Two-dimensional (2D) materials, in general, allow the realization of unique quantum phenomena unattainable in the common three-dimensional (3D) world. A prime example is graphene. Transition metal dichalcogenides (TMDs) have a similar structure. Both can be stacked to form van der Waals heterostructures or can be exfoliated into single layers. But TMDs have an extra variety of excellent properties, including strong spin-orbit coupling and superconductivity.
In 2D (single atomic layer film) NbSe2, a prominent example of TMD, the combination of these two effects with the crystal symmetries leads to the so-called Ising superconductivity (IS), which can withstand extremely high magnetic fields oriented parallel to the crystal plane. Perhaps more exciting than this resilience against magnetic fields is the potential application of IS in realizing various exotic phenomena such as equal spin Andreev reflections, topological superconductivity, and Majorana fermions.
However, 2D structures are prone to degradation and impractical for applications. 3D materials are robust, easily scalable and accessible to a larger range of scientific analytical techniques. Therefore, it is desirable to find ways of protecting unique features of 2D materials in their 3D counterparts.









