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Product Overview
RTS2 Multi-functional Laser Confocal Micro-Raman Spectrometer
RTS2 multi-functional laser confocal microscope Raman spectroscopy system, based on a new generation of micro confocal technology, with good scalability, according to the demand for expansion into the main function of the Raman micro-spectroscopy workstations, it is a high-quality choice for your scientific research!
Low wave number performance: 60cm-1 typical, 90cm-1 guaranteed, sample: sulfur, integration time 0.1s. <30cm-1 option available
Ultraviolet resonance Raman spectroscopy in the study of catalytic materials Ultra-low content of isolated transition metal ions in the skeleton of microporous-mesoporous materials
(e.g. Ti-MCM-41) can be reliably and accurately identified by UV-resonance Raman spectroscopy.
Using UV Raman, which avoids fluorescence and increases sensitivity, it is possible to study the evolution of precursors, intermediates, and molecular sieve crystals during the molecular sieve synthesis process.
UV Raman spectroscopy allows selective surface phase information to be obtained for substances with strong absorption in the UV region (e.g. TiO2 and ZrO2).
RTS2 multi-functional laser confocal microscope Raman spectroscopy system, based on a new generation of micro confocal technology, with good scalability, according to the demand for expansion into the main function of the Raman micro-spectroscopy workstations, it is a high-quality choice for your scientific research!
Typical advantages of the RTS2 multifunctional laser confocal micro-Raman spectrometer
- Compact and stable Raman optical path with reduced optical range for improved system stability and repeatability
- Built-in 532,638,785 common lasers, laser light path curing without switching and adjustment
- Expandable fourth single-mode fiber laser or free light path coupling, compatible with all types of lasers
- Fiber optic confocal, space light confocal and pinhole confocal options are available for both microscopic imaging and high confocal experiments.
- Research-grade orthostatic microscope without any modifications to ensure that the original function of the microscope remains unaffected
- Configurable autofocus module to keep the sample in focus at all times
- Standard with 320mm focal length image-corrected high-throughput spectrometer, high-megapixel deep-cooling spectral CCD camera
- Expandable detectors such as EMCCD, ICCD, InGaAs arrays, etc. to expand system functionality
- Ultra-high precision motorized stage, 1μm positioning accuracy, upgradable Raman Mapping function
- Provides a wide range of solutions for use with open-loop and closed-loop high and low temperatures and other sample stations.
- Directly coupled with hyperspectral systems for micro-area trans-absorption, dark-field scattering spectroscopy, and wide-field fluorescence spectroscopy.
① Raman interface box: built-in common laser and filter set, extended laser including free light and single-mode fiber inputs
② Optical path steering control: Optical path steering control can be downward and leftward, and can be used in conjunction with peripherals such as atomic force, cryogenics, and probe stage, with upgradable galvanometer options.
③ Bright-field camera: bright-field camera instead of eyepiece
④ Raman microscope: orthogonal research-grade metallurgical microscope, standard with falling light and dark field illumination, other illumination methods can be upgraded
⑤ Motorized sample stage: 75x50mm stroke high-precision motorized stage, 1μm positioning accuracy.
⑥ Fiber-optic confocal or pinhole confocal mode: improves Z-axis confocal resolution, Z resolution <1.5 μm @ 10 μm Pinhole
(vii) CCD-Slit Confocal Coupling: Standard free light CCD-slit coupling mode, spectrometer imaging mode available, high throughput
⑧ Spectral CCD: Back-illuminated deep depletion spectral CCD camera, 200-1100nm operating band, peak QE>90%
⑨ 320mm Spectrometer: F/4.2 High Flux Impact Corrected Spectrometer, 1×10^-5 stray light rejection ratio
Silicon third-order peak signal-to-noise ratio >20:1, silicon fourth-order peak visible
Detection conditions: 532nm laser, 100um slit width, 50um pixel size, 100x objective (0.9NA), 10mW on-sample laser power, integration time 300s, accumulation count 1, 600 line grating
Spectral resolution (half-height width): ≤ 1.5 cm-1; typical, 2 cm-1 guaranteed (320 mm spectrometer), (585 nm half-height width of neon line measured)
Detection conditions: in the visible wavelength band: neon lamp measurement, 10x objective lens, 1800g/mm grating, grating in the +1 level conditions, the slit width of 10mm. experiments will be placed in the neon lamp under the microscope, the measurement of the spectral line is 585 nm, the full width at half-magnitude (FWHM) ≤ 1.5cm-1;
Low wave number performance: 60cm-1 typical, 90cm-1 guaranteed, sample: sulfur, integration time 0.1s. <30cm-1 option available
Raman mapping
Examples of applications
Ultraviolet resonance Raman spectroscopy in the study of catalytic materials Ultra-low content of isolated transition metal ions in the skeleton of microporous-mesoporous materials
(e.g. Ti-MCM-41) can be reliably and accurately identified by UV-resonance Raman spectroscopy.
Using UV Raman, which avoids fluorescence and increases sensitivity, it is possible to study the evolution of precursors, intermediates, and molecular sieve crystals during the molecular sieve synthesis process.
UV Raman spectroscopy allows selective surface phase information to be obtained for substances with strong absorption in the UV region (e.g. TiO2 and ZrO2).
Flexible Configuration of the RTS2 Multifunctional Laser Confocal Microscopy Raman Spectroscopy SystemSee pdf download for details
RTS2 Inverted Confocal Raman System
RTS2 Microscopic Hyperspectral System
RTS2 Dual Spectrometer Dynamic High Voltage Time-Resolved Raman System
RTS2 Pulsed Raman System
Full angle polarization option
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