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Featured researches published by R. Schurig.


Journal of Physics: Conference Series | 2011

Operation of the superconducting RF photo gun at ELBE

Jochen Teichert; Andre Arnold; H. Büttig; U. Lehnert; P. Michel; Petr Murcek; Ch Schneider; R. Schurig; G Staats; Rong Xiang; P Kneisel; T. Kamps; J. Rudolph; M. Schenk; G. Klemz; I. Will

As the first superconducting RF photo-injector (SRF gun) in practical operation, the SRF gun has been successfully connected to the superconducting linac ELBE at Forschungzentrum Dresden-Rossendorf. The injection with this new gun will improve the beam quality for the users of the radiation source. The SRF gun contains a 3½ cell superconducting accelerating cavity with a frequency of 1.3 GHz. The design is for use of normal conducting photocathodes. At present, caesium telluride photocathodes are applied which are illuminated by an ultraviolet laser beam. The kinetic energy of the produced electron beam is 3 MeV which belongs to a peak electric field of 16 MV/m in the cavity. The maximum bunch charge which is obtained and measured in a Faraday cup is about 400 pC (20 μA average current at a repetition rate of 50 kHz). The SRF gun injector is connected to the ELBE accelerator via a dogleg with two 45° deflection magnets. This connection beam line was commissioned in January 2010. A first beam injection into the ELBE accelerator has been carried out with a bunch charge of 120 pC (6 μA at 50 kHz). Detailed measurements showed that beam loss occurred in the dogleg above 60 pC due to the correlated energy spread. In order to find the optimal operation conditions, energy spread was measured in dependence of bunch charge, laser phase and further gun parameters. The Cs2Te photocathode shows an excellent life time. It is in the gun since May 2010 with about 300 h beam time and about 7 C extracted charge. In the present cavity, the limit for the acceleration gradient is field emission due to some defect on the cavity surface and problems during cleaning. Therefore a modified 3½ niobium cavity has been fabricated, which will increase the RF gradient in the gun and thus improve the beam parameters further.


SPIN PHYSICS: 18th International Spin Physics Symposium | 2009

Rossendorf SRF‐Gun Cavity Characteristics

Andre Arnold; H. Büttig; D. Janssen; Matthias Justus; T. Kamps; G. Klemz; U. Lehnert; P. Michel; K. Möller; Petr Murcek; J. Rudolph; A. Schamlott; M. Schenk; Ch. Schneider; R. Schurig; F. Staufenbiel; Jochen Teichert; V. Volkov; I. Will; Rong Xiang

At the Forschungszentrum Dresden‐Rossendorf the development and the setup of the 2nd superconducting radio frequency photo electron injector (SRF‐Photo‐Gun) is finished. This new injector is placed next to the existing thermionic gun of the superconducting linear accelerator ELBE. A connection between the accelerator and the SRF‐Gun will provide improved beam parameters for the users at the second half of 2009. At the moment the commissioning is fully under way. We will report on important results concerning cavity commissioning like measurements of: Q vs. E, microphonics, Lorentz detuning, tuner parameters, pressure sensibility and in‐situ fundamental mode field distribution calculated from measured pass band.


ieee nuclear science symposium | 2008

The new superconducting RF photoinjector at the ELBE linac

Jochen Teichert; Andre Arnold; Hartmut Büttig; D. Janssen; Matthias Justus; U. Lehnert; P. Michel; Petr Murcek; Arndt Schamlott; Christof Schneider; R. Schurig; F. Staufenbiel; Rong Xiang; T. Kamps; Jeniffa Rudolph; Mario Schenk; Axel Matheisen; G. Klemz; I. Will; Peter vom Stein

Most of the proposed electron accelerator projects for future free electron lasers, energy recovery linacs, or 4th generation light sources require electron beams with an unprecedented combination of high-brightness, low emittance and high average current. For that reason existing electron injectors must be considerably improved or new injector concepts developed. One very promising approach represents the superconducting radio frequency photoinjector (SRF gun). This injector type combines the advantages of a conventional photoelectron injector with that of superconducting acceleration, i.e. the very low RF losses and simple continuous wave operation. A SRF gun was developed and installed at Forschungszentrum Dresden-Rossendorf for operation at the ELBE superconducting linear accelerator. In November 2007 the first beam was produced. First commissioning results have been collected. Besides an improvement of beam quality and parameter range the SRF gun serves as a test bench for further development, evaluation and optimization since it is the first injector of its type which is operating at an accelerator worldwide


