2006/04/30 by C. W. J. Beenakker · 17 citations
Materials Science · Physics and Astronomy · #Andreev reflection #Condensed matter physics #Electron #Fermi level #Graphene #Graphene research and applications #Physics #Quantum and electron transport phenomena #Quantum mechanics #Reflection (computer programming) #Specular reflection #Superconductivity #Topological Materials and Phenomena #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevlett.97.067007
published as Phys. Rev. Lett. 97, 067007 (2006) · 7 pages, 6 figures; version 3: added an appendix with details of the calculation
arxiv created 2006/05/19 · openalex publication_date 2006/08/10 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
By combining the Dirac equation of relativistic quantum mechanics with the Bogoliubov-de Gennes equation of superconductivity we investigate the electron-hole conversion at a normal-metal-superconductor interface in graphene. We find that the Andreev reflection of Dirac fermions has several unusual features: (1) the electron and hole occupy different valleys of the band structure; (2) at normal incidence the electron-hole conversion happens with unit efficiency in spite of the large mismatch in Fermi wavelengths at the two sides of the interface; and, most fundamentally: (3) away from normal incidence the reflection angle may be the same as the angle of incidence (retroreflection) or it may be inverted (specular reflection). Specular Andreev reflection dominates in weakly doped graphene, when the Fermi wavelength in the normal region is large compared to the superconducting coherence length.