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Featured researches published by J. Rossbach.


Optics Letters | 2011

Yb:YAG Innoslab amplifier: efficient high repetition rate subpicosecond pumping system for optical parametric chirped pulse amplification

M. Schulz; R. Riedel; Arik Willner; T. Mans; C. Schnitzler; Peter Russbueldt; J. Dolkemeyer; E. Seise; T. Gottschall; Steffen Hädrich; S. Duesterer; Holger Schlarb; J. Feldhaus; Jens Limpert; B. Faatz; Andreas Tünnermann; J. Rossbach; Markus Drescher; F. Tavella

We report on a Yb:YAG Innoslab laser amplifier system for generation of subpicsecond high energy pump pulses for optical parametric chirped pulse amplification (OPCPA) at high repetition rates. Pulse energies of up to 20 mJ (at 12.5 kHz) and repetition rates of up to 100 kHz were attained with pulse durations of 830 fs and average power in excess of 200 W. We further investigate the possibility to use subpicosecond pulses to derive a stable continuum in a YAG crystal for OPCPA seeding.


Archive | 2009

Ultraviolet and Soft X-Ray Free-Electron Lasers

Peter Schmüser; Martin Dohlus; J. Rossbach

The main goal of the book is to provide a systematic and didactic approach to the physics and technology of free-electron lasers. Numerous figures are used for illustrating the underlying ideas and concepts, and many links to other fields of physics are provided. After an introduction to undulator radiation and the low-gain FEL, the one-dimensional theory of the high-gain FEL is developed in a systematic way. Particular emphasis is put on explaining and justifying the various assumptions and approximations that are needed to obtain the differential equations governing the FEL dynamics. The predictive power of the 1D FEL theory is demonstrated with numerous examples and figures, including exponential gain, saturation and FEL bandwidth. One of the most important features of a high-gain FEL, the formation of microbunches, is studied at length and illustrated with several figures. 3D corrections to the 1D theory are discussed. The process of self amplified spontaneous emission (SASE) is explained mathematically, and many experimental results are shown. The layout of the worlds first SASE FEL in the soft X-ray regime, FLASH, is described in some detail and the technological challenges of X-ray FELs are outlined. Important concepts of accelerator physics are explained while some of the more involved mathematical computations are put into the appendices.


Optics Express | 2010

High average and peak power few-cycle laser pulses delivered by fiber pumped OPCPA system

Jan Rothhardt; Steffen Hädrich; Enrico Seise; Manuel Krebs; F. Tavella; Arik Willner; S. Düsterer; H. Schlarb; J. Feldhaus; Jens Limpert; J. Rossbach; Andreas Tünnermann

We report on a high power optical parametric amplifier delivering 8 fs pulses with 6 GW peak power. The system is pumped by a fiber amplifier and operated at 96 kHz repetition rate. The average output power is as high as 6.7 W, which is the highest average power few-cycle pulse laser reported so far. When stabilizing the seed oscillator, the system delivered carrier-envelop phase stable laser pulses. Furthermore, high harmonic generation up to the 33(th) order (21.8 nm) is demonstrated in a Krypton gas jet. In addition, the scalability of the presented laser system is discussed.


Optics Express | 2012

Pulsed operation of a high average power Yb:YAG thin-disk multipass amplifier

M. Schulz; R. Riedel; Arik Willner; S. Düsterer; M. J. Prandolini; J. Feldhaus; Bart Faatz; J. Rossbach; Markus Drescher; F. Tavella

An Yb:YAG thin-disk multipass laser amplifier system was developed operating in a 10 Hz burst operation mode with 800 µs burst duration and 100 kHz intra-burst repetition rate. Methods for the suppression of parasitic amplified spontaneous emission are presented. The average output pulse energy is up to 44.5 mJ and 820 fs compressed pulse duration. The average power of 4.45 kW during the burst is the highest reported for this type of amplifier.


Optics Express | 2010

Fiber-amplifier pumped high average power few-cycle pulse non-collinear OPCPA.

F. Tavella; Arik Willner; Jan Rothhardt; Steffen Hädrich; Enrico Seise; S. Düsterer; Th. Tschentscher; H. Schlarb; J. Feldhaus; Jens Limpert; Andreas Tünnermann; J. Rossbach

We report on the performance of a 60 kHz repetition rate sub-10 fs, optical parametric chirped pulse amplifier system with 2 W average power and 3 GW peak power. This is to our knowledge the highest average power sub-10 fs kHz-amplifier system reported to date. The amplifier is conceived for applications at free electron laser facilities and is designed such to be scalable in energy and repetition rate.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996

Interdependence of parameters of an X-ray FEL

J. Rossbach; E.L. Saldin; E.A. Schneidmiller; M.V. Yurkov

Abstract This article presents a dimensionless analysis of a self amplified spontaneous emission (SASE) FEL operating in an X-ray wavelength band. Using similarity techniques we have performed an analysis of the results of numerical simulations and derived simple design formulae for the calculation of the characteristics of the SASE FEL. We have also shown that the growth of the energy spread due to the quantum fluctuations of synchrotron radiation imposes a limit on the minimal achievable value of the wavelength in the X-ray FEL.


