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.”.

Profile picture of Uwe Bergmann
Uwe Bergmann
profile photo of Tom Linker
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

Zain Abhari selected for SACLA graduate internship

a woman stands in front of a tree with a Japanese castle in the near background
Zain Abhari on a tour at Himeji Castle, which is one of the last few fully intact castles in Japan and is located near the SACLA facility | Photo provided by Zain Abhari

Congrats to Physics PhD student Zain Abhari for being selected to the SACLA Research Support Program for Graduate Students. The one-year internship run by SACLA (the SPring-8 Angstrom Compact free electron LAser) accepts graduate students with a demonstrated interest in using X-ray free electron lasers (XFELs) for their research and provides them with training and beam time at the facility in Japan.

Prior to her acceptance in the program, Abhari had already spent time at SACLA as part of her research in Uwe Bergmann’s group. While there, her collaborator told her about the program and recommended she apply.

“My goal after the PhD is to work at one of these large-scale facilities, specifically the X-ray free electron lasers and there’s only six of them right now in the world,” Abhari says. “If I can get my foot in the door in Japan, or get the experience to then help me with any of the other ones, that would be pretty awesome.”

Abhari was also interested in the program because SACLA’s laser aligns well with the goals of her thesis research, which is to obtain intense, stable XFEL pulses to apply to different spectroscopy techniques. For about the past decade, XFEL has allowed researchers to make ultrafast movies of molecular changes, essentially helping them to see chemical reactions take place. But x-ray lasers are “dirty,” and they contain multiple wavelengths of light of varying intensity. Last year, Bergmann and his colleagues somewhat accidentally discovered a way to make the pulses cleaner through two intense, femtosecond-spaced pulses.

Even though the researchers think they know how the useful pulses work, producing and controlling them are a completely different story — and one that Abhari hopes to unravel in her research.

“Right now, they’re just random,” Abhari says. “So the goal is to understand them. And then if we understand them, can we control them? If we can control them, can we apply them?”

Abhari will travel to Japan for three months beginning in September, where the program provides on-campus housing and time on the laser. Without the access she is now granted by this internship, her research would have been much more focused on short rounds of data collection followed by off-site data analysis.

“Now, I can get my hands on the laser and collect data to try to understand parameters that allow us to get the specific output we’re looking for,” Abhari says. “I have data that allude me to what those parameters will be, but now in real time, I can be like, ‘If I do this, I see this; if I do that, I see that.’”

In addition to her thesis research, Abhari will be working with her SACLA collaborators on a machine learning project to optimize beam focusing, and helping learn about and improve a portable beam nanofocusing apparatus.