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Jean-Yves Raguin

Bio: Jean-Yves Raguin is an academic researcher from Paul Scherrer Institute. The author has contributed to research in topics: Collider & Beam (structure). The author has an hindex of 8, co-authored 11 publications receiving 597 citations.

Papers
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Journal ArticleDOI
Christopher J. Milne, Thomas Schietinger, M. Aiba, Arturo Alarcon, J. Alex, Alexander Anghel, Vladimir Arsov, Carl Beard, Paul Beaud, Simona Bettoni, M. Bopp, H. Brands, Manuel Brönnimann, Ingo Brunnenkant, Marco Calvi, A. Citterio, Paolo Craievich, Marta Csatari Divall, Mark Dällenbach, Michael D’Amico, Andreas Dax, Yunpei Deng, Alexander Dietrich, Roberto Dinapoli, Edwin Divall, Sladana Dordevic, Simon Ebner, Christian Erny, Hansrudolf Fitze, Uwe Flechsig, Rolf Follath, F. Frei, Florian Gärtner, Romain Ganter, Terence Garvey, Zheqiao Geng, I. Gorgisyan, C. Gough, A. Hauff, Christoph P. Hauri, Nicole Hiller, Tadej Humar, Stephan Hunziker, Gerhard Ingold, Rasmus Ischebeck, Markus Janousch, Pavle Juranić, M. Jurcevic, Maik Kaiser, Babak Kalantari, Roger Kalt, B. Keil, Christoph Kittel, Gregor Knopp, W. Koprek, Henrik T. Lemke, Thomas Lippuner, Daniel Llorente Sancho, Florian Löhl, C. Lopez-Cuenca, Fabian Märki, F. Marcellini, G. Marinkovic, Isabelle Martiel, Ralf Menzel, Aldo Mozzanica, Karol Nass, Gian Luca Orlandi, Cigdem Ozkan Loch, Ezequiel Panepucci, Martin Paraliev, Bruce D. Patterson, Bill Pedrini, Marco Pedrozzi, Patrick Pollet, Claude Pradervand, Eduard Prat, Peter Radi, Jean-Yves Raguin, S. Redford, Jens Rehanek, Julien Réhault, Sven Reiche, Matthias Ringele, J. Rittmann, Leonid Rivkin, Albert Romann, Marie Ruat, C. Ruder, Leonardo Sala, Lionel Schebacher, T. Schilcher, Volker Schlott, Thomas J. Schmidt, Bernd Schmitt, Xintian Shi, M. Stadler, L. Stingelin, Werner Sturzenegger, Jakub Szlachetko, D. Thattil, D. Treyer, A. Trisorio, Wolfgang Tron, S. Vetter, Carlo Vicario, Didier Voulot, Meitian Wang, Thierry Zamofing, Christof Zellweger, R. Zennaro, Elke Zimoch, Rafael Abela, Luc Patthey, Hans-Heinrich Braun 
TL;DR: The SwissFEL X-ray Free Electron Laser (XFEL) facility as discussed by the authors started construction at the Paul Scherrer Institute (Villigen, Switzerland) in 2013 and will be ready to accept its first users in 2018 on the Aramis hard Xray branch.
Abstract: The SwissFEL X-ray Free Electron Laser (XFEL) facility started construction at the Paul Scherrer Institute (Villigen, Switzerland) in 2013 and will be ready to accept its first users in 2018 on the Aramis hard X-ray branch. In the following sections we will summarize the various aspects of the project, including the design of the soft and hard X-ray branches of the accelerator, the results of SwissFEL performance simulations, details of the photon beamlines and experimental stations, and our first commissioning results.

295 citations

DOI
12 Aug 2016
TL;DR: The Compact Linear Collider (CLIC) is a multi-teV high-luminosity linear e+e-collider under development as discussed by the authors, which is foreseen to be built and operated in a staged approach with three center-of-mass energy stages ranging from a few hundred GeV up to 3 TeV.
Abstract: The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e+e- collider under development. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in a staged approach with three centre-of-mass energy stages ranging from a few hundred GeV up to 3 TeV. The first stage will focus on precision Standard Model physics, in particular Higgs and top-quark measurements. Subsequent stages will focus on measurements of rare Higgs processes, as well as searches for new physics processes and precision measurements of new states, e.g. states previously discovered at LHC or at CLIC itself. In the 2012 CLIC Conceptual Design Report, a fully optimised 3 TeV collider was presented, while the proposed lower energy stages were not studied to the same level of detail. This report presents an updated baseline staging scenario for CLIC. The scenario is the result of a comprehensive study addressing the performance, cost and power of the CLIC accelerator complex as a function of centre-of-mass energy and it targets optimal physics output based on the current physics landscape. The optimised staging scenario foresees three main centre-of-mass energy stages at 380 GeV, 1.5 TeV and 3 TeV for a full CLIC programme spanning 22 years. For the first stage, an alternative to the CLIC drive beam scheme is presented in which the main linac power is produced using X-band klystrons.

