4.6 Article

Microstructure and Anisotropic Order Parameter of Boron-Doped Nanocrystalline Diamond Films

Journal

CRYSTALS
Volume 12, Issue 8, Pages -

Publisher

MDPI
DOI: 10.3390/cryst12081031

Keywords

boron-doped diamond; superconductivity; grain boundaries; transmission electron microscopy; electrical transport; magnetoresistance; topological insulator

Funding

  1. CSIR-NLC
  2. National Research Foundation

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Unconventional superconductivity in heavily boron-doped nanocrystalline diamond films has attracted significant interest. The anisotropic superconducting order parameter in these films is believed to be due to the complex structure formed by boron atoms and the introduction of spin-orbit coupling. Breaking the structural symmetry in a layered microstructure reveals the signature of the anisotropic order parameter and explains various transport features observed in these films. The interface states in diamond films can be described by the Shockley model, forming a topologically protected system.
Unconventional superconductivity in heavily boron-doped nanocrystalline diamond films (HBDDF) produced a significant amount of interest. However, the exact pairing mechanism has not been understood due to a lack of understanding of crystal symmetry, which is broken at the grain boundaries. The superconducting order parameter (Delta) of HBDDF is believed to be anisotropic since boron atoms form a complex structure with carbon and introduce spin-orbit coupling to the diamond system. From ultra-high resolution transmission electron microscopy, the internal symmetry of the grain boundary structure of HBDDF is revealed, which can explain these films' unconventional superconducting transport features. Here, we show the signature of the anisotropic Delta in HBDDF by breaking the structural symmetry in a layered microstructure, enabling a Rashba-type spin-orbit coupling. The superlattice-like structure in diamond describes a modulation that explains strong insulator peak features observed in temperature-dependent resistance, a transition of the magnetic field-dependent resistance, and their oscillatory, as well as angle-dependent, features. Overall, the interface states of the diamond films can be explained by the well-known Shockley model describing the layers connected by vortex-like structures, hence forming a topologically protected system.

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