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        <title>potfit wiki - interactions</title>
        <description>open source force-matching</description>
        <link>https://www.potfit.net/wiki/</link>
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            <title>potfit wiki</title>
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        <item>
            <title>adp</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:adp&amp;rev=1516639689</link>
            <description>Angular Dependent Potentials

----------

The angular dependent potentials were developed for the Fe-Ni system. It is a generalization of the EAM model for the simulation of the covalent component of bonding.

The angular dependent potential (ADP) for $$E_{\text{total}}=\frac{1}{2}\sum_{i,j(j\neq i)}^N\Phi_{ij}(r_{ij})+\sum_iF_i(n_i)+\frac{1}{2}\sum_{i,\alpha}(\mu_i^\alpha)^2+\frac{1}{2}\sum_{i,\alpha,\beta}(\lambda_i^{\alpha\beta})^2-\frac{1}{6}\sum_i\nu_i^2$$$i$$j$$\alpha,\beta=1,2,3$$$\mu_i^\…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 22 Jan 2018 16:48:09 +0000</pubDate>
        </item>
        <item>
            <title>angular_coulomb_potentials</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:angular_coulomb_potentials&amp;rev=1515233929</link>
            <description>Angular Coulomb Potentials

----------


Info:
This page is incomplete and may contain invalid/wrong information!


The angular coulomb potentials are a combination of the regular coulomb potentials and a angular dependent term similar to MEAM:

$$
V=V_{Coulomb}+\frac{1}{2}\sum f_{ij}(r_{ij})f_{ik}(r_{ik})g_i(\cos(\theta_{ijk}))
$$

Number of potential functions
$N$$N(N+2)$$\phi_{ij}$$f_{ij}$$g_i$$N$$N(N+1)/2$$N(N+1)/2$$N$$N(N+2)$$N$$\phi_{00}, \ldots, \phi_{0N}, \phi_{11}, \ldots, \phi_{1N}, \l…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 06 Jan 2018 10:18:49 +0000</pubDate>
        </item>
        <item>
            <title>angular_pair_potentials</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:angular_pair_potentials&amp;rev=1515233094</link>
            <description>Angular Pair Potentials

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The angular pair potentials are a combination of the regular pair potentials and a angular dependent term similar to MEAM:

$$
V=\frac{1}{2}\sum\phi_{ij}(r_{ij})+\frac{1}{2}\sum f_{ij}(r_{ij})f_{ik}(r_{ik})g_i(\cos(\theta_{ijk}))
$$

With this approach it is possible to fit potentials such as this one here.

Or it can be used to consider non-bonded angular interactions as DL_POLY does for the three-body terms (see &#039;tbp&#039; interaction, p. 174 in the $f_{ij} = 1$…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 06 Jan 2018 10:04:54 +0000</pubDate>
        </item>
        <item>
            <title>coulomb</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:coulomb&amp;rev=1521473362</link>
            <description>Coulomb Interactions

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Electrostatics can be enabled with the coulomb option. A charge $q$, which has to be given 
in the potential file, is assigned to each atom type. The coulomb interaction of a set of $N$ ions
is calculated as
$$E_\text{total}^\text{Coul} = \frac{1}{2} \sum_{i\neq j} E(r_{ij}) \qquad \text{with} \qquad
E(r_{ij}) \sim \frac{q_{i}q_{j}}{r_{ij}}.$$

There are three modifications required for a proper numerical calculation.$$E_\text{total}^\text{Coul} = \frac{1}{2} \s…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 19 Mar 2018 15:29:22 +0000</pubDate>
        </item>
        <item>
            <title>dipole</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:dipole&amp;rev=1515601628</link>
            <description>Dipole Interactions

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To enable the calculation of electric dipole moments, potfit has to be compiled with the dipole
option. The dipole $\vec P_{i,n}$ of atom $i$ in iteration step 
$n$ is then calculated self-consistently by the use of the Tangney-Scandolo potential model$$\vec P_{i,n} =  \vec P_{i,\text{NF}} + \vec P_{i,\text{IND}}$$$$\vec P_{i,\text{NF}} = \alpha \sum\limits_{j \neq i} \frac{q_j \vec r_{ij}}{r_{ij}^3} f_{ij}$$$$\vec P_{i,\text{IND}} = \alpha \vec E (\vec P_{j,n-1}…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Wed, 10 Jan 2018 16:27:08 +0000</pubDate>
        </item>
        <item>
            <title>eam_elstat</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:eam_elstat&amp;rev=1635179554</link>
            <description>EAM + electrostatic potential

----------


Info:
This page is incomplete and may contain invalid/wrong information!


