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Free-electron lasers (FELs) provide a revolutionary tool for capturing the structure and dynamics of matter in real time at the atomic scale. The size and cost of FELs can be substantially reduced by using laser wakefield acceleration…

Accelerator Physics · Physics 2026-03-31 Hengyuan Xiao , Fei Li , Shuang Liu , Yuchen Jiang , Siqin Ding , Zhi Song , Jianfei Hua , Wei Lu

The variety of applications and especially the unique European XFEL time structure will require adequate instrumentation to be developed to exploit the full potential of the light source. Two-dimensional integrating X-ray detectors with…

Instrumentation and Detectors · Physics 2015-06-11 Andreas Koch , Markus Kuster , Jolanta Sztuk-Dambietz , Monica Turcato

X-ray free-electron lasers (XFELs) are cutting-edge scientific instruments for a wide range of disciplines. Conventionally, the narrow bandwidth is pursued in an XFEL. However, in recent years, the large-bandwidth XFEL operation schemes are…

Accelerator Physics · Physics 2019-02-27 Jiawei Yan , Haixiao Deng

We study vacuum birefringence and x-ray photon scattering in the head-on collision of x-ray free electron and high-intensity laser pulses. Resorting to analytical approximations for the numbers of attainable signal photons, we analyze the…

High Energy Physics - Phenomenology · Physics 2021-08-02 Elena A. Mosman , Felix Karbstein

This paper describes a scheme for pump-probe experiments that can be performed at LCLS and at the European XFEL and determines what additional hardware development will be required to bring these experiments to fruition. It is proposed to…

Accelerator Physics · Physics 2010-01-21 Gianluca Geloni , Vitali Kocharyan , Evgeni Saldin

For the SwissFEL project, an advanced high gradient low emittance gun is under development. Reliable operation with an electric field, preferably above 125 MV/m at a 4 mm gap, in the presence of an UV laser beam, has to be achieved in a…

Accelerator Physics · Physics 2014-11-20 F. Le Pimpec , C. Gough , M. Paraliev , R. Ganter , C. Hauri , S. Ivkovic

There are definite plans for the construction of X-ray free electron lasers (FEL), both at DESY, where the so-called XFEL is part of the design of the electron-positron linear collider TESLA, as well as at SLAC, where the so-called Linac…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Ringwald

X-ray absorption fine structure (XAFS) and x-ray emission spectroscopy (XES) are advanced x-ray spectroscopies that impact a wide range of disciplines. However, unlike the majority of other spectroscopic methods, XAFS and XES are…

In the framework of the Eupraxia Design Study an advanced accelerator facility EUPRAXIA@SPARC_LAB has been proposed to be realized at Frascati (Italy) Laboratories of INFN. Two advanced acceleration schemes will be applied, namely an…

Laser Plasma Acceleration (LPA) [1] is an emerging concept enabling to generate electron beams with high energy, high peak current and small transverse emittance within a very short distance. The use of LPA can be applied to the Free…

Accelerator Physics · Physics 2016-08-03 M Khojoyan , F. Briquez , M. Labat , A. Loulergue , O. Marcouillé , F. Marteau , G. Sharma , M. E. Couprie

Accelerator-based X-ray free-electron lasers (XFELs) are the latest addition to the revolutionary tools of discovery for the 21st century. The two major components of an XFEL are an accelerator-produced electron beam and a magnetic…

The advance in laser plasma acceleration techniques pushes the regime of the resulting accelerated particles to higher energies and intensities. In particular the upcoming experiments with the FLAME laser at LNF will enter the GeV regime…

The assistance of an intense optical laser pulse on electron-positron pair production by the Breit-Wheeler and Schwinger processes in XFEL fields is analyzed. The impact of a laser beam on high-energy photon collisions with XFEL photons…

High Energy Physics - Phenomenology · Physics 2016-04-04 T. Nousch , A. Otto , D. Seipt , B. Kämpfer , A. I. Titov , D. Blaschke , A. D. Panferov , S. A. Smolyansky

In this Technical Design Report (TDR) we describe the LZ detector to be built at the Sanford Underground Research Facility (SURF). The LZ dark matter experiment is designed to achieve sensitivity to a WIMP-nucleon spin-independent cross…

