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1
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Orlandi GL. Absolute and non-invasive determination of the electron bunch length in a free electron laser using a bunch compressor monitor. Sci Rep 2024; 14:6319. [PMID: 38491040 PMCID: PMC10943132 DOI: 10.1038/s41598-024-56586-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/02/2023] [Accepted: 03/08/2024] [Indexed: 03/18/2024] Open
Abstract
In a linac driven Free Electron Laser (FEL), the shot-to-shot and non-invasive monitoring of the electron bunch length is normally ensured by Bunch Compressor Monitors (BCMs). The bunch-length dependent signal of a BCM results from the detection and integration-over a given frequency band-of the temporal coherent enhancement of the radiation spectral energy emitted by the electron beam while experiencing a longitudinal compression. In this work, we present a method that permits to express the relative variation of the bunch length as a function of the relative statistical fluctuations of the BCM and charge signals. Furthermore, in the case of a BCM equipped with two detectors simultaneously operating in two distinct wavelength bands, the method permits an absolute determination of the electron bunch length. The proposed method is beneficial to a FEL. Thanks to it, the machine compression feedback can be tuned against the absolute measurement of the bunch length rather than a bunch-length dependent signal. In a CW-superconducting-linac driven FEL, it can offer the precious opportunity to implement a fully non-invasive and absolute diagnostics of the bunch length.
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Affiliation(s)
- Gian Luca Orlandi
- Paul Scherrer Institut, Forschungsstrasse 111, Villigen PSI, 5232, Switzerland.
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Carulla M, Barten R, Baruffaldi F, Bergamaschi A, Borghi G, Boscardin M, Brückner M, Butcher TA, Centis Vignali M, Dinapoli R, Ebner S, Ficorella F, Fröjdh E, Greiffenberg D, Hammad Ali O, Hasanaj S, Heymes J, Hinger V, King T, Kozlowski P, Lopez Cuenca C, Mezza D, Moustakas K, Mozzanica A, Paternoster G, Paton KA, Ronchin S, Ruder C, Schmitt B, Sieberer P, Thattil D, Vogelsang K, Xie X, Zhang J. Quantum Efficiency Measurement and Modeling of Silicon Sensors Optimized for Soft X-ray Detection. SENSORS (BASEL, SWITZERLAND) 2024; 24:942. [PMID: 38339659 PMCID: PMC10856868 DOI: 10.3390/s24030942] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/30/2023] [Revised: 01/19/2024] [Accepted: 01/22/2024] [Indexed: 02/12/2024]
Abstract
Hybrid pixel detectors have become indispensable at synchrotron and X-ray free-electron laser facilities thanks to their large dynamic range, high frame rate, low noise, and large area. However, at energies below 3 keV, the detector performance is often limited because of the poor quantum efficiency of the sensor and the difficulty in achieving single-photon resolution due to the low signal-to-noise ratio. In this paper, we address the quantum efficiency of silicon sensors by refining the design of the entrance window, mainly by passivating the silicon surface and optimizing the dopant profile of the n+ region. We present the measurement of the quantum efficiency in the soft X-ray energy range for silicon sensors with several process variations in the fabrication of planar sensors with thin entrance windows. The quantum efficiency for 250 eV photons is increased from almost 0.5% for a standard sensor to up to 62% as a consequence of these developments, comparable to the quantum efficiency of backside-illuminated scientific CMOS sensors. Finally, we discuss the influence of the various process parameters on quantum efficiency and present a strategy for further improvement.
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Affiliation(s)
- Maria Carulla
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Rebecca Barten
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Filippo Baruffaldi
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Anna Bergamaschi
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Giacomo Borghi
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Maurizio Boscardin
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Martin Brückner
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Tim A. Butcher
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Matteo Centis Vignali
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Roberto Dinapoli
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Simon Ebner
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Francesco Ficorella
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Erik Fröjdh
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Dominic Greiffenberg
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Omar Hammad Ali
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Shqipe Hasanaj
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Julian Heymes
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Viktoria Hinger
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Thomas King
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Pawel Kozlowski
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Carlos Lopez Cuenca
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Davide Mezza
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Konstantinos Moustakas
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Aldo Mozzanica
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Giovanni Paternoster
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Kirsty A. Paton
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Sabina Ronchin
- Fondazione Bruno Kessler, Via Sommarive 18, 38126 Povo, Italy; (G.B.); (M.B.); (M.C.V.); (F.F.); (O.H.A.); (G.P.); (S.R.)