international free electron laser conference | 2003

Study of the statistical properties of the radiation from a VUV SASE FEL operating in the femtosecond regime

V Ayvazyan; J.-P Carneiro; P Castro; B. Faatz; A.A Fateev; J. Feldhaus; Ch. Gerth; V Gretchko; B Grigoryan; U. Hahn; K. Honkavaara; M Hüning; R. Ischebeck; U. Jastrow; R Kammering; J Menzel; M Minty; D Nölle; J Pflüger; Ph Piot; L. Plucinski; K Rehlich; J. Rossbach; E.L. Saldin; H. Schlarb; E. A. Schneidmiller; S. Schreiber; R. Sobierajski; B. Steeg; F Stulle

The Free-Electron Laser (FEL) at the TESLA Test Facility at DESY operates in the self-amplified spontaneous emission mode and generates sub-100-fs radiation pulses in the vacuum ultraviolet spectral region. During operation in the saturation regime, radiation pulses with GW peak power are produced. The statistical properties of the FEL radiation have been studied for different amplification regimes as well as behind a narrow-band monochromator and found to be in good agreement with the results of numerical simulations. Information about the spectral and temporal structure of the FEL radiation has been deduced from the statistical properties. The pulse duration of the FEL radiation can be varied by tailoring the electron bunch that drives the FEL.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997

FUNDAMENTAL LIMITATIONS OF AN X-RAY FEL OPERATION DUE TO QUANTUM FLUCTUATIONS OF UNDULATOR RADIATION

J. Rossbach; E.L. Saldin; E.A. Schneidmiller; M.V. Yurkov

Abstract In this paper we show that the effect of energy diffusion in the electron beam due to quantum fluctuations of undulator radiation imposes fundamental limit towards achieving very short wavelength in the FEL amplifier.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001

Development of a pump-probe facility combining a far-infrared source with laser-like characteristics and a VUV free electron laser

Bart Faatz; A.A Fateev; Josef Feldhaus; J. Krzywinski; J. Pflueger; J. Rossbach; E.L. Saldin; E.A. Schneidmiller; M.V. Yurkov

Abstract The TESLA Test Facility (TTF) at DESY is a facility producing sub-picosecond electron pulses for the generation of VUV or soft X-ray radiation in a free electron laser (FEL). The same electron pulses would also allow the direct production of high-power coherent radiation by passing the electron beam through an undulator. Intense, coherent far-infrared (FIR) undulator radiation can be produced from electron bunches at wavelengths longer than or equal to the bunch length. The source described in this paper provides, in the wavelength range 50– 300 μm , a train of about 1– 10 ps long radiation pulses, with about 1 mJ of optical energy per pulse radiated into the central cone. The average output power can exceed 50 W . In this conceptual design, we intend to use a conventional electromagnetic undulator with a 60 cm period length and a maximum field of 1.5 T . The FIR source will use the spent electron beam coming from the VUV FEL which allows one to significantly extend the scientific potential of the TTF without interfering with the main option of the TTF FEL operation. The pulses of the coherent FIR radiation are naturally synchronized with the VUV pulses from the main TTF FEL, enabling pump-probe techniques using either the FEL pulse as a pump or the FIR pulse as a probe, or vice versa.


Proceedings of the 2005 Particle Accelerator Conference | 2005

Recent Developments at PITZ

M. Krasilnikov; K. Abrahamyan; G. Asova; J. Bahr; G. Dimitrov; U. Gensch; H.-J. Grabosch; J.H. Han; S. Khodyachykh; S. Liu; Velizar Miltchev; A. Oppelt; B. Petrosyan; S. Riemann; L. Staykov; F. Stephan; M.V. Hartrott; E. Jaeschke; D. Kramer; D. Lipka; D. Richter; J.-P. Carneiro; K. Flottmann; S. Schreiber; J. Ronsch; J. Rossbach; P. Michelato; L. Monaco; C. Pagani; D. Sertore

The ability to produce high brightness electron beams as required for modern Free Electron Lasers (FELs) has been demonstrated during the first stage of the Photo Injector Test Facility at DESY Zeuthen (PITZ1). The electron source optimization at PITZ1 was successfully completed, resulting in the installation of the PITZ rf gun at the VUV-FEL (DESY, Hamburg). One of the main goals of the second stage of PITZ (PITZ2) is to apply higher gradients in the rf gun cavity in order to obtain smaller beam emittance by faster acceleration of the space charge dominated beams. In order to reach the required gradients a 10 MW klystron has to be installed and the gun cavity has to be conditioned for higher peak power. Another important goal of PITZ2 is a detailed study of the emittance conservation principle by using proper electron beam acceleration with a booster. Further photo injector optimization, including update of the photocathode laser and diagnostic tools, is foreseen as well. Recent progress on the PITZ developments will be reported.

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M.V. Yurkov

Joint Institute for Nuclear Research

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Arik Willner

Helmholtz Institute Jena

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F. Tavella

Helmholtz Institute Jena

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E.A. Schneidmiller

Joint Institute for Nuclear Research

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