Abstract

A crystal structure has a profound influence on the physical properties of the corresponding material. By synthesizing crystals with particular symmetries, one can strongly tune their properties, even for the same chemical configuration (compare graphite and diamond, for instance). Even more interesting opportunities arise when the structural phases of crystals can be changed dynamically through external stimulations. Such abilities, though rare, lead to a number of exciting phenomena, such as phase-change memory effects. In the case of trilayer graphene, there are two common stacking configurations (ABA and ABC) that have distinct electronic band structures and exhibit very different behaviors. Domain walls exist in the trilayer graphene with both stacking orders, showing fascinating new physics such as the quantum valley Hall effect. Extensive efforts have been dedicated to the phase engineering of trilayer graphene. However, the manipulation of domain walls to achieve precise control of local structures and properties remains a considerable challenge. Here, we experimentally demonstrate that we can switch from one structural phase to another by laser irradiation, creating domains of different shapes in trilayer graphene. The ability to control the position and orientation of the domain walls leads to fine control of the local structural phases and properties of graphene, offering a simple but effective approach to create artificial two-dimensional materials with designed atomic structures and electronic and optical properties.

Highlights

  • The stacking configuration of layered materials plays an important role in determining their electronic and optical properties

  • The darker domain was identified as ABA-stacked trilayer graphene (TLG), and the brighter domain was identified as ABC stacking

  • The spectra are different from one another in at least three ways: first, the 2D band of ABC-stacked TLG shows more asymmetric features with an enhanced peak and shoulder compared with the symmetric feature shown in ABA-stacked TLG; second, the G band of the ABC-stacked domain is redshifted by ~1 cm−1 compared with that of the ABA-stacked domain; and third, the G’ band of the ABC-stacked TLG domain exhibits more asymmetric features than its ABAstacked counterpart[10,25,27]

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Summary

Introduction

The stacking configuration of layered materials plays an important role in determining their electronic and optical properties. Fascinating phenomena, such as Hofstadter’s butterfly, Mott insulators, ferromagnetism, and unconventional superconductivity, can emerge in van der Waals heterostructures by carefully controlling the layer stacking sequence[1,2,3,4,5,6,7,8]. Previous reports have shown that applying molecular absorption or an external electric field can drive the stacking order transition and generate domain wall motion in graphene layers[17,22,23]. Applying an electrical field or strain usually leads to global control of the stacking order phase and hinders precise manipulation of the local structure. A simple and controllable approach to engineer the stacking phase and domain walls into designed atomic structures is still lacking

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