Scientific research
2 13: 213 nm emission determines compatible optics, coatings and detectors for Scientific research. Beam quality, divergence and pointing stability should be checked against the experiment geometry.
Pulse energy, repetition rate, pulse width
2 13 is a 213 nm Pulsed laser. Used for scientific research, icp-ms, laser processing, measure. Rep. rate (Hz): 100 Hz-10 kHz; Cooled method: Air or Water Cooled. Key specifications: pulse energy 1-100 uJ, repetition rate 100 Hz-10 kHz, pulse width <1.5@<5 kHz. View specifications, datasheet and enquiry options from Precisometer.
Specifications
5 specification rows
| Wavelength | 213 nm |
|---|---|
| Pulse energy | 1-100 uJ |
| Repetition rate | 100 Hz-10 kHz |
| Beam / notes | Rep. rate (Hz): 100 Hz-10 kHz; Cooled method: Air or Water Cooled |
| Pulse width | <1.5@<5 kHz |
| Cooling | Air or Water Cooled |
Application context
Typical uses for this laser type, with the selection logic tied to the model record.
2 13: 213 nm emission determines compatible optics, coatings and detectors for Scientific research. Beam quality, divergence and pointing stability should be checked against the experiment geometry.
2 13: 213 nm emission determines compatible optics, coatings and detectors for ICP-MS. Beam quality, divergence and pointing stability should be checked against the experiment geometry.
2 13: Laser processing depends on how optical energy is delivered to the target; 213 nm emission governs absorption, while the listed temporal parameter (1-100 uJ) governs peak intensity and heat deposition.
2 13: Measure benefits from a stable, focusable source. 213 nm emission fixes the compatible coatings and detector response, while M², divergence and pointing stability should be confirmed for the intended beam path.
System integration
Use these checks to connect 2 13 to the surrounding optical, mechanical and control system. Every value shown is taken from this model's own specification record.
Technical FAQ
Cooling: Air or Water Cooled. Provide the stated cooling method and keep the laser-head base thermally coupled; temperature drift moves wavelength, output power and beam pointing.
Share wavelength, operating mode, output power or pulse energy, linewidth or pulse width, delivery, control, and safety requirements and we will qualify the matching configuration and lead time.
Model selection
Compare 2 13 with the closest available models in the Pulsed Lasers family. Confirm option-dependent values on the final configuration before ordering.
| Selection parameter | 2 13 (current) | DPS-213-Pico | EO-213-Subnano-Hi |
|---|---|---|---|
| Wavelength | 213 nm | 213 nm | 213 nm |
| Optical power / pulse energy | 1-100 uJ | 1~30 mW | 1-100 uJ |
| Operating mode / pulse width | 100 Hz-10 kHz | Pulsed | 100 Hz-10 kHz |
| Beam quality | Confirm for this model | <3 | ≤3 |
Compare the 2 13 with nearby pulsed lasers across the wavelength range.
Choosing a laser
Which specifications decide the experiment, and which ones cost money without changing the result.
PhotonicsLinewidth, spectral width, RIN, M², and coherence length answer five different questions. Translate each into the units your experiment is designed in — and learn which ones not to pay for.
Open guide
Photoacoustic imagingConnect optical absorption to wavelength, pulse fluence, stress confinement, acoustic bandwidth, repetition rate, and synchronization at the sample.
Open guide
Ultrafast spectroscopyDesign the pump, probe, delay line, monochromator, visible or SWIR camera, synchronization, and transient-signal budget as one experiment.
Open guide