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Dive into the research topics where H. Loos is active.

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Featured researches published by H. Loos.


Nature Communications | 2014

Few-femtosecond time-resolved measurements of X-ray free-electron lasers

C. Behrens; F.-J. Decker; Y. Ding; V. A. Dolgashev; J. Frisch; Zhirong Huang; P. Krejcik; H. Loos; Alberto Lutman; Timothy Maxwell; J. J. Turner; J. Wang; M.-H. Wang; J. Welch; J. Wu

X-ray free-electron lasers, with pulse durations ranging from a few to several hundred femtoseconds, are uniquely suited for studying atomic, molecular, chemical and biological systems. Characterizing the temporal profiles of these femtosecond X-ray pulses that vary from shot to shot is not only challenging but also important for data interpretation. Here we report the time-resolved measurements of X-ray free-electron lasers by using an X-band radiofrequency transverse deflector at the Linac Coherent Light Source. We demonstrate this method to be a simple, non-invasive technique with a large dynamic range for single-shot electron and X-ray temporal characterization. A resolution of less than 1 fs root mean square has been achieved for soft X-ray pulses. The lasing evolution along the undulator has been studied with the electron trapping being observed as the X-ray peak power approaches 100 GW.


Nature Communications | 2015

High-intensity double-pulse X-ray free-electron laser.

Agostino Marinelli; Daniel Ratner; Alberto Lutman; J. J. Turner; J. Welch; F.-J. Decker; H. Loos; C. Behrens; S. Gilevich; A. Miahnahri; Sharon Vetter; Timothy Maxwell; Y. Ding; Ryan Coffee; Soichi Wakatsuki; Zhirong Huang

The X-ray free-electron laser has opened a new era for photon science, improving the X-ray brightness by ten orders of magnitude over previously available sources. Similar to an optical laser, the spectral and temporal structure of the radiation pulses can be tailored to the specific needs of many experiments by accurately manipulating the lasing medium, that is, the electron beam. Here we report the generation of mJ-level two-colour hard X-ray pulses of few femtoseconds duration with an XFEL driven by twin electron bunches at the Linac Coherent Light Source. This performance represents an improvement of over an order of magnitude in peak power over state-of-the-art two-colour XFELs. The unprecedented intensity and temporal coherence of this new two-colour X-ray free-electron laser enable an entirely new set of scientific applications, ranging from X-ray pump/X-ray probe experiments to the imaging of complex biological samples with multiple wavelength anomalous dispersion.


Journal of Applied Physics | 2009

Terahertz laser modulation of electron beams

J. G. Neumann; R. Fiorito; P. G. O’Shea; H. Loos; B. Sheehy; Y. Shen; Z. Wu

The study of modulated electron beams is important because they can be used to produce coherent radiation, but the modulations can cause unwanted instabilities in some devices. Specifically, in a free electron laser, proper prebunching at the desired emission frequency can enhance performance, while bunching resulting from instabilities and bunch compression schemes can degrade performance. In a photoinjector accelerator, tailoring the shape of the drive laser pulse could be used as a technique to either enhance or mitigate the effect of these modulations. This work explores the possibility of creating deeply modulated electron beams at the photocathode by using a modified drive laser designed to produce multiple subpicosecond pulses repeated at terahertz frequencies. Longitudinal space charge forces can strongly influence the evolution of modulations by converting density modulations to energy modulations. Experiments at the Source Development Laboratory electron accelerator at Brookhaven National Laboratory and PARMELA simulations are employed to explore the dynamics of electron beams with varying charge and with varying initial modulation. Finally, terahertz light generated by a transition radiator is used to confirm the structure of the electron beam.


