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@ -182,8 +182,24 @@ the method in <A HREF = "#Jaramillo-Botero">(Jaramillo-Botero)</A>.
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<P>Work is underway to extend the eFF to higher Z elements with
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increasingly non-spherical electrons (p-block and d-block), to provide
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explicit terms for electron correlation/exchange, and to improve its
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computational efficiency for atoms with a large number of core
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electrons using core approximating pseudo-potentials.
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computational efficiency via atom models with fixed 2 s core electrons
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and atom models represented as pseudo-cores plus valence electrons.
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</P>
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<P>The current version adds support for models with fixed-core and
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effective pseudo-core (i.e. effective core pseudopotentials, ECP)
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definitions. to enable larger timesteps (i.e. by avoiding the high
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frequency vibrational modes -translational and radial- of the 2 s
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electrons), and in the ECP case to reduce the p-character effects in
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higher Z elements (e.g. Silicon). A fixed-core should be defined with
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a mass that includes the corresponding nuclear mass plus the 2 s
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electrons in atomic mass units (2x5.4857990943e-4), and a radius
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equivalent to that of minimized 1s electrons (see examples under
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/examples/USER/eff/fixed-core). An pseudo-core should be described
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with a mass that includes the corresponding nuclear mass, plus all the
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core electrons (i.e no outer shell electrons), and a radius equivalent
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to that of a corresponding minimized full-electron system. The charge
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for a pseudo-core atom should be given by the number of outer shell
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electrons.
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</P>
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<P>In general, eFF excels at computing the properties of materials in
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extreme conditions and tracing the system dynamics over multi-picosend
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@ -266,9 +282,9 @@ Dense Matter, Phys Rev Lett, 99:185003 (2007).
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</P>
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<A NAME = "Jaramillo-Botero"></A>
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<P><B>(Jaramillo-Botero_2010)</B> Jaramillo-Botero, Su, Qi, Goddard,
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Large-scale, Long-term Non-adiabatic Electron Molecular Dynamics for
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Describing Material Properties and Phenomena in Extreme Environments,
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to appear in J Comp Chem (2010).
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<P><B>(Jaramillo-Botero)</B> Jaramillo-Botero, Su, Qi, Goddard, Large-scale,
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Long-term Non-adiabatic Electron Molecular Dynamics for Describing
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Material Properties and Phenomena in Extreme Environments, J Comp
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Chem, 32, 497-512 (2011).
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</P>
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</HTML>
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@ -179,8 +179,24 @@ the method in "(Jaramillo-Botero)"_#Jaramillo-Botero.
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Work is underway to extend the eFF to higher Z elements with
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increasingly non-spherical electrons (p-block and d-block), to provide
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explicit terms for electron correlation/exchange, and to improve its
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computational efficiency for atoms with a large number of core
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electrons using core approximating pseudo-potentials.
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computational efficiency via atom models with fixed 2 s core electrons
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and atom models represented as pseudo-cores plus valence electrons.
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The current version adds support for models with fixed-core and
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effective pseudo-core (i.e. effective core pseudopotentials, ECP)
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definitions. to enable larger timesteps (i.e. by avoiding the high
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frequency vibrational modes -translational and radial- of the 2 s
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electrons), and in the ECP case to reduce the p-character effects in
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higher Z elements (e.g. Silicon). A fixed-core should be defined with
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a mass that includes the corresponding nuclear mass plus the 2 s
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electrons in atomic mass units (2x5.4857990943e-4), and a radius
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equivalent to that of minimized 1s electrons (see examples under
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/examples/USER/eff/fixed-core). An pseudo-core should be described
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with a mass that includes the corresponding nuclear mass, plus all the
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core electrons (i.e no outer shell electrons), and a radius equivalent
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to that of a corresponding minimized full-electron system. The charge
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for a pseudo-core atom should be given by the number of outer shell
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electrons.
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In general, eFF excels at computing the properties of materials in
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extreme conditions and tracing the system dynamics over multi-picosend
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@ -257,12 +273,11 @@ If not specified, eradius_limit_flag = 0 and pressure_flag = 0.
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:line
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:link(Su)
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[(Su)] Su and Goddard, Excited Electron Dynamics Modeling of Warm
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Dense Matter, Phys Rev Lett, 99:185003 (2007).
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:link(Jaramillo-Botero)
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[(Jaramillo-Botero_2010)] Jaramillo-Botero, Su, Qi, Goddard,
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Large-scale, Long-term Non-adiabatic Electron Molecular Dynamics for
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Describing Material Properties and Phenomena in Extreme Environments,
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to appear in J Comp Chem (2010).
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[(Jaramillo-Botero)] Jaramillo-Botero, Su, Qi, Goddard, Large-scale,
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Long-term Non-adiabatic Electron Molecular Dynamics for Describing
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Material Properties and Phenomena in Extreme Environments, J Comp
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Chem, 32, 497-512 (2011).
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@ -303,8 +303,8 @@ of analysis.
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<LI>x,y,z = coordinates of atom
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<LI>mux,muy,muz = direction of dipole moment of atom
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<LI>quatw,quati,quatj,quatk = quaternion components for orientation of atom
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<LI>spin = electron spin (+1/-1), 0 for nuclei
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<LI>eradius = electron radius
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<LI>spin = electron spin (+1/-1), 0 = nuclei, 2 = fixed-core, 3 = pseudo-cores (i.e. ECP)
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<LI>eradius = electron radius (or fixed-core radius)
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</UL>
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<P>The units for these quantities depend on the unit style; see the
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<A HREF = "units.html">units</A> command for details.
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@ -704,11 +704,11 @@ style dipole or ellipsoid.
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<P>where the keywords have these meanings:
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</P>
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<UL><LI>vx,vy,vz = translational velocity of atom
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<LI>lx,ly,lz = angular momentum of aspherical atom
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<LI>wx,wy,wz = angular velocity of granular atom
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<LI>evel = electron radial velocity
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</UL>
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<P>vx,vy,vz = translational velocity of atom
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lx,ly,lz = angular momentum of aspherical atom
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wx,wy,wz = angular velocity of granular atom
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evel = electron radial velocity (0 for fixed-core):ul
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</P>
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<P>The velocity lines can appear in any order. This section can only be
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used after an <I>Atoms</I> section. This is because the <I>Atoms</I> section
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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)
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x,y,z = coordinates of atom
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mux,muy,muz = direction of dipole moment of atom
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quatw,quati,quatj,quatk = quaternion components for orientation of atom
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spin = electron spin (+1/-1), 0 for nuclei
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eradius = electron radius :ul
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spin = electron spin (+1/-1), 0 = nuclei, 2 = fixed-core, 3 = pseudo-cores (i.e. ECP)
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eradius = electron radius (or fixed-core radius) :ul
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The units for these quantities depend on the unit style; see the
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"units"_units.html command for details.
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@ -619,7 +619,7 @@ where the keywords have these meanings:
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vx,vy,vz = translational velocity of atom
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lx,ly,lz = angular momentum of aspherical atom
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wx,wy,wz = angular velocity of granular atom
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evel = electron radial velocity :ul
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evel = electron radial velocity (0 for fixed-core):ul
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The velocity lines can appear in any order. This section can only be
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used after an {Atoms} section. This is because the {Atoms} section
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