git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@5711 f3b2605a-c512-4ea7-a41b-209d697bcdaa

This commit is contained in:
sjplimp 2011-02-22 22:29:54 +00:00
parent 38cf9047ea
commit 46104f1588
4 changed files with 54 additions and 23 deletions

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@ -182,8 +182,24 @@ the method in <A HREF = "#Jaramillo-Botero">(Jaramillo-Botero)</A>.
<P>Work is underway to extend the eFF to higher Z elements with
increasingly non-spherical electrons (p-block and d-block), to provide
explicit terms for electron correlation/exchange, and to improve its
computational efficiency for atoms with a large number of core
electrons using core approximating pseudo-potentials.
computational efficiency via atom models with fixed 2 s core electrons
and atom models represented as pseudo-cores plus valence electrons.
</P>
<P>The current version adds support for models with fixed-core and
effective pseudo-core (i.e. effective core pseudopotentials, ECP)
definitions. to enable larger timesteps (i.e. by avoiding the high
frequency vibrational modes -translational and radial- of the 2 s
electrons), and in the ECP case to reduce the p-character effects in
higher Z elements (e.g. Silicon). A fixed-core should be defined with
a mass that includes the corresponding nuclear mass plus the 2 s
electrons in atomic mass units (2x5.4857990943e-4), and a radius
equivalent to that of minimized 1s electrons (see examples under
/examples/USER/eff/fixed-core). An pseudo-core should be described
with a mass that includes the corresponding nuclear mass, plus all the
core electrons (i.e no outer shell electrons), and a radius equivalent
to that of a corresponding minimized full-electron system. The charge
for a pseudo-core atom should be given by the number of outer shell
electrons.
</P>
<P>In general, eFF excels at computing the properties of materials in
extreme conditions and tracing the system dynamics over multi-picosend
@ -266,9 +282,9 @@ Dense Matter, Phys Rev Lett, 99:185003 (2007).
</P>
<A NAME = "Jaramillo-Botero"></A>
<P><B>(Jaramillo-Botero_2010)</B> Jaramillo-Botero, Su, Qi, Goddard,
Large-scale, Long-term Non-adiabatic Electron Molecular Dynamics for
Describing Material Properties and Phenomena in Extreme Environments,
to appear in J Comp Chem (2010).
<P><B>(Jaramillo-Botero)</B> Jaramillo-Botero, Su, Qi, Goddard, Large-scale,
Long-term Non-adiabatic Electron Molecular Dynamics for Describing
Material Properties and Phenomena in Extreme Environments, J Comp
Chem, 32, 497-512 (2011).
</P>
</HTML>

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@ -179,8 +179,24 @@ the method in "(Jaramillo-Botero)"_#Jaramillo-Botero.
Work is underway to extend the eFF to higher Z elements with
increasingly non-spherical electrons (p-block and d-block), to provide
explicit terms for electron correlation/exchange, and to improve its
computational efficiency for atoms with a large number of core
electrons using core approximating pseudo-potentials.
computational efficiency via atom models with fixed 2 s core electrons
and atom models represented as pseudo-cores plus valence electrons.
The current version adds support for models with fixed-core and
effective pseudo-core (i.e. effective core pseudopotentials, ECP)
definitions. to enable larger timesteps (i.e. by avoiding the high
frequency vibrational modes -translational and radial- of the 2 s
electrons), and in the ECP case to reduce the p-character effects in
higher Z elements (e.g. Silicon). A fixed-core should be defined with
a mass that includes the corresponding nuclear mass plus the 2 s
electrons in atomic mass units (2x5.4857990943e-4), and a radius
equivalent to that of minimized 1s electrons (see examples under
/examples/USER/eff/fixed-core). An pseudo-core should be described
with a mass that includes the corresponding nuclear mass, plus all the
core electrons (i.e no outer shell electrons), and a radius equivalent
to that of a corresponding minimized full-electron system. The charge
for a pseudo-core atom should be given by the number of outer shell
electrons.
In general, eFF excels at computing the properties of materials in
extreme conditions and tracing the system dynamics over multi-picosend
@ -257,12 +273,11 @@ If not specified, eradius_limit_flag = 0 and pressure_flag = 0.
:line
:link(Su)
[(Su)] Su and Goddard, Excited Electron Dynamics Modeling of Warm
Dense Matter, Phys Rev Lett, 99:185003 (2007).
:link(Jaramillo-Botero)
[(Jaramillo-Botero_2010)] Jaramillo-Botero, Su, Qi, Goddard,
Large-scale, Long-term Non-adiabatic Electron Molecular Dynamics for
Describing Material Properties and Phenomena in Extreme Environments,
to appear in J Comp Chem (2010).
[(Jaramillo-Botero)] Jaramillo-Botero, Su, Qi, Goddard, Large-scale,
Long-term Non-adiabatic Electron Molecular Dynamics for Describing
Material Properties and Phenomena in Extreme Environments, J Comp
Chem, 32, 497-512 (2011).

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@ -303,8 +303,8 @@ of analysis.
<LI>x,y,z = coordinates of atom
<LI>mux,muy,muz = direction of dipole moment of atom
<LI>quatw,quati,quatj,quatk = quaternion components for orientation of atom
<LI>spin = electron spin (+1/-1), 0 for nuclei
<LI>eradius = electron radius
<LI>spin = electron spin (+1/-1), 0 = nuclei, 2 = fixed-core, 3 = pseudo-cores (i.e. ECP)
<LI>eradius = electron radius (or fixed-core radius)
</UL>
<P>The units for these quantities depend on the unit style; see the
<A HREF = "units.html">units</A> command for details.
@ -704,11 +704,11 @@ style dipole or ellipsoid.
<P>where the keywords have these meanings:
</P>
<UL><LI>vx,vy,vz = translational velocity of atom
<LI>lx,ly,lz = angular momentum of aspherical atom
<LI>wx,wy,wz = angular velocity of granular atom
<LI>evel = electron radial velocity
</UL>
<P>vx,vy,vz = translational velocity of atom
lx,ly,lz = angular momentum of aspherical atom
wx,wy,wz = angular velocity of granular atom
evel = electron radial velocity (0 for fixed-core):ul
</P>
<P>The velocity lines can appear in any order. This section can only be
used after an <I>Atoms</I> section. This is because the <I>Atoms</I> section
must have assigned a unique atom ID to each atom so that velocities

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@ -282,8 +282,8 @@ volume = volume of atom (distance^3 units)
x,y,z = coordinates of atom
mux,muy,muz = direction of dipole moment of atom
quatw,quati,quatj,quatk = quaternion components for orientation of atom
spin = electron spin (+1/-1), 0 for nuclei
eradius = electron radius :ul
spin = electron spin (+1/-1), 0 = nuclei, 2 = fixed-core, 3 = pseudo-cores (i.e. ECP)
eradius = electron radius (or fixed-core radius) :ul
The units for these quantities depend on the unit style; see the
"units"_units.html command for details.
@ -619,7 +619,7 @@ where the keywords have these meanings:
vx,vy,vz = translational velocity of atom
lx,ly,lz = angular momentum of aspherical atom
wx,wy,wz = angular velocity of granular atom
evel = electron radial velocity :ul
evel = electron radial velocity (0 for fixed-core):ul
The velocity lines can appear in any order. This section can only be
used after an {Atoms} section. This is because the {Atoms} section