2008
DOI: 10.1103/physrevb.78.024504
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Self-consistent solution for proximity effect and Josephson current in ballistic graphene SNS Josephson junctions

Abstract: We use a tight-binding Bogoliubov-de Gennes (BdG) formalism to self-consistently calculate the proximity effect, Josephson current, and local density of states in ballistic graphene SNS Josephson junctions. Both short and long junctions, with respect to the superconducting coherence length, are considered, as well as different doping levels of the graphene. We show that self-consistency does not notably change the current-phase relationship derived earlier for short junctions using the non-selfconsistent Dirac… Show more

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Cited by 99 publications
(130 citation statements)
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“…17 Subsequently, numerous other theoretical works investigated the Josephson current in SGS structures. 14,[18][19][20][21][22][23] The tunneling effect in SG structures has been studied in several works [24][25][26][27][28] as well. Other works in the field of graphene-superconductor heterostructures include studies on crossed Andreev reflection in a graphene bipolar transistor, 29,30 on s-and d-wave SG junctions 31,32 and on ferromagnetic SG structures.…”
Section: Introductionmentioning
confidence: 99%
“…17 Subsequently, numerous other theoretical works investigated the Josephson current in SGS structures. 14,[18][19][20][21][22][23] The tunneling effect in SG structures has been studied in several works [24][25][26][27][28] as well. Other works in the field of graphene-superconductor heterostructures include studies on crossed Andreev reflection in a graphene bipolar transistor, 29,30 on s-and d-wave SG junctions 31,32 and on ferromagnetic SG structures.…”
Section: Introductionmentioning
confidence: 99%
“…Theoretically, it is expected 13,26 that a JJG can carry a non-zero supercurrent even at the CNP, where the charge density is tuned to zero. In this case, the I c R n product is nearly constant as B2D/e with V bg in a ballistic short junction 13 , which is in essence the Ambegaokar-Baratoff relation 14 ; in a diffusive long junction, it is given by aE Th /e (refs 11,27), where E Th is the Thouless energy and a is a coefficient depending on E Th /D.…”
mentioning
confidence: 99%
“…In contrast to traditional JJ, in which the weak links are insulators, normal metals (N) or constrictions, a superconductor/graphene/superconductor (SGS) JJ consists of a ballistic, 2D relativistic system with gate-tunable conductance [11][12][13][14]. Several unusual phenomena were predicted to arise in this novel system, such as specular Andreev reflection [15], novel propagating modes of Andreev electrons [16] and oscillation of tunneling probability with barrier width [17].…”
mentioning
confidence: 99%