| | - Christian Ruder
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Bernd Schmitt
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Patrick Sieberer
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Dhanya Thattil
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Konrad Vogelsang
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Xiangyu Xie
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
| | - Jiaguo Zhang
- Paul Scherrer Institut, Forschungsstrasse 111, 5232 Villigen, Switzerland (F.B.); (A.B.); (T.A.B.); (R.D.); (E.F.); (D.G.); (J.H.); (V.H.); (D.M.); (K.M.); (A.M.); (K.A.P.); (B.S.); (P.S.); (X.X.); (J.Z.)
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3
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Hu K, Zhu Y, Wu C, Li Q, Xu Z, Wang Q, Zhang W, Yang C. Spatiotemporal response of concave VLS grating to ultra-short X-ray pulses. OPTICS EXPRESS 2023; 31:31969-31981. [PMID: 37859010 DOI: 10.1364/oe.501464] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/24/2023] [Accepted: 09/04/2023] [Indexed: 10/21/2023]
Abstract
In soft X-ray free-electron laser (FEL) beamlines, variable-line-spacing (VLS) gratings are often used as dispersive components of monochromators and spectrometers due to their combined dispersion and focusing properties. X-ray FEL pulses passing through the VLS grating can result in not only transverse focusing but also spatiotemporal coupling effects, such as pulse front tilt, pulse front rotation, and pulse stretching. In this paper, we present a theoretical study of the spatiotemporal response of concave VLS gratings to ultra-short X-ray pulses. The theoretical analysis indicates that the tilt angle of the non-zero diffraction orders varies with the propagation distance, and disappears at the focus, where the focal lengths and pulse stretching differ for different diffraction orders. The model demonstrates the pulse duration after the concave VLS grating is the convolution of the initial pulse duration and the stretching term induced by dispersion, while the beam size at the focus in x dimension is the convolution of the geometric scaling beam size and the dispersion term. This work provides a mathematical explanation for the spatiotemporal response of concave VLS grating to ultra-short X-ray pulses and offers valuable insights into the design of FEL grating monochromators, spectrometers, pulse compressors, and pulse stretchers.
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4
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Prat E, Al Haddad A, Arrell C, Augustin S, Boll M, Bostedt C, Calvi M, Cavalieri AL, Craievich P, Dax A, Dijkstal P, Ferrari E, Follath R, Ganter R, Geng Z, Hiller N, Huppert M, Ischebeck R, Juranić P, Kittel C, Knopp G, Malyzhenkov A, Marcellini F, Neppl S, Reiche S, Sammut N, Schietinger T, Schmidt T, Schnorr K, Trisorio A, Vicario C, Voulot D, Wang G, Weilbach T. An X-ray free-electron laser with a highly configurable undulator and integrated chicanes for tailored pulse properties. Nat Commun 2023; 14:5069. [PMID: 37604879 PMCID: PMC10442322 DOI: 10.1038/s41467-023-40759-z] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/14/2023] [Accepted: 08/09/2023] [Indexed: 08/23/2023] Open
Abstract
X-ray free-electron lasers (FELs) are state-of-the-art scientific tools capable to study matter on the scale of atomic processes. Since the initial operation of X-ray FELs more than a decade ago, several facilities with upgraded performance have been put in operation. Here we present the first lasing results of Athos, the soft X-ray FEL beamline of SwissFEL at the Paul Scherrer Institute in Switzerland. Athos features an undulator layout based on short APPLE-X modules providing full polarisation control, interleaved with small magnetic chicanes. This versatile configuration allows for many operational modes, giving control over many FEL properties. We show, for example, a 35% reduction of the required undulator length to achieve FEL saturation with respect to standard undulator configurations. We also demonstrate the generation of more powerful pulses than the ones obtained in typical undulators. Athos represents a fundamental step forward in the design of FEL facilities, creating opportunities in FEL-based sciences.