182 citations

Posted ContentDOI
TL;DR: The Compact Linear Collider (CLIC) as mentioned in this paper is a TeV-scale high-luminosity linear $e+e^-$ collider under development at CERN, which uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam.
Abstract: The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. CLIC uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept has been refined using improved software tools. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations and parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25-30 years.

143 citations

Journal ArticleDOI
Eduard Prat1, Rafael Abela1, M. Aiba1, Arturo Alarcon1, J. Alex1, Yunieski Arbelo1, Christopher Arrell1, Vladimir Arsov1, Camila Bacellar2, Camila Bacellar1, Carl Beard1, Paul Beaud1, Simona Bettoni1, Roger Biffiger1, M. Bopp1, Hans-Heinrich Braun1, Marco Calvi1, Ariana Cassar3, Tine Celcer1, Majed Chergui2, Pavel Chevtsov1, Claudio Cirelli1, A. Citterio1, Paolo Craievich1, Marta Csatari Divall1, Andreas Dax1, Micha Dehler1, Yunpei Deng1, Alexander Dietrich1, Philipp Dijkstal1, Philipp Dijkstal4, Roberto Dinapoli1, Sladana Dordevic1, Simon Ebner1, Daniel Engeler1, Christian Erny1, Vincent Esposito1, Vincent Esposito5, Eugenio Ferrari1, Uwe Flechsig1, Rolf Follath1, F. Frei1, Romain Ganter1, Terence Garvey1, Zheqiao Geng1, Alexandre Gobbo1, C. Gough1, A. Hauff1, Christoph P. Hauri1, Nicole Hiller1, Stephan Hunziker1, Martin Huppert1, Gerhard Ingold1, Rasmus Ischebeck1, Markus Janousch1, Philip J. M. Johnson1, Steven L. Johnson4, Steven L. Johnson1, Pavle Juranić1, M. Jurcevic1, Maik Kaiser1, Roger Kalt1, B. Keil1, Daniela Kiselev1, Christoph Kittel1, Gregor Knopp1, W. Koprek1, Michael Laznovsky1, Henrik T. Lemke1, Daniel Llorente Sancho1, Florian Löhl1, Alexander Malyzhenkov1, Giulia F. Mancini1, Giulia F. Mancini2, Roman Mankowsky1, F. Marcellini1, G. Marinkovic1, Isabelle Martiel1, Fabian Märki1, Christopher J. Milne1, Aldo Mozzanica1, Karol Nass1, Gian Luca Orlandi1, Cigdem Ozkan Loch1, Martin Paraliev1, Bruce D. Patterson1, Luc Patthey1, Bill Pedrini1, Marco Pedrozzi1, Claude Pradervand1, Peter Radi1, Jean-Yves Raguin1, S. Redford1, Jens Rehanek1, Sven Reiche1, Leonid Rivkin1, Albert Romann1, Leonardo Sala1, Mathias Sander1, Thomas Schietinger1, T. Schilcher1, Volker Schlott1, Thomas J. Schmidt1, Mike Seidel1, M. Stadler1, L. Stingelin1, C. Svetina1, D. Treyer1, A. Trisorio1, Carlo Vicario1, Didier Voulot1, A. Wrulich1, Serhane Zerdane1, Elke Zimoch1 
TL;DR: In this article, the first lasing results of SwissFEL, a hard X-ray free-electron laser (FEL) that recently came into operation at the Paul Scherrer Institute in Switzerland, were presented.
Abstract: We present the first lasing results of SwissFEL, a hard X-ray free-electron laser (FEL) that recently came into operation at the Paul Scherrer Institute in Switzerland. SwissFEL is a very stable, compact and cost-effective X-ray FEL facility driven by a low-energy and ultra-low-emittance electron beam travelling through short-period undulators. It delivers stable hard X-ray FEL radiation at 1-A wavelength with pulse energies of more than 500 μJ, pulse durations of ~30 fs (root mean square) and spectral bandwidth below the per-mil level. Using special configurations, we have produced pulses shorter than 1 fs and, in a different set-up, broadband radiation with an unprecedented bandwidth of ~2%. The extremely small emittance demonstrated at SwissFEL paves the way for even more compact and affordable hard X-ray FELs, potentially boosting the number of facilities worldwide and thereby expanding the population of the scientific community that has access to X-ray FEL radiation. The first lasing results at SwissFEL, an X-ray free-electron laser, are presented, highlighting the facility’s unique capabilities. A general comparison to other major facilities is also provided.

