Bergmann Group achieves shortest hard X-ray pulses to date

Once only a part of science fiction, lasers are now everyday objects used in research, healthcare and even just for fun. Previously available only in low-energy light, lasers are now available in wavelengths from microwaves through X-rays, opening up a range of different downstream applications.”.

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Uwe Bergmann
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Tom Linker

In a new study published online June 11 in the journal Nature, an international collaboration led by scientists at the University of Wisconsin–Madison has generated the shortest hard X-ray pulses to date through the first demonstration of strong lasing phenomena. The resulting pulses can lead to several potential applications, from quantum X-ray optics to visualizing electron motion inside molecules.

“We have observed strong lasing phenomena in inner-shell X-ray lasing and been able to simulate and calculate how it evolves,” says Uwe Bergmann, physics professor at UW–Madison, and senior author on the study. “When you calculate the X-ray pulses that come out, they can be incredibly short — shorter than 100 attoseconds.”

An attosecond is one quintillionth of a second and this extremely short duration of the pulses is what could drive new, advanced LASER applications.

a log-scale timeline shows time in seconds from 10^-18 to 10^18. An attosecond is 1*10^-18 and the time since the big bang, which is also shown on this timeline, is 10^18 seconds, showing that an attosecond is so short it's the same relative to a second as a second is to the age of the Universe (also the text in the title)
What’s an attosecond? An attosecond is one quintillionth of a second, or one billionth of a billionth of a second, or 10^-18 seconds. Put another way, an attosecond is to one second roughly the same timescale as one second is to the age of our universe since the Big Bang. Note, the line is showing log scale. | Credit: Sarah Perdue, UW–Madison

The inner-shell X-ray lasing process is similar as in optical lasing, just at a much shorter wavelengths. An initial pulse of X-ray photons excites atoms’ inner-shell electrons. These excited electrons then emit photons of different X-ray wavelengths as they return to their state. Their emitted photons sometimes hit an already-excited atom, leading to an avalanche of stimulated emission radiation (the SER of LASER) in one direction.

Because inner-shell electrons are held very tightly, powerful X-ray pulses, like those from X-ray free-electron lasers (XFEL), are required to excite enough of them simultaneously to result in lasing. In turn, the photons they emit in this process are also at X-ray wavelengths. But XFEL pulses are generally “dirty,” with each pulse really being made of several short, intense spikes in time, and a range of spikes with different wavelengths, limiting some of their applications.

“They’re just not clean, beautiful pulses (like visible lasers),” says Thomas Linker, joint postdoctoral researcher at UW–Madison and the Stanford PULSE Institute at SLAC and lead author of the publication. “But it’s the only thing we have. We have to live with it.”

In this study, the researchers tightly focused XFEL pulses onto a sample made of copper or manganese. The input pulse is still dirty, but very short and incredibly powerful: the equivalent of focusing all the sunlight that hits the Earth into one square millimeter. The X-ray photons that the sample emits in the same forward direction as the input pulse hit a piece of instrumentation that disperses them by wavelength, much like a prism disperses visible light into a rainbow, and reflects it based on its angle. This dispersed X-ray light is next read by a detector, which measures its properties.

a blue pump beam is focused on a sample, which, if stimulated emission occurs, beams out of the sample (depicted as a red beam here). It is then reflected off a silcon analyzer that separates it based on wavelength (similar to how a prism spreads out white light into a visible rainbow) to a detector.
Experimental setup Tightly focused XFEL pulses are directed at a sample made of copper or manganese. Any X-ray photons that the sample emits in the same forward direction as the input pulse hit a piece of instrumentation that disperses them by wavelength and reflects it based on its angle. This dispersed X-ray light is next read by a detector, which measures its properties. | Credit: this study

First, the researchers confirmed that stimulated emission is occurring in their sample by measuring a strong signal in the detector.

They noticed something else about the emitted light. In terms of its light spectrum, it contained all of the expected wavelengths. Spatially, however, the team sometimes detected a few hotspots instead of the expected smooth signal. Applying a 3D simulation, Linker was able to show what was happening to lead to these results. His calculations illustrated that the emitted X-rays underwent a process that created filaments when moving through the samples.

“This is filamentation, a strong lasing phenomenon which, in optical science, is when the index of refraction changes because of this very, very strong field,” Linker says. “You get spatial phenomena leading to the observed hotspots.”

When the team further increased the intensity of their input pulse, they saw another unexpected result: instead of seeing hotspots of one wavelength, they observed spectral broadening and sometimes multiple spectral lines. They ran the simulation on this new data and realized that this result can only be explained by another lasing phenomenon called Rabi cycling, where the pulse is so strong that the sample will cyclically absorb photons and emit them by stimulated emission. They used their simulation to plot the emitted pulse intensity over time and found that their dirty input pulses resulted in extremely short stimulated emission pulses that were sometimes 60-100 attoseconds in length — the shortest hard X-ray pulses observed by anyone to date.

“We have generated hard X-ray attosecond pulses with this strong lasing phenomenon,” Linker says. “The timescale at which chemical bonds are formed and broken is the femtosecond (1,000 times longer than attosecond) timescale. But if you want to see electron dynamics, how they move inside their orbitals, that’s the attosecond timescale.”

the experimental and simulated data of the highest intensity pulses is shown as a rainbow of scattered, but organized, detected pulses. The right shows a graph of time vs intensity and shows a clearly offset stimulated emission pulse that is 60-100 attoseconds wide, indicating it's lifetime.
Generation of attosecond pulses The experimental data (left) are used in simulation (center) to plot the emitted pulse intensity over time (right). The dirty input pulse (blue line) resulted in extremely short emission pulses (red line) that were as short as 60-100 attoseconds in length. | Credit: this study

XFELs have only been around for about 15 years, so scientists are still learning about them and how to apply them. This study is not the first to “clean up” hard X-ray pulses, but it is the first to achieve emitted pulses on this timescale and to show evidence of strong lasing phenomenon.

