光谱仪由于平面闪耀光栅的角度可调,因此可选用多种不同波长的激光器作为激发光源;对于某一特定激光波长,还可通过调节平面闪耀光栅的角度,实现较宽范围的拉曼光谱测量。

The utility model proposes a Raman spectrometer with variable wavelength excitation and adjustable spectral range, including a laser, and the Raman light generated by the laser beam emitted by the laser to excite the sample is scattered to the incident slit, and the Raman light passes through the first plane in turn After being reflected by the reflector and the first concave reflector, the parallel beams are transformed into parallel beams incident on the surface of the plane blazed grating. The plane blazed grating is fixed on the rotating platform, and the plane blazed grating can be rotated through the rotating platform; the reflected light after being split by the plane blazed grating Focusing on the surface of the detector after passing through the second concave reflector and the second plane reflector, the detector is connected with the signal processing system, and the signal processing system is also connected with the display. Because the angle of the plane blazed grating is adjustable, the above-mentioned Raman spectrometer can use a variety of lasers with different wavelengths as the excitation light source; for a specific laser wavelength, a wide range of Raman can be realized by adjusting the angle of the plane blazed grating Spectral measurement.

Description

变波长激发及光谱范围可调的拉曼光谱仪Raman spectrometer with variable wavelength excitation and adjustable spectral range

技术领域technical field

本实用新型涉及拉曼光谱仪,尤其涉及一种变波长激发及光谱范围可调的拉曼光谱仪。The utility model relates to a Raman spectrometer, in particular to a Raman spectrometer with variable wavelength excitation and adjustable spectral range.

背景技术Background technique

拉曼光谱仪在化工、生物、农业、食品、地矿等领域检测应用日益广泛,根据实际应用情况,常见的激发光源一般采用单频固体或半导体激光器,激发波长包括266nm、355nm、405nm、450nm、466nm、485nm、532nm、785nm、1064nm等等。目前绝大多数拉曼光谱仪只能采用一种单频激光器作为激发源,为保证较高的光谱分辨率,波数测量范围一般限定为2500cm-1-4000cm-1。由于对于不同样品往往存在不同的最佳激发波长,因此为实现不同样品检测往往需要多台拉曼光谱仪配合使用,增加了检测成本及操作的复杂性。Raman spectrometers are increasingly used in chemical, biological, agricultural, food, geological and mining fields. According to actual applications, common excitation light sources generally use single-frequency solid-state or semiconductor lasers. Excitation wavelengths include 266nm, 355nm, 405nm, 450nm, 466nm, 485nm, 532nm, 785nm, 1064nm, etc. At present, most Raman spectrometers can only use a single-frequency laser as the excitation source. In order to ensure high spectral resolution, the wavenumber measurement range is generally limited to 2500cm -1 -4000cm -1 . Since there are often different optimal excitation wavelengths for different samples, multiple Raman spectrometers are often required to be used together in order to detect different samples, which increases the cost of detection and the complexity of operation.

实用新型内容Utility model content

为了解决现有技术中存在的问题。本实用新型提出了一种变波长激发及光谱范围可调的拉曼光谱仪。In order to solve the problems existing in the prior art. The utility model provides a Raman spectrometer with variable wavelength excitation and adjustable spectral range.

