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Dive into the research topics where S. G. Biedron is active.

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Featured researches published by S. G. Biedron.


Nature Photonics | 2012

Highly coherent and stable pulses from the FERMI seeded free-electron laser in the extreme ultraviolet

E. Allaria; Roberto Appio; L.Badano; William A. Barletta; S.Bassanese; S. G. Biedron; A.O.Borga; E.Busetto; D. Castronovo; Paolo Cinquegrana; S. Cleva; D.Cocco; M.Cornacchia; P. Craievich; Ivan Cudin; G.D'Auria; M.Dal Forno; M.B. Danailov; R.De Monte; G.De Ninno; Paolo Delgiusto; Alexander Demidovich; S. Di Mitri; B. Diviacco; Alessandro Fabris; Riccardo Fabris; William M. Fawley; Mario Ferianis; Eugenio Ferrari; S.Ferry

Researchers demonstrate the FERMI free-electron laser operating in the high-gain harmonic generation regime, allowing high stability, transverse and longitudinal coherence and polarization control.


IEEE Journal of Quantum Electronics | 2000

Nonlinear harmonic generation in free-electron lasers

H.P. Freund; S. G. Biedron; S.V. Milton

A three-dimensional nonlinear simulation code to treat multiple frequencies simultaneously is described and used to study nonlinear harmonic generation in free-electron lasers (FELs). Strong nonlinear harmonic gain is found where the gain length varies inversely with the harmonic number. Substantial power levels are found in the harmonics. The odd harmonics are favored with generally higher power levels since a planar wiggler geometry is employed; however, the second harmonic exhibits substantial power as well. The analysis is relevant to the emission expected from self-amplified spontaneous emission (SASE) free-electron laser schemes.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002

Two harmonic undulators and harmonic generation in high gain free electron lasers

G. Dattoli; L. Giannessi; P. L. Ottaviani; H.P. Freund; S. G. Biedron; S.V. Milton

We consider an undulator scheme to enhance harmonic generation in high gain free electron lasers. The configuration we consider consists of an undulator providing an on axis field oscillating in both transverse directions, with relatively integer multiple spatial periods. We discuss the spectral properties of the radiation emitted by relativistic electrons crossing this undulator and derive the equations describing the free electron laser evolution. We show that a device, exploiting such an undulator configuration, is a fairly useful tool to obtain simultaneous laser power at different harmonics. The analysis of the system evolution is achieved with two different simulation codes.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000

Nonlinear harmonic generation and proposed experimental verification in SASE FELs

H.P. Freund; S. G. Biedron; S.V. Milton

Recently, a 3D, polychromatic, nonlinear simulation code was developed to study the growth of nonlinear harmonics in self-amplified spontaneous emission (SASE) free-electron lasers (FELs). The simulation was applied to the parameters for each stage of the Advanced Photon Source (APS) SASE FEL, intended for operation in the visible, UV, and short UV wavelength regimes, respectively, to study the presence of nonlinear harmonic generation. Significant nonlinear harmonic growth is seen. Here, a discussion of the code development, the APS SASE FEL, the simulations and results, and, finally, the proposed experimental procedure for verification of such nonlinear harmonic generation at the APS SASE FEL will be given.


Proceedings of the IEEE | 2007

Compact, High-Power Electron Beam Based Terahertz Sources

S. G. Biedron; J.W. Lewellen; S.V. Milton; N. Gopalsami; J.F. Schneider; L. Skubal; Li Yuelin; M. Virgo; G.P. Gallerano; A. Doria; E. Giovenale; G. Messina; I. Spassovsky

Although terahertz (THz) radiation was first observed about 100 years ago, this portion of the electromagnetic spectrum at the boundary between the microwaves and the infrared has been, for a long time, rather poorly explored. This situation changed with the rapid development of coherent THz sources such as solid-state oscillators, quantum cascade lasers, optically pumped solid-state devices, and novel coherent radiator devices. These in turn have stimulated a wide variety of applications from material science to telecommunications, from biology to biomedicine. Recently, there have been two related compact coherent radiation devices invented able to produce up to megawatts of peak THz power by inducing a ballistic bunching effect on the electron beam, forcing the beam to radiate coherently. An introduction to the two systems and the corresponding output photon beam characteristics will be provided.


international free electron laser conference | 2002

Measurements of nonlinear harmonic generation at the Advanced Photon Source's SASE FEL

S. G. Biedron; Roger J. Dejus; Zhirong Huang; S.V. Milton; V. Sajaev; W. Berg; M. Borland; P. Den Hartog; M. Erdmann; William M. Fawley; H.P. Freund; E. Gluskin; Kwang-Je Kim; John W. Lewellen; Y. Li; A. H. Lumpkin; E. R. Moog; A. Nassiri; G. Wiemerslage; B. X. Yang

SASE saturation was recently achieved at the Advanced Photon Sources SASE FEL in the low-energy undulator test line (LEUTL) at 530 nm and 385 nm. The electron beam microbunching becomes more and more prominent until saturation is achieved. This bunching causes nonlinear harmonic emission that extends the usefulness of a SASE system in achieving shorter FEL wavelengths for the same electron beam energy. They have investigated the intensity of the fundamental and second-harmonic undulator radiation as a function of distance along the undulator line and present the experimental results and compare them to numerical simulations. In addition, they have measured the single-shot second harmonic spectra as well as the simultaneous fundamental and second harmonic spectra and present the experimental results.


