NL230

High Energy Q-switched DPSS Nd:YAG Lasers

The NL230 series diode-pumped short nanosecond lasers are designed to produce high-intensity, high-brightness pulses and are targeted for applications such as material ablation, Light Detection And Ranging (LIDAR), remote sensing, mass spectroscopy, OPO, Ti:Sapphire or dye laser pumping and many more.

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NL230
Overview

Features

  • Customers recognized reliability
  • Two years warranty
  • Diode-pumped
  • Rugged sealed laser cavity
  • Up to 190 mJ at 1064 nm pulse energy
  • Up to 100 Hz pulse repetition rate
  • Short pulse duration in the 3 – 6 ns range
  • Variable reflectivity output coupler for low-divergence beam
  • Quiet operation: no more flashlamp firing sound
  • Remote control via keypad and/or any controller running on any OS using REST API commands
  • Temperature-stabilized second and third harmonic generators (optional)
  • Electromechanical shutter (optional)
  • Easy replaceable output window

Applications

  • LIBS (Light Induced Breakdown Spectroscopy)
  • Material ablation
  • OPO pumping
  • Remote Sensing
  • LIDAR (Light Detection And Ranging)
  • Mass Spectroscopy
  • LIF (Light Induced Fluorescence)

Description

The NL230 series diode-pumped short nanosecond lasers are designed to produce high-intensity, high-brightness pulses and are targeted for applications such as material ablation, Light Detection And Ranging (LIDAR), remote sensing, mass spectroscopy, OPO, Ti:Sapphire or dye laser pumping and many more. Diode pumping allows maintenance-free laser operation for an extended period of time – more than 3 years for an estimated eight working hours per day.

Because laser head components are placed in a robust, sealed and precisely machined monolithic aluminium block, this laser can reliably work in a harsh industrial environment with applications such as laser-induced breakdown spectroscopy (LIBS).

Second and third harmonic options allows for an expanded range of applications, where high pulse energy and high pulse to pulse stability are required.

For easy and seamless control and integration with other industrial equipment, the NL230 series laser is equipped with USB/RS232 interfaces and can be externally triggered with a jitter as low as < 0.5 ns StDev.

NL230 series lasers are designed to work reliably 24/7 in an industrial environment.

Benefits

  • Short duration 3 – 6 ns pulses ensures strong interaction with material, are highly suitable for LIBS
  • User selectable wavelength single axis output is superior for experiments, where alternating wavelengths are required, like material ablation, LIBS
  • Rugged, monolithic design enables laser usage in hash environment
  • Diode pumped design provides quiet operation, eliminates the irritation of flash light
  • Variety of interfaces USB, RS232, LAN, WLAN ensures easy control and integration with other equipment

Specifications

ModelNL231-50NL231-100
Main specifications 1)
Pulse energy (not less than) 2)
at 1064 nm190 mJ150 mJ
at 532 nm110 mJ90 mJ
at 355 nm55 mJ40 mJ
at 266 nm3 mJ1.2 mJ
Pulse energy stability (StdDev) 3)
at 1064 nm< 1.0 %< 1.0 %
at 532 nm< 2.5 %< 2.5 %
at 355 nm< 3.5 %< 3.5 %
at 266 nm< 5 %< 5 %
Pulse repetition rate50 Hz100 Hz
Power drift 4)< ±3 %< ±3 %
Pulse duration 5)3 – 6 ns3 – 6 ns
Linewidth< 1 cm‑1 at 1064 nm< 1 cm‑1 at 1064 nm
Beam profile 6)“Top Hat” in near field
and close to Gaussian in far field
“Top Hat” in near field
and close to Gaussian in far field
Beam divergence 7)< 0.8 mrad< 0.8 mrad
Beam pointing stability (RMS) 8)≤ 60 μrad≤ 60 μrad
Polarizationlinear, > 90 % at 1064 nmlinear, > 90 % at 1064 nm
Typical beam diameter 9)5 mm5 mm
Optical pulse jitter (StDev)
Internal triggering regime< 0.5 ns< 0.5 ns
External triggering regime< 0.5 ns< 0.5 ns
Typical warm-up time10 min10 min
Physical characteristics
Laser head size (W × L × H)251 × 290 × 167 ± 3 mm251 × 290 × 167 ± 3 mm
Power supply unit (W × L × H)
Desktop case449 × 390 × 140 ± 3 mm449 × 390 × 140 ± 3 mm
19″ module483 × 390 × 140 ± 3 mm483 × 390 × 140 ± 3 mm
External chillerinquireinquire
Umbilical length3 m3 m
Operating requirements
Cooling (air cooled) 10)external chillerexternal chiller
Ambient temperature18 – 30 °C18 – 30 °C
Relative humidity20 – 80 %
(non-condensing)
20 – 80 %
(non-condensing)
Power requirements100 – 240 V AC,
single phase, 50/60 Hz
100 – 240 V AC,
single phase, 50/60 Hz
Power consumption< 1.0 kW< 1.0 kW
Cleanliness of the roomnot worse than ISO Class 9not worse than ISO Class 9
ModelNL231-50NL231-100
  1. Due to continuous improvement, all specifications are subject to change. The parameters marked typical may vary with each unit we manufacture. Unless stated otherwise all specifications are measured at 1064 nm and for basic system without options.
  2. Outputs are not simultaneous. Inquire for higher energy (up to 350 mJ at 50 Hz, 250 mJ at 100 Hz) custom models.
  3. Averaged from pulses, emitted during 30 sec time interval.
  4. Measured over 8 hours period after 20 min warm-up when ambient temperature variation is less than ± 2 °C and humidity <± 5%.
  5. FWHM.
  6. Near field (at the output aperture) TOP HAT fit is >80%.
  7. Full angle measured at the 1/e2 level.
  8. Beam pointing stability is evaluated as movement of the beam centroid in the focal plane of a focusing element.
  9. Beam diameter is measured at 1064 nm at the 1/e2 level.
  10. Adequate room air conditioning should be provided.

Note: Laser must be connected to the mains electricity all the time. If there will be no mains electricity for longer that 1 hour then laser (system) needs warm up for a few hours before switching on.

Publications

Engineering electrochemical sensors using nanosecond laser treatment of thin gold film on ITO glass

E. Stankevičius, M. Garliauskas, L. Laurinavičius, R. Trusovas, N. Tarasenko, and R. Pauliukaitė, Electrochimica Acta 297, 511-522 (2019). DOI: 10.1016/j.electacta.2018.11.197.

Photoacoustic/Ultrasound/Optical Coherence Tomography Evaluation of Melanoma Lesion and Healthy Skin in a Swine Model

K. Kratkiewicz, R. Manwar, A. Rajabi‑Estarabadi, J. Fakhoury, J. Meiliute, S. Daveluy et al., Sensors 19 (12), 2815 (2019). DOI: 10.3390/s19122815.

Enhancement of Laser-Induced Breakdown Spectroscopy (LIBS) Detection Limit Using a Low-Pressure and Short-Pulse Laser-Induced Plasma Process

Z. Z. Wang, Y. Deguchi, M. Kuwahara, J. J. Yan, and J. P. Liu, Applied Spectroscopy 67 (11), 1242-1251 (2013). DOI: 10.1366/13-07131.

Laser Induced Breakdown Spectroscopy and Applications Toward Thin Film Analysis

T. N. Owens, UC Berkeley Electronic Theses and Dissertations (2011).

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