为了实现上述目的,本实用新型提出了一种变波长激发及光谱范围可调的拉曼光谱仪,包括激光器,所述激光器可选用固体、气体或半导体激光器,其发射波长可变,所述激光器发射的激光束激发样品所产生的拉曼光散射到入射狭缝,上述拉曼光依次经过第一平面反射镜、第一凹面反射镜反射后转变为平行光束入射到平面闪耀光栅表面,所述平面闪耀光栅固定在旋转平台上,通过所述旋转平台可使平面闪耀光栅旋转;经所述平面闪耀光栅分光后的反射光依次经过第二凹面反射镜以及第二平面反射镜后聚焦在探测器的表面,所述探测器与信号处理系统相连接,所述信号处理系统还与显示器相连接。In order to achieve the above object, the utility model proposes a Raman spectrometer with variable wavelength excitation and adjustable spectral range, including a laser, the laser can be a solid, gas or semiconductor laser, the emission wavelength is variable, and the laser emits The Raman light generated by the sample excited by the laser beam scatters to the incident slit, and the above-mentioned Raman light is reflected by the first plane reflector and the first concave reflector in turn, and then transformed into a parallel beam incident on the surface of the plane blazed grating. The blazed grating is fixed on the rotating platform, and the planar blazed grating can be rotated through the rotating platform; the reflected light after the splitting of the planar blazed grating passes through the second concave reflector and the second planar reflector in sequence, and then focuses on the detector. On the surface, the detector is connected with a signal processing system, and the signal processing system is also connected with a display.

优选的是,所述激光器发射的激光束直接或通过光纤入射到样品。Preferably, the laser beam emitted by the laser is incident on the sample directly or through an optical fiber.

优选的是,所述激光器发射的激光束激发样品所产生的拉曼光直接入射或通过光纤入射到入射狭缝。Preferably, the Raman light generated by exciting the sample with the laser beam emitted by the laser is directly incident or incident into the incident slit through an optical fiber.

优选的是,所述探测器采用线阵或面阵成像器件。Preferably, the detector adopts a line array or area array imaging device.

优选的是,所述探测器采用CCD或CMOS器件。Preferably, the detector adopts CCD or CMOS device.

本实用新型的该方案的有益效果在于上述变波长激发及光谱范围可调的拉曼光谱仪,由于平面闪耀光栅的角度可调,因此可选用多种不同波长的激光器作为激发光源;对于某一特定激光波长,还可通过调节平面闪耀光栅的角度,实现较宽范围的拉曼光谱测量。本实用新型所涉及的变波长激发及光谱范围可调的拉曼光谱仪具有结构紧凑、体积小的优点。The beneficial effect of this scheme of the utility model is that the above-mentioned Raman spectrometer with variable wavelength excitation and adjustable spectral range, because the angle of the plane blazed grating can be adjusted, so a variety of lasers with different wavelengths can be used as the excitation light source; for a specific The laser wavelength can also be adjusted by adjusting the angle of the planar blazed grating to achieve a wide range of Raman spectrum measurement. The Raman spectrometer with variable wavelength excitation and adjustable spectral range involved in the utility model has the advantages of compact structure and small volume.

附图说明Description of drawings

图1示出了本实用新型所涉及的变波长激发及光谱范围可调的拉曼光谱仪的结构示意图。Fig. 1 shows a schematic structural diagram of a Raman spectrometer with variable wavelength excitation and adjustable spectral range involved in the present invention.

附图标记:1-激光器,2-样品,3-入射狭缝,4-第一平面反射镜,5-第一凹面反射镜,6-平面闪耀光栅,7-旋转平台,8-旋转旋钮,9-第二凹面反射镜,10-第二平面反射镜,11-探测器,12-信号处理系统,13-显示器。Reference signs: 1-laser, 2-sample, 3-incident slit, 4-first flat mirror, 5-first concave mirror, 6-plane blazed grating, 7-rotary platform, 8-rotary knob, 9-the second concave mirror, 10-the second plane mirror, 11-the detector, 12-the signal processing system, 13-the display.

具体实施方式Detailed ways

下面结合附图对本实用新型的具体实施方式作进一步的说明。Below in conjunction with accompanying drawing, the specific embodiment of the present utility model is described further.

