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For the first time semifluxons were observed using d-wave superconductors at so called tricrystal grain boundaries and later in YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub>–Nb ramp zigzags. In these systems the phase shift of π takes place inside the d-wave superconductor
For the first time semifluxons were observed using d-wave superconductors at so called tricrystal grain boundaries and later in YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub>–Nb ramp zigzags. In these systems the phase shift of π takes place inside the d-wave superconductor
and not at the barrier. Due to the advent of controlled coupling by proper chosen ferromagnetic thicknesses,
and not at the barrier. Due to the advent of controlled coupling by proper chosen ferromagnetic thicknesses,
0–π JJs have also recently been realized in low-T<sub>c</sub> SFS-like systems.
0–π JJs have also recently been realized in low-T<sub>c</sub> SFS-like systems and underdamped SIFS-type Josephson junctions [http://xxx.arxiv.org/cond-mat/0605656].


==References==
==References==

Revision as of 12:29, 5 October 2006

In superconductivity, a Semifluxon is a vortex of supercurrent carrying the magnetic flux equal to the half of the magnetic flux quantum. Semifluxons exist in the so-called 0-π long Josephson junctions at the boundary between 0 and π regions.

For the first time semifluxons were observed using d-wave superconductors at so called tricrystal grain boundaries and later in YBa2Cu3O7–Nb ramp zigzags. In these systems the phase shift of π takes place inside the d-wave superconductor and not at the barrier. Due to the advent of controlled coupling by proper chosen ferromagnetic thicknesses, 0–π JJs have also recently been realized in low-Tc SFS-like systems and underdamped SIFS-type Josephson junctions [1].

References

  • J. H. Xu, J. H. Miller, Jr., and C. S. Ting (1994). "π-vortex state in a long 0-π Josephson junction". Phys. Rev. B. 51: 11958. doi:10.1103/PhysRevB.51.11958.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  • C. C. Tsuei and J. R. Kirtley (2002). "d-Wave pairing symmetry in cuprate superconductors --- fundamental implications and potential applications". Physica C. 367: 1.
  • H. Hilgenkamp, Ariando, H.-J. H. Smilde, D. H. A. Blank, G. Rijnders, H. Rogalla, J. R. Kirtley and C. C. Tsuei, (2003). "Ordering and manipulation of the magnetic moments in large-scale superconducting π-loop arrays". Nature (London). 442: 50.{{cite journal}}: CS1 maint: extra punctuation (link) CS1 maint: multiple names: authors list (link)
  • M. L. Della Rocca, M. Aprili, T. Kontos, A. Gomez and P. Spatkis, (2005). "Ferromagnetic 0-π Junctions as Classical Spins". Phys. Rev. Lett. 94: 197003.{{cite journal}}: CS1 maint: extra punctuation (link) CS1 maint: multiple names: authors list (link)