Numéro |
J. Phys. I France
Volume 4, Numéro 4, April 1994
|
|
---|---|---|
Page(s) | 605 - 614 | |
DOI | https://doi.org/10.1051/jp1:1994164 |
J. Phys. I France 4 (1994) 605-614
Absence of inflation symmetric commensurate states in inflation symmetric networks
M. A. Itzler1, R. Bojko2 and P. M. Chaikin11 Department of Physics, Princeton University, Princeton, NJ 08544, U.S.A.
2 National Nanofabrication Facility, Cornell University, Ithaca, NY 14853, U.S.A.
(Received 14 September 1993, accepted 9 December 1993)
Abstract
In this paper we présent measurements of thé normal-to superconducting
phase boundary
Tc(H) for three différent networks possessing inflation
symmetry. Fluxoid quantization constraints induce thé formation of a
lattice of fluxoid quanta for any non-zéro perpendicular magnetic field,
and at particular fields,
Tc(H) exhibits cusp-like structure indicating
that thé lattice is commensurate with thé underlying network geometry.
For inflation symmetric networks studied in thé part, all commensurate
states have always been related to thé inflation symmetry. In thé three
networks studied here, none of thé commensurate phase boundary structure
derives from thé inflation symmetry. We propose that this structure can
instead be understood by considering thé Fourier transform of thé network
geometry and that thé transform actually provides a more universal
prescription for thé identification of commensurate states. The relevance
of thé transform (as opposed to thé inflation symmetry) in determining
commensurate states in two dimensions is consistent with analytical work
performed for one dimensional systems.
© Les Editions de Physique 1994