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Affiliation(s)
- Eduard Prat
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland.
| | | | | | - Sven Augustin
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Marco Boll
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Christoph Bostedt
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
- Ecole Polytechnique Fédérale de Lausanne, CH-1015, Lausanne, Switzerland
| | - Marco Calvi
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Adrian L Cavalieri
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
- Institute of Applied Physics, University of Bern, CH-3012, Bern, Switzerland
| | | | - Andreas Dax
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | | | - Eugenio Ferrari
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
- Deutsches Elektronen-Synchrotron, D-22607, Hamburg, Germany
| | - Rolf Follath
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Romain Ganter
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Zheqiao Geng
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Nicole Hiller
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Martin Huppert
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | | | - Pavle Juranić
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Christoph Kittel
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
- University of Malta, MSD2080, Msida, Malta
| | - Gregor Knopp
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Alexander Malyzhenkov
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
- CERN, CH-1211, Geneva 23, Switzerland
| | | | - Stefan Neppl
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Sven Reiche
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | | | | | - Thomas Schmidt
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | | | | | - Carlo Vicario
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Didier Voulot
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
| | - Guanglei Wang
- Paul Scherrer Institut, CH-5232, Villigen PSI, Switzerland
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Calvi M, Liang X, Ferrari E, Alarcon A, Prat E, Reiche S, Schmidt T, Voulot D, Zhang K, Ganter R. Versatile modulators for laser-based FEL seeding at SwissFEL. JOURNAL OF SYNCHROTRON RADIATION 2023; 30:276-283. [PMID: 36891841 PMCID: PMC10000804 DOI: 10.1107/s1600577522012073] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 10/14/2022] [Accepted: 12/22/2022] [Indexed: 06/18/2023]
Abstract
The Paul Scherrer Institute is implementing laser-based seeding in the soft X-ray beamline (Athos) of its free-electron laser, SwissFEL, to enhance the temporal and spectral properties of the delivered photon pulses. This technique requires, among other components, two identical modulators for coupling the electron beam with an external laser with a wavelength range between 260 and 1600 nm. The design, magnetic measurements results, alignment, operation and also details of the novel and exotic magnetic configuration of the prototype are described.
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Affiliation(s)
- Marco Calvi
- Photon Science Division, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Xiaoyang Liang
- Photon Science Division, Paul Scherrer Institute, 5232 Villigen, Switzerland
- Institute of Biomedical Engineering, ETH Zürich, 8092 Zürich, Switzerland
| | - Eugenio Ferrari
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
- M Division, Deutsches Elektronen-Synchrotron, Notkestraße 85, 22607 Hamburg, Germany
| | - Arturo Alarcon
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Eduard Prat
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Sven Reiche
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Thomas Schmidt
- Photon Science Division, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Didier Voulot
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Kai Zhang
- Photon Science Division, Paul Scherrer Institute, 5232 Villigen, Switzerland
| | - Romain Ganter
- Large Research Facility, Paul Scherrer Institute, 5232 Villigen, Switzerland
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6
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Nolting F, Bostedt C, Schietinger T, Braun H. The Swiss Light Source and SwissFEL at the Paul Scherrer Institute. EUROPEAN PHYSICAL JOURNAL PLUS 2023; 138:126. [PMID: 36779165 PMCID: PMC9900202 DOI: 10.1140/epjp/s13360-023-03721-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 09/30/2022] [Accepted: 01/19/2023] [Indexed: 06/18/2023]
Abstract
At the Paul Scherrer Institute, two electron accelerator-based photon sources are in operation, namely a synchrotron source, the swiss light source (SLS), and an X-ray free-electron laser, SwissFEL. SLS has been operational since 2001 and SwissFEL since 2017. In this time, unique and world-leading scientific programs and methods have developed from the SLS and the SwissFEL in fields as diverse as macromolecular biology, chemical and physical sciences, imaging, and the electronic structure and behaviour of novel and complex materials. To continue the success, a major upgrade of SLS, the SLS2.0 project, is ongoing and at SwissFEL further endstations are under construction.
