Ni_bulk1nm.mif2

# MIF 2.1
# a simple system of to illustrate the effect of temperature scaling in dependence of the cell size
# starting conditions are Mx = Ms, My = Mz = 0
# The temperature leads to a decrease of the magnetization
# make sure that the time step is small enough!
# for details see: 
#Temperature in micromagnetism: cell size and scaling effects of the stochastic Landau–Lifshitz equation
# https://doi.org/10.1088/2399-6528/ab31e6
# Marc Benjamin Hahn 2019 J. Phys. Commun. 3 075009

Destination archive1  mmArchive 
Schedule  DataTable archive1 Step 1

Destination archive2 mmArchive 
Schedule Oxs_TimeDriver::Magnetization archive2 Stage 1

Parameter temperatur 1850
Parameter damp 0.05
Parameter cells 1e-9
Parameter ani -5.7E3
Parameter dtime 1e-15

Specify Oxs_BoxAtlas:nickel "
  xrange {0 [expr {30*$cells}]}
  yrange {0 [expr {30*$cells}]}
  zrange {0 [expr {10*$cells}]}
"

Specify Oxs_RectangularMesh:mesh "
  cellsize {$cells $cells $cells}
  atlas :nickel
"


#specify exchange energies
Specify Oxs_Exchange6Ngbr {
  default_A 9e-12
  atlas nickel
  A {
    nickel nickel 9e-12
   }
}

Specify Oxs_Demag {}

Specify Oxs_CubicAnisotropy "
  K1 { Oxs_AtlasScalarField {
   atlas :nickel
    default_value -5.7E3
    values {
      nickel $ani
      }
    }}
   axis1 {1 0 0}
   axis2 {0 1 0}
"

# Specify a temperature and timestep you want to use
# make sure that the time step is small enough!
Specify UHH_ThetaEvolve "
  do_precess 1
  alpha $damp
	fixed_timestep $dtime
	temperature $temperatur
	uniform_seed 111
"



# specifiy evolver UHH_thetaevolve
Specify Oxs_TimeDriver [subst {
 basename ./NiThin_d"$damp"_c"$cells"_a"$ani"_dt"$dtime"_t"$temperatur"
 vector_field_output_format {binary 4}
 scalar_output_format %.15g
 evolver UHH_ThetaEvolve
 mesh :mesh
 stopping_time 5e-11
 stage_count 0
 Ms { Oxs_UniformScalarField  {value 490e3} }
 m0 { Oxs_UniformVectorField { norm 1  vector {1 0 0} } }
}
]