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Adam
Round
,
Pierre
Aller
,
Richard
Bean
,
Johan
Bielecki
,
Agata
Butryn
,
Nicholas E.
Devenish
,
Raphael
De Wijn
,
Thomas
Dietze
,
Katerina
Doerner
,
Fabio
Dall'Antonia
,
Gabriele
Giovanetti
,
Huijong
Han
,
Vincent
Hennicke
,
Chan
Kim
,
Yoonhee
Kim
,
Marco
Kloos
,
Jayanath C. P.
Koliyadu
,
Gabriel
Leen
,
Romain
Letrun
,
Luis
Lopez Morillo
,
Allen M.
Orville
,
Tim
Pakendorf
,
Marco
Ramilli
,
Nadja
Reimers
,
Patrick
Reinke
,
Juan
Sanchez-Weatherby
,
Tokushi
Sato
,
Robin
Schubert
,
Joachim
Schulz
,
Cedric
Signe Takem
,
Marcin
Sikorski
,
Prasad
Thute
,
Fabian
Trost
,
Oleksii
Turkot
,
Patrik
Vagovic
,
Mohammad
Vakili
,
Raul
Villanueva Guerrero
,
Henry N.
Chapman
,
Alke
Meents
,
Serguei
Molodtsov
,
Sakura
Pascarelli
,
Thomas
Tschentschera
,
Adrian
Mancuso
,
Pontus
Fischer
,
Sebastian
Guenther
Open Access
Abstract: The Single-Particle, Clusters and Biomolecules and Serial Femtosecond Crystallography (SPB/SFX) scientific instrument at the European X-Ray Free-Electron Laser (EuXFEL) became operational with user experiments in September 2017. The unique properties and capabilities of the EuXFEL, enabling megahertz data collection rates, provide more rapid data collection with improved statistics compared with other XFEL facilities. This improves the feasibility of obtaining multiple data points in time-resolved experiments and hence enables the observation of reactions in greater detail (molecular movies). In collaboration with the SFX User Consortium (SFX UC), the SPB/SFX instrument was designed to further increase user access and research outcomes. Focusing the pulses downstream of the first interaction region [described previously (Mancuso et al., 2019)], a second experiment plane is enabled, which allows for greater optimization and more efficient usage of available beam time. Additionally, the SFX UC provided further instrumentation to provide improved capabilities on SPB/SFX. The aim for additional and extended functionality for the second interaction region was to enable sample-efficient data collection at atmospheric pressure in an environment where the sample temperature and humidity can be controlled. This paper describes the extended capabilities of the downstream interaction region of the SPB/SFX instrument and its major components, in particular its X-ray focusing optics, vacuum to atmospheric pressure out-coupling, available sample delivery methods and 2D detector, and the supporting optical laser systems for pump–probe experiments.
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Nov 2025
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Kang
Xiang
,
Ling
Qin
,
Shi
Huang
,
Hongyuan
Song
,
Vasilii
Bazhenov
,
Sarlota
Birnšteinová
,
Raphael
De Wijn
,
Jayanath C. P.
Koliyadu
,
Faisal H. M.
Koua
,
Adam
Round
,
Ekaterina
Round
,
Abhisakh
Sarma
,
Tokushi
Sato
,
Marcin
Sikorski
,
Yuhe
Zhang
,
Eleni
Myrto Asimakopoulou
,
Pablo
Villanueva-Perez
,
Kyriakos
Porfyrakis
,
Iakovos
Tzanakis
,
Dmitry G.
Eskin
,
Nicole
Grobert
,
Adrian
Mancuso
,
Richard
Bean
,
Patrik
Vagovic
,
Jiawei
Mi
,
Valerio
Bellucci
Open Access
Abstract: Using megahertz x-ray free electron laser imaging with x-ray pulses of ~25 femtoseconds and a machine-learning strategy, we have conducted comprehensive in situ imaging studies on the dynamics of cavitation bubble clouds in ultrasound fields at the SPB/SFX beamline of the European XFEL. The research unambiguously revealed the quasi-simultaneous implosion of multiple bubbles and simultaneous collapse of bubble cloud in nanosecond scale and their dynamic impacts onto two-dimensional (2D) materials for layer exfoliation. We have also performed multiphysics modeling to simulate the shock wave emission, propagation, impact, and stresses produced. We elucidated the critical conditions for producing instant or fatigue exfoliation and the effects of bonding strengths and structural defects on the exfoliation rate. The discoveries have filled the long-standing missing knowledge gaps in the underlying physics of exfoliating 2D materials in ultrasound fields, providing a solid theoretical foundation for optimizing and scaling-up operation to produce 2D materials in a much more cost-effective and sustainable way.
