Merge branch 'DOI' of github.com:e-kwsm/lammps into doc-cleanup
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@ -41,7 +41,7 @@ coefficients.
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For the TIP4/Ice model (J Chem Phys, 122, 234511 (2005);
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http://dx.doi.org/10.1063/1.1931662) these values can be used:
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https://doi.org/10.1063/1.1931662) these values can be used:
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| O mass = 15.9994
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| H mass = 1.008
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@ -57,7 +57,7 @@ http://dx.doi.org/10.1063/1.1931662) these values can be used:
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For the TIP4P/2005 model (J Chem Phys, 123, 234505 (2005);
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http://dx.doi.org/10.1063/1.2121687), these values can be used:
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https://doi.org/10.1063/1.2121687), these values can be used:
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| O mass = 15.9994
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| H mass = 1.008
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@ -2339,8 +2339,8 @@ The expressions and their use are discussed in the following papers
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which discuss the `QuickFF <quickff_>`_ methodology.
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.. _vanduyfhuys2015: http://dx.doi.org/10.1002/jcc.23877
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.. _vanduyfhuys2018: http://dx.doi.org/10.1002/jcc.25173
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.. _vanduyfhuys2015: https://doi.org/10.1002/jcc.23877
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.. _vanduyfhuys2018: https://doi.org/10.1002/jcc.25173
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.. _quickff: http://molmod.github.io/QuickFF
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.. _yaff: https://github.com/molmod/yaff
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@ -193,7 +193,7 @@ Science, 117, 397-405 (2016).
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.. _Wicaksono2:
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**(Wicaksono2)** Wicaksono, figshare,
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https://dx.doi.org/10.6084/m9.figshare.1488628.v1 (2015).
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https://doi.org/10.6084/m9.figshare.1488628.v1 (2015).
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----------
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@ -203,19 +203,19 @@ the :doc:`dimension <dimension>` command, and nasr = 20.
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**(Campana)** C. Campana and
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M. H. Muser, *Practical Green's function approach to the
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simulation of elastic semi-infinite solids*\ , `Phys. Rev. B [74], 075420 (2006) <http://dx.doi.org/10.1103/PhysRevB.74.075420>`_
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simulation of elastic semi-infinite solids*\ , `Phys. Rev. B [74], 075420 (2006) <https://doi.org/10.1103/PhysRevB.74.075420>`_
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.. _Kong:
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**(Kong)** L.T. Kong, G. Bartels, C. Campana,
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C. Denniston, and Martin H. Muser, *Implementation of Green's
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function molecular dynamics: An extension to LAMMPS*\ , `Computer Physics Communications [180](6):1004-1010 (2009). <http://dx.doi.org/10.1016/j.cpc.2008.12.035>`_
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function molecular dynamics: An extension to LAMMPS*\ , `Computer Physics Communications [180](6):1004-1010 (2009). <https://doi.org/10.1016/j.cpc.2008.12.035>`_
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L.T. Kong, C. Denniston, and Martin H. Muser,
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*An improved version of the Green's function molecular dynamics
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method*\ , `Computer Physics Communications [182](2):540-541 (2011). <http://dx.doi.org/10.1016/j.cpc.2010.10.006>`_
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method*\ , `Computer Physics Communications [182](2):540-541 (2011). <https://doi.org/10.1016/j.cpc.2010.10.006>`_
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.. _Kong2011:
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**(Kong2011)** L.T. Kong, *Phonon dispersion measured directly from
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molecular dynamics simulations*\ , `Computer Physics Communications [182](10):2201-2207, (2011). <http://dx.doi.org/10.1016/j.cpc.2011.04.019>`_
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molecular dynamics simulations*\ , `Computer Physics Communications [182](10):2201-2207, (2011). <https://doi.org/10.1016/j.cpc.2011.04.019>`_
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@ -140,4 +140,4 @@ Related commands
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**(Anderson)** Anderson, Mukherjee, Critchley, Ziegler, and Lipton
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"POEMS: Parallelizable Open-source Efficient Multibody Software ",
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Engineering With Computers (2006). (`link to paper <http://dx.doi.org/10.1007/s00366-006-0026-x>`_)
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Engineering With Computers (2006). (`link to paper <https://doi.org/10.1007/s00366-006-0026-x>`_)
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@ -126,9 +126,14 @@ the work of :ref:`(Afshar) <Afshar>` and :ref:`(Phillips) <Phillips>`.
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.. note::
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The virial calculation for pressure when using this pair style
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The virial calculation for pressure when using these pair styles
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includes all the components of force listed above, including the
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random force.
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random force. Since the random force depends on random numbers,
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everything that changes the order of atoms in the neighbor list
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(e.g. different number of MPI ranks or a different neighbor list
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skin distance) will also change the sequence in which the random
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numbers are applied and thus the individual forces and therefore
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also the virial/pressure.
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----------
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@ -15,9 +15,9 @@ Syntax
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* distance = *min* or *mid*
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* zero or more keyword/value pairs may be appended
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* keyword = *exclude*
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.. parsed-literal::
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*bptype* value = atom type for bond particles
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*exclude* value = *yes* or *no*
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@ -31,7 +31,7 @@ Examples
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pair_coeff 1 2 none
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pair_coeff 2 2 srp 100.0 0.8
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pair_style hybrid dpd 1.0 1.0 12345 srp 0.8 \* min exclude yes
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pair_style hybrid dpd 1.0 1.0 12345 srp 0.8 * min exclude yes
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pair_coeff 1 1 dpd 60.0 50 1.0
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pair_coeff 1 2 none
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pair_coeff 2 2 srp 40.0
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@ -57,7 +57,7 @@ bond-pairwise potential, such that the force on bond *i* due to bond
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.. math::
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F^{SRP}_{ij} & = C(1-r/r_c)\hat{r}_{ij} \qquad r < r_c
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F^{\mathrm{SRP}}_{ij} = C(1-r/r_c)\hat{r}_{ij} \qquad r < r_c
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where *r* and :math:`\hat{r}_{ij}` are the distance and unit vector
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between the two bonds. Note that *btype* can be specified as an
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@ -70,8 +70,8 @@ lever rule,
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.. math::
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F_{i1}^{SRP} & = F^{SRP}_{ij}(L) \\
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F_{i2}^{SRP} & = F^{SRP}_{ij}(1-L)
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F_{i1}^{\mathrm{SRP}} & = F^{\mathrm{SRP}}_{ij}(L) \\
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F_{i2}^{\mathrm{SRP}} & = F^{\mathrm{SRP}}_{ij}(1-L)
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where *L* is the normalized distance from the atom to the point of
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closest approach of bond *i* and *j*\ . The *mid* option takes *L* as
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