The EAM + electrostatic potential is a combination of the regular EAM model with an additional coulomb term.

$$
E_{tot}=E_{EAM} + \frac{1}{2} \sum_{i\neq j} E(r_{ij}) \quad \text{with} \quad
E(r_{ij}) \sim \frac{q_{i}q_{j}}{r_{ij}}
$$

Number of potential functions
$N$$N(N+5)/2$$\Phi_{ij}$$\rho_j$$F_i$$N$$N(N+1)/2$$N$$N$$N(N+5)/2$$\Phi_{00}, \ldots, \Phi_{0N}, \Phi_{11}, \ldots…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 25 Oct 2021 16:32:34 +0000</pubDate>
        </item>
        <item>
            <title>eam</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:eam&amp;rev=1542903577</link>
            <description>Embedded Atom Method (EAM) Potentials

----------

The energy in potentials of the Embedded Atom type consists of two parts, a pair potential 
term specified by the function $\Phi(r)$ representing the electrostatic core-core repulsion, 
and a cohesive term specified by the function $F(n)$$\rho(r)$$F_i(n)$$\rho_j(r)$$j$$\Phi_{ij}(r)$$i$$j$$$E_\text{total}=\frac{1}{2}\sum_{i&lt;j}^N\Phi_{ij}(r_{ij})+\sum_iF_i(n_i)\qquad\text{where}\qquad n_i=\sum_{j\neq i}\rho_j(r_{ij})$$$\Phi_{ij}(r_{ij})$$F_i(n_i)$…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Thu, 22 Nov 2018 16:19:37 +0000</pubDate>
        </item>
        <item>
            <title>main</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:main&amp;rev=1537804091</link>
            <description>Interactions

----------

potfit supports various short and long range effective potentials. These potentials are defined either by tabulated functions or analytic parameters and are read from a potential file. The supported potentials can be found in the table below.</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 24 Sep 2018 15:48:11 +0000</pubDate>
        </item>
        <item>
            <title>meam</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:meam&amp;rev=1538028034</link>
            <description>MEAM Potentials

----------

The energy in potentials of the Modified Embedded Atom type behaves like the EAM type and 
consists of two parts, a pair potential term specified by the function $\Phi\left(r\right)$
representing the electrostatic core-core repulsion, and a cohesive term specified by the 
function $F\left(n\right)$$\rho\left(r\right)$$f\left(r\right)$$g\left(\cos\theta\right)$$F_i\left(n\right)$$g_i\left(\cos\theta\right)$$\rho_j\left(r\right)$$\Phi_{ij}\left(r\right)$$f_{ij}\left(r\…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Thu, 27 Sep 2018 06:00:34 +0000</pubDate>
        </item>
        <item>
            <title>pair_potentials</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:pair_potentials&amp;rev=1537804143</link>
            <description>Pair Potentials

----------

The most simple interaction that can be used are pair potentials.
They are assumed to be isotropic, i.e. they only depend on the pair distance
$r_{ij}=|\boldsymbol{r}_j-\boldsymbol{r}_i|$ of the two atoms $i$ and $j$. The potential energy for a system
described by pair interactions is given as
$$  E_\text{total} = \frac{1}{2} \sum_{i\neq j}V_2(\boldsymbol{r}_i,\boldsymbol{r}_j) = \sum_{i&lt;j}V_2(r_{ij}) $$$\boldsymbol{F}_i$$i$$$  \boldsymbol{F}_i = - \sum_{j}\nabla_iV_…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 24 Sep 2018 15:49:03 +0000</pubDate>
        </item>
        <item>
            <title>sidebar</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:sidebar&amp;rev=1550911578</link>
            <description>Main page

