forked from lijiext/lammps
git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@12818 f3b2605a-c512-4ea7-a41b-209d697bcdaa
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@ -50,7 +50,8 @@ vibrational modes in the system to inexpensive (approximate)
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modelling of nuclear quantum effects. Contrary to
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modelling of nuclear quantum effects. Contrary to
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<A HREF = "fix_langevin.html">fix langevin</A>, this fix performs both
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<A HREF = "fix_langevin.html">fix langevin</A>, this fix performs both
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thermostatting and evolution of the Hamiltonian equations of motion, so it
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thermostatting and evolution of the Hamiltonian equations of motion, so it
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does not need to be used together with <A HREF = "fix_nve.html">fix nve</A>.
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should not be used together with <A HREF = "fix_nve.html">fix nve</A> -- at least not
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on the same atom groups.
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</P>
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</P>
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<P>Each degree of freedom in the thermostatted group is supplemented
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<P>Each degree of freedom in the thermostatted group is supplemented
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with Ns additional degrees of freedom s, and the equations of motion
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with Ns additional degrees of freedom s, and the equations of motion
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@ -93,6 +94,14 @@ generate its own unique seed and its own stream of random numbers.
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Thus the dynamics of the system will not be identical on two runs on
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Thus the dynamics of the system will not be identical on two runs on
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different numbers of processors.
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different numbers of processors.
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</P>
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</P>
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<P>Note also that the Generalized Langevin Dynamics scheme that is
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implemented by the <A HREF = "fix_gld.html">fix gld</A> scheme is closely related
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to the present one. In fact, it should be always possible to cast the
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Prony series form of the memory kernel used by GLD into an appropriate
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input matrix for <A HREF = "fix_gle.html">fix_gle</A>. While the GLE scheme is more
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general, the form used by <A HREF = "fix_gld.html">fix gld</A> can be more directly
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related to the representation of an implicit solvent environment.
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</P>
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<P><B>Restart, fix_modify, output, run start/stop, minimize info:</B>
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<P><B>Restart, fix_modify, output, run start/stop, minimize info:</B>
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</P>
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</P>
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<P>The instantaneous values of the extended variables are written to
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<P>The instantaneous values of the extended variables are written to
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@ -127,6 +136,11 @@ with rigid bodies, SHAKE or RATTLE. It is expected that all the
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thermostatted degrees of freedom are fully flexible, and the sampled
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thermostatted degrees of freedom are fully flexible, and the sampled
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ensemble will not be correct otherwise.
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ensemble will not be correct otherwise.
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</P>
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</P>
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<P>In order to perform constant-pressure simulations please use
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<A HREF = "fix_press_berendsen.html">fix press/berendsen</A>, rather than
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<A HREF = "fix_npt.html">fix_npt</A>, to avoid duplicate integration of the
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equations of motion.
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</P>
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<P>This fix is part of the USER-MISC package. It is only enabled if LAMMPS
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<P>This fix is part of the USER-MISC package. It is only enabled if LAMMPS
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was built with that package. See the <A HREF = "Section_start.html#start_3">Making
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was built with that package. See the <A HREF = "Section_start.html#start_3">Making
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LAMMPS</A> section for more info.
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LAMMPS</A> section for more info.
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@ -40,7 +40,8 @@ vibrational modes in the system to inexpensive (approximate)
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modelling of nuclear quantum effects. Contrary to
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modelling of nuclear quantum effects. Contrary to
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"fix langevin"_fix_langevin.html, this fix performs both
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"fix langevin"_fix_langevin.html, this fix performs both
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thermostatting and evolution of the Hamiltonian equations of motion, so it
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thermostatting and evolution of the Hamiltonian equations of motion, so it
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does not need to be used together with "fix nve"_fix_nve.html.
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should not be used together with "fix nve"_fix_nve.html -- at least not
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on the same atom groups.
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|
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Each degree of freedom in the thermostatted group is supplemented
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Each degree of freedom in the thermostatted group is supplemented
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with Ns additional degrees of freedom s, and the equations of motion
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with Ns additional degrees of freedom s, and the equations of motion
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@ -83,6 +84,14 @@ generate its own unique seed and its own stream of random numbers.
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Thus the dynamics of the system will not be identical on two runs on
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Thus the dynamics of the system will not be identical on two runs on
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different numbers of processors.
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different numbers of processors.
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|
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Note also that the Generalized Langevin Dynamics scheme that is
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implemented by the "fix gld"_fix_gld.html scheme is closely related
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to the present one. In fact, it should be always possible to cast the
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Prony series form of the memory kernel used by GLD into an appropriate
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input matrix for "fix_gle"_fix_gle.html. While the GLE scheme is more
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general, the form used by "fix gld"_fix_gld.html can be more directly
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related to the representation of an implicit solvent environment.
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|
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[Restart, fix_modify, output, run start/stop, minimize info:]
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[Restart, fix_modify, output, run start/stop, minimize info:]
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The instantaneous values of the extended variables are written to
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The instantaneous values of the extended variables are written to
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@ -117,6 +126,11 @@ with rigid bodies, SHAKE or RATTLE. It is expected that all the
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thermostatted degrees of freedom are fully flexible, and the sampled
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thermostatted degrees of freedom are fully flexible, and the sampled
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ensemble will not be correct otherwise.
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ensemble will not be correct otherwise.
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|
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In order to perform constant-pressure simulations please use
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"fix press/berendsen"_fix_press_berendsen.html, rather than
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"fix_npt"_fix_npt.html, to avoid duplicate integration of the
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equations of motion.
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|
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This fix is part of the USER-MISC package. It is only enabled if LAMMPS
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This fix is part of the USER-MISC package. It is only enabled if LAMMPS
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was built with that package. See the "Making
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was built with that package. See the "Making
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LAMMPS"_Section_start.html#start_3 section for more info.
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LAMMPS"_Section_start.html#start_3 section for more info.
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