NL230 series

High Energy Q-switched DPSS Nd:YAG Lasers
  • Compact high energy and repetition rate nanosecond lasers
  • Up to 190 mJ energy
  • Up to 100 Hz repetition rate
  • Pulse duration in the 3 – 6 ns range
  • Compact high energy and repetition rate nanosecond lasers
  • Up to 190 mJ energy
  • Up to 100 Hz repetition rate
  • Pulse duration in the 3 – 6 ns range

Features & Applications


  • 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
  • Optional temperature-stabilized second and third harmonic generators
  • Electromechanical shutter (optional)
  • Easy replaceable output window


  • Short duration 2 – 4 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


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


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 rms.

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


Pulse energy (not less than) 2)
    at 1064 nm 190 mJ150 mJ
    at 532 nm 3)110 mJ90 mJ
    at 355 nm 4)55 mJ40 mJ
Pulse energy stability (StdDev) 5)
    at 1064 nm <1 %
    at 532 nm<2.5 %
    at 355 nm<3.5 %
Pulse repetition rate50 Hz100 Hz
Power drift 6)< ±1 %
Pulse duration 7)3 – 6 ns
Linewidth <1 cm-1 at 1064 nm
Beam profile 8)"Top Hat" in near field and close to Gaussian in far field
Beam divergence 9)<0.8 mrad
Beam pointing stability (StDev) 10) ≤60 µrad
Polarizationlinear, >95% at 1064 nm
Typical beam diameter 11) 5 mm
Optical pulse jitter (StDev)
    Internal triggering regime<0.5 ns
    External triggering regime<0.5 ns
Typical warm-up time10 min
Laser head size (W × L × H)251 × 291 × 167 ± 3 mm
Power supply unit (W × L × H)
    Desktop case470 × 390 × 140 ± 3 mm
    19" module483 × 390 × 140 ± 3 mm
    External chiller (where applicable)inquire
Umbilical length3 m
Cooling (air cooled) 12) external chiller
Ambient temperature18 – 30 °C
Relative humidity (non-condensing)20 – 80 %
Power requirements100 – 240 VAC, single phase, 50/60 Hz
Power consumption<1 kW
Cleanliness of the roomnot worse than ISO Class 9
  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. With H230SHC or H230STHC harmonic generator module.
  4. With H230THC or H230STHC generator modules.
  5. Averaged from pulses, emitted during 30 sec time interval.
  6. Measured over 8 hours period after 20 min warm-up when ambient temperature variation is less than ± 2 °C and humidity <± 5%.
  7. FWHM.
  8. Near field (at the output aperture) TOP HAT fit is >80%.
  9. Full angle measured at the 1/e² level.
  10. Beam pointing stability is evaluated as movement of the beam centroid in the focal plane of a focusing element.
  11. Beam diameter is measured at 1064 nm at the 1/e² level.
  12. 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.

Performance & Drawings


Found total :
4 articles, 4 selected
Application selected :
All Applications
All Applications
Laser Spectroscopy
LIBS – laser induced breakdown spectroscopy
Biomedical – applications focusing on the biology of human health and disease
Photoacoustic Imaging – biomedical imaging modality based on the photoacoustic effect
Material Processing
Nanoparticles Generation

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

Related applications:  Photoacoustic Imaging Biomedical

Authors:  K. Kratkiewicz, R. Manwar, A. Rajabi-Estarabadi, J. Fakhoury, J. Meiliute, S. Daveluy, D. Mehregan, and K. (Mohammad) Avanaki

The marked increase in the incidence of melanoma coupled with the rapid drop in the survival rate after metastasis has promoted the investigation into improved diagnostic methods for melanoma. High-frequency ultrasound (US), optical coherence tomography (OCT), and photoacoustic imaging (PAI) are three potential modalities that can assist a dermatologist by providing extra information beyond dermoscopic features. In this study, we imaged a swine model with spontaneous melanoma using these modalities and compared the images with images of nearby healthy skin. Histology images were used for validation.

