FILTER PRODUCTS

to
to
to

FILTER PRODUCTS

to
to
to

OPAs

The PT403 series laser systems integrate a picosecond 1 kHz repetition rate DPSS pump laser and optical parametric generator into a single housing, providing a wide tunable wavelength range from 210 to 2300 nm. This all-in-one-box solution offers motorized hands-free tuning, high pulse energy, and narrow linewidth for various ...

Specifications

Widest Tuning Range: 210 – 2300 nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 410 – 709 nm
Peak Efficiency (S+I): Not Specified
Idler Polarization: Vertical, Horizontal
The PGx01 series is a high energy broadly tunable picosecond Optical Parametric Amplifier (OPA) designed to offer ultra-broad tuning capabilities from 193 to 16,000 nm. With its high peak power (>50 MW), this OPA is ideal for various non-linear spectroscopy applications. It boasts a narrow linewidth of <6 cm⁻¹ (for UV ...

Specifications

Widest Tuning Range: 193 – 16000 nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 420 – 4500 nm
Peak Efficiency (S+I): Not Specified
Idler Polarization: Vertical, Horizontal
AVUS is the very latest Optical Parametric Amplifier (OPA) providing widely tunable high-energy pulses. It is ideal for use with 1 μm femtosecond lasers and opens doors for up to 50 W pump power. The user-friendly and maintenance-free unit is air-cooled and constructed with a monolithic case design for long-term thermal stability, ...

Specifications

Widest Tuning Range: 200 – 10000 nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 630 – 2600 nm
Peak Efficiency (S+I): 12 %
Idler Polarization: Vertical, Horizontal

Ultrafast Optical Parametric Amplifiers (OPAs): Expanding the Horizons of Tunable Ultrafast Light

Ultrafast Optical Parametric Amplifiers (OPAs) are pivotal in modern photonics, enabling the generation of ultrashort laser pulses with tunable wavelengths. By exploiting nonlinear optical processes, OPAs convert fixed-frequency pump pulses into variable-frequency signal and idler pulses, offering broad spectral coverage from the ultraviolet (UV) to the mid-infrared (MIR) regions.

Operating Principles

At the heart of an OPA is a nonlinear crystal, such as beta barium borate (BBO) or potassium titanyl phosphate (KTP). When a high-intensity pump pulse interacts with a lower-intensity signal pulse within the crystal, energy is transferred from the pump to the signal, amplifying it. Simultaneously, an idler pulse is generated to conserve energy and momentum. The phase-matching conditions within the crystal determine the efficiency and bandwidth of this process, allowing for tunable output across a wide range of wavelengths.

Key Features

  • Broad Wavelength Tunability: OPAs can produce coherent light spanning from approximately 240 nm to over 10 µm, covering UV, visible, and MIR regions.

  • Ultrashort Pulse Generation: Capable of generating pulses as short as a few femtoseconds, OPAs are ideal for time-resolved studies.

  • High Peak Powers: The amplification process allows for the generation of high-intensity pulses suitable for nonlinear optical experiments.

  • Compatibility with Various Pump Lasers: OPAs can be pumped by different laser systems, including Ti:Sapphire and Ytterbium-based lasers, providing flexibility in experimental setups.

Applications

  • Time-Resolved Spectroscopy: OPAs enable the study of ultrafast phenomena in chemistry and physics by providing tunable, short-duration pulses.

  • Nonlinear Microscopy: In techniques like multiphoton microscopy, OPAs offer the necessary wavelengths and pulse durations for deep tissue imaging with high resolution.

  • Quantum Optics: OPAs are instrumental in generating entangled photon pairs and squeezed states, essential for quantum communication and computing.

  • Material Processing: The high peak powers and tunable wavelengths of OPAs make them suitable for precise micromachining and surface structuring applications.

Recent Developments

Advancements in OPA technology have led to the development of compact, automated systems with improved stability and user-friendly interfaces. For instance, the Apollo-T OPA offers a fully automated, single-port output across a tuning range of 240 nm to 10 µm, optimized for time-resolved spectrometry. Similarly, the Spirit-OPA provides high repetition rates up to 1 MHz with ultra-wide, gap-free wavelength coverage from UV to mid-IR, facilitating applications in ultrafast spectroscopy.

Conclusion

Ultrafast Optical Parametric Amplifiers are indispensable tools in the field of photonics, offering unparalleled flexibility in generating tunable, high-intensity ultrashort pulses. Their broad wavelength coverage and compatibility with various laser systems make them suitable for a wide array of applications, from fundamental research to industrial processes. As technology continues to advance, OPAs are poised to play an even more significant role in expanding the capabilities of ultrafast optics.

Did You know?

Optical parametric amplifier (OPA), is a coherent light source that emits light of variable wavelengths generated by an optical parametric amplification process without optical cavity. The signal beam and the pump beam propagate through the crystal. Photons of the pump wave are then converted into lower-energy signal photons and idler photons; the photon energy of the idler wave is the difference between the photon energies of pump and signal waves, determined by phase matching condition. In an OPA, the input is two light beams, of frequency ωp and ω1. The OPA will make the ωp beam weaker, and amplify the ω1 beam, and also create a new beam at the frequency ω2: ωp=ω1+ω2. As an example of OPA, the incident pump pulse is at 800 nm (12500 cm−1), and the two outputs, signal and idler, are in the near-infrared region, the sum of the wavenumber of which is equal to 12500 cm−1.