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Nov 2025
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Jaydeep
Patel
,
Adam
Round
,
Raphael
De Wijn
,
Mohammad
Vakili
,
Gabriele
Giovanetti
,
Diogo Filipe Monrroy Vilan E
Melo
,
Juncheng
E
,
Marcin
Sikorski
,
Jayanth
Koliyadu
,
Faisal H. M.
Koua
,
Tokushi
Sato
,
Adrian
Mancuso
,
Andrew
Peele
,
Brian
Abbey
Open Access
Abstract: Automated evaluation of optical microscopy images of liquid jets, commonly used for sample delivery at X-ray free-electron lasers (XFELs), enables real-time tracking of the jet position and liquid jet hit rates, defined here as the proportion of XFEL pulses intersecting with the liquid jet. This method utilizes machine vision for preprocessing, feature extraction, segmentation and jet detection as well as tracking to extract key physical characteristics (such as the jet angle) from optical microscopy images captured during experiments. To determine the effectiveness of these tools in monitoring jet stability and enhancing sample delivery efficiency, we conducted XFEL experiments with various sample compositions (pure water, buffer and buffer with crystals), nozzle designs and jetting conditions. We integrated our real-time analysis algorithm into the Karabo control system at the European XFEL. The results indicate that the algorithm performs well in monitoring the jet angle and provides a quantitative characterization of liquid jet stability through optical image analysis conducted during experiments.
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Dec 2024
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Zhou
Shen
,
Paul Lourdu
Xavier
,
Richard
Bean
,
Johan
Bielecki
,
Martin
Bergemann
,
Benedikt
Daurer
,
Tomas
Ekeberg
,
Armando D.
Estillore
,
Hans
Fangohr
,
Klaus
Giewekemeyer
,
Mikhail
Karnevskiy
,
Richard A.
Kirian
,
Henry
Kirkwood
,
Yoonhee
Kim
,
Jayanath C. P.
Koliyadu
,
Holger
Lange
,
Romain
Letrun
,
Jannik
Lübke
,
Abhishek
Mall
,
Thomas
Michelat
,
Andrew J.
Morgan
,
Nils
Roth
,
Amit K.
Samanta
,
Tokushi
Sato
,
Marcin
Sikorski
,
Florian
Schulz
,
Patrik
Vagovic
,
Tamme
Wollweber
,
Lena
Worbs
,
Filipe
Maia
,
Daniel A.
Horke
,
Jochen
Küpper
,
Adrian P.
Mancuso
,
Henry
Chapman
,
Kartik
Ayyer
,
N. Duane
Loh
Open Access
Abstract: Nanoparticles, exhibiting functionally relevant structural heterogeneity, are at the forefront of cutting-edge research. Now, high-throughput single-particle imaging (SPI) with X-ray free-electron lasers (XFELs) creates opportunities for recovering the shape distributions of millions of particles that exhibit functionally relevant structural heterogeneity. To realize this potential, three challenges have to be overcome: (1) simultaneous parametrization of structural variability in real and reciprocal spaces; (2) efficiently inferring the latent parameters of each SPI measurement; (3) scaling up comparisons between 105 structural models and 106 XFEL-SPI measurements. Here, we describe how we overcame these three challenges to resolve the nonequilibrium shape distributions within millions of gold nanoparticles imaged at the European XFEL. These shape distributions allowed us to quantify the degree of asymmetry in these particles, discover a relatively stable “shape envelope” among nanoparticles, discern finite-size effects related to shape-controlling surfactants, and extrapolate nanoparticles’ shapes to their idealized thermodynamic limit. Ultimately, these demonstrations show that XFEL SPI can help transform nanoparticle shape characterization from anecdotally interesting to statistically meaningful.
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May 2024
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Mohammad
Vakili
,
Huijong
Han
,
Christina
Schmidt
,
Agnieszka
Wrona
,
Marco
Kloos
,
Iñaki
De Diego
,
Katerina
Dörner
,
Tian
Geng
,
Chan
Kim
,
Faisal H. M.
Koua
,
Diogo V. M.
Melo
,
Mathieu
Rappas
,
Adam
Round
,
Ekaterina
Round
,
Marcin
Sikorski
,
Joana
Valerio
,
Tiankun
Zhou
,
Kristina
Lorenzen
,
Joachim
Schulz
Open Access
Abstract: Time-resolved crystallography enables the visualization of protein molecular motion during a reaction. Although light is often used to initiate reactions in time-resolved crystallography, only a small number of proteins can be activated by light. However, many biological reactions can be triggered by the interaction between proteins and ligands. The sample delivery method presented here uses a mix-and-extrude approach based on 3D-printed microchannels in conjunction with a micronozzle. The diffusive mixing enables the study of the dynamics of samples in viscous media. The device design allows mixing of the ligands and protein crystals in 2 to 20 s. The device characterization using a model system (fluorescence quenching of iq-mEmerald proteins by copper ions) demonstrated that ligand and protein crystals, each within lipidic cubic phase, can be mixed efficiently. The potential of this approach for time-resolved membrane protein crystallography to support the development of new drugs is discussed.