118 citations

Journal ArticleDOI
TL;DR: The SwissFEL Injector Test Facility operated at the Paul Scherrer Institute between 2010 and 2014, serving as a pilot plant and testbed for the development and realization of Swiss FEL, the X-ray Free-Electron Laser facility under construction at the same institute as mentioned in this paper.
Abstract: The SwissFEL Injector Test Facility operated at the Paul Scherrer Institute between 2010 and 2014, serving as a pilot plant and testbed for the development and realization of SwissFEL, the X-ray Free-Electron Laser facility under construction at the same institute. The test facility consisted of a laser-driven rf electron gun followed by an S-band booster linac, a magnetic bunch compression chicane and a diagnostic section including a transverse deflecting rf cavity. It delivered electron bunches of up to 200 pC charge and up to 250 MeV beam energy at a repetition rate of 10 Hz. The measurements performed at the test facility not only demonstrated the beam parameters required to drive the first stage of an FEL facility, but also led to significant advances in instrumentation technologies, beam characterization methods and the generation, transport and compression of ultra-low-emittance beams. We give a comprehensive overview of the commissioning experience of the principal subsystems and the beam physics measurements performed during the operation of the test facility, including the results of the test of an in-vacuum undulator prototype generating radiation in the vacuum ultraviolet and optical range.

51 citations


Cited by
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Journal ArticleDOI
A. Abada1, Marcello Abbrescia2, Marcello Abbrescia3, Shehu S. AbdusSalam4  +1491 moreInstitutions (239)
TL;DR: In this article, the authors present the second volume of the Future Circular Collider Conceptual Design Report, devoted to the electron-positron collider FCC-ee, and present the accelerator design, performance reach, a staged operation scenario, the underlying technologies, civil engineering, technical infrastructure, and an implementation plan.
Abstract: In response to the 2013 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) study was launched, as an international collaboration hosted by CERN. This study covers a highest-luminosity high-energy lepton collider (FCC-ee) and an energy-frontier hadron collider (FCC-hh), which could, successively, be installed in the same 100 km tunnel. The scientific capabilities of the integrated FCC programme would serve the worldwide community throughout the 21st century. The FCC study also investigates an LHC energy upgrade, using FCC-hh technology. This document constitutes the second volume of the FCC Conceptual Design Report, devoted to the electron-positron collider FCC-ee. After summarizing the physics discovery opportunities, it presents the accelerator design, performance reach, a staged operation scenario, the underlying technologies, civil engineering, technical infrastructure, and an implementation plan. FCC-ee can be built with today’s technology. Most of the FCC-ee infrastructure could be reused for FCC-hh. Combining concepts from past and present lepton colliders and adding a few novel elements, the FCC-ee design promises outstandingly high luminosity. This will make the FCC-ee a unique precision instrument to study the heaviest known particles (Z, W and H bosons and the top quark), offering great direct and indirect sensitivity to new physics.

