Updated and simplified documentation
This commit is contained in:
@ -13,7 +13,7 @@ min_modify command :h3
|
||||
min_modify keyword values ... :pre
|
||||
|
||||
one or more keyword/value pairs may be listed :ulb,l
|
||||
keyword = {dmax} or {line} or {norm} or {alpha_damp} or {discrete_factor}
|
||||
keyword = {dmax} or {line} or {norm} or {alpha_damp} or {discrete_factor} or {integrator} or {tmax}
|
||||
{dmax} value = max
|
||||
max = maximum distance for line search to move (distance units)
|
||||
{line} value = {backtrack} or {quadratic} or {forcezero} or {spin_cubic} or {spin_none}
|
||||
@ -25,38 +25,17 @@ keyword = {dmax} or {line} or {norm} or {alpha_damp} or {discrete_factor}
|
||||
{alpha_damp} value = damping
|
||||
damping = fictitious Gilbert damping for spin minimization (adim)
|
||||
{discrete_factor} value = factor
|
||||
factor = discretization factor for adaptive spin timestep (adim) :pre
|
||||
:ule
|
||||
|
||||
these keywords apply only to the "min_style"_min_style.html {fire2} :ulb,l
|
||||
keyword = {integrator} or {tmax} or {tmin} or {delaystep} or {dtgrow} or {dtshrink}
|
||||
or {alpha0} or {alphashrink} or {halfstepback} or {initialdelay} or {vdfmax}
|
||||
{integrator} arg = {eulerimplicit} or {eulerexplicit} or {verlet}
|
||||
eulerimplicit,eulerexplicit,verlet = integration scheme
|
||||
{tmax} arg = coef
|
||||
coef = factor defining the maximum timestep
|
||||
{tmin} arg = coef
|
||||
coef = factor defining the minimum timestep
|
||||
{delaystep} arg = delay
|
||||
delay = number of steps for dynamics delay
|
||||
{dtgrow} arg = grow
|
||||
grow = factor increasing the timestep
|
||||
{dtshrink} arg = shrink
|
||||
shrink = factor decreasing the timestep
|
||||
{alpha0} arg = alpha
|
||||
alpha = coefficient mixing velocities and forces
|
||||
{alphashrink} arg = shrink
|
||||
shrink = factor decreasing alpha
|
||||
{vdfmax} arg = max
|
||||
max = maximum number of consecutive iterations with P(t) < 0 before forced interruption
|
||||
{halfstepback} arg = {yes} or {no}
|
||||
{initialdelay} arg = {yes} or {no} :pre
|
||||
factor = discretization factor for adaptive spin timestep (adim)
|
||||
{integrator} value = {eulerimplicit} or {eulerexplicit} or {verlet}
|
||||
time integration scheme for fire2 minimization
|
||||
{tmax} value = factor
|
||||
factor = maximum adaptive timestep for fire2 minimization :pre
|
||||
:ule
|
||||
|
||||
[Examples:]
|
||||
|
||||
min_modify dmax 0.2
|
||||
min_modify integrator verlet tmax 0.4 :pre
|
||||
min_modify integrator verlet tmax 4 :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
@ -142,20 +121,23 @@ The {spin_none} is a default value for {line} keyword for both {spin/lbfgs}
|
||||
and {spin/cg}. Convergence of {spin/lbfgs} can be more robust if
|
||||
{spin_cubic} line search is used.
|
||||
|
||||
The style {fire2} has several parameters that can be tuned in order
|
||||
to optimize the relaxation: {integrator}, {tmax}, {tmin}, {delaystep}, {dtgrow}, {dtshrink},
|
||||
{alpha0}, and {alphashrink}.
|
||||
Different Newton {integrator} can be selected: explicit Euler,
|
||||
semi-implicit Euler (= symplectic Euler) and velocity Verlet.
|
||||
The parameters {tmax} and {tmin} define the maximum and minimum timestep
|
||||
allowed during an fire2 minimization. Those are not in time unit, but are
|
||||
multiplication factor applied to the "timestep"_timestep.html. Thus
|
||||
{tmax} = 10.0 in metal "units"_units.html means that the maximum value
|
||||
the timestep can be reached during the relaxation is 10 fs (with the default
|
||||
"timestep"_timestep.html value).
|
||||
Note that even with the default parameters being chosen to be reliable in most
|
||||
cases, adjusting "timestep"_timestep.html, {tmax} and {tmin} should be consider
|
||||
to optimize the minimization, in particular for large/complex system.
|
||||
The Newton {integrator} used for {fire2} minimization can be selected to be
|
||||
either the symplectic Euler ({eulerimplicit}), explicit Euler (eulerexplicit)
|
||||
or velocity Verlet ({verlet}). Note that explicit Euler is not recommended
|
||||
as it will lead to results similar to a {fire} minimization.
|
||||
{tmax} define the maximum value for the adaptive timestep
|
||||
during a {fire2} minimization. It is multiplication factor applied
|
||||
to the current "timestep"_timestep.html (not in time unit). For example,
|
||||
{tmax} = 4.0 in metal "units"_units.html means that the maximum value
|
||||
the timestep can reach during a minimization is 4fs (with the default
|
||||
"timestep"_timestep.html value). Note that parameters defaults has been
|
||||
chosen to be reliable in most cases, but one should consider adjusting
|
||||
"timestep"_timestep.html and {tmax} to optimize the minimization for large
|
||||
or complex systems.
|
||||
Others parameters of the {fire2} minimization can be tuned ({tmin}, {delaystep},
|
||||
{dtgrow}, {dtshrink}, {alpha0}, and {alphashrink}). Please refer to the article
|
||||
describing the {fire2} "min_style"_min_style.html.
|
||||
|
||||
An additional stopping criteria {vdfmax} is added in order to avoid unnecessary looping
|
||||
when it is reasonable to think the system will not be relaxed further.
|
||||
Note that in this case the system will NOT be relaxed. This could
|
||||
|
||||
@ -62,9 +62,8 @@ the velocity non-parallel to the current force vector. The velocity
|
||||
of each atom is initialized to 0.0 by this style, at the beginning of
|
||||
a minimization.
|
||||
|
||||
Style {fire2} is a re-implementation of the style {fire} with
|
||||
additional optimizations of the method described
|
||||
in "(Bitzek)"_#Bitzek, including different time integration schemes.
|
||||
Style {fire2} is an optimization of the style {fire}, including different
|
||||
time integration schemes, described in "(Guenole)"_#Guenole.
|
||||
|
||||
Style {spin} is a damped spin dynamics with an adaptive
|
||||
timestep.
|
||||
@ -142,3 +141,6 @@ Jonsson, Mills, Jacobsen.
|
||||
[(Bitzek)] Bitzek, Koskinen, Gahler, Moseler, Gumbsch, Phys Rev Lett,
|
||||
97, 170201 (2006).
|
||||
|
||||
:link(Guenole)
|
||||
[(Guenole)] Guenole, Nöhring, Vaid, Houllé, Xie, Prakash, Bitzek,
|
||||
Preprint, arXiv:190802038 (2019).
|
||||
|
||||
Reference in New Issue
Block a user