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Edwin Divall

Bio: Edwin Divall is an academic researcher from Paul Scherrer Institute. The author has contributed to research in topics: Ultrashort pulse & Diffraction. The author has an hindex of 4, co-authored 8 publications receiving 314 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

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

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 test bed 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 test bed 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 ultralow-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.

43 citations

Journal ArticleDOI
TL;DR: In this article, a diamond phase grating in an X-ray beam path creates a periodic excitation pattern on a sample via the Talbot effect, which is then probed by an optical pulse.
Abstract: Optical-domain transient grating (TG) spectroscopy is a versatile background-free four-wave-mixing technique that is used to probe vibrational, magnetic and electronic degrees of freedom in the time domain1. The newly developed coherent X-ray free-electron laser sources allow its extension to the X-ray regime. X-rays offer multiple advantages for TG: their large penetration depth allows probing the bulk properties of materials, their element specificity can address core excited states, and their short wavelengths create excitation gratings with unprecedented momentum transfer and spatial resolution. Here, we demonstrate TG excitation in the hard X-ray range at 7.1 keV. In bismuth germanate (BGO), the non-resonant TG excitation generates coherent optical phonons detected as a function of time by diffraction of an optical probe pulse. This experiment demonstrates the ability to probe bulk properties of materials and paves the way for ultrafast coherent four-wave-mixing techniques using X-ray probes and involving nanoscale TG spatial periods. A four-wave mixing technique is developed in the hard X-ray range. A diamond phase grating in an X-ray beam path creates a periodic excitation pattern on a sample via the Talbot effect. The response of the periodic excitation is probed by an optical pulse.

16 citations

Journal ArticleDOI
TL;DR: In this paper, the authors demonstrate the ability to probe bulk properties of materials and paves the way for ultrafast coherent four-wave-mixing techniques using X-ray probes and involving nanoscale TG spatial periods.
Abstract: Optical-domain Transient Grating (TG) spectroscopy is a versatile background-free four-wave-mixing technique used to probe vibrational, magnetic and electronic degrees of freedom in the time domain. The newly developed coherent X-ray Free Electron Laser sources allow its extension to the X-ray regime. Xrays offer multiple advantages for TG: their large penetration depth allows probing the bulk properties of materials, their element-specificity can address core-excited states, and their short wavelengths create excitation gratings with unprecedented momentum transfer and spatial resolution. We demonstrate for the first time TG excitation in the hard X-ray range at 7.1 keV. In Bismuth Germanate (BGO), the nonresonant TG excitation generates coherent optical phonons detected as a function of time by diffraction of an optical probe pulse. This experiment demonstrates the ability to probe bulk properties of materials and paves the way for ultrafast coherent four-wave-mixing techniques using X-ray probes and involving nanoscale TG spatial periods.

16 citations


Cited by
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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

01 Jan 2013
TL;DR: In this paper, a simple experiment demonstrating that room-temperature thermal transport in Si significantly deviates from the diffusion model already at micron distances is presented, indicating a transition from the diffusive to the ballistic transport regime for the low-frequency part of the phonon spectrum.
Abstract: The "textbook" phonon mean free path of heat carrying phonons in silicon at room temperature is ∼40 nm. However, a large contribution to the thermal conductivity comes from low-frequency phonons with much longer mean free paths. We present a simple experiment demonstrating that room-temperature thermal transport in Si significantly deviates from the diffusion model already at micron distances. Absorption of crossed laser pulses in a freestanding silicon membrane sets up a sinusoidal temperature profile that is monitored via diffraction of a probe laser beam. By changing the period of the thermal grating we vary the heat transport distance within the range ∼1-10 μm. At small distances, we observe a reduction in the effective thermal conductivity indicating a transition from the diffusive to the ballistic transport regime for the low-frequency part of the phonon spectrum.

285 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

Journal ArticleDOI
Eduard Prat1, Rafael Abela1, M. Aiba1, Arturo Alarcon1, J. Alex1, Yunieski Arbelo1, Christopher Arrell1, Vladimir Arsov1, Camila Bacellar1, Camila Bacellar2, 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 Dijkstal4, Philipp Dijkstal1, 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. Johnson1, Steven L. Johnson4, 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
20 May 2020-Nature
TL;DR: Crystallographic ‘snapshots’ taken at intervals of femtoseconds to milliseconds after activation show how a light-activated sodium pump carries sodium ions across the cell membrane and provide direct molecular insight into the dynamics of active cation transport across biological membranes.
Abstract: Light-driven sodium pumps actively transport small cations across cellular membranes1. These pumps are used by microorganisms to convert light into membrane potential and have become useful optogenetic tools with applications in neuroscience. Although the resting state structures of the prototypical sodium pump Krokinobacter eikastus rhodopsin 2 (KR2) have been solved2,3, it is unclear how structural alterations over time allow sodium to be translocated against a concentration gradient. Here, using the Swiss X-ray Free Electron Laser4, we have collected serial crystallographic data at ten pump-probe delays from femtoseconds to milliseconds. High-resolution structural snapshots throughout the KR2 photocycle show how retinal isomerization is completed on the femtosecond timescale and changes the local structure of the binding pocket in the early nanoseconds. Subsequent rearrangements and deprotonation of the retinal Schiff base open an electrostatic gate in microseconds. Structural and spectroscopic data, in combination with quantum chemical calculations, indicate that a sodium ion binds transiently close to the retinal within one millisecond. In the last structural intermediate, at 20 milliseconds after activation, we identified a potential second sodium-binding site close to the extracellular exit. These results provide direct molecular insight into the dynamics of active cation transport across biological membranes.

94 citations