1997
DOI: 10.1063/1.119909
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Observation of coherent modes of Josephson vortices in Bi2Sr2CaCu2Ox

Abstract: We report strong evidence for coherent modes of moving Josephson vortices in mesas patterned on the surface of Bi2Sr2CaCu2Ox single crystals. The vortex flow current–voltage curves are characterized by a sharp up-turn and the appearance of multiple branches as the current is ramped up and down at a fixed magnetic field and temperature. These results are consistent with weakly damped motion of Josephson vortices in which different coherent modes can occur in a close stack of Josephson coupled multilayers.

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Cited by 46 publications
(31 citation statements)
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“…7,8,9 Note that these supercurrent sub-branches differ from the observed multiple quasiparticle branches 12,19,13 in the I-V data for LJJ stacks.…”
Section: Multiple Sub-branching Of Supercurrentmentioning
confidence: 74%
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“…7,8,9 Note that these supercurrent sub-branches differ from the observed multiple quasiparticle branches 12,19,13 in the I-V data for LJJ stacks.…”
Section: Multiple Sub-branching Of Supercurrentmentioning
confidence: 74%
“…(28) To observe these branches, a magnetic field, stronger than B ∼ H o , may be needed because of their stability conditions. Note that the appearance of these high velocity branches is expected when the interaction between the vortices is increased by the field, 8 suggesting that a complete sub-branch structure may be more easily obtained from the I-V characteristics of a LJJ stack with increasing microwave irradiation power (i.e., AC magnetic fields). 9 These results are consistent with the data 7,8,9 exhibiting supercurrent branch splitting.…”
Section: Multiple Sub-branching Of Supercurrentmentioning
confidence: 99%
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“…In a higher magnetic field of H=3.9 T as in the region (ii) of the main panel of Fig. 2, however, the single vortexflow branch splits into multiple vortex-flow sub-branches, which arise as a result of phase-locking of a Josephson vortex lattice on multiple SJP modes [14,15]. SJP oscillations in each mode, standing along the c axis, propagate along junctions with a characteristic collective mode velocity [7,8], c n = c 0 / 1 − cos[πn/(N + 1)].…”
mentioning
confidence: 99%