5th Int. Particle Accelerator Conf. (IPAC'14), Dresden, Germany, June 15-20, 2014 | 2014

TWO YEARS EXPERIENCE WITH THE UPGRADED ELBE RF-SYSTEM DRIVEN BY 20 kW SOLID STATE AMPLIFIER BLOCKS (SSPA)

Hartmut Büttig; Andre Arnold; Andree Büchner; Matthias Justus; Michael Kuntzsch; U. Lehnert; P. Michel; R. Schurig; Gerald Staats; Jochen Teichert

Since January 2012 the Superconducting 1.3 GHz CW Linac ELBE is equipped and in permanent operation with four 20 kW Solid State Amplifier Blocks (SSPA). The project and the design of the new RF system have been described in the papers [1] and. The experience gained within the first two years of operation is encouraging.


international free electron laser conference | 2003

First operation of a superconducting RF-gun

D. Janssen; H. Büttig; Pavel Evtushenko; M. Freitag; F. Gabriel; B. Hartmann; U. Lehnert; P. Michel; K. Möller; T. Quast; B. Reppe; A. Schamlott; Ch. Schneider; R. Schurig; Jochen Teichert; S. Konstantinov; S Kruchkov; A.M. Kudryavtsev; O. Myskin; V.V Petrov; A Tribendis; V. Volkov; W. Sandner; I. Will; A. Matheisen; W. Moeller; M. Pekeler; P.v. Stein; Ch. Haberstroh


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2007

Development of a superconducting radio frequency photoelectron injector

Andre Arnold; H. Büttig; D. Janssen; T. Kamps; G. Klemz; W.D. Lehmann; U. Lehnert; D. Lipka; F. Marhauser; P. Michel; K. Möller; Petr Murcek; Ch. Schneider; R. Schurig; F. Staufenbiel; J. Stephan; Jochen Teichert; V. Volkov; I. Will; Rong Xiang


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2008

A high-brightness SRF photoelectron injector for FEL light sources

Andre Arnold; H. Büttig; D. Janssen; T. Kamps; G. Klemz; W.D. Lehmann; U. Lehnert; D. Lipka; F. Marhauser; P. Michel; K. Möller; Petr Murcek; Ch. Schneider; R. Schurig; F. Staufenbiel; J. Stephan; Jochen Teichert; V. Volkov; I. Will; Rong Xiang


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2014

Free-electron laser operation with a superconducting radio-frequency photoinjector at ELBE

Jochen Teichert; Andre Arnold; H. Büttig; M. Justus; T. Kamps; U. Lehnert; P. Lu; P. Michel; Petr Murcek; Jeniffa Rudolph; R. Schurig; W. Seidel; H. Vennekate; I. Will; Rong Xiang


Physical Review Special Topics-accelerators and Beams | 2010

Cs 2 Te normal conducting photocathodes in the superconducting rf gun

Rong Xiang; Andre Arnold; H. Buettig; D. Janssen; Matthias Justus; U. Lehnert; P. Michel; Petr Murcek; A. Schamlott; Ch. Schneider; R. Schurig; F. Staufenbiel; Jochen Teichert


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006

Technology challenges for SRF guns as ERL sources in view of Rossendorf work

D. Janssen; Hartmut Buettig; Pavel Evtushenko; U. Lehnert; P. Michel; Karsten Moeller; Petr Murcek; Christof Schneider; R. Schurig; F. Staufenbiel; Jochen Teichert; Rong Xiang; Juergen Stephan; Wolf-Dietrich Lehmann; T. Kamps; D. Lipka; V. Volkov; I. Will

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U. Lehnert

Helmholtz-Zentrum Dresden-Rossendorf

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P. Michel

Helmholtz-Zentrum Dresden-Rossendorf

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Jochen Teichert

Helmholtz-Zentrum Dresden-Rossendorf

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Rong Xiang

Helmholtz-Zentrum Dresden-Rossendorf

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Andre Arnold

Helmholtz-Zentrum Dresden-Rossendorf

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Petr Murcek

Helmholtz-Zentrum Dresden-Rossendorf

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F. Staufenbiel

Helmholtz-Zentrum Berlin

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T. Kamps

Helmholtz-Zentrum Berlin

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H. Büttig

Helmholtz-Zentrum Dresden-Rossendorf

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