Optoelectronics '99 - Integrated Optoelectronic Devices | 1999

FEL development at the Advanced Photon Source

S.V. Milton; N. Arnold; C. Benson; S. Berg; W. Berg; S. G. Biedron; Y.-C. Chae; E. Crosbie; G. Decker; B. Deriy; Roger J. Dejus; Pat D. Hartog; R. Dortwegt; M. Erdmann; Zhirong Huang; H. Friedsam; H.P. Freund; J. Galayda; E. Gluskin; G. A. Goeppner; A. Grelick; J. Jones; Y.W. Kang; Kwang J. Kim; Suk Kim; Kim Kinoshita; B. Lill; John W. Lewellen; Alex H. Lumpkin; G. M. Markovich

Construction of a single-pass free-electron laser (FEL) based on the self-amplified spontaneous emission (SASE) mode of operation is nearing completion at the Advanced Photon Source (APS) with initial experiments imminent. The APS SASE FEL is a proof-of-principle fourth-generation light source. As of January 1999 the undulator hall, end-station building, necessary transfer lines, electron and optical diagnostics, injectors, and initial undulators have been constructed and, with the exception of the undulators, installed. All preliminary code development and simulations have also been completed. The undulator hall is now ready to accept first beam for characterization of the output radiation. It is the project goal to push towards full FEL saturation, initially in the visible, but ultimately to UV and VUV, wavelengths.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000

Multi-dimensional free-electron laser simulation codes: a comparison study☆

S. G. Biedron; Y.-C. Chae; Roger J. Dejus; B. Faatz; H.P. Freund; S.V. Milton; H.-D. Nuhn; S. Reiche

A self-amplified spontaneous emission (SASE) free-electron laser (FEL) is under construction at the Advanced Photon Source (APS). Five FEL simulation codes were used in the design phase: GENESIS, GINGER, MEDUSA, RON, and TDA3D. Initial comparisons between each of these independent formulations show good agreement for the parameters of the APS SASE FEL.


Optoelectronics '99 - Integrated Optoelectronic Devices | 1999

3D FEL code for the simulation of a high-gain harmonic generation experiment

S. G. Biedron; H.P. Freund; S.V. Milton

Over the last few years, there has been a growing interest in self-amplified spontaneous emission (SASE) free-electron lasers (FELs) as a means for achieving a fourth-generation light source. In order to correctly and easily simulate the many configurations that have been suggested, such as multi- segmented wigglers and the method of high-gain harmonic generation, we have developed a robust three-dimensional code. The specifics of the code, the comparison to the linear theory as well as future plans will be presented.


international free electron laser conference | 2002

The sensitivity of nonlinear harmonic generation to electron beam quality in free electron lasers

S. G. Biedron; Zhirong Huang; Kwang-Je Kim; S.V. Milton; G. Dattoli; P. L. Ottaviani; A. Renieri; William M. Fawley; H.P. Freund; H.-D. Nuhn

The generation of harmonics through a nonlinear mechanism driven by bunching at the fundamental has sparked interest as a path toward enhancing and extending the usefulness of an x-ray free-electron laser (FEL) facility. The sensitivity of the nonlinear harmonic generation to undulator imperfections, electron beam energy spread, peak current, and emittance is important in an evaluation of the process. Typically, linear instabilities in FELs are characterized by increased sensitivity to both electron beam and undulator quality with increasing harmonic number. However, since the nonlinear harmonic generation mechanism is driven by the growth of the fundamental, the sensitivity of the nonlinear harmonic mechanism is not expected to be significantly greater than that of the fundamental. In this paper, they study the effects of electron beam quality, more specifically, emittance, energy spread, and peak current, on the nonlinear harmonics in a 1.5-{angstrom} FEL, and show that the decline in the harmonic emission roughly follows that of the fundamental.

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S.V. Milton

Argonne National Laboratory

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H.P. Freund

Science Applications International Corporation

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John W. Lewellen

Argonne National Laboratory

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V. Sajaev

Argonne National Laboratory

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Roger J. Dejus

Argonne National Laboratory

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Kwang-Je Kim

Argonne National Laboratory

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M. Borland

Argonne National Laboratory

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E. R. Moog

Argonne National Laboratory

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W. Berg

Argonne National Laboratory

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