Ultrafast Electronic Characterization of Proteins and Materials

Researchers at the University of Tsukuba use an optoelectronic resonator to increase the sensitivity of an electron pulse detector, which may lead to ultrafast electronic characterization of proteins or materials. Credit: University of Tsukuba.

Researchers use an optoelectronic resonator to increase the sensitivity of an electron pulse detector, which may lead to ultrafast electronic characterization of proteins and materials.

Scientists from the University of Tsukuba in Japan have shown how adding a tiny resonator structure to an ultrafast electron pulse detector reduced the intensity of terahertz radiation required to characterize the pulse duration.

To study proteins—for example, when determining the mechanisms of their biological actions—researchers need to understand the motion of individual atoms within a sample. This is difficult not just because atoms are so tiny, but also because such rearrangements usually occur in picoseconds—that is, trillionths of a second.

One method to examine these systems is to excite them with an ultrafast blast of laser light, and then immediately probe them with a very short electron pulse. Based on the way the electrons scatter off the sample as a function of the delay time between the laser and electron pulses, researchers can obtain a great deal of information about the atomic dynamics. However, characterizing the initial electron pulse is difficult and requires complex setups or high-powered THz radiation.

Now, a team of researchers at the University of Tsukuba has used an optical resonator to enhance the electric field of a terahertz (THz) light pulse generated with a crystal, which reduces the required THz light to characterize the duration of the electron pulse. THz radiation refers to beams of light with wavelengths between those of infrared and microwave. “Accurate characterization of the probe electron pulse is essential, because it lasts longer and is generally more difficult to control compared with the excitation laser beam that starts the atoms in motion,” explains co-author, Professor Yusuke Arashida.

Similar to how a room with the right acoustics can amplify the perception of sound, a resonator can enhance the amplitude of THz radiation with wavelengths that match its size and shape. In this case, the team used a butterfly-shaped resonator, which was previously designed by an independent research group, to concentrate the energy of the pulse. Through simulations, they found that the electric field enhancement was concentrated where the “head” and the “tail” of the butterfly would be. They found that they could measure the electron pulse duration up to more than a picosecond using the THz streaking method. This approach uses incident light to spread out the electron pulse along a perpendicular direction. A “streak” in the camera is formed with time information now encoded into the spatial distribution of the resulting image.

“Ultrafast measurements using electron pulses can show the atomic-level structural dynamics of molecules or materials as they relax after being excited by a laser,” says senior author, Professor Masaki Hada.

Use of this resonator with a weak THz field and intensity of a few kV/cm was shown to be sufficient for characterizing electron pulses at picosecond timescales. This work may lead to a more efficient examination of atomic-level motions on very short time scales, potentially aiding in the study of biomolecules or industrial materials.

Reference: “Streaking of a Picosecond Electron Pulse with a Weak Terahertz Pulse” by Wataru Yajima, Yusuke Arashida, Ryota Nishimori, Yuga Emoto, Yuki Yamamoto, Kohei Kawasaki, Yuri Saida, Samuel Jeong, Keishi Akada, Kou Takubo, Hidemi Shigekawa, Jun-ichi Fujita, Shin-ya Koshihara, Shoji Yoshida and Masaki Hada, 13 December 2022, ACS Photonics.
DOI: 10.1021/acsphotonics.2c01304

This research was supported by Kakenhi Grants-in-Aid (Nos. JP18H05208, JP19H00847, and JP20H01832) and the Leading Initiative for Excellent Young Researchers of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan. This work was also supported by JST FOREST Program, Grant Number JPMJFR211V. A part of this work was supported by “Advanced Research Infrastructure for Materials and Nanotechnology in Japan (ARIM)” of MEXT, Grant Number JPMXP1222BA0009.