/dports/math/openturns/openturns-1.18/python/src/ |
H A D | CenteredFiniteDifferenceHessian_doc.i.in | 27 f_k(x + \epsilon_i + \epsilon_j) - 28 f_k(x + \epsilon_i - \epsilon_j) + 29 f_k(x - \epsilon_i - \epsilon_j) - 30 f_k(x - \epsilon_i + \epsilon_j)} 31 {4 \epsilon_i \epsilon_j}
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/dports/science/dalton/dalton-66052b3af5ea7225e31178bf9a8b031913c72190/DALTON/test/cc2mm_atmvdw/ |
H A D | cc2mm_atmvdw.dal | 11 EPSMLT # (epsilon_ij=sqrt[epsilon_i*epsilon_j]: Option 2: .EPSADD)
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/dports/science/lammps/lammps-stable_29Sep2021/doc/src/ |
H A D | pair_gayberne.rst | 105 The :math:`\epsilon_i` and :math:`\epsilon_j` coefficients are actually 115 atom type J. If all three epsilon_j values are zero, they are ignored. 117 :math:`\epsilon_j` coefficients is to list their values in "pair_coeff
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H A D | pair_modify.rst | 94 \epsilon_{ij} = & \sqrt{\epsilon_i \epsilon_j} \\ 101 \epsilon_{ij} = & \sqrt{\epsilon_i \epsilon_j} \\ 108 …\epsilon_{ij} = & \frac{2 \sqrt{\epsilon_i \epsilon_j} \sigma_i^3 \sigma_j^3}{\sigma_i^6 + \sigma_…
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H A D | pair_resquared.rst | 118 The :math:`\epsilon_i` and :math:`\epsilon_j` coefficients are defined 130 :math:`\epsilon_j` coefficients is to list their values in "pair_coeff
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H A D | pair_lj_switch3_coulgauss_long.rst | 66 \epsilon_{ij} & = \sqrt{\epsilon_i \epsilon_j}
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/dports/math/gap/gap-4.11.0/pkg/homalg-2019.09.01/gap/ |
H A D | Complexes.gi | 398 …, j, dMj, dNj, mu, SyzygiesObjectEmb_j_M, SyzygiesObjectEmb_j_N, epsilonM, epsilonN, epsilon_j, Pj; 465 epsilon_j := CoproductMorphism( epsilonN, epsilonM ); 467 Pj := Source( epsilon_j ); 469 dEj := PreCompose( epsilon_j, mu ); 502 dj, SetEpi, Pj, dE, d_psi, d_phi, horse_shoe, mu, epsilon_j;
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/dports/misc/openmvg/openMVG-2.0/src/third_party/ceres-solver/docs/source/ |
H A D | automatic_derivatives.rst | 143 the property that :math:`\forall i, j\ :\epsilon_i\epsilon_j = 0`. Then 148 x = a + \sum_j v_{j} \epsilon_j
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/dports/math/ceres-solver/ceres-solver-2.0.0/docs/source/ |
H A D | automatic_derivatives.rst | 143 the property that :math:`\forall i, j\ :\epsilon_i\epsilon_j = 0`. Then 148 x = a + \sum_j v_{j} \epsilon_j
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/dports/science/nwchem/nwchem-7b21660b82ebd85ef659f6fba7e1e73433b0bd0a/src/rimp2_grad/doc/ |
H A D | rimp2-grad.tex | 569 2 \Ptwo_{ij} \left( \epsilon_j V^x_{ji} + \bra ip || jn \ket 584 2 \Ptwo_{ij} \left( \epsilon_j V^x_{ji} + \bra ip || jn \ket 617 2 \Ptwo_{ij} \epsilon_j V^x_{ji} \label{eqn:deriv1}\nonumber 625 2 \Ptwo_{ij} \epsilon_j V^x_{ji} \label{eqn:deriv1-ri}\nonumber 634 zero. Also, close examination of $L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j$ 645 \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + L^3_{ji} \right] 646 V^x_{ji} = \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + L^3_{ji} 697 \Wtwo_{ij} & = & -\half \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + 756 \Ptwo_{ij} \epsilon_j \\ 1025 \Ptwo_{ij} \epsilon_j \\