如图1所示,本实用新型所涉及的变波长激发及光谱范围可调的拉曼光谱仪包括激光器1,所述激光器1可选用固体、气体或半导体激光器,其发射波长可变,所述激光器1可根据不同样品的激发波长需求进行更换,所述激光器1发射的激光束激发样品2所产生的拉曼光散射到入射狭缝3,在本实施例中,所述激光器1发射的激光束直接或通过光纤入射到样品2;所述激光器1发射的激光束激发样品2所产生的拉曼光直接入射或通过光纤入射到入射狭缝3。As shown in Figure 1, the Raman spectrometer with variable wavelength excitation and adjustable spectral range involved in the utility model includes a laser 1, and the laser 1 can be a solid, gas or semiconductor laser, whose emission wavelength is variable, and the laser 1 can be replaced according to the excitation wavelength requirements of different samples. The Raman light generated by the laser beam emitted by the laser 1 to excite the sample 2 is scattered to the incident slit 3. In this embodiment, the laser beam emitted by the laser 1 It is incident on the sample 2 directly or through an optical fiber; the Raman light generated by the laser beam emitted by the laser 1 to excite the sample 2 is directly incident or incident on the incident slit 3 through an optical fiber.

上述拉曼光依次经过第一平面反射镜4、第一凹面反射镜5反射后转变为平行光束入射到平面闪耀光栅6表面,所述平面闪耀光栅6固定在旋转平台7上,通过所述旋转平台7可使平面闪耀光栅6旋转,具体的所述旋转平台7可采用电控或手动的控制方式实现旋转,在本实施例中,所述旋转平台7采用手动的控制方式实现旋转,具体是在所述旋转平台7上设有旋转旋钮8,通过手动旋转旋钮8可控制旋转平台7旋转。The above-mentioned Raman light is reflected by the first plane reflector 4 and the first concave reflector 5 in sequence, and then converted into a parallel light beam incident on the surface of the plane blazed grating 6. The plane blazed grating 6 is fixed on the rotating platform 7. The platform 7 can make the plane blazed grating 6 rotate. Specifically, the rotating platform 7 can be rotated by electric control or manual control. In this embodiment, the rotating platform 7 can be rotated by manual control. Specifically, A rotary knob 8 is provided on the rotary platform 7 , and the rotation of the rotary platform 7 can be controlled by manually rotating the knob 8 .

经所述平面闪耀光栅6分光后的反射光依次经过第二凹面反射镜9以及第二平面反射镜10后聚焦在探测器11的表面,由于平面闪耀光栅6的分光作用,不同波长的光线聚焦在探测器11表面的不同位置,所述探测器11与信号处理系统12相连接,经过所述信号处理系统12进行计算分析,以输出光谱数据;所述信号处理系统12还与显示器13相连接,由所述显示器13显示光谱曲线。在本实施例中,所述探测器11可采用线阵或面阵成像器件,具体的所述探测器11可采用CCD或CMOS器件;所述信号处理系统12以及显示器13均为现有技术,在此不做赘述。The reflected light after being split by the planar blazed grating 6 passes through the second concave reflector 9 and the second planar reflector 10 in turn, and then focuses on the surface of the detector 11. Due to the spectroscopic effect of the planar blazed grating 6, light rays of different wavelengths are focused At different positions on the surface of the detector 11, the detector 11 is connected to the signal processing system 12, and the calculation and analysis are performed through the signal processing system 12 to output spectral data; the signal processing system 12 is also connected to the display 13 , the spectral curve is displayed by the display 13 . In this embodiment, the detector 11 can use a linear or area array imaging device, and specifically the detector 11 can use a CCD or CMOS device; the signal processing system 12 and the display 13 are all prior art, I won't go into details here.

本实用新型所涉及的变波长激发及光谱范围可调的拉曼光谱仪,由于平面闪耀光栅6的角度可调,因此可选用多种不同波长的激光器作为激发光源;对于某一特定激光波长,还可通过调节平面闪耀光栅6的角度,实现较宽范围的拉曼光谱测量。本实用新型所涉及的变波长激发及光谱范围可调的拉曼光谱仪具有结构紧凑、体积小的优点。The Raman spectrometer with variable wavelength excitation and adjustable spectral range involved in the utility model, because the angle of the plane blazed grating 6 can be adjusted, so multiple lasers with different wavelengths can be used as the excitation light source; for a certain specific laser wavelength, also By adjusting the angle of the planar blazed grating 6, a wider range of Raman spectrum measurement can be realized. The Raman spectrometer with variable wavelength excitation and adjustable spectral range involved in the utility model has the advantages of compact structure and small volume.

