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OPAs

The Harmony Optical Parametric Amplifier is a sophisticated solution for converting ultrafast pulses emitted by Ytterbium-based lasers into broadly tunable pulses spanning an extensive wavelength range from 210 to over 10,000 nm. Engineered with precision and compactness in mind, Harmony features an integrated mini spectrometer and ...

Specifications

Widest Tuning Range: 630-2600nm
Signal Polarization: Not Applicable
Core Tuning Range: 630-900nm
Peak Efficiency (S+I): >9 %
Idler Polarization: Not Applicable
...
Data Sheet
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: 210-2300nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 410-709nm
Peak Efficiency (S+I): - %
Idler Polarization: Vertical, Horizontal
...
Data Sheet
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: 193-16000nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 420-4500nm
Peak Efficiency (S+I): - %
Idler Polarization: Vertical, Horizontal
...
Data Sheet
The AVUS Optical Parametric Amplifier is a laser frequency conversion device that utilizes optical parametric amplifiers (OPA) to provide a wide range of adjustable high energy pulses. It is designed to be used with a 1μm femtosecond laser pump source and offers two versions: AVUS SP with a pulse duration of less than 70 fs and ...

Specifications

Widest Tuning Range: 630-1020nm
Signal Polarization: Not Applicable
Core Tuning Range: 1040-2600nm
Peak Efficiency (S+I): -- %
Idler Polarization: Not Applicable
...
Data Sheet
Thorlabs Ytterbia Femtosecond Optical Parametric Amplifier (OPA) with an integratedYtterbium Fiber Laser, Thorlabs FSL1030X1, converts single-frequency light (1035 nm) into a fixed wavelength NIR using white light and optical parametric amplification. The OPA is coherently seeded from white-light continuum ...

Specifications

Widest Tuning Range: 1650-1650nm
Signal Polarization: Vertical
Core Tuning Range: 1650-1650nm
Peak Efficiency (S+I): NA %
Idler Polarization: Vertical
...
Data Sheet
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: 200-10000nm
Signal Polarization: Vertical, Horizontal
Core Tuning Range: 630-2600nm
Peak Efficiency (S+I): 12 %
Idler Polarization: Vertical, Horizontal
Data Sheet
There are 6 different OPAs from suppliers and manufacturers listed in this category. In just a few clicks you can compare different OPAs with each other and get an accurate quote based on your needs and specifications. Please note that the prices of OPAs vary significantly for different products based on various factors including technical parameters, features, brand name, etc. Please contact suppliers directly to inquire about the details and accurate pricing information for any product model. Simply navigate to the product page of interest and use the orange button to directly reach out to the respective supplier with one click.

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.