Physics World 05月05日 17:29
Quantum twisting microscope measures phasons in cryogenic graphene
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研究人员通过改进量子扭曲显微镜,使其能够在低温下工作,首次观测到扭曲双层石墨烯中存在的一种声子——相位子。这些相位子可能对材料中的电子动力学产生影响。该研究由魏茨曼科学研究所的Shahal Ilani领导,利用量子扭曲显微镜,精确控制两层石墨烯之间的相对方向,尤其关注扭转角度。实验在低温下进行,证实了电子与相位子耦合的现有理论,并有望帮助理解“奇异金属”的特性。研究人员通过测量动量传递,探测电子-声子耦合强度,为理解扭曲双层石墨烯的电子行为提供了新的视角。

🔬量子扭曲显微镜的低温改进:研究人员对量子扭曲显微镜进行改造,使其能在低温环境下运行,从而首次观测到扭曲双层石墨烯中的相位子。

⚛️相位子与电子动力学:研究表明,相位子作为一种特殊的声子模式,可能对扭曲双层石墨烯材料中的电子行为产生重要影响,尤其是在层间电子跃迁方面。

🌡️奇异金属研究的新途径:通过表征电子与相位子的耦合,这项研究有望帮助理解“奇异金属”的特性,即电阻随温度降低而增加的反常现象。

📐扭转角度的影响:实验发现,随着石墨烯层间扭转角度接近对齐,相位子与电子的耦合强度显著增强,这与理论预测相符,但研究目前受限于技术因素,尚未在更小角度下进行。

🔭独特的研究视角:量子扭曲显微镜提供了一种独特的视角来观察声子,特别是在莫尔条纹系统中,通过测量动量传递,可以量化电子-声子耦合强度。

By adapting their quantum twisting microscope to operate at cryogenic temperatures, researchers have made the first observations of a type of phonon that occurs in twisted bilayer graphene.  These “phasons” could have implications for the electron dynamics in these materials.

Graphene is a layer of carbon just one atom thick and it has range of fascinating and useful properties – as do bilayer and multilayer versions of graphene. Since 2018, condensed-matter physicists have been captivated by the intriguing electron behaviour in two layers of graphene that are rotated with respect to each other.

As the twist angle deviates from zero, the bilayer becomes a moiré superlattice. The emergence of this structure influences electronic properties of the material, which can transform from a semiconductor to a superconductor.

In 2023, researchers led by Shahal Ilani at the Weizmann Institute of Science in Israel developed a quantum twisting microscope to study these effects. Based on a scanning probe microscope with graphene on the substrate and folded over the tip such as to give it a flat end, the instrument allows precise control over the relative orientation between two graphene surfaces – in particular, the twist angle.

Strange metals

Now Ilani and an international team have operated the microscope at cryogenic temperatures for the first time. So far, their measurements support the current understanding of how electrons couple to phasons, which are specific modes of phonons (quantized lattice vibrations). Characterizing this coupling could help us understand “strange metals”, whose electrical resistance increases at lower temperatures – which is the opposite of normal metals.

There are different types of phonons, such as acoustic phonons where atoms within the same unit cell oscillate in phase with each other, and optical phonons where they oscillate out of phase. Phasons are phonons involving lattice oscillations in one layer that are out of phase or antisymmetric with oscillations in the layer above.

“This is the one that turns out to be very important for how the electrons behave between the layers because even a small relative displacement between the two layers affects how the electrons go from one layer to the other,” explains Weizmann’s John Birkbeck as he describes the role of phasons in twisted bilayer graphene materials.

For most phonons the coupling to electrons is weaker the lower the energy of the phonon mode. However for twisted bilayer materials, theory suggests that phason coupling to electrons increases as the twist between the two layers approaches alignment due to the antisymmetric motion of the two layers and the heightened sensitivity of interlayer tunnelling to small relative displacements.

Unique perspective

“There are not that many tools to see phonons, particularly in moiré systems” adds Birkbeck. This is where the quantum twisting microscope offers a unique perspective. Thanks to the atomically flat end of the tip, electrons can tunnel between the layer on the substrate and the layer on the tip whenever there is a matching state in terms of not just energy but also momentum too.

Where there is a momentum mismatch, tunnelling between tip and substrate is still possible by balancing the mismatch with the emission or absorption of a phonon. By operating at cryogenic temperatures, the researchers were able to get a measure of these momentum transactions and probe the electron phonon coupling too.

“What was interesting from this work is not only that we could image the phonon dispersion, but also we can quantify it,” says Birkbeck stressing the absolute nature of these quantified electron phonon coupling-strength measurements.

The measurements are the first observations of phasons in twisted bilayer graphene and reveal a strong increase in coupling as the layers approach alignment, as predicted by theory. However, the researchers were not able to study angles smaller than 6°. Below this angle the tunnelling resistance is so low that the contact resistance starts to warp readings, among other limiting factors.

Navigating without eyes

A certain amount of technical adjustment was needed to operate the tool at cryogenic temperatures, not least to “to navigate without eyes” because the team was not able to incorporate their usual optics with the cryogenic set up. The researchers hope that with further technical adjustments they will be able to use the quantum twisting microscope in cryogenic conditions at the magic angle of 1.1°, where superconductivity occurs.

Pablo Jarillo Herrero, who led the team at MIT that first reported superconductivity in twisted bilayer graphene in 2018 but was not involved in this research describes it as an “interesting study” adding, “I’m looking forward to seeing more interesting results from low temperature QTM research!”

Hector Ochoa De Eguileor Romillo at Columbia University in the US, who proposed a role for phason–electron interactions in these materials in 2019, but was also not involved in this research describes it as “a beautiful experiment”. He adds, “I think it is fair to say that this is the most exciting experimental technique of the last 15 years or so in condensed matter physics; new interesting data are surely coming.”

The research is described in Nature.

The post Quantum twisting microscope measures phasons in cryogenic graphene appeared first on Physics World.

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量子扭曲显微镜 扭曲双层石墨烯 相位子 低温物理 电子-声子耦合
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