526 citations

Journal ArticleDOI
Christopher J. Milne, Thomas Schietinger, M. Aiba, Arturo Alarcon, J. Alex, Alexander Anghel, Vladimir Arsov, Carl Beard, Paul Beaud, Simona Bettoni, M. Bopp, H. Brands, Manuel Brönnimann, Ingo Brunnenkant, Marco Calvi, A. Citterio, Paolo Craievich, Marta Csatari Divall, Mark Dällenbach, Michael D’Amico, Andreas Dax, Yunpei Deng, Alexander Dietrich, Roberto Dinapoli, Edwin Divall, Sladana Dordevic, Simon Ebner, Christian Erny, Hansrudolf Fitze, Uwe Flechsig, Rolf Follath, F. Frei, Florian Gärtner, Romain Ganter, Terence Garvey, Zheqiao Geng, I. Gorgisyan, C. Gough, A. Hauff, Christoph P. Hauri, Nicole Hiller, Tadej Humar, Stephan Hunziker, Gerhard Ingold, Rasmus Ischebeck, Markus Janousch, Pavle Juranić, M. Jurcevic, Maik Kaiser, Babak Kalantari, Roger Kalt, B. Keil, Christoph Kittel, Gregor Knopp, W. Koprek, Henrik T. Lemke, Thomas Lippuner, Daniel Llorente Sancho, Florian Löhl, C. Lopez-Cuenca, Fabian Märki, F. Marcellini, G. Marinkovic, Isabelle Martiel, Ralf Menzel, Aldo Mozzanica, Karol Nass, Gian Luca Orlandi, Cigdem Ozkan Loch, Ezequiel Panepucci, Martin Paraliev, Bruce D. Patterson, Bill Pedrini, Marco Pedrozzi, Patrick Pollet, Claude Pradervand, Eduard Prat, Peter Radi, Jean-Yves Raguin, S. Redford, Jens Rehanek, Julien Réhault, Sven Reiche, Matthias Ringele, J. Rittmann, Leonid Rivkin, Albert Romann, Marie Ruat, C. Ruder, Leonardo Sala, Lionel Schebacher, T. Schilcher, Volker Schlott, Thomas J. Schmidt, Bernd Schmitt, Xintian Shi, M. Stadler, L. Stingelin, Werner Sturzenegger, Jakub Szlachetko, D. Thattil, D. Treyer, A. Trisorio, Wolfgang Tron, S. Vetter, Carlo Vicario, Didier Voulot, Meitian Wang, Thierry Zamofing, Christof Zellweger, R. Zennaro, Elke Zimoch, Rafael Abela, Luc Patthey, Hans-Heinrich Braun 
TL;DR: The SwissFEL X-ray Free Electron Laser (XFEL) facility as discussed by the authors started construction at the Paul Scherrer Institute (Villigen, Switzerland) in 2013 and will be ready to accept its first users in 2018 on the Aramis hard Xray branch.
Abstract: The SwissFEL X-ray Free Electron Laser (XFEL) facility started construction at the Paul Scherrer Institute (Villigen, Switzerland) in 2013 and will be ready to accept its first users in 2018 on the Aramis hard X-ray branch. In the following sections we will summarize the various aspects of the project, including the design of the soft and hard X-ray branches of the accelerator, the results of SwissFEL performance simulations, details of the photon beamlines and experimental stations, and our first commissioning results.

295 citations

01 Jan 2015
TL;DR: Density functional theory calculations indicate that new electronic states appear in the O K-edge x-ray absorption spectrum that result from changes in the adsorption site and bond formation between CO and O with a distribution of OC–O bond lengths close to the transition state (TS).
Abstract: Catching CO oxidation Details of the transition state that forms as carbon monoxide (CO) adsorbed on a ruthenium surface is oxidized to CO2 have been revealed by ultrafast excitation and probe methods. Öström et al. initiated the reaction between CO and adsorbed oxygen atoms with laser pulses that rapidly heated the surface and then probed the changes in electronic structure with oxygen x-ray absorption spectroscopy. They observed transition-state configurations that are consistent with density functional theory and a quantum oscillator model. Science, this issue p. 978 Ultrafast x-ray spectroscopy reveals electronic changes that occur during the oxidation of carbon monoxide on a ruthenium surface. Femtosecond x-ray laser pulses are used to probe the carbon monoxide (CO) oxidation reaction on ruthenium (Ru) initiated by an optical laser pulse. On a time scale of a few hundred femtoseconds, the optical laser pulse excites motions of CO and oxygen (O) on the surface, allowing the reactants to collide, and, with a transient close to a picosecond (ps), new electronic states appear in the O K-edge x-ray absorption spectrum. Density functional theory calculations indicate that these result from changes in the adsorption site and bond formation between CO and O with a distribution of OC–O bond lengths close to the transition state (TS). After 1 ps, 10% of the CO populate the TS region, which is consistent with predictions based on a quantum oscillator model.

