A Maciolek 1996 J. Phys. A: Math. Gen. 29 3837 doi:10.1088/0305-4470/29/14/011
Ising strip with opposite surface fields
A Maciolek
Show affiliationsWe obtain an exact solution of the d = 2 infinite
Ising strip with surface fields of opposite signs
,
. Earlier predictions by Parry et al are confirmed of the crucial importance of wetting for a system confined between two parallel walls that exert competitive surface fields. The transition of the magnetization profile m(z) from the partial wetting regime below the critical wetting temperature at a single wall
with a surface field
, to the soft-mode single phase in the temperature range
, where
is the critical temperature of the bulk system, is described in detail. A scaling ansatz is verified for the singular part of the surface excess free energy,
and for the profile,
. The modification of the magnetization profile near one wall, due to wetting, is studied. Near the (-) wall at
the profile is found to be a linear function of the scaled distance but its slope is different than for the case of perfect asymmetry system
hence these two cases belong to the different universality regime.
05.50.+q Lattice theory and statistics (Ising, Potts, etc.)
75.30.Kz Magnetic phase boundaries (including magnetic transitions, metamagnetism, etc.)
75.60.Ej Magnetization curves, hysteresis, Barkhausen and related effects
82B26 Phase transitions (general)
82B20 Lattice systems (Ising, dimer, Potts, etc.) and systems on graphs
Condensed matter: electrical, magnetic and optical
Issue 14 (21 July 1996)
Received 17 May 1995, in final form 8 February 1996
Ising strip with opposite surface fields
A Maciolek 1996 J. Phys. A: Math. Gen. 29 3837
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