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/dports/science/nwchem-data/nwchem-7.0.2-release/src/rimp2_grad/doc/ |
H A D | rimp2-grad.tex | 569 2 \Ptwo_{ij} \left( \epsilon_j V^x_{ji} + \bra ip || jn \ket 584 2 \Ptwo_{ij} \left( \epsilon_j V^x_{ji} + \bra ip || jn \ket 617 2 \Ptwo_{ij} \epsilon_j V^x_{ji} \label{eqn:deriv1}\nonumber 625 2 \Ptwo_{ij} \epsilon_j V^x_{ji} \label{eqn:deriv1-ri}\nonumber 634 zero. Also, close examination of $L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j$ 645 \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + L^3_{ji} \right] 646 V^x_{ji} = \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + L^3_{ji} 697 \Wtwo_{ij} & = & -\half \left[ L^1_{ij} + 2 \Ptwo_{ij} \epsilon_j + 756 \Ptwo_{ij} \epsilon_j \\ 1025 \Ptwo_{ij} \epsilon_j \\
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/dports/biology/protomol/protomol/framework/frontend/ |
H A D | buildTopology.cpp | 560 Real epsilon_j = par.nonbondeds[bj].epsilon; in buildTopology() local 565 Real e_ij = sqrt(epsilon_i * epsilon_j); in buildTopology()
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/dports/science/gromacs/gromacs-2021.4/docs/reference-manual/topologies/ |
H A D | parameter-files.rst | 100 \epsilon_{ij} & = & \sqrt{\epsilon_i\,\epsilon_j}
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/dports/biology/protomol/protomol/applications/iSGProtomol-app/frontend/ |
H A D | buildISGTopology.cpp | 606 Real epsilon_j = par.nonbondeds[AtomJ].epsilon[identity_J]; in buildISGTopology() local 612 Real e_ij = sqrt(epsilon_i * epsilon_j); in buildISGTopology()
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/dports/math/gap/gap-4.11.0/lib/ |
H A D | algliess.gi | 687 ## x^{\alpha+\beta-\epsilon_i}D_j-{(\alpha+\beta-\epsilon_j)\choose(\beta)}* 688 ## x^{\alpha+\beta-\epsilon_j}D_i.
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/dports/science/py-pyscf/pyscf-2.0.1/doc_legacy/source/ |
H A D | tutorial.rst | 330 {\epsilon_i + \epsilon_j - \epsilon_a - \epsilon_b}
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/dports/security/helib/HElib-1.3.1/documentation/Design_Document/old/ |
H A D | he-library.tex | 1664 \sum_j \epsilon_j(X)\cdot\sk_j^{\;r_j}(X^{t_j})$ (with $a\in\A$). 1666 $\epsilon_j$'s behave as if they are chosen uniformly in the interval 1669 \EXP\left[\left|\epsilon_j(\tau_m)\right|^2\right] = \phi(m)\cdot p^2/12, 1672 $p^2/12$, and $\epsilon_j(\tau_m)$ is a sum of $\phi(m)$ such 1674 heuristically that the $\epsilon_j$'s are independent of the public 1678 = \sum_j \EXP\left[\left|\epsilon_j(\rho_m)\right|^2\right]
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/dports/science/dalton/dalton-66052b3af5ea7225e31178bf9a8b031913c72190/DALTON/test/trueresult/ |
H A D | cc2mm_atmvdw.ref | 175 EPSMLT # (epsilon_ij=sqrt[epsilon_i*epsilon_j]:
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/dports/science/dalton/dalton-66052b3af5ea7225e31178bf9a8b031913c72190/DALTON/test/cc2mm_atmvdw/result/ |
H A D | cc2mm_atmvdw.out | 195 EPSMLT # (epsilon_ij=sqrt[epsilon_i*epsilon_j]: Option 2: .EPSADD)
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