PL2250 series

Flash-Lamp Pumped Picosecond Nd:YAG Lasers

PL2250 series mode-locked picosecond Nd:YAG lasers provide high up to 100 mJ energy picosecond pulses at a 20 Hz pulse repetition rate. Laser features cost-effective design while still maintaining laser reliability and reducing running and maintenance costs.

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PL2250
Overview

Features

  • Hermetically sealed DPSS master oscillator
  • Diode pumped regenerative amplifier
  • Flashlamp pumped power amplifier producing up to 100 mJ per pulse at 1064 nm
  • 30 ps pulse duration (20 ps optional)
  • Excellent pulse duration stability
  • Up to 20 Hz repetition rate
  • Streak camera triggering pulse with <10 ps jitter
  • Excellent beam pointing stability
  • Thermo-stabilized second, third, fourth and fifth harmonic generator options
  • PC control
  • Remote control via keypad

Applications

  • Time resolved fluorescence (including streak camera measurements)
  • SFG/SHG spectroscopy
  • Nonlinear spectroscopy
  • Laser-induced breakdown spectroscopy
  • OPG pumping
  • Remote laser sensing
  • Satellite ranging
  • Other spectroscopic and nonlinear optics experiments

Description

Innovative design

PL2250 series lasers cost-effective design improves laser reliability and reduces running and maintenance costs.

The heart of the system is a diode pumped solid state (DPSS) master oscillator placed in a hermetically sealed monolithic block. The flashlamp pumped regenerative amplifier is replaced by an innovative diode pumped regenerative amplifier. Diode pumping results in negligible thermal lensing, which allows operation of the regenerative amplifier at variable repetition rates, as well as improved long-term stability and maintenance-free operation.

The optimized multiple-pass power amplifier is flashlamp pumped and is optimized for efficient amplification of pulse while maintaining a near Gaussian beam profile and low wavefront distortion. The output pulse energy can be adjusted in approximately 1% steps, at the same time as pulse-to-pulse energy stability remains less than 0.8% rms at 1064 nm.

Angle-tuned KD*P and KDP crystals mounted in thermostabilised ovens are used for second, third and fourth harmonic generation. Harmonic separators ensure the high spectral purity of each harmonic directed to different output ports.

Built-in energy monitors continuously monitor output pulse energy. Data from the energy monitor can be seen on the remote keypad or PC monitor. The laser provides several triggering pulses for synchronization of the customer‘s equipment. The lead or delay of the triggering pulse can be adjusted in 0.25 ns steps from the control pad or PC. Up to 1000 μs lead of triggering pulse is available as a pretrigger feature.

Precise pulse energy control, excellent short-term and long-term stability, and up to 20 Hz repetition rate makes PL2250 series lasers an excellent choice for many demanding scientific applications.

Simple and convenient laser control

For customer convenience the laser can be operated from master device or personal computer through USB (VCP, ASCII commands), RS232 (ASCII commands), LAN (REST API) or RS232 (ASCII commands), LAN (REST API) depending on the system configuration or from remote control pad with backlit display that is easy to read even while wearing laser safety glasses.

Communication interfaceDescription
USBvirtual serial port, ASCII commands
RS232ASCII commands
LANREST API
WLANREST API