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Affiliation(s)
| | | | | | - Hans Braun
- Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland
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Abstract
Major advances in X-ray sources including the development of circularly polarized and orbital angular momentum pulses make it possible to probe matter chirality at unprecedented energy regimes and with Ångström and femtosecond spatiotemporal resolutions. We survey the theory of stationary and time-resolved nonlinear chiral measurements that can be carried out in the X-ray regime using tabletop X-ray sources or large scale (XFEL, synchrotron) facilities. A variety of possible signals and their information content are discussed.
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Affiliation(s)
- Jérémy R Rouxel
- Université de Lyon, UJM-Saint-Etienne, CNRS, IOGS, Laboratoire Hubert Curien UMR 5516, Saint-Etienne F-42023, France
| | - Shaul Mukamel
- Department of Chemistry and Physics & Astronomy, University of California, Irvine, California 92697-2025, United States
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Rashid MH, Borca CN, Xto JM, Huthwelker T. X-Ray absorption spectroscopy on airborne aerosols. ENVIRONMENTAL SCIENCE: ATMOSPHERES 2022; 2:1338-1350. [PMID: 36561554 PMCID: PMC9648630 DOI: 10.1039/d2ea00016d] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 03/07/2022] [Accepted: 09/26/2022] [Indexed: 11/07/2022]
Abstract
Here we demonstrate a method for performing X-ray absorption spectroscopy (XAS) on airborne aerosols. XAS provides unique insight into elemental composition, chemical and phase state, local coordination and electronic structure of both crystalline and amorphous matter. The aerosol is generated from different salt solutions using a commercial atomizer and dried using a diffusion drier. Embedded in a carrier gas, the aerosol is guided into the experimental chamber for XAS analysis. Typical particle sizes range from some 10 to a few 100 nm. Inside the chamber the aerosol bearing gas is then confined into a region of about 1-2 cm3 in size, by a pure flow of helium, generating a stable free-flowing stream of aerosol. It is hit by a monochromatic X-ray beam, and the emitted fluorescent light is used for spectroscopic analysis. Using an aerosol generated from CaCl2, KCl, and (NH4)2SO4 salt solutions, we demonstrate the functionality of the system in studying environmentally relevant systems. In addition, we show that the detection limits are sufficient to also observe subtle spectroscopic signatures in XAS spectra with integration times of about 1-2 hours using a bright undulator beamline. This novel setup opens new research opportunities for studying the nucleation of new phases in multicomponent aerosol systems in situ, and for investigating (photo-) chemical reactions on airborne matter, as relevant to both atmospheric science and also for general chemical application.
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Affiliation(s)
- Muhammad H. Rashid
- Paul Scherrer Institute, Swiss Light Source, Laboratory for FemtochemistryForschungsstrasse 111Villigen PSISwitzerland
| | - Camelia N. Borca
- Paul Scherrer Institute, Swiss Light Source, Laboratory for FemtochemistryForschungsstrasse 111Villigen PSISwitzerland
| | - Jacinta M. Xto
- Paul Scherrer Institute, Swiss Light Source, Laboratory for FemtochemistryForschungsstrasse 111Villigen PSISwitzerland
| | - Thomas Huthwelker
- Paul Scherrer Institute, Swiss Light Source, Laboratory for FemtochemistryForschungsstrasse 111Villigen PSISwitzerland
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9
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Morgan J, McNeil BWJ. X-ray pulse generation with ultra-fast flipping of its orbital angular momentum. OPTICS EXPRESS 2022; 30:31171-31181. [PMID: 36242205 DOI: 10.1364/oe.470503] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/13/2022] [Accepted: 07/14/2022] [Indexed: 06/16/2023]
Abstract
A method to temporally tailor the properties of X-ray radiation carrying Orbital Angular Momentum (OAM) is presented. In simulations, an electron beam is prepared with a temporally modulated micro-bunching structure which, when radiating at the second harmonic in a helical undulator, generates OAM light with a corresponding temporally modulated intensity. This method is shown to generate attosecond pulse trains of OAM light without the need for any additional external optics, making the wavelength range tunable. In addition to the OAM pulse train, the method can be adapted to generate radiation where the handedness of the OAM mode may also be temporally modulated (flipped).