Physical Review Special Topics-accelerators and Beams | 2003

Subpicosecond compression by velocity bunching in a photoinjector

Ph Piot; L. Carr; W. Graves; H. Loos

We present an experimental evidence of a bunch compression scheme that uses a traveling wave accelerating structure as a compressor. The bunch length issued from a laser-driven radio-frequency electron source was compressed by a factor


international free electron laser conference | 2003

Electron beam modulation using a laser-driven photocathode

J. Neumann; P.G. O'Shea; D. Demske; W.S. Graves; B. Sheehy; H. Loos; G. L. Carr

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ieee particle accelerator conference | 2007

Initial commissioning experience with the LCLS injector

R. Akre; J. Castro; Y. Ding; D. Dowell; P. Emma; J. Frisch; S. Gilevich; G. Hays; Z. Hering; R.I. Huang; P. Krejcik; C. Limborg-Deprey; H. Loos; A. Miahnahri; C. Rivetta; M. Saleski; J.F. Schmerge; D. Schultz; J. J. Turner; J. Welch; W. White; J. Wu; L. Froelich; T. Limberg; E. Prat

using an


ieee particle accelerator conference | 2007

LCLS injector drive laser

D. Dowell; J. Castro; P. Emma; J. Frisch; S. Gilevich; G. Hays; P. Hering; C. Limborg-Deprey; H. Loos; A. Miahnahri; W. White

S


ieee particle accelerator conference | 2007

Relative bunch length monitor for the Linac Coherent Light Source (LCLS) using coherent edge radiation

H. Loos; T. Borden; P. Emma; J. Frisch; J. Wu

-band traveling wave structure located immediately downstream from the electron source. Experimental data are found to be in good agreement with particle tracking simulations.


Proceedings of the 2005 Particle Accelerator Conference | 2005

Simulations and Experiments of Electron Beams Pre-Modulated at the Photocathode

J. Neumann; R. Fiorito; P.G. O'Shea; G. L. Carr; W. Graves; H. Loos; T. Shaftan; B. Sheehy; Y. Shen; Z. Wu

Coherent synchrotron radiation may lead to a microwave instability on an electron bunch at wavelengths much smaller than the bunch length. It is possible that ripples (prebunching) on the electron bunch distribution may seed this instability. We report on research exploring this effect using a longitudinally modulated drive laser to generate a modulated electron beam. Our first step is to develop simulations that will help us study the beam generation process using PARMELA. Preliminary experiments on laser beam and electron beam modulation, conducted at the Source Development Laboratory at the National Synchrotron Light Source, show modulation at frequencies in the terahertz regime is attainable. Longitudinal prebunching may enhance the performance of FEL or other radiative devices in the terahertz regime. Alternatively, longitudinal control over the electron beam might be an effective method of suppressing coherent synchrotron radiation instabilities that cause beam break-up.


Proceedings of the 2005 Particle Accelerator Conference | 2005

Temporal E-Beam Shaping in an S-Band Accelerator

H. Loos; D. Dowell; S. Gilevich; C. Limborg-Deprey; Y. Shen; J. Murphy; B. Sheehy; T. Tsang; X. Wang; Z. Wu; L. Serafini; M. Boscolo; M. Ferrario; M. Petrarca; C. Vicario

The linac coherent light source (LCLS) is a SASE X- ray free-electron laser (FEL) project presently under construction at SLAC [1]. The injector section, from drive-laser and RF photocathode gun through first bunch compressor chicane, was installed in fall 2006. Initial system commissioning with an electron beam is taking place during the spring and summer of 2007. The second phase of construction, including second bunch compressor and full linac, will begin later, in the fall of 2007. We report here on experience gained during the first phase of machine commissioning, including RF photocathode gun, linac booster section, S-band and X-band RF systems, first bunch compressor, and the various beam diagnostics.

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Y. Ding

SLAC National Accelerator Laboratory

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B. Sheehy

Brookhaven National Laboratory

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J. Wu

SLAC National Accelerator Laboratory

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T. Shaftan

Brookhaven National Laboratory

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D. Dowell

SLAC National Accelerator Laboratory

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Daniel Ratner

SLAC National Accelerator Laboratory

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W. Graves

Massachusetts Institute of Technology

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S. Gilevich

SLAC National Accelerator Laboratory

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