Specifications

ModelPL2251APL2251BPL2251C
Main specifications 1)
Pulse energy
at 1064 nm50 mJ 2)80 mJ 2)100 mJ
at 532 nm 3)25 mJ40 mJ50 mJ
at 355 nm 4)15 mJ24 mJ30 mJ
at 266 nm 5)7 mJ10 mJ12 mJ
at 213 nm 6)inquireinquireinquire
Pulse energy stability (StdDev) 7)
at 1064 nm< 0.8 %< 0.8 %< 0.8 %
at 532 nm< 1.0 %< 1.0 %< 1.0 %
at 355 nm< 1.1 %< 1.1 %< 1.1 %
at 266 nm< 1.2 %< 1.2 %< 1.2 %
Pulse duration (FWHM) 8)29 ± 5 ps29 ± 5 ps29 ± 5 ps
Pulse duration stability 9)± 1.0 ps± 1.0 ps± 1.0 ps
Repetition rate20 or 10 Hz20 or 10 Hz10 Hz
Polarizationlinear, vertical, > 99 %linear, vertical, > 99 %linear, vertical, > 99 %
Pre-pulse contrast 10)> 200 : 1> 200 : 1> 200 : 1
Optical pulse jitterinternal / externalinternal / externalinternal / external
Internal triggering regime 11)< 50 ps< 50 ps< 50 ps
External triggering regime 12)~3 ns~3 ns~3 ns
SYNC OUT pulse delay 13)-500 … 50 ns-500 … 50 ns-500 … 50 ns
Beam divergence 14)< 0.5 mrad< 0.5 mrad< 0.5 mrad
Beam pointing stability (RMS) 15)≤ 20 µrad≤ 20 μrad≤ 20 μrad
Beam diameter 16)~ 8 mm~ 10 mm~ 12 mm
Typical warm-up time30 min30 min30 min
Physical characteristics
Laser head size (W × L × H)
with harmonic456×1233×249 mm ± 3 mm456×1233×249 mm ± 3 mm456×1233×249 mm ± 3 mm
without harmonic456×1031×249 mm ± 3 mm 456×1031×249 mm ± 3 mm 456×1233×249 mm ± 3 mm
Electrical cabinet size (W × L × H)550×600×550 ± 3 mm
(19″ standard, MR-9)
550×600×550 ± 3 mm
(19″ standard, MR-9)
550×600×550 ± 3 mm
(19″ standard, MR-9)
Umbilical length2.5 m2.5 m2.5 m
Operating requirements
Coolingwater cooledwater cooledwater cooled
Water consumption< 8 l/min, 2 bar, max. 20 °C< 8 l/min, 2 bar, max. 20 °C< 8 l/min, 2 bar, max. 20 °C
Room temperature22 ± 2 °C22 ± 2 °C22 ± 2 °C
Relative humidity20 – 80 %
(non-condensing)
20 – 80 %
(non-condensing)
20 – 80 %
(non-condensing)
Power requirements 17)200 – 240 V AC, 16 A,
single phase, 50/60 Hz
200 – 240 V AC, 16 A,
single phase, 50/60 Hz
200 – 240 V AC, 16 A,
single phase, 50/60 Hz
Power consumption 18)< 1.5 kVA< 2.5 kVA< 2.5 kVA
ModelPL2251APL2251BPL2251C
  1. Due to continuous improvement, all specifications are subject to change without notice. Parameters marked typical are not specifications. They are indications of typical performance and will vary with each unit we manufacture. Unless stated otherwise, all specifications are measured at 1064 nm and for basic system without options.
  2. PL2251B-20 has 70 mJ at 1064 nm output energy. Inquire for these energies at other wavelengths.
  3. For -SH option. Outputs are not simultaneous. Please inquire for pulse energies at other wavelengths.
  4. For -TH option. Outputs are not simultaneous. Please inquire for pulse energies at other wavelengths.
  5. For -FH option. Outputs are not simultaneous. Please inquire for pulse energies at other wavelengths.
  6. For PL2250 series laser with custom -FiH option.
  7. Averaged from pulses, emitted during 30 sec time interval.
  8. FWHM. Inquire for optional pulse durations in 20 – 90 ps range. Pulse energy specifications may differ from indicated here.
  9. Measured over 1 hour period when ambient temperature variation is less than ±1 °C.
  10. Peak-to-peak with respect to residual pulses.
  11. StdDev. With respect to TRIG1 OUT pulse. <10 ps jitter is provided optionally with PRETRIG feature.
  12. StdDev. With respect to SYNC IN pulse.
  13. TRIG1 OUT lead or delay can be adjusted with 0.25 ns steps in specified range.
  14. Average of X- and Y-plane full angle divergence values measured at the 1/e² level at 1064 nm.
  15. Beam pointing stability is evaluated from fluctuations of beam centroid position in the far field.
  16. Beam diameter is measured at 1064 nm at the 1/e² point.
  17. Three phase 208 or 380 VAC mains are required for 50 Hz versions.
  18. For 10 Hz version.

Notes:
If laser is optimised for pumping parametrical generator, maximum output energy may be different than specified for stand alone application.
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.

Ordering information of PL2250 lasers

Ordering information of PL2250 lasers.

Options

-P20

Provides 20 ps ± 10% output pulse duration. Pulse energies are 30% lower in comparison to the 30 ps pulse duration version. Linewidth <2 cm‑1 at 1064 nm. See table below for pulse energy specifications:

ModelPL2251A-10PL2251B-10PL2251C -10
1064 nm35 mJ60 mJ80 mJ
532 nm17 mJ30 mJ40 mJ
355 nm12 mJ18 mJ24 mJ
266 nm5 mJ8 mJ10 mJ
ModelPL2251A-10PL2251B-10PL2251C -10

-P80

Provides 80 ps ± 10% output pulse duration. Pulse energy specifications as below:

ModelPL2251APL2251BPL2251C
1064 nm70 mJ100 mJ160 mJ
ModelPL2251APL2251BPL2251C

Publications

Aggregation states of poly (4-methylpentene-1) at a solid interface

K. Yamamoto, D. Kawaguchi, K. Sasahara, M. Inutsuka, S. Yamamoto, K. Uchida et al., Polymer Journal 51 (2), 247-255 (2019). DOI: 10.1038/s41428-018-0134-7.

Soft x-ray emission from laser-produced strontium ions

T. Miyazaki, G. O’Sullivan, and P. Dunne, Journal of Physics B: Atomic, Molecular and Optical Physics 53 (2), 025001 (2019). DOI: 10.1088/1361-6455/ab53be.

How nature covers its bases

S. Boldissar, and M. S. de Vries, Phys. Chem. Chem. Phys. 20, 9701-9716 (2018). DOI: 10.1039/C8CP01236A.

Excited State Dynamics of 6-Thioguanine

F. M. Siouri, S. Boldissar, J. A. Berenbeim, and M. S. de Vries, The Journal of Physical Chemistry A 121 (28), 5257-5266 (2017). DOI: 10.1021/acs.jpca.7b03036.

Intraoperative diagnostics and elimination of residual microtumours with plasmonic nanobubbles

E. Y. Lukianova‑Hleb, Y. Kim, I. Belatsarkouski, A. M. Gillenwater, B. E. O’Neill, and D. O. Lapotko, Nature Nanotechnology 11 (6), 525-532 (2016). DOI: 10.1038/NNANO.2015.343.

Large fluctuations at the lasing threshold of solid-and liquid-state dye lasers

S. Basak, A. Blanco, and C. López, Scientific reports 6 (1), 32134 (2016). DOI: 10.1038/srep32134.

On-demand intracellular amplification of chemoradiation with cancer-specific plasmonic nanobubbles

E. Y. Lukianova‑Hleb, X. Ren, R. R. Sawant, X. Wu, V. P. Torchilin, and D. O. Lapotko, Nature Medicine , 778-784 (2014). DOI: 10.1038/nm.3484.

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