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10
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A perfect X-ray beam splitter and its applications to time-domain interferometry and quantum optics exploiting free-electron lasers. Proc Natl Acad Sci U S A 2022; 119:2117906119. [PMID: 35140184 PMCID: PMC8851450 DOI: 10.1073/pnas.2117906119] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Accepted: 12/30/2021] [Indexed: 12/13/2022] Open
Abstract
X-ray free-electron lasers (FELs) deliver ultrabright X-ray pulses, but not the sequences of phase-coherent pulses required for time-domain interferometry and control of quantum states. For conventional split-and-delay schemes to produce such sequences, the challenge stems from extreme stability requirements when splitting Ångstrom wavelength beams, where the tiniest path-length differences introduce phase jitter. We describe an FEL mode based on selective electron-bunch degradation and transverse beam shaping in the accelerator, combined with a self-seeded photon emission scheme. Instead of splitting the photon pulses after their generation by the FEL, we split the electron bunch in the accelerator, prior to photon generation, to obtain phase-locked X-ray pulses with subfemtosecond duration. Time-domain interferometry becomes possible, enabling the concomitant program of classical and quantum optics experiments with X-rays. The scheme leads to scientific benefits of cutting-edge FELs with attosecond and/or high-repetition rate capabilities, ranging from the X-ray analog of Fourier transform infrared spectroscopy to damage-free measurements.
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11
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Arginine and Arginine/ADMA Ratio Predict 90-Day Mortality in Patients with Out-of-Hospital Cardiac Arrest-Results from the Prospective, Observational COMMUNICATE Trial. J Clin Med 2020; 9:jcm9123815. [PMID: 33255752 PMCID: PMC7760544 DOI: 10.3390/jcm9123815] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/09/2020] [Revised: 11/08/2020] [Accepted: 11/19/2020] [Indexed: 02/07/2023] Open
Abstract
(1) Background: In patients with shock, the L-arginine nitric oxide pathway is activated, causing an elevation of nitric oxide, asymmetric dimethylarginine (ADMA) and symmetric dimethylarginine (SDMA) levels. Whether these metabolites provide prognostic information in patients after out-of-hospital cardiac arrest (OHCA) remains unclear. (2) Methods: We prospectively included OHCA patients, recorded clinical parameters and measured plasma ADMA, SDMA and Arginine levels by liquid chromatography tandem mass spectrometry (LC-MS). The primary endpoint was 90-day mortality. (3) Results: Of 263 patients, 130 (49.4%) died within 90 days after OHCA. Compared to survivors, non-survivors had significantly higher levels of ADMA and lower Arginine and Arginine/ADMA ratios in univariable regression analyses. Arginine levels and Arginine/ADMA ratio were significantly associated with 90-day mortality (OR 0.51 (95%CI 0.34 to 0.76), p < 0.01 and OR 0.40 (95%CI 0.26 to 0.61), p < 0.001, respectively). These associations remained significant in several multivariable models. Arginine/ADMA ratio had the highest predictive value with an area under the curve (AUC) of 0.67 for 90-day mortality. Results for secondary outcomes were similar with significant associations with in-hospital mortality and neurological outcome. (4) Conclusion: Arginine and Arginine/ADMA ratio were independently associated with 90-day mortality and other adverse outcomes in patients after OHCA. Whether therapeutic modification of the L-arginine-nitric oxide pathway has the potential to improve outcome should be evaluated.