160 citations

Journal ArticleDOI
Halina Abramowicz1, Angel Abusleme2, K. Afanaciev3, N. Alipour Tehrani4, Csaba Balázs5, Yan Benhammou1, M. Benoit6, B. Bilki7, J. J. Blaising8, Mark Boland9, M. Boronat10, O. Borysov1, I. Božović-Jelisavčić11, M. Buckland12, S. Bugiel13, Philip Burrows14, Tessa Charles5, W. Daniluk15, D. Dannheim4, R. Dasgupta13, M. Demarteau7, M. A. Diaz Gutierrez2, G. Eigen16, K. Elsener4, U. Felzmann9, Miroslaw Firlej13, E. Firu, Tomasz Fiutowski13, Jose Luis Fuster10, Michelle Gabriel17, F. Gaede4, I. García10, V. Ghenescu, Jerry Goldstein18, S. Green19, C. Grefe4, M. Hauschild4, C. M. Hawkes20, D. Hynds4, Marek Idzik13, G. Kačarević11, J. Kalinowski21, S. Kananov1, W. Klempt4, M. Kopec13, Maria Krawczyk21, B. Krupa15, Marcin Kucharczyk15, Szymon Kulis4, Tomas Lastovicka22, T. Lesiak15, Aharon Levy1, I. Levy1, L. Linssen4, Strahinja Lukić11, Alexander Maier4, V. Makarenko3, John Marshall19, V. J. Martin23, K. Mei19, G. Milutinović-Dumbelović11, Jakub Moron13, A. Moszczynski15, D. Moya24, R.M. Münker4, A. Münnich4, Alexandra Neagu, Nikiforos Nikiforou4, Konstantinos Nikolopoulos20, Andreas Nürnberg4, Mila Pandurovic11, B. Pawlik15, E. Perez Codina4, Ivan Peric25, Marko Petrič4, F. Pitters4, Stephane Poss4, T. Preda, D. Protopopescu26, Roger Rassool9, S. Redford4, Jose Repond7, Aidan Robson26, Philipp Roloff4, Eduardo Ros10, O. Rosenblat1, A. Ruiz-Jimeno24, Andre Sailer4, D. Schlatter4, Daniel Schulte4, Nikolai Shumeiko3, Eva Sicking4, Frank Simon17, Rosa Simoniello4, P. Sopicki15, S. Stapnes4, R. Ström4, Jan Strube4, K.P. Świentek13, M. Szalay17, Michal Tesař17, M. A. Thomson19, J. Trenado27, Ulrik I. Uggerhøj28, N. van der Kolk17, E. van der Kraaij16, M. Vicente Barreto Pinto6, Ivan Vila24, M. Vogel Gonzalez2, Marcel Vos10, J. H. Vossebeld12, M. F. Watson20, Nigel Watson20, Matthias Artur Weber4, H. Weerts7, James D. Wells29, L. Weuste17, A. Winter20, T. Wojtoń15, L. Xia7, B. Xu19, A.F. Żarnecki21, L. Zawiejski15, I. S. Zgura 
TL;DR: In this article, the authors present a comprehensive analysis of the Higgs physics reach of the Compact Linear Collider (CLIC) operating at three energy stages: sqrt(s) = 350 GeV, 1.4 TeV and 3 TeV.
Abstract: The Compact Linear Collider (CLIC) is an option for a future e+e- collider operating at centre-of-mass energies up to 3 TeV, providing sensitivity to a wide range of new physics phenomena and precision physics measurements at the energy frontier. This paper is the first comprehensive presentation of the Higgs physics reach of CLIC operating at three energy stages: sqrt(s) = 350 GeV, 1.4 TeV and 3 TeV. The initial stage of operation allows the study of Higgs boson production in Higgsstrahlung (e+e- -> ZH) and WW-fusion (e+e- -> Hnunu), resulting in precise measurements of the production cross sections, the Higgs total decay width Gamma_H, and model-independent determinations of the Higgs couplings. Operation at sqrt(s) > 1 TeV provides high-statistics samples of Higgs bosons produced through WW-fusion, enabling tight constraints on the Higgs boson couplings. Studies of the rarer processes e+e- -> ttH and e+e- -> HHnunu allow measurements of the top Yukawa coupling and the Higgs boson self-coupling. This paper presents detailed studies of the precision achievable with Higgs measurements at CLIC and describes the interpretation of these measurements in a global fit.

146 citations

Journal ArticleDOI
TL;DR: In this article, the time-energy information of ultrashort X-ray free-electron laser pulses generated by the Linac Coherent Light Source is measured with attosecond resolution via angular streaking of neon 1s photoelectrons.
Abstract: The time–energy information of ultrashort X-ray free-electron laser pulses generated by the Linac Coherent Light Source is measured with attosecond resolution via angular streaking of neon 1s photoelectrons. The X-ray pulses promote electrons from the neon core level into an ionization continuum, where they are dressed with the electric field of a circularly polarized infrared laser. This induces characteristic modulations of the resulting photoelectron energy and angular distribution. From these modulations we recover the single-shot attosecond intensity structure and chirp of arbitrary X-ray pulses based on self-amplified spontaneous emission, which have eluded direct measurement so far. We characterize individual attosecond pulses, including their instantaneous frequency, and identify double pulses with well-defined delays and spectral properties, thus paving the way for X-ray pump/X-ray probe attosecond free-electron laser science.

144 citations