Our compact fiber stretchers offer the attractive feature to modify the optical path from 0 to 0,1ps. The fiber is fixed on a multilayer piezoelectric actuator. The stretcher uses the piezoelectronic element to change the optical path and phase. IDIL Fibres Optiques stretchers are available in SM, PM or RC (reduced cladding) ...

The Pulse Delay Generator offers several operating modes including pulse generator, frequency divider, burst andpulse picker. This unit generates accurate pulses with a repetition rate up to 20 MHz, variable pulse widths from 5 ns to 2^62 ns and pulse delays from 10 ps to 2^62 ns. Output levels are adjustable between 1 V, 3.3 V and 5 ...

Castech\'s Faraday Rotators and Isolators have high power handling up to 100W of average input power in 1010-1080nm wavelength range, could maintain stability of optical system such as Nd or Yb-doped lasers. Isolators are based on Rotatorswhich non-reciprocally rotator the plane of polarized light in 45 degree.

This mirror mount accepts rectangular optics/mirrors with a height up to either 20 or 25mm (depending on the chosen version). The design allows for a direct mounting into standard 1\" mirror mounts. The slim design with no side-frame is ideally suited to build up compressor beam lines using rectangular mirrors with multi-bounces. To ...

The glass wedges pair allows for dispersion compensation, fine tuning and optimal compression in combination with dispersion compensating mirrors such as the DCM range. Glass wedge pairs The dispersion characteristics of the DCM mirrors are specially designed to work together with specific glass materials, (DCM7:Calcium Floride / ...

This pair of wedge mounting adapters is designed to accept up to 4mm thick glass wedges that provide fine control of the pulse compression set up in combination with the DCM mirror range. One of the adapters can be directly screwed onto M4 threaded pedestal posts whereas the other features a M2 grid to allow a direct mounting onto ...

This fix mirror mount is designed to accept 1/2 inch (12.7mm) optics where no adjustment is required but an increased stability is. The dimensions of this mount are similar to standard 1/2\" adjustable mirror mounts and can be directly used to exchange those if the degree of adjustability is not required. Specifications: Mounts ...

For steering few-cycle pulse beams, usually protected silver mirrors are the first choice and widely used, since they deliver a broadband reflectivity without dispersion problems or angle dependence at a very competitive price. A protected silver mirror that is enhanced for femtosecond applications and tested for sub-5fs pulses. ...

The \"DCM9\" is a GVD mirror shifted to the \"blue\" now covering a wavelength range of 450nm-950nm. These mirrors are specially designed to be suitable for pulse compression of femtosecond pulses generated by amplification, filamentation, OPA/OPG and others. Featuring negative GVD of -60 fs² for the mirror pair @ 700nm and are ...

The \"DCM7\" is a ultra-broadband (600nm-1200nm) dispersion compensating mirror pair used for the compensation of positive dispersion affecting femtosecond laser pulses. The unique pair design enables to achieve a reflectivity greater than 99.9% over the whole supported spectral bandwidth next to a defined negative dispersion. These ...

  The \"DCM11\" is a GVD mirror pair specially designed for OPCPA compression. This mirror type covers a wide wavelength range of 650-1050 nm while offering a large dispersion of -130 fs2 /pair at the centre wavelength of 800 nm. These mirrors are specially designed to recompress the output of the venteon OPCPA after passing ...

The \"DCM10\" is a broadband (500-850nm) dispersion compensating mirror pair designed for the compensation of the positive dispersion caused by fused silica like material. The wavelength range suits femtosecond applications using few-cycle pulses generated by hollow core fibers or filamentation. The unique pair design enables to ...

Femtosecond laser pulses with spectral widths approaching one octave and beyond, require specialised optical components to avoid the accumulation of phase distortions that cannot be pre-compensated for. An all-dielectric ultrabroadband beamsplitters with constant splitting ratio and balanced dispersion in transmission and reflection. ...

Automated hands-free and manual versions Compatible with standardfemtosecond andpicosecond Ti:sapphire oscillators A femtosecond and picosecond SHG module which converts the IR Ti:sapphire wavelengths, across 680-1080 nm, into the UV, across 340-540 nm. Based on novel nonlinear technology, the Oria® Blue offers exceptional ...

HIRO harmonic generator by Light Conversion. HIRO is a valuable option for PHAROS lasers and fLint oscillators that provides high power harmonics radiation at 515nm, 343nm and 258nm wavelengths. We offer several standard HIRO models (with open prospect of future upgrades) whichmeet most users’ needs. the active harmonic is selected ...

SHBC second harmonic bandwidth compressor by Light Conversion. PHAROS harmonic generator product line features second harmonic bandwidth compressor abbreviated as SHBC. The device is dedicated for the formation of narrow bandwidth picosecond pulses from broadband output of ultrafast laser.

PISMO pulse picker by Del Mar Photonics. As the name implies pulse pickers are used to selectively pick off pulses from the pulse train of a femtosecond or picosecond laser. Pismo pulse picker models areavailable as stand-alone devices that use a Pockels cell as an ultrafast shutter. Pismo pulse pickers operate in a broad wavelength ...