Optical emission spectrometer LB-10OES is a tabletop spectrometer with a wavelength range of 130 nm to 800 nm and spark frequency of 100 Hz – 1000 Hz. Vacuum optical chamber design with advanced CCD detectors and high speed data readout system. It contains integrated optics room and Paschen Runge construction design, making all the spectrum lines focused on the gratings.
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Wavelength range | 130 nm ̴ 800 nm |
Degree of vacuum | Auto control within 6 pa ̴ 20 pa |
Pixel resolution | 30 pm |
Focal length | 400 nm |
Grating line | 2400 m1 / mm |
First order spectral line dispersion rare | 1.2 nm / mm |
Average resolution ratio | 10 pm / pixel |
Spark frequency | 100 Hz ̴ 1000 Hz |
Plasma current | 1 A ̴ 80 A |
Ignition voltage | > 15000 V |
Storage temperature | 0°C - 45°C |
Operating temperature | 10 °C – 35 °C, 23 ± 2 °C |
Power | AC 220 V / 50 Hz |
Power consumption | Excitation : 700 W Stand by : 100 W |
Argon quality | 99.999 %, Argon pressure > 4 Mpa |
Argon consumption | 5L / min during spark mode |
Features
Applications
Used for metal and trace elemental analysis, foundry, mechanical engineering, scientific research, product inspection, automobile, petrochemical engineering, shipbuilding, electrics, aerospace, nuclear power, metallic and nonferrous metallic smelting, processing and recycling.
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Wavelength range | 200 nm ̴ 560 nm |
Degree of vacuum | |
Pixel resolution | 30 pm |
Spectrum Width | 18 mm |
Wavelength range | 130 nm ̴ 800 nm |
Degree of vacuum | |
Pixel resolution | |
Spectrum Width |
Wavelength range | 130 nm ̴ 800 nm |
Degree of vacuum | Auto control within 6 pa ̴ 20 pa |
Pixel resolution | 30 pm |
Spectrum Width |
Our Raman Spectrometers operate under controlled temperature conditions for precise analysis in various environments. These spectrometers are equipped with high-sensitivity detectors such as CCDs and photodiode arrays. They achieve ultra-high resolution by precisely focusing the laser spots on the samples. They feature optimized excitation wavelengths, automatic focusing, and auto-scan functionality. These are integrated with confocal optics and provide exceptional spatial resolution for high-precision analysis.
Excitation Wavelength | 785 nm |
Spectral Range | 250 to 3500 cmˉ¹ |
Spectral Resolution | 6 to 8 cmˉ¹ |
Maximum Laser Power | 500 mW (Power for 532 nm: 100 mW) |
Excitation Wavelength | 785 nm |
Spectral Range | 250 to 2700 cmˉ¹ |
Spectral Resolution | 5 cmˉ¹ |
Maximum Laser Power | 500 mW (Power for 532 nm: 100 mW) |
Excitation Wavelength | 785 nm |
Spectral Range | 250 to 4300 cm⁻1 |
Spectral Resolution | 8 to 11 cm⁻1 |
Maximum Laser Power | 500 mW (Power for 532 nm: 100 mW) |
The ICP (Inductively Coupled Plasma) Spectrometer is a sophisticated analytical instrument used for elemental analysis in diverse samples. By employing high-temperature plasma to ionize and excite atoms in a sample, the ICP spectrometer enables the precise measurement of emission or absorption lines characteristic of different elements. Widely utilized in fields such as environmental monitoring, geology, and metallurgy, ICP spectrometers offer exceptional sensitivity and multi-element capability, providing valuable insights into the composition of complex materials with applications in research, quality control, and compliance testing.
Oscillation frequency | 27.12 MHz |
Gas | Nitrogen/Argon |
Torch position | Electrically adjusted |
Torch position optimization | Automatic by software |
Wavelength range | 180 nm ̴̴ 900 nm |
Analytical speed | 10 elements every minute |
Accuracy | Relative standard deviation RSD ≤ 2 % |
Stability | Relative standard deviation RSD ≤ 3 % |
Labotronics Energy Dispersive X-Ray Fluorescence Spectrometer provides analysis of elements from light to heavy with minimal preparation. Its easy software ensures a smooth, hassle-free analytical process. Our spectrometer's durable design ensures reliability and reduces maintenance. Offers versatile analysis of multiple materials, revealing detailed composition and purity insights. It guarantees safety, meets standards, and minimizes radiation, all while delivering high performance.
Elemental Analysis Range | Fluorine (F) to Uranium (U) |
Temperature Range | 15°C to 30°C |
Analytical Range | ppm to 99.99% |
Detection Limit | As low as 0.2 ppm (for light matrices) |
Elemental Analysis Range | From Na to U |
Analytical range | 1 ppm to 99.99% |
Operating temperature | 15 to 30 ℃ |
Relative humidity | 40% to 50% |
Our Photomultiplier tube (PMT) spectrometers are advanced optical instruments used for sensitive and precise detection of light signals across different wavelengths. Employing a photomultiplier to amplify weak light signals, these spectrometers excel in applications requiring high sensitivity, such as fluorescence spectroscopy, Raman spectroscopy, and low-light-level measurements. PMT spectrometers convert incoming photons into electrical signals, offering excellent signal-to-noise ratios and wide dynamic ranges. Their versatility makes them essential in scientific research, biomedical diagnostics, and environmental monitoring, where the ability to detect and analyze faint light signals is crucial.
Analysis wave band(width range) | 120 nm ̴ 800 nm |
Optical system(large focal length) | Curvature radius : 750 mm |
Optical room | 35 °C ± 0.2 °C |
Working temperature | 10 ° C ̴ 30 ° C |
Labotronics Inductively Coupled Plasma Mass Spectrometry (ICP-MS) is a highly sensitive analytical technique used for elemental analysis. It combines the ionization capability of inductively coupled plasma with the precision of mass spectrometry. Our ICP-MS can detect and quantify a wide range of elements at trace levels, making it crucial in environmental, pharmaceutical, and geological research. With its high sensitivity, accuracy, and speed, ICP-MS is a powerful tool for applications requiring the quantification of elements in complex matrices, contributing to advancements in various scientific fields.
Mass Range | 2 amu ~ 255 amu |
Dynamic ( Linear ) range | ≥ 108 |
Sensitivity | Be ≥ 5 × 106 ( cps/mg/L ) In ≥ 60 × 106 ( cps/mg/L ) U ≥ 60 × 106 ( cps/mg/L ) |
Limit of detection | Be ≤ 5 ( ng/L ) In ≤ 0.5 ( ng/L ) U ≤ 0 .5 ( ng/L ) |
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