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Aug 2023
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I03-Macromolecular Crystallography
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Max O.
Wiedorn
,
Dominik
Oberthuer
,
Richard
Bean
,
Robin
Schubert
,
Nadine
Werner
,
Brian
Abbey
,
Martin
Aepfelbacher
,
Luigi
Adriano
,
Aschkan
Allahgholi
,
Nasser
Al-Qudami
,
Jakob
Andreasson
,
Steve
Aplin
,
Salah
Awel
,
Kartik
Ayyer
,
Saša
Bajt
,
Imrich
Barák
,
Sadia
Bari
,
Johan
Bielecki
,
Sabine
Botha
,
Djelloul
Boukhelef
,
Wolfgang
Brehm
,
Sandor
Brockhauser
,
Igor
Cheviakov
,
Matthew A.
Coleman
,
Francisco
Cruz-Mazo
,
Cyril
Danilevski
,
Connie
Darmanin
,
R. Bruce
Doak
,
Martin
Domaracky
,
Katerina
Dörner
,
Yang
Du
,
Hans
Fangohr
,
Holger
Fleckenstein
,
Matthias
Frank
,
Petra
Fromme
,
Alfonso M.
Gañán-Calvo
,
Yaroslav
Gevorkov
,
Klaus
Giewekemeyer
,
Helen Mary
Ginn
,
Heinz
Graafsma
,
Rita
Graceffa
,
Dominic
Greiffenberg
,
Lars
Gumprecht
,
Peter
Göttlicher
,
Janos
Hajdu
,
Steffen
Hauf
,
Michael
Heymann
,
Susannah
Holmes
,
Daniel A.
Horke
,
Mark S.
Hunter
,
Siegfried
Imlau
,
Alexander
Kaukher
,
Yoonhee
Kim
,
Alexander
Klyuev
,
Juraj
Knoška
,
Bostjan
Kobe
,
Manuela
Kuhn
,
Christopher
Kupitz
,
Jochen
Küpper
,
Janine Mia
Lahey-Rudolph
,
Torsten
Laurus
,
Karoline
Le Cong
,
Romain
Letrun
,
P. Lourdu
Xavier
,
Luis
Maia
,
Filipe R. N. C.
Maia
,
Valerio
Mariani
,
Marc
Messerschmidt
,
Markus
Metz
,
Davide
Mezza
,
Thomas
Michelat
,
Grant
Mills
,
Diana C. F.
Monteiro
,
Andrew
Morgan
,
Kerstin
Mühlig
,
Anna
Munke
,
Astrid
Münnich
,
Julia
Nette
,
Keith A.
Nugent
,
Theresa
Nuguid
,
Allen M.
Orville
,
Suraj
Pandey
,
Gisel
Pena
,
Pablo
Villanueva-Perez
,
Jennifer
Poehlsen
,
Gianpietro
Previtali
,
Lars
Redecke
,
Winnie Maria
Riekehr
,
Holger
Rohde
,
Adam
Round
,
Tatiana
Safenreiter
,
Iosifina
Sarrou
,
Tokushi
Sato
,
Marius
Schmidt
,
Bernd
Schmitt
,
Robert
Schönherr
,
Joachim
Schulz
,
Jonas A.
Sellberg
,
M. Marvin
Seibert
,
Carolin
Seuring
,
Megan L.
Shelby
,
Robert L.
Shoeman
,
Marcin
Sikorski
,
Alessandro
Silenzi
,
Claudiu A.
Stan
,
Xintian
Shi
,
Stephan
Stern
,
Jola
Sztuk-Dambietz
,
Janusz
Szuba
,
Aleksandra
Tolstikova
,
Martin
Trebbin
,
Ulrich
Trunk
,
Patrik
Vagovic
,
Thomas
Ve
,
Britta
Weinhausen
,
Thomas A.
White
,
Krzysztof
Wrona
,
Chen
Xu
,
Oleksandr
Yefanov
,
Nadia
Zatsepin
,
Jiaguo
Zhang
,
Markus
Perbandt
,
Adrian P.