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12
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Ho PJ, Daurer BJ, Hantke MF, Bielecki J, Al Haddad A, Bucher M, Doumy G, Ferguson KR, Flückiger L, Gorkhover T, Iwan B, Knight C, Moeller S, Osipov T, Ray D, Southworth SH, Svenda M, Timneanu N, Ulmer A, Walter P, Hajdu J, Young L, Maia FRNC, Bostedt C. The role of transient resonances for ultra-fast imaging of single sucrose nanoclusters. Nat Commun 2020; 11:167. [PMID: 31919346 PMCID: PMC6952381 DOI: 10.1038/s41467-019-13905-9] [Citation(s) in RCA: 20] [Impact Index Per Article: 5.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/12/2018] [Accepted: 12/04/2019] [Indexed: 11/09/2022] Open
Abstract
Intense x-ray free-electron laser (XFEL) pulses hold great promise for imaging function in nanoscale and biological systems with atomic resolution. So far, however, the spatial resolution obtained from single shot experiments lags averaging static experiments. Here we report on a combined computational and experimental study about ultrafast diffractive imaging of sucrose clusters which are benchmark organic samples. Our theoretical model matches the experimental data from the water window to the keV x-ray regime. The large-scale dynamic scattering calculations reveal that transient phenomena driven by non-linear x-ray interaction are decisive for ultrafast imaging applications. Our study illuminates the complex interplay of the imaging process with the rapidly changing transient electronic structures in XFEL experiments and shows how computational models allow optimization of the parameters for ultrafast imaging experiments. X-ray free electron lasers provide high photon flux to explore single particle diffraction imaging of biological samples. Here the authors present dynamic electronic structure calculations and benchmark them to single-particle XFEL diffraction data of sucrose clusters to predict optimal single-shot imaging conditions.
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Affiliation(s)
- Phay J Ho
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA.
| | - Benedikt J Daurer
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden
| | - Max F Hantke
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden.,Chemistry Research Laboratory, Department of Chemistry, Oxford University, 12 Mansfield Rd, Oxford, OX1 3TA, UK
| | - Johan Bielecki
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden.,European XFEL GmbH, Holzkoppel 4, D-22869, Schenefeld, Germany
| | - Andre Al Haddad
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA
| | - Maximilian Bucher
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA
| | - Gilles Doumy
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA
| | - Ken R Ferguson
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Leonie Flückiger
- ARC Centre of Excellence for Advanced Molecular Imaging, La Trobe University, Bundoora, VIC, 3086, Australia
| | - Tais Gorkhover
- Stanford Pulse Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Bianca Iwan
- Stanford Pulse Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Christopher Knight
- Computational Science Division, Argonne National Laboratory, Argonne, IL, 60439, USA
| | - Stefan Moeller
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Timur Osipov
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Dipanwita Ray
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Stephen H Southworth
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA
| | - Martin Svenda
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden
| | - Nicusor Timneanu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden.,Department of Physics and Astronomy, Uppsala University, SE-751 20, Uppsala, Sweden
| | - Anatoli Ulmer
- Institut für Optik und Atomare Physik, Technische Universität Berlin, 10623, Berlin, Germany
| | - Peter Walter
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Janos Hajdu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden
| | - Linda Young
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA.,Department of Physics and James Franck Institute, The University of Chicago, Chicago, IL, 60637, USA
| | - Filipe R N C Maia
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, SE-751 24, Uppsala, Sweden.
| | - Christoph Bostedt
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL, 60439, USA. .,Department of Physics and Astronomy, Northwestern University, Evanston, IL, USA. .,Paul-Scherrer Institute, CH-5232, Villigen PSI, Switzerland. .,LUXS Laboratory for Ultrafast X-ray Sciences, Institute of Chemical Sciences and Engineering, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015, Lausanne, Switzerland.
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13
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Laser-Driven Modulation of Electron Beams in a Dielectric Micro-Structure for X-Ray Free-Electron Lasers. Sci Rep 2019; 9:19773. [PMID: 31874977 PMCID: PMC6930261 DOI: 10.1038/s41598-019-56201-8] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/09/2019] [Accepted: 12/09/2019] [Indexed: 11/15/2022] Open
Abstract
We describe an application of laser-driven modulation in a dielectric micro-structure for the electron beam in a free-electron laser (FEL). The energy modulation is transferred into longitudinal bunching via compression in a magnetic chicane before entering the undulator section of the FEL. The bunched electron beam comprises a series of enhanced current spikes separated by the wavelength of the modulating laser. For beam parameters of SwissFEL at a total bunch charge of 30 pC, the individual spikes are expected to be as short as 140 as (FWHM) with peak currents exceeding 4 kA. The proposed modulation scheme requires the electron beam to be focused into the micrometer scale aperture of the dielectric structure, which imposes strict emittance and charge limitations, but, due to the small interaction region, the scheme is expected to require ten times less laser power as compared to laser modulation in a wiggler magnet, which is the conventional approach to create a pulse train in FELs.
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