Current-Phase Relation of Ballistic Graphene Josephson Junctions

被引:64
|
作者
Nanda, G. [1 ]
Aguilera-Servin, J. L. [1 ,2 ]
Rakyta, P. [3 ]
Kormanyos, A. [4 ]
Kleiner, R. [5 ,6 ]
Koelle, D. [5 ,6 ]
Watanabe, K. [7 ]
Taniguchi, T. [7 ]
Vandersypen, L. M. K. [1 ,8 ]
Goswami, S. [1 ,8 ]
机构
[1] Delft Univ Technol, Kavli Inst Nanosci, NL-2600 GA Delft, Netherlands
[2] IST Austria, Campus 1, A-3400 Klosterneuburg, Austria
[3] Eotvos Lorand Univ, Dept Phys Complex Syst, Pazmany Peter Setany 1-A, H-1117 Budapest, Hungary
[4] Univ Konstanz, Dept Phys, D-78464 Constance, Germany
[5] Eberhard Karls Univ Tubingen, Phys Inst, Morgenstelle 14, D-72076 Tubingen, Germany
[6] Eberhard Karls Univ Tubingen, Ctr Quantum Sci CQ LISA, Morgenstelle 14, D-72076 Tubingen, Germany
[7] Natl Inst Mat Sci, 1-1 Namiki, Tsukuba, Ibaraki 3050044, Japan
[8] Delft Univ Technol, QuTech, NL-2600 GA Delft, Netherlands
关键词
Graphene; Josephson junctions; SQUID; current-phase relation;
D O I
10.1021/acs.nanolett.7b00097
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The current-phase relation (CPR) of a Josephson junction (JJ) determines how the supercurrent evolves with the superconducting phase difference across the junction. Knowledge of the CPR is essential in order to understand the response of a JJ to various external parameters. Despite the rising interest in ultra-clean encapsulated graphene JJs, the CPR of such junctions remains unknown. Here, we use a fully gate-tunable graphene superconducting quantum intereference device (SQUID) to determine the CPR of ballistic graphene JJs. Each of the two JJs in the SQUID is made with graphene encapsulated in hexagonal boron nitride. By independently controlling the critical current of the JJs, we can operate the SQUID either in a symmetric or asymmetric configuration. The highly asymmetric SQUID allows us to phase-bias one of the JJs and thereby directly obtain its CPR. The CPR is found to be skewed, deviating significantly from a sinusoidal form. The skewness can be tuned with the gate voltage and oscillates in anti-phase with Fabry-Perot resistance oscillations of the ballistic graphene cavity. We compare our experiments with tight-binding calculations which include realistic graphene-superconductor interfaces and find a good qualitative agreement.
引用
收藏
页码:3396 / 3401
页数:6
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