Changes to the NH fix enabling Cauchy stress control (Cauhchystat) due to Miller, Tadmor, Gibson, Bernstein and Pavia, J Chem Phys,
144, 184107 (2016).
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@ -54,6 +54,9 @@ keyword = {temp} or {iso} or {aniso} or {tri} or {x} or {y} or {z} or {xy} or {y
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{scaleyz} value = {yes} or {no} = scale yz with lz
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{scalexz} value = {yes} or {no} = scale xz with lz
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{flip} value = {yes} or {no} = allow or disallow box flips when it becomes highly skewed
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{cauchystat} cauchystat values = alpha continue
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alpha = strength of Cauchystat control parameter
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continue = {yes} or {no} = whether of not to continue from a previous run
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{fixedpoint} values = x y z
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x,y,z = perform barostat dilation/contraction around this point (distance units)
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{update} value = {dipole} or {dipole/dlm}
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@ -606,6 +609,39 @@ can only be used if the 2nd dimension in the keyword is periodic,
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and if the tilt factor is not coupled to the barostat via keywords
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{tri}, {yz}, {xz}, and {xy}.
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Without the {cauchystat} keyword, the barostat algorithm
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controls the Second-Piola Kirchhoff stress, which is a stress measure
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referred to the undeformed (initial) simulation box. If the box
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deforms substantially during the equilibration, the difference between
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the set values and the final true (Cauchy) stresses can be
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considerable.
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The {cauchystat} keyword modifies the barostat as per Miller et
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al. (Miller)_"#nh-Miller" so that the Cauchy stress is controlled.
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{alpha} is the non-dimensional parameter, typically set to 0.001 or
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0.01 that determines how aggresively the algorithm drives the system
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towards the set Cauchy stresses. Larger values of {alpha} will modify
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the system more quickly, but can lead to instabilities. Smaller
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values will lead to longer convergence time. Since {alpha} also
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influences how much the stress fluctuations deviate from the
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equilibrium fluctuations, it should be set as small as possible.
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A {continue} value of {yes} indicates that the fix is subsequent to a
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previous run with the Cauchystat fix, and the intention is to continue
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from the converged stress state at the end of the previous run. This
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may be required, for example, when implementing a multi-step loading/unloading
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sequence over several fixes.
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Setting {alpha} to zero is not permitted. To "turn off" the
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Cauchystat control and thus restore the equilibrium stress
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fluctuations, two subsequent fixes should be used. In the first, the
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Cauchystat is used and the simulation box equilibrates to the correct
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shape for the desired stresses. In the second, the {fix} statement is
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identical except that the {cauchystat} keyword is removed (along with
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related {alpha} and {continue} values). This restores the original
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Parrinello-Rahman algorithm, but now with the correct simulation box
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shape from the first fix.
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These fixes can be used with dynamic groups as defined by the
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"group"_group.html command. Likewise they can be used with groups to
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which atoms are added or deleted over time, e.g. a deposition
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@ -623,6 +659,7 @@ over time or the atom count becomes very small.
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The keyword defaults are tchain = 3, pchain = 3, mtk = yes, tloop =
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ploop = 1, nreset = 0, drag = 0.0, dilate = all, couple = none,
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cauchystat = no,
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scaleyz = scalexz = scalexy = yes if periodic in 2nd dimension and
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not coupled to barostat, otherwise no.
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@ -644,3 +681,7 @@ Martyna, J Phys A: Math Gen, 39, 5629 (2006).
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:link(nh-Dullweber)
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[(Dullweber)] Dullweber, Leimkuhler and McLachlan, J Chem Phys, 107,
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5840 (1997).
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:link(nh-Miller)
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[(Miller)] Miller, Tadmor, Gibson, Bernstein and Pavia, J Chem Phys,
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144, 184107 (2016).
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