15–20 Jun 2014
Laurentian University / Université Laurentienne
America/Toronto timezone
Welcome to the 2014 CAP Congress! / Bienvenue au congrès de l'ACP 2014!

Andreev quantum dots in graphene/superconductor hybrid devices

18 Jun 2014, 13:45
30m
C-204 (Laurentian University / Université Laurentienne)

C-204

Laurentian University / Université Laurentienne

Sudbury, Ontario
Invited Speaker / Conférencier invité Condensed Matter and Materials Physics / Physique de la matière condensée et matériaux (DCMMP-DPMCM) (W2-1) Low Dimensional Systems - DCMMP / Systèmes de basse dimension - DPMCM

Speaker

Dr Lucian Covaci (University of Antwerp, Belgium)

Description

Although graphene is not intrinsically superconducting, Cooper pairs from a superconducting contact can diffuse through it. The superconducting proximity effect was observed experimentally in graphene Josephson junctions with contacts made of various superconducting materials like Al, Pb, Nb and even layered materials like NbSe$_2$ [1,2]. When the energy of the electrons in the graphene layer is below the superconducting gap of the contacts, they will be bound in the normal region. These are the well known Andreev bound states. We consider a graphene layer deposited on top of a superconducting surface such that the graphene layer can be considered to be partially freestanding and/or strained. It was recently shown that strain has a peculiar effect on the electronic properties in graphene, namely that it will coupled exactly like a gauge field [3,4]. Under certain conditions it is thus possible to have strong pseudo-magnetic fields and even pseudo-Landau levels coexisting with superconducting correlations [5]. By using an efficient numerical method [6] we solve the Bogoliubov-de Gennes equations for a tight binding model of the graphene layer. We show that in the regions where the sheet is freestanding, bound states due to Andreev reflections appear, thus forming Andreev quantum dots. We provide various ways to manipulate the energy states inside the dots, and further more devise inter-dot coupling. [1] H. B. Heersche, P. Jarillo-Herrero, J. B. Oostinga, L. M. K. Vandersypen, and A. F. Morpurgo, Nature (London) 446, 56 (2007). [2] A. Kanda, T. Sato, H. Goto, H. Tomori, S. Takana, Y. Ootuka, and K. Tsukagoshi, Physica C 470, 1477 (2010). [3] F. Guinea, M. I. Katsnelson, and A. K. Geim, Nat. Phys. 6, 30 (2009). [4] N. Levy, S. A. Burke, K. L. Meaker, M. Panlasigui, A. Zettl, F. Guinea, A. H. C. Neto, and M. F. Crommie, Science 29, 544 (2010). [5] L. Covaci and F. M. Peeters, Phys. Rev. B 84, 241401(R) (2011). [6] L. Covaci, F. M. Peeters, and M. Berciu, Phys. Rev. Lett. 105, 167006 (2010).

Author

Dr Lucian Covaci (University of Antwerp, Belgium)

Presentation materials