TY - GEN
T1 - Cooperative behavior and manifestation of dimensional crossover in SISIS-type Nb-based structures
AU - Nevirkovets, Ivan P.
AU - Evetts, J. E.
AU - Blamire, Mark G.
PY - 1994
Y1 - 1994
N2 - We have fabricated and investigated three-terminal Nb/Al-AlOx-Nb/Al-AlOx-Nb tunnel devices with a thin (≈ 13 nm) Nb/Al middle layer. By measuring I-V characteristics and Ic vs. H dependences of the whole device and particular junctions separately, we have demonstrated strong interaction between the junctions. As a result, at V = 0 the system behaves like a single junction. The pronounced feature of this state is the critical current locking of the junctions, with a `common' critical current larger than the critical currents of the individual junctions. This state can be characterized by identical phase difference distributions for both junctions, and is stable at least for the region of superconducting current and magnetic field values corresponding to the first period of the diffraction pattern of the whole structure. At V = 0 and some value of magnetic field near to that where critical current of the system first falls to zero, the system undergoes a transition into the 2D state, in which the individual junctions have different phase distributions and behave relatively independently. In a high magnetic field, when many vortices enter the multilayer structure, along with the current locking, there is evidence of phase locking.
AB - We have fabricated and investigated three-terminal Nb/Al-AlOx-Nb/Al-AlOx-Nb tunnel devices with a thin (≈ 13 nm) Nb/Al middle layer. By measuring I-V characteristics and Ic vs. H dependences of the whole device and particular junctions separately, we have demonstrated strong interaction between the junctions. As a result, at V = 0 the system behaves like a single junction. The pronounced feature of this state is the critical current locking of the junctions, with a `common' critical current larger than the critical currents of the individual junctions. This state can be characterized by identical phase difference distributions for both junctions, and is stable at least for the region of superconducting current and magnetic field values corresponding to the first period of the diffraction pattern of the whole structure. At V = 0 and some value of magnetic field near to that where critical current of the system first falls to zero, the system undergoes a transition into the 2D state, in which the individual junctions have different phase distributions and behave relatively independently. In a high magnetic field, when many vortices enter the multilayer structure, along with the current locking, there is evidence of phase locking.
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U2 - 10.1117/12.179174
DO - 10.1117/12.179174
M3 - Conference contribution
AN - SCOPUS:0028730073
SN - 0819414522
SN - 9780819414526
T3 - Proceedings of SPIE - The International Society for Optical Engineering
SP - 363
EP - 372
BT - Proceedings of SPIE - The International Society for Optical Engineering
PB - Publ by Society of Photo-Optical Instrumentation Engineers
T2 - Superconducting Superlattices and Multilayers
Y2 - 24 January 1994 through 25 January 1994
ER -