Instrumentation and Detectors · Physics 2017-03-29 B. J. Mount , S. Hans , R. Rosero , M. Yeh , C. Chan , R. J. Gaitskell , D. Q. Huang , J. Makkinje , D. C. Malling , M. Pangilinan , C. A. Rhyne , W. C. Taylor , J. R. Verbus , Y. D. Kim , H. S. Lee , J. Lee , D. S. Leonard , J. Li , J. Belle , A. Cottle , W. H. Lippincott , D. J. Markley , T. J. Martin , M. Sarychev , T. E. Tope , M. Utes , R. Wang , I. Young , H. M. Araújo , A. J. Bailey , D. Bauer , D. Colling , A. Currie , S. Fayer , F. Froborg , S. Greenwood , W. G. Jones , V. Kasey , M. Khaleeq , I. Olcina , B. López Paredes , A. Richards , T. J. Sumner , A. Tomás , A. Vacheret , P. Brás , A. Lindote , M. I. Lopes , F. Neves , J. P. Rodrigues , C. Silva , V. N. Solovov , M. J. Barry , A. Cole , A. Dobi , W. R. Edwards , C. H. Faham , S. Fiorucci , N. J. Gantos , V. M. Gehman , M. G. D. Gilchriese , K. Hanzel , M. D. Hoff , K. Kamdin , K. T. Lesko , C. T. McConnell , K. O'Sullivan , K. C. Oliver-Mallory , S. J. Patton , J. S. Saba , P. Sorensen , K. J. Thomas , C. E. Tull , W. L. Waldron , M. S. Witherell , A. Bernstein , K. Kazkaz , J. Xu , D. Yu. Akimov , A. I. Bolozdynya , A. V. Khromov , A. M. Konovalov , A. V. Kumpan , V. V. Sosnovtsev , C. E. Dahl , D. Temples , M. C. Carmona-Benitez , L. de Viveiros , D. S. Akerib , H. Auyeung , T. P. Biesiadzinski , M. Breidenbach , R. Bramante , R. Conley , W. W. Craddock , A. Fan , A. Hau , C. M. Ignarra , W. Ji , H. J. Krebs , R. Linehan , C. Lee , S. Luitz , E. Mizrachi , M. E. Monzani , F. G. O'Neill , S. Pierson , M. Racine , B. N. Ratcliff , G. W. Shutt , T. A. Shutt , K. Skarpaas , K. Stifter , W. H. To , J. Va'vra , T. J. Whitis , W. J. Wisniewski , X. Bai , R. Bunker , R. Coughlen , C. Hjemfelt , R. Leonard , E. H. Miller , E. Morrison , J. Reichenbacher , R. W. Schnee , M. R. Stark , K. Sundarnath , D. R. Tiedt , M. Timalsina , P. Bauer , B. Carlson , M. Horn , M. Johnson , J. Keefner , C. Maupin , D. J. Taylor , S. Balashov , P. Ford , V. Francis , E. Holtom , A. Khazov , A. Kaboth , P. Majewski , J. A. Nikkel , J. O'Dell , R. M. Preece , M. G. D. van der Grinten , S. D. Worm , R. L. Mannino , T. M. Stiegler , P. A. Terman , R. C. Webb , C. Levy , J. Mock , M. Szydagis , J. K. Busenitz , M. Elnimr , J. Y-K. Hor , Y. Meng , A. Piepke , I. Stancu , L. Kreczko , B. Krikler , B. Penning , E. P. Bernard , R. G. Jacobsen , D. N. McKinsey , R. Watson , J. E. Cutter , S. El-Jurf , R. M. Gerhard , D. Hemer , S. Hillbrand , B. Holbrook , B. G. Lenardo , A. G. Manalaysay , J. A. Morad , S. Stephenson , J. A. Thomson , M. Tripathi , S. Uvarov , S. J. Haselschwardt , S. Kyre , C. Nehrkorn , H. N. Nelson , M. Solmaz , D. T. White , M. Cascella , J. E. Y. Dobson , C. Ghag , X. Liu , L. Manenti , L. Reichhart , S. Shaw , U. Utku , P. Beltrame , T. J. R. Davison , M. F. Marzioni , A. St. J. Murphy , A. Nilima , B. Boxer , S. Burdin , A. Greenall , S. Powell , H. J. Rose , P. Sutcliffe , J. Balajthy , T. K. Edberg , C. R. Hall , J. S. Silk , S. Hertel , C. W. Akerlof , M. Arthurs , W. Lorenzon , K. Pushkin , M. Schubnell , K. E. Boast , C. Carels , T. Fruth , H. Kraus , F. -T. Liao , J. Lin , P. R. Scovell , E. Druszkiewicz , D. Khaitan , M. Koyuncu , W. Skulski , F. L. H. Wolfs , J. Yin , E. V. Korolkova , V. A. Kudryavtsev , P. Rossiter , D. Woodward , A. A. Chiller , C. Chiller , D. -M. Mei , L. Wang , W. -Z. Wei , M. While , C. Zhang , S. K. Alsum , T. Benson , D. L. Carlsmith , J. J. Cherwinka , S. Dasu , G. Gregerson , B. Gomber , A. Pagac , K. J. Palladino , C. O. Vuosalo , Q. Xiao , J. H. Buckley , V. V. Bugaev , M. A. Olevitch , E. M. Boulton , W. T. Emmet , T. W. Hurteau , N. A. Larsen , E. K. Pease , B. P. Tennyson , L. Tvrznikova

The output SASE characteristics of the baseline European XFEL, recently used in the TDRs of scientific instruments and X-ray optics, have been previously optimized assuming uniform undulators without considering the potential of undulator…

The lack of available table-top extreme ultraviolet (XUV) sources with high enough fluxes and coherence properties have limited the availability of nonlinear XUV and x-ray spectroscopies to free electron lasers (FEL). Here, we demonstrate…

The European X-ray Free Electron Laser (XFEL.EU) is currently being commissioned in Schenefeld, Germany. From 2017 onwards it will provide spatially coherent X-rays of energies between 0.25\,keV and 25\,keV with a unique timing structure.…

Instrumentation and Detectors · Physics 2016-12-13 Friederike Januschek , Ivana Klackova , Nord Andresen , Peter Denes , Steffen Hauf , John Joseph , Markus Kuster , Craig Tindall

DarkSHINE is a newly proposed fixed-target experiment initiative to search for the invisible decay of Dark Photon via missing energy/momentum signatures, based on the high repetition rate electron beam to be deployed/delivered by the…

Motivated by recent experimental initiatives, such as at the Helmholtz International Beamline for Extreme Fields (HIBEF) at the European X-ray Free Electron Laser (XFEL), we calculate the birefringent scattering of x-rays at the combined…

This paper discusses the potential for enhancing the capabilities of the European FEL in the soft X-ray regime. A high longitudinal coherence will be the key to such performance upgrade. In order to reach this goal we study a very compact…

Accelerator Physics · Physics 2012-02-24 Gianluca Geloni , Vitaly Kocharyan , Evgeni Saldin
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