Specifications
| Parameter | Value |
|---|---|
| Laser | 532nm TEM00 Single-Mode Laser, 50mW |
| Laser | 638nm Single-Mode Laser, 50mW |
| Laser | 785nm Single-Mode Laser, 100mW |
| High-Sensitivity Spectrometer Focal Length | 300 mm |
| Spectrometer Spectral Range | Can Cover 200-1100nm |
| Grating | Three gratings with 600, 1200 and 1800 lines can be installed simultaneously; fully automatic software-controlled switching without manual grating replacement |
| Raman Spectral Range | Can Cover 100-5000cm-1 |
| White-Light Spectrum [Without Rotating the Grating] | Entire 530nm to 800nm spectrum acquired in one exposure without rotating the grating or stitching spectra by grating rotation |
| Spectral Resolution | Better Than 2 cm⁻¹ |
| Spectral Repeatability [Routine-lab test: single-crystal silicon; 532nm excitation; 100x objective; 100 repeats; repeatability of the 520cm⁻¹ silicon Raman-peak position] | Better Than 0.05 cm⁻¹ |
| High Sensitivity [Test: single-crystal silicon; 532nm laser, ≤10.0mW; 60s integration; 5 accumulations; 100x microscope objective] | The fourth-order silicon Raman peak is clearly observable. The third-order silicon Raman peak (about 1440cm⁻¹) has signal-to-noise ratio better than 20:1. No obvious N₂ or O₂ Raman peaks; their intensities must not exceed the fourth-order peak. |
| Spectral Detector | High-end back-illuminated CCD; peak quantum efficiency >=90%; TE cooling to -60 degrees |
| True Pinhole Confocal System | For optimum confocal performance, the system must use true pinhole confocal operation rather than slit-based pseudo-confocal operation. Pinhole diameter is automatically and continuously adjustable from 10 to 100um. |
| Lateral (XY) Optical Spatial Resolution [100× dry obj.; confocal hole≥50mm; auto stage. 1D nanomaterial Ø≤50nm (perfect graphene edge OK; no grating); Raman scan⊥material, 50nm steps; intensity-profile FWHM defines lateral Raman optical resolution.] | ≤ 500 nm @ 532 nm |
| Longitudinal (Z) Spatial Resolution [100× dry obj.; confocal aperture≥50mm. Suspended few-layer graphene; Raman Z scan in 50nm steps with 100X obj.; FWHM of G-peak intensity profile defines axial Raman-imaging optical resolution.] | ≤ 1000 nm@532 nm |
| Optical Microscope | The Optical Microscope Uses Köhler Illumination |
| Brightfield/Darkfield Objective | 10x Objective, 50x Objective (Long Working Distance), 100x Objective |
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Supplier Information
Guangzhou Betops Science and Technology Co., Ltd. is a one-stop service manufacturer integrating production, installation, training, and maintenance. For more than ten years, we have focused on providing fully automatic contact angle measuring instruments, handheld Raman spectrometers, fully automatic surface/interface tensiometers, domestic surface tensiometers, domestic nanoparticle size analyzers, and other equipment. The detection indicators of our instruments have reached the leading domestic and advanced international levels. We also possess core technical capabilities in optical design, mechanical design, software programming, and algorithm programming. Our products are sold well in Beijing, Shanghai, Shenzhen, Zhejiang, Guangdong, Jiangsu, Shandong, and other places across the country.
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