Chiral Majorana edge states can survive in a 2D Dirac semimetal/superconductor heterostructure even after bulk Bogoliubov Fermi surfaces appear, because the inter-sublattice hopping vanishes at the edge momenta where the edge modes cross.
Identifying Bogoliubov Fermi surfaces via thermoelectric response in a $d$-wave superconductor heterostructure
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
We theoretically investigate the thermoelectric response of Bogoliubov Fermi surfaces (BFSs) generated in a two dimensional unconventional $d$-wave superconductor subjected to an external in-plane Zeeman field. These BFSs exhibiting the same dimension as the underlying normal state Fermi surface are topologically protected by combinations of discrete symmetries. Utilizing the Blonder-Tinkham-Klapwijk formalism and considering normal-$d$-wave superconductor hybrid junction, we compute the thermoelectric coefficients including thermal conductance, Seebeck coefficient, figure of merit ($zT$), and examine the validation of Widemann-Franz law in the presence of both voltage and temperature bias. Importantly, as a signature of anisotropic nature of $d$-wave pairing, Andreev bound states (ABSs) formed at the normal-superconductor interface play a significant role in the thermoelectric response. In the presence of ABSs, we observe a substantial enhancement in Seebeck coefficient ($\sim 200\,\mu$V/K) and $zT$ ($\sim 3.5$) due to the generation of the BFSs and thus making such setup a potential candidate for device applications. Finally, we strengthen our continuum model results by computing the thermoelectric coefficients based on a lattice-regularized version of our continuum model.
fields
cond-mat.mes-hall 1years
2024 1verdicts
CONDITIONAL 1representative citing papers
citing papers explorer
-
Coexistence of Chiral Majorana Edge States and Bogoliubov Fermi Surfaces in Two-Dimensional Nonsymmorphic Dirac Semimetal/Superconductor Heterostructures
Chiral Majorana edge states can survive in a 2D Dirac semimetal/superconductor heterostructure even after bulk Bogoliubov Fermi surfaces appear, because the inter-sublattice hopping vanishes at the edge momenta where the edge modes cross.