OPOLETTE 2731 / 3034

Ultra-compact, light-weight Mid-Infrared (MIR) tunable laser system.
Tuning Range
2700 – 3100 nm (2731 model)
3000 – 3450 nm (3034 model)
Peak OPO Energy
6 mJ @ 2940 nm (2731 model)
5 mJ @ 3400 nm (3034 model)

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Opolette 2731 / 3034

The Opolette 2731 / 3034 tunable laser series utilizes optical parametric oscillator (OPO) technology to generate wavelengths over a broad range in the MIR. Designed for portability, the entire laserhead fits into a 7×12” footprint and ships completely sealed to protect optical components from the environment. Requiring no installation, the system includes verification hardware to check alignment after shipping or relocation. A built-in red laser diode is aligned to overlap with the mid-IR output for beam guidance. Wavelength tuning is motorized and computer-controlled.

Product Features

  • Hermetically sealed, light-weight, compact tunable laser system
  • Integrated pump laser with quick connect cables
  • End-user replaceable flashlamp (50 million shot lifetime) and DI cartridge
  • All tunable wavelengths output from a single port
  • Alignment verification
  • Integrated alignment diode laser for OPO beam path identification
  • Computer-controlled tuning via control software/software development kit (SDK)
  • Flashlamp and/or Q-Switch external triggering
  • Access to residual beams
  • WARRANTY: One year on the entire system. Includes all options except fibers.

Product Options

  • Protective Hard Shell Cases (PHSC)
    Includes two protective hard cases with custom foam padding.
  • External Motorized Variable Attenuator (eMVA)
    End-user installable/removable. Reduces max OPO by 10-15% when installed. Computer-controlled. Can only be used with visible and near-infrared wavelengths.
  • Fiber Delivery Kit (FD)
    Can be optimized for either ultra-violet (UV), visible (VIS), or near-infrared (NIR) tuning ranges.
    Externally mounted fiber delivery kit includes mounts, coupling lens, and fiber. Fiber specifications: 2.5 m long, 1 mm diameter core, NA = 0.22
  • Harmonic Generation (HG)
    355 nm generated from residual 1064 nm.
  • Extended Warranty (EXW)
    Extends full system warranty for one additional year, for a total of two years. Includes all options except for fibers.


Opolette HE 2731

Tuning Range 2700 – 3100 nm
Peak Energy 6 mJ @ 2940 nm
Repetition Rate 20 Hz
Pulse Width 5 – 7 ns
Beam Diameter 4 mm
Divergence 10 (H) x 2 (V) mrad

Opolette HE 3034

Tuning Range 3000 – 3450 nm
Peak Energy 5 mJ @ 3400 nm
Repetition Rate 20 Hz
Pulse Width 5 – 7 ns
Beam Diameter 4 mm
Divergence 10 (H) x 2 (V) mrad


Mass Spectrometry

Mass spectrometry is an application used to identify molecules within a sample by measuring the mass-to-charge ratio of ions. There are three components of mass spectroscopy: ionizing, analyzing, and detecting.

A sample is ionized and then ions are accelerated and sent through an electric and magnetic field, which affects speed and trajectory. The magnitude at which an ion changes trajectory depends on the mass-to-charge ratio. Ions with the same ratio will be deflected in the same amount.

The differences in mass-to-charge ratio allows a mass analyzer to sort the ions, and results are displayed as spectra of the relative abundance of the detected ions, based on the mass-to-charge ratio. Components of the sample are identified by correlating known masses of substances to the masses identified in the sample or through fragmentation pattern.

Lasers are used in two different ways in mass spectrometry.  They are used to vaporize the sample and to ionize it.

Two-step laser mass spectrometry (L2MS) requires two steps using two different laser pulses.  In the first step, a pulsed infrared laser is focused on the sample to cause rapid heating and desorption of molecules in the sample.  In the second step, a pulse ultraviolet laser causes ionization of the desorbed molecules.  The molecules are then analyzed.  In this method, desorption and ionization are independently tunable.  This allows trace amounts of organic molecules to be detected in complex materials.

Matrix-assisted laser desorption ionization (MALDI) uses one step and one laser pulse to both vaporize and ionize the sample.  Before starting, the sample is mixed into a laser energy absorbing matrix material.  A pulsed laser triggers ablation and desorption of the sample and the matrix material.  Molecules are ionized in the hot plume of ablated gases and then analyzed.

Contact us for assistance in selecting the appropriate system for your mass spectrometry application.




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