Mancuso
,
Christian
Betzel
,
Henry
Chapman
,
Anton
Barty
Open Access
Abstract: The new European X-ray Free-Electron Laser is the first X-ray free-electron laser capable of delivering X-ray pulses with a megahertz inter-pulse spacing, more than four orders of magnitude higher than previously possible. However, to date, it has been unclear whether it would indeed be possible to measure high-quality diffraction data at megahertz pulse repetition rates. Here, we show that high-quality structures can indeed be obtained using currently available operating conditions at the European XFEL. We present two complete data sets, one from the well-known model system lysozyme and the other from a so far unknown complex of a β-lactamase from K. pneumoniae involved in antibiotic resistance. This result opens up megahertz serial femtosecond crystallography (SFX) as a tool for reliable structure determination, substrate screening and the efficient measurement of the evolution and dynamics of molecular structures using megahertz repetition rate pulses available at this new class of X-ray laser source.
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Oct 2018
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Iris D.
Young
,
Mohamed
Ibrahim
,
Ruchira
Chatterjee
,
Sheraz
Gul
,
Franklin D.
Fuller
,
Sergey
Koroidov
,
Aaron S.
Brewster
,
Rosalie
Tran
,
Roberto
Alonso-Mori
,
Thomas
Kroll
,
Tara
Michels-Clark
,
Hartawan
Laksmono
,
Raymond G.
Sierra
,
Claudiu A.
Stan
,
Rana
Hussein
,
Miao
Zhang
,
Lacey
Douthit
,
Markus
Kubin
,
Casper
De Lichtenberg
,
Long
Vo Pham
,
Håkan
Nilsson
,
Mun Hon
Cheah
,
Dmitriy
Shevela
,
Claudio
Saracini
,
Mackenzie A.
Bean
,
Ina
Seuffert
,
Dimosthenis
Sokaras
,
Tsu-Chien
Weng
,
Ernest
Pastor
,
Clemens
Weninger
,
Thomas
Fransson
,
Louise
Lassalle
,
Philipp
Bräuer
,
Pierre
Aller
,
Peter T.
Docker
,
Babak
Andi
,
Allen M.
Orville
,
James M.
Glownia
,
Silke
Nelson
,
Marcin
Sikorski
,
Diling
Zhu
,
Mark S.
Hunter
,
Thomas J.
Lane
,
Andy
Aquila
,
Jason E.
Koglin
,
Joseph
Robinson
,
Mengning
Liang
,
Sébastien
Boutet
,
Artem Y.
Lyubimov
,
Monarin
Uervirojnangkoorn
,
Nigel W.
Moriarty
,
Dorothee
Liebschner
,
Pavel V.
Afonine
,
David G.
Waterman
,
Gwyndaf
Evans
,
Philippe
Wernet
,
Holger
Dobbek
,
William I.
Weis
,
Axel T.
Brunger
,
Petrus H.
Zwart
,
Paul D.
Adams
,
Athina
Zouni
,
Johannes
Messinger
,
Uwe
Bergmann
,
Nicholas K.
Sauter
,
Jan
Kern
,
Vittal K.
Yachandra
,
Junko
Yano
Abstract: Light-induced oxidation of water by photosystem II (PS II) in plants, algae and cyanobacteria has generated most of the dioxygen in the atmosphere. PS II, a membrane-bound multi-subunit pigment protein complex, couples the one-electron photochemistry at the reaction centre with the four-electron redox chemistry of water oxidation at the Mn4CaO5 cluster in the oxygen-evolving complex (OEC). Under illumination, the OEC cycles through five intermediate S-states (S0 to S4)1, in which S1 is the dark-stable state and S3 is the last semi-stable state before O–O bond formation and O2 evolution2, 3. A detailed understanding of the O–O bond formation mechanism remains a challenge, and will require elucidation of both the structures of the OEC in the different S-states and the binding of the two substrate waters to the catalytic site4, 5, 6. Here we report the use of femtosecond pulses from an X-ray free electron laser (XFEL) to obtain damage-free, room temperature structures of dark-adapted (S1), two-flash illuminated (2F; S3-enriched), and ammonia-bound two-flash illuminated (2F-NH3; S3-enriched) PS II. Although the recent 1.95 Å resolution structure of PS II at cryogenic temperature using an XFEL7 provided a damage-free view of the S1 state, measurements at room temperature are required to study the structural landscape of proteins under functional conditions8, 9, and also for in situ advancement of the S-states. To investigate the water-binding site(s), ammonia, a water analogue, has been used as a marker, as it binds to the Mn4CaO5 cluster in the S2 and S3 states10. Since the ammonia-bound OEC is active, the ammonia-binding Mn site is not a substrate water site10, 11, 12, 13. This approach, together with a comparison of the native dark and 2F states, is used to discriminate between proposed O–O bond formation mechanisms.
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Nov 2016
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