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4-1 Development and Implementation of Laser Systems and Measuring Techniques
Project coordinator: I. Will, M. Zhavoronkov
UP1: Development, installation and maintenance of lasers for particle accelerators
(Ingo Will, Guido Klemz, Ingo Templin)
Another major effort of the project is devoted to the development of picosecond lasers systems at very high average powers, both in the burst-mode and the quasi-cw operation mode. MBI burst-mode lasers operate with average powers up to 5kW during bursts, making these laser systems unique for research on high-power laser plasma sources, e.g. for the EUV lithography. The main applications, however, arise from various collaborations with national and international high-energy accelerator and Free Electron Laser projects. MBI as an early member of the international TESLA Collaboration has been instrumental since 1994 in providing photocathode lasers for the TESLA Test Facilities TTFI and TTFII at DESY Hamburg, the PITZ facility at Zeuthen, and the DESY VUV-FEL as well as the future European X-FEL. In addition, MBI provides an EU-funded OPCPA fs-laser as a user station at the VUV-FEL, and the quasi-cw photocathode laser for the superconducting gun at the ELBE FEL in Rossendorf, and participates in several research projects for the planned VUV-FEL at BESSY. Since late 2003 MBI is embedded in international consortia from several European FEL projects to participate in EU-funded Design Studies on future FEL's.

Photinjector drive lasers

At present, the special lasers developed at the MBI drive the photo injectors of the linacs in the following laboratories of our cooperation partners:

  • FLASH FEL at DESY Hamburg
  • Photoinjector Test Facility at Zeuthen
  • Superconducting RF gun being developed at the Forschungszentrum Dresden Rossendorf (FZD) for the ELBE FEL

To see how a laser works together with a photo injector click here. (Macromedia Flash needed)

Generation of flat-top UV pulses for PITZ, FLASH and the upcoming XFEL

We have recently developed a photoinjector drive laser generating trains (bursts) of UV pulses of programmable shape, in particular of flat-top pulses with sharp rising and falling edges. It is expected, that the emittance of the generated electron beam can be significantly improved by appropriately shaping the laser pulses.
The present laser developed at the MBI for the PITZ installation at DESY Zeuthen allows for a large variety of the shape of the generated pulses. The figure below shows some of them:

many_pulse_shapes.jpg (51666 bytes)

Figure: Different shapes of the UV pulses produced with the Yb:YAG laser system

The laser system generating the desired trains of shaped picosecond UV pulses consists of the following components:

  • A femtosecond Yb:KGW laser oscillator, that is precisely synchronized to the RF master oscillator of the linear accelerator,
  • the pulse shaper,
  • a chain of Yb:YAG amplifiers,
  • a wavelength converter that converts the infrared laser pulses of the laser to the ultraviolet (4-th harmonics),
  • a so-called optical sampling system for measuring the pulse shape by cross correlation,
  • a computerized control system that allows for full remote control of the laser.

The actual shaping of the pulses is accomplished by a multicrystal birefringent filter located before the entrance of the amplifier chain of the laser system. The pulse shaping process can be explained by a coherent staking of 14 replicas of the short input pulse. In order to control the mutual phase of these replicas precisely, the temperatures of the 13 birefringent crystals of the shaper are tuned with 0.01° C accuracy.

The described laser developed at the MBI is used since summer 2008 for driving the photo injector of the PITZ installation at DESY Zeuthen. During 2009, the laser was further improved. In particular, the number of generated pulse shapes was increased.
We expect that with an optimized pulse shape the emittance of the electron beam will be reduced to a value below 1 pi mm mrad in summer 2010. This low emittance is required for the electron beams of the upcoming XFEL at DESY in Hamburg. To reach that emittance, DESY is presently building a new RF photo injector and an improved RF system.

Figure: Shape of the produced flat-top picosecond pulses with sharp edges

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