Photon counting Raman spectrometer capable of realizing full spectrum direct-reading performance
A Raman spectrometer and photon counting technology, applied in spectrometry/spectrophotometry/monochromator, instruments, scientific instruments, etc., can solve the problems of high production and operation cost, complex structure, and inability to read the full spectrum directly. , to achieve the effect of low production and operation cost, large linear dynamic range and good operation stability
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Embodiment 1
[0066] like figure 1 As shown, a photon counting full-spectrum direct-reading Raman spectrometer is mainly composed of a laser 1, a spectroscopic system 2, a photon counting imaging detector 3, and information processing and display 4:
[0067] Laser 1 is used to output laser to excite the sample to generate characteristic Raman spectrum;
[0068] Spectroscopic system 2 is a dispersion spectroscopic device capable of dispersing composite light into monochromatic light or spectral intensity distribution images;
[0069] The photon counting imaging detector 3 is an image sensor capable of position-sensitive detection and photon counting;
[0070] Information processing and display 4 is used to receive and process optical images, and express the processing and analysis results in various graphic forms that are easy for people or machines to understand;
[0071] The optical connections between the laser 1 and the sample, between the sample and the spectroscopic system 2, and bet...
Embodiment 2
[0089] This embodiment is basically the same as Embodiment 1, except that: on the basis of the photon counting imaging detector 3 described in Embodiment 1, a semiconductor layer can be added between the MCP output terminal and the position-sensitive anode,
[0090] There is a gap between the MCP output terminal and the semiconductor layer, the semiconductor layer is plated on the insulating substrate, and the DC high-voltage power supply is electrically connected to the semiconductor layer through a high-voltage lead wire or a conductive electrode (such as image 3 shown). At this time, the above step S540, that is, the physical process of collecting the electron cloud by the position-sensitive anode, evolves into: the electron cloud first crosses to the semiconductor layer under the action of the accelerating bias electric field, and then is induced to the position-sensitive anode through charge induction.
Embodiment 3
[0092] This embodiment is basically the same as Embodiment 1, the difference is that: on the basis of the Raman spectrometer described in Embodiment 1, the laser 1 can use a variety of different types of laser output devices, which can not only use a single wavelength output laser, Multi-wavelength output lasers, fixed-wavelength lasers, and wavelength-continuous or discretely tunable lasers can also use other excitation light sources that can provide high-intensity light output, thereby deriving a variety of photons based on different lasers or other excitation light sources Counting full-spectrum direct-reading Raman spectrometer.
[0093] For example: when a continuously adjustable wavelength laser is used, the characteristic Raman spectral lines produced by a single material component can be analyzed at a time; when a fixed multi-wavelength laser is used, multiple pairs of characteristic Raman spectral lines produced by multiple material components can be analyzed at the sa...
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