----------

Download

Publications

Contact

About potfit

User Guide

	*  Compiling potfit
	*  Options
	*  Running potfit
	*  Parameters
	*  Configuration files
	*  Potential models
	*  Potential files
	*  Interactions
		*  Pair potentials
		*  Angular pair potentials
		*  Angular Coulomb potentials
		*  EAM
		*  Two band EAM
		*  MEAM
		*  ADP
		*  Coulomb (pair)
		*  Dipole (pair)
		*  EAM + electrostatics
		*  Stillinger-Weber
		*  Tersoff
		*  modified Tersoff

	*  Algorithms
	* …</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 23 Feb 2019 08:46:18 +0000</pubDate>
        </item>
        <item>
            <title>stiweb</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:stiweb&amp;rev=1515231549</link>
            <description>Stillinger-Weber Potentials

----------

The Stillinger-Weber potential
is available when potfit is compiled with the stiweb flag, which also implies the apot
flag for analytic potentials.

Basic Theory

The total potential energy is defined as

$$E_{\text{total}}=\sum_{i&lt;j}V_2(r_{ij}) + \sum_{\substack{i\neq j,k\\j&lt;k}}V_3(r_{ij},r_{ik},r_{jk}),$$

$V_2$$V_3$$$V_2(r_{ij}) = \left(A_{ij}r_{ij}^{-p_{ij}}-B_{ij}r_{ij}^{-q_{ij}}\right)\exp\left(\frac{\delta_{ij}}{r_{ij}-a_{ij}}\right)$$$$V_3(r_{ij},…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 06 Jan 2018 09:39:09 +0000</pubDate>
        </item>
        <item>
            <title>tbeam</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:tbeam&amp;rev=1516639643</link>
            <description>Two band EAM Potentials

----------

Basic Theory

The two band EAM potentials are an extension to the regular EAM potentials. Instead
of single transfer and embedding functions, different functions to model two bands are used.
Usually they are reffered to as d- and s-band contributions.$$E_\text{total}=\frac{1}{2}\sum_{i&lt;j}^N\Phi_{ij}(r_{ij})+\sum_iF_i^d(n_i^d)+\sum_iF_i^s(n_i^s)$$$$n^d_i=\sum_{j\neq i}\rho^d_j(r_{ij}) \qquad \text{and} \qquad n^s_i=\sum_{j\neq i}\rho^s_j(r_{ij})$$$N$$N(N+9)/2$…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Mon, 22 Jan 2018 16:47:23 +0000</pubDate>
        </item>
        <item>
            <title>tersoff</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:tersoff&amp;rev=1515231549</link>
            <description>Tersoff Potentials

----------

The Tersoff potential
is available when potfit is compiled with the tersoff flag, which also implies 
the apot flag for analytic potentials.

Basic Theory

The total potential energy is defined as

$$E_{\text{total}}=
\frac{1}{2}\sum_{i,j}f_c(r_{ij})\left(A_{ij}e^{-\lambda_{ij}r_{ij}}+b_{ij}B_{ij}
e^{-\mu_{ij}r_{ij}}\right)$$

where

$$b_{ij} = \chi_{ij}\left(1+\gamma_{ij}^{n_i}\zeta_{ij}^{n_i}\right)^{-\frac{1}{2n_i}},$$

$$\zeta_{ij} = \sum_{k\neq i,j}f_c(r_{ik}…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 06 Jan 2018 09:39:09 +0000</pubDate>
        </item>
        <item>
            <title>tersoffmod</title>
            <link>https://www.potfit.net/wiki/doku.php?id=interactions:tersoffmod&amp;rev=1515231549</link>
            <description>modified Tersoff Potential

----------

The modified Tersoff potential
is available when potfit is compiled with the tersoffmod flag, which also implies 
the apot flag for analytic potentials.

Basic Theory

The total potential energy is defined as$$E_{\text{total}}=
\frac{1}{2}\sum_{i,j}f_c(r_{ij})\left(A_{ij}e^{-\lambda_{ij}r_{ij}}+b_{ij}B_{ij}
e^{-\mu_{ij}r_{ij}}\right)$$$$b_{ij} = \left(1+\zeta_{ij}^{\eta}\right)^{-\delta},$$$$\zeta_{ij} = \sum_{k\neq i,j}f_c(r_{ik})g(\theta_{ijk})\exp[\alph…</description>
            <author>anonymous@undisclosed.example.com (Anonymous)</author>
            <pubDate>Sat, 06 Jan 2018 09:39:09 +0000</pubDate>
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