Published: 2019.   Source: Sensors. 2019; 19(12):2815

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

Related applications:  Material Processing Nanoparticles Generation

Authors:  E. Stankevičius, M. Garliauskas, L. Laurinavičius, R. Trusovas, N. Tarasenko, R. Pauliukaitė

Direct generation of gold nanoparticles on ITO glass using a nanosecond laser is presented and the electrochemical properties of the gold modified ITO electrodes for detection of the ascorbic acid are analyzed. Gold nanoparticles were generated by nanosecond laser pulse irradiation of thin, 3–30 nm thick, gold films. It was found that diameters and the number of generated nanoparticles per unit area strongly depends on the thickness of the gold film when it is less than 10 nm. Furthermore, experiments have shown that the influence of laser processing parameters (the laser pulse energy and pulse number) to the size, the distribution and the area density of generated gold nanoparticles on ITO glass is negligible. Characterization of the electrochemical properties of the gold modified ITO electrodes by nanosecond laser showed that the fabricated electrodes could be employed in electrochemical sensing. Therefore, the demonstrated generation of gold nanoparticles on ITO by using the nanosecond laser approach opens new opportunities for the development of highly sensitive and low-cost electrochemical sensors.

Published: 2019.   Source: Electrochimica Acta 297, 511-522 (2019)

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

Related applications:  Laser Spectroscopy LIBS

Authors:  Z. Zhen Wang, Y. Deguchi, M. Kuwahara, J. Jie Yan, J. Ping Liu

Laser-induced breakdown spectroscopy (LIBS) technology is an appealing technique compared with many other types of elemental analysis because of the fast response, high sensitivity, real-time, and noncontact features. One of the challenging targets of LIBS is the enhancement of the detection limit. In this study, the detection limit of gas-phase LIBS analysis has been improved by controlling the pressure and laser pulse width. In order to verify this method, low-pressure gas plasma was induced using nanosecond and picosecond lasers. The method was applied to the detection of Hg. The emission intensity ratio of the Hg atom to NO (IHg/ INO) was analyzed to evaluate the LIBS detection limit because the NO emission (interference signal) was formed during the plasma generation and cooling process of N2 and O2 in the air. It was demonstrated that the enhancement of IHg/INO arose by decreasing the pressure to a few kilopascals, and the IHg/INO of the picosecond breakdown was always much higher than that of the nanosecond breakdown at low buffer gas pressure. Enhancement of IHg/INO increased more than 10 times at 700 Pa using picosecond laser with 35 ps pulse width. The detection limit was enhanced to 0.03 ppm (parts per million). We also saw that the spectra from the center and edge parts of plasma showed different features. Comparing the central spectra with the edge spectra, IHg/INO of the edge spectra was higher than that of the central spectra using the picosecond laser breakdown process.

Published: 2013.   Source: Applied Spectroscopy 67(11):1242-51

Laser Induced Breakdown Spectroscopy and Applications Toward Thin Film Analysis

Related applications:  Laser Spectroscopy LIBS

Authors:  T. N. Owens

Laser induced breakdown spectroscopy (LIBS) provides the opportunity to analyze almost any element, from any material, in any environment. Among the many applications of LIBS is the analysis of thin lms and multilayered structures. An automated system was designed and built to conduct LIBS using Nd:YAG and Ti:Sapphire lasers, broadband and high-resolution spectrometers and detectors. This system incorporates the sample manipulation as well as laser and spectrometer control and timing. A series of experiments were conducted to analyze the ability of nanosecond and femtosecond lasers to detect Mg impurities in thin TiO2 lms using LIBS. It was determined that optimal detection occurs early in the plasma ionic/atomic emission with detection capabilities in the parts-per-million range. Another series of experiments were conducted using LIBS to analyze thin transparent organic lms, with speci c emphasis on the e ect of lm thickness and interplay between lm and substrate. The challenges of ablating and measuring multiple layers have also been explored using various laser wavelengths. The e ectiveness of LIBS has been demonstrated for depth pro ling of CIGS solar cells. Ablation crater and ablation threshold analysis aided in understanding and overcoming some of the obstacles in depth pro ling. One of the challenges with LIBS is the identi cation and mitigation of matrix e ects. This problem was explored using a Mg tracer element and various compositions of the suspected elements Si, Ca, and Sr which can cause errors in LIBS analysis. The goal of this dissertation is to investigate the ability of LIBS to conduct detailed thin lm analysis for a variety of materials and potential applications. This includes analyzing trace elements from a traditionally noisy background, measuring dicult to ablate thin lms, and the unique challenges associated with multilayered structures.

Published: 2011.   Source: UC Berkeley Electronic Theses and Dissertations

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