At mean-field level, positive gradient stiffness favours a spatially uniform order parameter. Writing , minimization of gives
with arbitrary constant . The minimized density is zero above the transition and below it. The order parameter vanishes continuously as ; the first derivative of the minimized free energy is continuous while the second changes. This is the continuous mean-field transition.
The broken symmetry is global U(1) symmetry, not merely the Ising sign symmetry. Selecting one ordered phase breaks this continuous symmetry and leaves a soft phase direction. These are minima of the supplied Landau free energy, not an exact finite-temperature long-range-order claim in one dimension: phase fluctuations invalidate that inference for a short-range one-dimensional system.[ref]
Set and . The trial density is . At fixed , its minimum is if and otherwise, with density . Minimizing uses
For , minimizes the quadratic coefficient. For , the minima are at and have . Thus
Everywhere else the minimum is ; at the transition boundary the ordered amplitude tends to zero. The zero-field minimum is respectively or in the two ordered regions. For the helical solution is lower than a uniform ordered extremum whenever the latter exists, and lower than the disordered state whenever its amplitude is nonzero. The assumed positive-amplitude ansatz must allow its zero-amplitude boundary to describe disorder.
The phase remains arbitrary because the functional has global U(1) symmetry. At nonzero , a translation shifts that phase; separate translation and phase operations retain a combined unbroken subgroup. The two signs of also select opposite handedness. The meeting point of the uniform, modulated and disordered mean-field regions is the Lifshitz point .
Figure 1.
Uniform, helical and disordered minima of the specified complex Landau free energy
. Details.