“There are so many nonlinear technologies and phenomena that the laser community uses now, but very few of those have dared to have been tried with hard X-rays,” Bergmann says. “Hard X-rays are very powerful: they have Angstrom wavelengths that provide atomic spatial resolution, and they are sensitive to different elements. This work is a step towards pushing the exciting field of real laser science into this powerful hard X-ray regime.”

This work was largely supported by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES) under contract Nos. DE-SC0023270 and DEAC02-76SF00515. The experiments were performed at the Linac Coherent Light Source at SLAC National Accelerator Laboratory and the SACLA X-ray laser at the Japan Synchrotron Radiation Research Institute

Congrats to Prof. Rzchowski on his retirement!

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Mark Rzchowski

Congrats to Prof. Mark Rzchowski who has announced his retirement, effective January 17! Rzchowski is a condensed matter experimentalist who joined the department as an assistant professor in 1992 and has been a full professor since 2004. He served as Associate Chair for Undergraduate Program and Academic Affairs from 2008-10 and again from 2011-24.

When Rzchowski arrived to UW–Madison, high-temperature superconductivity had recently been discovered, and his early research largely centered on that topic, focusing on novel measurements of their fundamental physical properties.

“But I soon moved in different directions, collaborating with Chang-Beom Eom, a new faculty member in materials science and engineering expert in thin film growth,” Rzchowski recalls. “He had been working in superconductivity but had been branching out into some new systems, and we moved together in those directions.”

Rzchowski and Eom have collaborated for over two decades now, pairing forefront growth and manipulation of crystalline thin films with state-of-the art measurement approaches. Their collaboration has resulted in over 70 co-authored papers largely focused on quantum correlations and topologies in complex oxide thin-film materials. In spintronics, a technology that takes advantage of the intrinsic quantum spin state of an electron to substitute spin currents for the charge currents in “elec”tronics, they developed an all-thin-film membrane-based system that demonstrated an intrinsic coupling between voltage and spin. This helped to address a persistent problem in spintronics, namely better controlling magnetism at the nanoscale: the extreme thinness of the material allows low operating voltages to control the spin properties.

In another spintronics study in 2023, Rzchowski and Eom demonstrated uniquely oriented thin films of oxide crystals that controls the natural symmetry of the crystals, allowing them to produce vastly more useful spin currents — a critical step forward in advancing next-gen computer memory devices.

“I am so lucky to have known Mark — as a collaborator, colleague, and friend,” Eom says. “His brilliance as a scientist and kindness as a person will stay with me. I wish him happiness and fulfillment in the years ahead and I hope to continue sharing the joys of life for many years.”

two men stand in front of lab equipment
Chang Beom-Eom (left), a professor of materials science and engineering, and Mark Rzchowski, a professor of physics, in the lab. Photo: Joel Hallberg.

In 2022, Rzchowski was elected a Fellow of the American Physical Society for “pioneering discoveries and understanding of physical principles governing correlated complex materials and interfaces, including superconductors, correlated oxide systems multiferroic systems, and spin currents in noncollinear antiferromagnets.” He was nominated by the Division of Materials Physics.

Rzchowski has provided decades of service to the department, some of this time as associate chair. In this role, he led the redevelopment of several of the large courses, for example hiring course coordinators to provide consistency. He also was largely involved in the overhaul of algebra-based Physics 103 and 104, supported by the provost’s REACH initiative. REACH is designed to give students as many chances as possible to actively engage with physics principles and ideas, and to collaborate in group settings. An assessment of the program’s implementation showed a significant increase in concept mastery in these  . He has represented the department at conferences presenting the REACH implementation and analysis of learning outcomes.

In March 2020, Rzchowski successfully led the transition of every course to all-online instruction when the Covid-19 pandemic abruptly sent everyone off campus, then to hybrid online/in-person instruction as students slowly returned. More recently, he helped leverage what was learned from those semesters into offering the summer session of Physics 103, and, now this year, Physics 104, as fully online courses. These online offerings have more than tripled summer enrollments — both UW–Madison students as well as visiting students.

Rzchowski was also chair of the department’s space committee in the early 2000s and oversaw the design of new laboratory and office space in Chamberlin Hall, and the transition from Sterling Hall to Chamberlin  .

Prof. Emerit Bob Joynt, who overlapped with Rzchowski as associate chair when Joynt served as department chair from 2011-2014, says: “I worked closely with Mark Rzchowski for over 30 years. Of all my colleagues, he was the one whose advice I valued most, and the one who could most be trusted to follow through on everything he ever promised (which was a lot). He was not only a talented researcher, but he also was very generous with his time for the department, particularly the teaching program. He always did the jobs that were the most needed, usually those that were also the most thankless. So now, one last time, thank you Mark!”

Prof. Mark Eriksson, who served as department chair from 2021-2024, also overlapping with Rzchowski’s tenure as associate chair, says: “Mark Rzchowski made many contributions during his career in teaching research and service. In this last category for many years Mark served in the essential role of Associate Chair for Academic Affairs in which he solved — semester after semester — the complex riddle of matching instructors to courses in an optimal way.

 

— By Sarah Perdue, department of physics. Adam Malecek and Jason Daley of the College of Engineering contributed to this story