modernize use of \it and \sf
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@ -139,11 +139,11 @@ mapped on to a third polar angle :math:`\theta_0` defined by,
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.. math::
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\theta_0 = {\sf rfac0} \frac{r-r_{min0}}{R_{ii'}-r_{min0}} \pi
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\theta_0 = \mathsf{rfac0} \frac{r-r_{min0}}{R_{ii'}-r_{min0}} \pi
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In this way, all possible neighbor positions are mapped on to a subset
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of the 3-sphere. Points south of the latitude :math:`\theta_0` =
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*rfac0* :math:`\pi` are excluded.
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of the 3-sphere. Points south of the latitude
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:math:`\theta_0 = \mathsf{rfac0} \pi` are excluded.
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The natural basis for functions on the 3-sphere is formed by the
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representatives of *SU(2)*, the matrices :math:`U^j_{m,m'}(\theta, \phi,
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@ -108,12 +108,12 @@ potential energy of the system as a function of the N atom
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coordinates:
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.. math::
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E(r_1,r_2, \ldots ,r_N) = & \sum_{i,j} E_{\it pair}(r_i,r_j) +
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\sum_{ij} E_{\it bond}(r_i,r_j) +
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\sum_{ijk} E_{\it angle}(r_i,r_j,r_k) + \\
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& \sum_{ijkl} E_{\it dihedral}(r_i,r_j,r_k,r_l) +
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\sum_{ijkl} E_{\it improper}(r_i,r_j,r_k,r_l) +
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\sum_i E_{\it fix}(r_i)
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E(r_1,r_2, \ldots ,r_N) = & \sum_{i,j} E_{pair}(r_i,r_j) +
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\sum_{ij} E_{bond}(r_i,r_j) +
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\sum_{ijk} E_{angle}(r_i,r_j,r_k) + \\
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& \sum_{ijkl} E_{dihedral}(r_i,r_j,r_k,r_l) +
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\sum_{ijkl} E_{improper}(r_i,r_j,r_k,r_l) +
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\sum_i E_{fix}(r_i)
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where the first term is the sum of all non-bonded :doc:`pairwise
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interactions <pair_style>` including :doc:`long-range Coulombic
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