NASOR Series Lamp-Pumped Nd:YAG Nanosecond Lasers NASOR-800
The entire NASOR series uses an efficient Nd:YAG resonator design with Gaussian-mirror coupling for flat-top output. A compact, rugged indium-steel resonator structure ensures reliability and consistency during long-term laser operation.
Save to Favorites
Overview
Specifications
| Parameter | Value |
|---|---|
| Repetition Rate [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | 1-10Hz |
| Energy [Wavelength :1064nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ＞800 |
| Energy [Wavelength :532nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ＞400 |
| Energy [Wavelength :355nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ＞240 |
| Energy [Wavelength :266nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ＞80 |
| Energy Stability [Wavelength :1064nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | <0.7% |
| Energy Stability [Wavelength :532nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | <1.2% |
| Energy Stability [Wavelength :355nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | <2.5% |
| Energy Stability [Wavelength :266nm; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | <3% |
| Beam Characteristics — Power Drift [Wavelength: 1064nm; unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; average energy variation over 8 hours with room temperature fluctuations below 3℃] | 3% |
| Beam Characteristics — Power Drift [Wavelength: 532nm; unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; average energy variation over 8 hours with room temperature fluctuations below 3℃] | 5% |
| Beam Characteristics — Power Drift [Wavelength: 355nm; unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; average energy variation over 8 hours with room temperature fluctuations below 3℃] | 8% |
| Beam Characteristics — Power Drift [Wavelength: 266nm; unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; average energy variation over 8 hours with room temperature fluctuations below 3℃] | 10% |
| Pulse Width at Half Maximum [Unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; the pulse width at half the peak power is the full width at half maximum] | ≤9 ns@1064nm |
| Divergence [Unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; full angle enclosing 86.5% of the energy] | ＜0.6mrad |
| Beam Pointing [Unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; RMS deviation from the mean beam centroid] | <20μrad |
| RMS Timing Jitter [Unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; optical emission timing jitter relative to the external trigger signal] | ＜0.5ns |
| Spot Size [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ~9 mm |
| Spatial Beam Profile [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | Flat-Top Distribution |
| Near-Field Gaussian Fit [＜1m; Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | 70% |
| Far-Field Gaussian Fit (∞) [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | 95% |
| Beam Characteristics — Polarity [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | Linear Polarization |
| Linewidth - Standard Model [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | 1 cm⁻¹ |
| Linewidth - Seed-Injected Single Longitudinal Mode [Unless otherwise stated, all parameters are measured at 1064nm and a 10Hz repetition rate; seed-injection mode reduces energy by 10%] | 0.005 cm⁻¹ |
| Pump-Lamp Life [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | >5×10⁷ cycles |
| Power Input [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | 220 VAC ±5% 50-60Hz |
| Energy Loss [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | ＜3 kW(1200 mJ@10 Hz) |
| Operating Conditions [Unless otherwise noted , All parameters are measured at 1064nm,10Hz repetition rate] | Temperature 15-30℃, humidity ＜70% (noncondensing) |
Applications
Key Features
Datasheet
Supplier Information
Related Products
-
DTS pulsed laser
Laser Modules & Systems
Oe-photonics
Operating Wavelength: typical:1550 nm Peak output optical power: typical:30 W Pulse Width: min:5 ns; typical:10 ns
The DTS pulsed laser integrates a nanosecond seed laser and fiber power amplifier for distributed fiber temperature sensing, laser ranging, and fiber sensing. Optimized nanosecond drive circuitry and a low-noise erbium-doped amplifier produce stable pulses with high peak power and low distortion. External triggering and serial configuration of width, peak power, and other parameters provide high integration, compact size, and easy setup. Rigorous environmental testing supports long-term reliability and stability.
-
Ultra-narrow-linewidth fiber laser (single-mode/polarization-maintaining) Laser Modules & Systems Oe-photonics
Operating Wavelength Range: typical:1550.12 nm Output Optical Power: typical:10 dBm Equivalent spectral linewidth: typical:3 kHz
The UNL fiber-laser series for sensing offers narrow linewidth, long coherence length, low noise, and strong environmental-interference resistance. Distinctive optics and precise drive/control eliminate external temperature and vibration effects on wavelength for stable single-longitudinal-mode, ultra-narrow-linewidth, single-frequency output. Serial configuration, high integration, compact size, and easy setup are provided, with custom single-mode or PM-fiber outputs.
-
Industrial laser welding wire feeder Laser Modules & Systems Qilinlaser
-
Industrial laser wire-feed assembly-SST30 Laser Modules & Systems Qilinlaser
-
Energy Storage Industrial Welding Head Laser Modules & Systems Qilinlaser
Interface Type (Interface): QBH/RD Clear Aperture (Optical Aperture): 20 mm Power Handling (Power): 4000 W
QBH/RD compatibility with different fiber lasers; drawer optics for easy replacement, rated for 4000W; modular quick assembly with optimized optics, water cooling, and double sealing for durability and stability; ring, filled, and rectangular wobble patterns for multifunction welding; efficient, time-saving energy-storage welding with a youthful design, lower labor costs, strong interference resistance, safety, and stability; industrial uses including new-energy, battery, and condenser-tube welding.
Related Articles
The LZFL405‑80mW‑3 series from Shenzhen Leirte Optoelectronics Co., Ltd. is a coaxial‑packaged violet‑blue single‑mode fiber‑coupled laser diode. It delivers 80 mW continuous‑wave output at 405 nm. Light is coupled into 3 μm core‑diameter single‑mode fiber for clean beam quality and easy integration into diverse optical systems. It serves as a compact violet‑blue light source for medical instruments and industrial printing applications.
Wuhan Optics Valley Quantum Technology Co., Ltd. is a leading domestic developer of high‑speed semiconductor optical chips and photodetector components. Our product portfolio covers InGaAs avalanche photodiode bare dies and PIN photodetector chips designed for fiber‑optic communication
As a professional ultraviolet‑laser solution provider, Precilasers has launched its 266 nm narrow‑linewidth industrial laser, delivering reliable single‑frequency output for high‑precision interference lithography, semiconductor inspection and precision metrology applications.
Electro-optic deflectors (EODs) are optical devices used to steer or deflect light beams by applying an electric field to a specialized optical crystal. Unlike mechanical beam steering systems that rely on moving mirrors, electro-optic deflectors enable high-speed, non-mechanical beam control with exceptional precision and responsiveness. They are widely used in laser scanning, optical communications, microscopy, laser printing, spectroscopy, and scientific research, where rapid and accurate laser beam positioning is essential.
Loading...
Name
Phone
Organization
Use Case
Database Platform