光谱测量的波数与光谱仪探测器的像素点存在对应关系,波数ν与像素位置x满足多项式ν=a+bx+cx2+dx3+……的函数关系,在本实施例中,采用线性拟合即可满足误差要求,即采用ν=a+bx。具体的所述变波长激发及光谱范围可调的拉曼光谱仪的校准拼接方法包括以下步骤:There is a corresponding relationship between the wavenumber of the spectral measurement and the pixel point of the spectrometer detector, and the wavenumber ν and the pixel position x satisfy the functional relationship of the polynomial ν=a+bx+cx 2 +dx 3 +... In this embodiment, a linear quasi- Combined to meet the error requirements, that is, using ν = a + bx. The specific method for calibrating and splicing the Raman spectrometer with variable wavelength excitation and adjustable spectral range includes the following steps:

步骤1、采用激光器1对已知拉曼光谱的样品2进行激发。Step 1. Using a laser 1 to excite a sample 2 with a known Raman spectrum.

步骤2、调节旋转旋钮8,使平面闪耀光栅6转动,使得激光干扰恰好在拉曼光谱图显示之外,将此时的拉曼光谱的波数范围确定为第一段拉曼光谱位置,记录此刻旋转旋钮8的位置为第一位置。Step 2. Adjust the rotary knob 8 to rotate the flat blazed grating 6 so that the laser interference is just outside the display of the Raman spectrum. Determine the wavenumber range of the Raman spectrum at this time as the position of the first segment of the Raman spectrum, and record the position at this moment The position of the rotary knob 8 is the first position.

步骤3、利用步骤2中已知拉曼光谱的样品2的两个拉曼峰,即该两个拉曼峰的ν和x均已知,求取ν=a+bx中的参数a和b,以便确定步骤2中所获取的第一段拉曼光谱曲线中各点位置的波数,将所述第一段拉曼光谱曲线的波数和强度导出数据表格(例如EXCEL表格),记作第一数据表格。Step 3, utilize two Raman peaks of the sample 2 of known Raman spectrum in step 2, i.e. v and x of these two Raman peaks are all known, obtain parameter a and b in v=a+bx , so as to determine the wavenumber of each point position in the first section of the Raman spectrum curve acquired in step 2, the wavenumber and intensity of the first section of the Raman spectrum curve are derived from a data table (such as an EXCEL form), and are recorded as the first data table.

步骤4、调节旋转旋钮8,使步骤2中所得的拉曼峰左移,使得波数初始值增加,此时参数b数值保持不变,参数a发生变化,变成a1,将此时的拉曼光谱的波数范围确定为第二段拉曼光谱位置,记录此刻旋转旋钮8的位置为第二位置。Step 4. Adjust the rotary knob 8 to move the Raman peak obtained in step 2 to the left, so that the initial value of the wave number increases. At this time, the value of parameter b remains unchanged, and the value of parameter a changes to a 1 . The wavenumber range of the Mann spectrum is determined as the position of the second segment of the Raman spectrum, and the position at which the knob 8 is rotated at this moment is recorded as the second position.

步骤5、利用步骤4中已知拉曼光谱的样品2的一个拉曼峰,即该拉曼峰的ν和x已知,求取ν=a1+bx中的参数a1,以便确定步骤4中所获取的第二段拉曼光谱曲线中各点位置的波数,将所述第二段拉曼光谱曲线的波数和强度导出数据表格,记作第二数据表格。Step 5, using a Raman peak of the sample 2 whose Raman spectrum is known in step 4, that is, the ν and x of the Raman peak are known, and obtain the parameter a 1 in ν=a 1 +bx, so as to determine the step The wave number of each point in the second segment of the Raman spectrum curve obtained in 4, and the wave number and intensity of the second segment of the Raman spectrum curve are exported to a data table, which is recorded as the second data table.

