pulseSlicer

pulseSlicer

Spectrum Slicer: Narrowing the Bandwidth of Pulsed Lasers by Spectral Cutting


Narrowing the Spectral Bandwidth of Pulsed Lasers by Spectral Cutting with a Spectrum Slicer / Laser Monochromator


Spectral Cutting with pulseSlicer

The principle task of the spectrum slicer (or laser monochromator) pulseSlicer is to cut out a very narrow spectral part of an ultra-short laser pulse. This function is similar to a band pass filter at a first glance. For example, in the spectral domain this could mean the narrowing of the spectral width of Ti:Sapphire pulses at 800 nm from Δλ = 7 nm to Δλ = 0.35 nm. In the time domain this corresponds with to a pulse stretching from approximately 140 up to 2700 fs.

Standard laser sources typically generate fixed or slightly variable pulses only. Therefore, the pulseSlicer acts as a spectrum slicer and is an economic solution for narrowing broadband laser pulses by spectral cutting. An optical system disperses the pulses spatially, and in the plane where the spectrum is spatially dispersed, the spectrum is controlled via a mask. Afterwards, the dispersed pulse is recollimated.

With the narrowing of the spectrum the spectral pulse width is modified accordingly, resulting in longer pulses. The transmitted power is reduced proportionally to the amount of spectral cutting, but many applications are not power limited when considering the available laser input power.

pulseSlicer in Combination with Pulsed Laser Sources

  • Automized, narrow-band laser source
  • Large wavelength tuning range
  • User adjustable spectral bandwidth and output pulse durations
  • High spectral power density compared to common lasers or OPOs
  • High repetition rates (80 / 160 / 320 MHz) to cope with weak single-photon signal detection

Quantum Dot Single-Photon Generation

The combination of the pulseSlicer and the tunable picosecond laser picoEmerald supports customers in the field of quantum research.

At a Glance

  • Easily variable output bandwidth / pulse duration
  • Simple solution for narrowing broadband laser pulses
  • Automated and software controlled
  • TCP/IP software interface for easy remote automation
Principle of a spectrum slicer: Pulse spectrum of the incident pulses (blue) and pulse spectrum (red) shaped by the spectrum slicer

Specifications

pulseSlicer NIRF25F50F100
Wavelength range650 nm … 1080 nm
Minmal bandwidth at 1000 nm0.11 nm0.06 nm0.03 nm
Static transmission50% … 70% between 700 nm … 1050 nm
Total transmissionDepends on slicing ratio
pulseSlicer IRF25F50F100
Wavelength range1000 nm … 1600 nm
Minimal bandwidth at 1550 nm0.17 nm0.08 nm0.04 nm
Static transmission50% … 70% between 1050 nm … 1600 nm
Total transmissionDepends on slicing ratio
Features for all pulseSlicer models:
Input beam polarizationLinear, horizontal, polarization rotator optional
Software and automationIncluded
Remote controlPossible via TCP/IP interface

Data

Minimal output bandwidth pulseSlicer NIR
Minimal output bandwidth for pulseSlicer IR

Datasheets & Brochures


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APE Angewandte Physik & Elektronik GmbH
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APE Angewandte Physik & Elektronik GmbH
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Fax: +49 30 986011333

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APE Angewandte Physik & Elektronik GmbH
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Fax: +49 30 986011333

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Laser Sciences Services Pvt. Ltd.

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APE Angewandte Physik & Elektronik GmbH
Plauener Strasse 163-165 | Haus N
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Fax: +49 30 986011333

Sales: sales@ape-berlin.de
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