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@ -92,13 +92,13 @@ correctly, the time-averaged temperature and stress tensor of the
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particles will match the target values specified by Tstart/Tstop and
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Pstart/Pstop.
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</P>
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<P>The equations of motion used are those of Shinoda et al. in
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<P>The equations of motion used are those of Shinoda et al in
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<A HREF = "#Shinoda">(Shinoda)</A>, which combine the hydrostatic equations of
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Martyna, Tobias and Klein in <A HREF = "#Martyna">(Martyna)</A> with the strain
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energy proposed by Parrinello and Rahman in
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<A HREF = "#Parrinello">(Parrinello)</A>. The time integration schemes closely
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follow the time-reversible measure-preserving Verlet and
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rRESPA integrators derived by Tuckerman et al. in <A HREF = "#Tuckerman">(Tuckerman)</A>.
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<A HREF = "#Parrinello">(Parrinello)</A>. The time integration schemes closely
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follow the time-reversible measure-preserving Verlet and rRESPA
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integrators derived by Tuckerman et al. in <A HREF = "#Tuckerman">(Tuckerman)</A>.
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</P>
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<HR>
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@ -83,13 +83,13 @@ correctly, the time-averaged temperature and stress tensor of the
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particles will match the target values specified by Tstart/Tstop and
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Pstart/Pstop.
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The equations of motion used are those of Shinoda et al. in
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The equations of motion used are those of Shinoda et al in
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"(Shinoda)"_#Shinoda, which combine the hydrostatic equations of
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Martyna, Tobias and Klein in "(Martyna)"_#Martyna with the strain
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energy proposed by Parrinello and Rahman in
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"(Parrinello)"_#Parrinello. The time integration schemes closely
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follow the time-reversible measure-preserving Verlet and
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rRESPA integrators derived by Tuckerman et al. in "(Tuckerman)"_#Tuckerman.
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"(Parrinello)"_#Parrinello. The time integration schemes closely
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follow the time-reversible measure-preserving Verlet and rRESPA
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integrators derived by Tuckerman et al. in "(Tuckerman)"_#Tuckerman.
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:line
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