步骤6、将步骤3中获得的第一数据表格和步骤5中获得的第二数据表格进行拼接,进而生成拼接后的拉曼光谱曲线图。Step 6, splicing the first data table obtained in step 3 and the second data table obtained in step 5, and then generating a spliced Raman spectrum graph.

若想将多段拉曼光谱曲线进行拼接,原理同上所述,在此不做赘述。通过以上方法已经对拉曼光谱仪的某一发射波长的激光器1的拉曼光谱进行校准,若更换激光器1,则需要重新校准。用户购买已经校准过的拉曼光谱仪对未知拉曼光谱的样品进行测量时,直接将旋转旋钮8调节至相应的标记位置即可,之后再对获得的两个数据表格进行拼接,以生成拼接后的拉曼光谱曲线图。If you want to splice multiple Raman spectrum curves, the principle is the same as above, so I won’t go into details here. The Raman spectrum of the laser 1 of a certain emission wavelength of the Raman spectrometer has been calibrated by the above method, and if the laser 1 is replaced, recalibration is required. When the user purchases a Raman spectrometer that has been calibrated to measure a sample with an unknown Raman spectrum, he can directly adjust the rotary knob 8 to the corresponding mark position, and then splice the two obtained data tables to generate a spliced The Raman spectrum curve.

Claims (5)

1. a kind of change wavelength excitation and the adjustable Raman spectrometer of spectral region, it is characterised in that:Including laser, the laser Solid, gas or semiconductor laser can be selected in device, and launch wavelength is variable, and the laser beam of the laser transmitting excites sample Generated Raman light scattering is to entrance slit, and above-mentioned Raman light is successively by the first plane mirror, the first concave mirror It is changed into parallel beam incident after reflection to plane balzed grating, surface, the plane balzed grating, is fixed on rotating platform, Plane balzed grating, can be made to rotate by the rotating platform;Reflected light after plane balzed grating, light splitting is passed through successively The surface of detector, the detector and signal processing system are focused on after second concave mirror and second plane mirror It is connected, the signal processing system is also connected with display.
2. change wavelength excitation according to claim 1 and the adjustable Raman spectrometer of spectral region, it is characterised in that:It is described The laser beam of laser transmitting is incident on sample directly or by optical fiber.
3. change wavelength excitation according to claim 1 and the adjustable Raman spectrometer of spectral region, it is characterised in that:It is described Raman light is directly incident caused by the laser beam excitation sample of laser transmitting or is incident on entrance slit by optical fiber.
4. change wavelength excitation according to claim 1 and the adjustable Raman spectrometer of spectral region, it is characterised in that:It is described Detector is using linear array or face battle array image device.
5. change wavelength excitation according to claim 4 and the adjustable Raman spectrometer of spectral region, it is characterised in that:It is described Detector uses CCD or cmos device.
CN201820297839.XU 2018-03-05 2018-03-05 Become wavelength excitation and the adjustable Raman spectrometer of spectral region Expired - Fee Related CN207816830U (en)

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* Cited by examiner, † Cited by third party
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CN108303407A (en) * 2018-03-05 2018-07-20 哈尔滨工业大学(威海) Become wavelength excitation and the adjustable Raman spectrometer of spectral region and calibration joining method
CN111521266A (en) * 2020-04-23 2020-08-11 佛山科学技术学院 A spectrometer optical path construction device
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108303407A (en) * 2018-03-05 2018-07-20 哈尔滨工业大学(威海) Become wavelength excitation and the adjustable Raman spectrometer of spectral region and calibration joining method
CN113155786A (en) * 2020-01-22 2021-07-23 纬创资通股份有限公司 Detection device
CN111521266A (en) * 2020-04-23 2020-08-11 佛山科学技术学院 A spectrometer optical path construction device
CN118670999A (en) * 2024-07-01 2024-09-20 深圳市康立生物医疗有限公司 Multi-protein detection system and method based on spectrometer and reagent method

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