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OPO

Lumispot Tech 1064nm/1570 OPO Solid-State Laser: a pinnacle of precision and versatility. Designed for the medical industry and beyond, this laser combines efficiency with portability, thanks to laser diode pumping and full air-cooling. Tailor your experience with customizable energy, divergence angle, and wavelength ...

Specifications

Total Tuning Range: 1570 – 1064 nm
Core Tuning Range: 1570 – 1064 nm
Pulse Energy: 20 mJ
Repetition Rate: 20 Hz
Signal Polarization: N/A
The Aurora II-355 DPSS Integra range of type II BBO OPOs has been designed with reliability, stability and ease of use in mind. This allows researchers to concentrate on their experiments and industrial systems integrators the peace of mind that their process will be consistent and robust. With a wide choice of integrated and ...

Specifications

Total Tuning Range: 450 – 1064 nm
Core Tuning Range: 1065 – 2300 nm
Pulse Energy: 10 mJ
Repetition Rate: 100 Hz
Signal Polarization: Horizontal
Aurora II Integra OPO - An innovative, fully motorised, type II BBO OPO and Nd:YAG pump laser integrated into a single system. The Aurora II Integra is designed with reliability, stability and ease of use in mind. This allows researchers to concentrate on their experiments and industrial system integrators the peace of mind ...

Specifications

Total Tuning Range: 205 – 2300 nm
Core Tuning Range: 410 – 710 nm
Pulse Energy: 65 mJ
Repetition Rate: 10 Hz
Signal Polarization: Vertical
The Peacock 532 is a tunable pulsed nanosecond laser source from 680 nm to 2,2 µm. It includes a compact and rugged CFR‐type Nd:YAG laser pumping a state‐of‐the‐art OPO. The whole unit is integrated on a single bench, which can easily be inserted into a complex system. It shows outstanding versatility thanks to a ...

Specifications

Total Tuning Range: 680 – 2200 nm
Core Tuning Range: 680 – 980 nm
Pulse Energy: 35 mJ
Repetition Rate: 30 Hz
Signal Polarization: N/A
The Peacock 532 is a tunable pulsed nanosecond laser source from 680 nm to 2,2 µm. It includes a compact and rugged CFR‐type Nd:YAG laser pumping a state‐of‐the‐art OPO. The whole unit is integrated on a single bench, which can easily be inserted into a complex system. It shows outstanding versatility thanks to a fully ...

Specifications

Total Tuning Range: 680 – 2200 nm
Core Tuning Range: 680 – 980 nm
Pulse Energy: 35 mJ
Repetition Rate: 30 Hz
Signal Polarization: N/A
Q-TUNE is single housing tunable wavelength laser. It employs Optical Parametric Oscillator (OPO) to produce tunable wavelength in 410-2300 nm range with linewidth narrower that 6 cm-1. Optional second harmonic generator extends tuning range to 210-410 nm with linewidth narrower that 12 cm-1. Combined with shorter than 5 ns pulse ...

Specifications

Total Tuning Range: 410 – 2300 nm
Core Tuning Range: 410 – 2300 nm
Pulse Energy: 1 mJ
Repetition Rate: 10 Hz
Signal Polarization: Vertical
The Aurora II-532 Integra range of type II BBO OPOs has been designed with reliability, stability and ease of use in mind. This allows researchers to concentrate on their experiments and industrial systems integrators the peace of mind that their process will be consistent and robust. With a wide choice of integrated ...

Specifications

Total Tuning Range: 670 – 1064 nm
Core Tuning Range: 1065 – 2300 nm
Pulse Energy: 60 mJ
Repetition Rate: 10 Hz
Signal Polarization: Horizontal

Optical Parametric Oscillators (OPOs): Versatile Light Sources for Advanced Applications

Optical Parametric Oscillators (OPOs) are nonlinear optical devices that convert a single pump photon into two lower-energy photons, known as the signal and idler waves, through a process called parametric down-conversion. This unique mechanism allows OPOs to generate tunable coherent light across a wide range of wavelengths, making them invaluable in various scientific and industrial applications.

Operating Principle

An OPO typically consists of a nonlinear crystal, such as periodically poled lithium niobate (PPLN) or potassium titanyl phosphate (KTP), within an optical cavity. When a high-energy pump photon enters the nonlinear crystal, it splits into two lower-energy photons: the signal and idler. The frequencies of these output photons are related to the pump photon frequency by energy conservation, and their wavelengths are determined by phase-matching conditions within the crystal. By adjusting parameters like temperature or crystal orientation, the OPO can be tuned to emit light over a broad spectral range.

Key Features

  • Wavelength Tunability: OPOs can generate light from the ultraviolet to the mid-infrared regions, offering flexibility that is challenging to achieve with traditional lasers.

  • High Coherence: The output from an OPO is coherent and can have a narrow linewidth, making it suitable for high-resolution spectroscopy.

  • High Conversion Efficiency: With proper phase-matching and pump conditions, OPOs can achieve high conversion efficiencies, efficiently utilizing the pump energy.

Applications

  • Spectroscopy: OPOs are widely used in molecular and environmental spectroscopy due to their tunability and coherence.

  • LIDAR Systems: In Light Detection and Ranging (LIDAR), OPOs provide tunable wavelengths for atmospheric sensing and remote sensing applications.

  • Quantum Optics: OPOs are fundamental in generating squeezed states and entangled photon pairs for quantum information processing and communication.

  • Medical Diagnostics: The tunable nature of OPOs allows for selective excitation of specific biomolecules, aiding in advanced imaging and diagnostic techniques.

Recent Developments

Advancements in OPO technology have led to the development of compact, all-solid-state systems that are more robust and easier to integrate into various setups. For instance, OPOs based on periodically poled lithium niobate (PPLN) crystals have been demonstrated to emit tunable light in the mid-infrared region, which is valuable for molecular spectroscopy and environmental monitoring. These developments have expanded the practical applications of OPOs in both research and industry.

Conclusion

Optical Parametric Oscillators are versatile and powerful tools that provide tunable coherent light across a wide spectral range. Their unique capabilities make them indispensable in various fields, including spectroscopy, remote sensing, quantum optics, and medical diagnostics. As technology continues to advance, OPOs are expected to play an increasingly significant role in scientific research and industrial applications.

Did You know?

The first optical parametric oscillator was demonstrated by Joseph Giordmaine and Bob Miller in 1965, five years after the invention of the laser, at Bell Labs. Wavelength tunability and the possibility to attain wavelengths in infrared, far-infrared and terahertz region are the attributes which make OPOs so fascinating. Optical parametric oscillators are used as coherent light sources for various scientific applications, such as generating squeezed light for research in the area of quantum physics and spectroscopy. OPOs can be singly-resonant and pumped with an actively Q-switched Nd:YAG laser.