| /dports/science/liggghts/LIGGGHTS-PUBLIC-3.8.0-26-g6e873439/doc/Eqs/ |
| H A D | pair_zbl.tex | 6 …E^{ZBL}_{ij} & = & \frac{1}{4\pi\epsilon_0} \frac{Z_i Z_j \,e^2}{r_{ij}} \phi(r_{ij}/a)+ S(r_{ij})…
|
| /dports/science/lammps/lammps-stable_29Sep2021/src/KOKKOS/ |
| H A D | pair_tersoff_zbl_kokkos.h | 156 … bigr=0;bigd=0;lam1=0;biga=0;cutsq=0;c1=0;c2=0;c3=0;c4=0;Z_i=0;Z_j=0;ZBLcut=0;ZBLexpscale=0;}; in params_ters()
159 … bigr=0;bigd=0;lam1=0;biga=0;cutsq=0;c1=0;c2=0;c3=0;c4=0;Z_i=0;Z_j=0;ZBLcut=0;ZBLexpscale=0;}; in params_ters()
161 bigd, lam1, biga, cutsq, c1, c2, c3, c4, Z_i, Z_j, ZBLcut, ZBLexpscale; member
|
| H A D | pair_tersoff_zbl_kokkos.cpp | 159 k_params.h_view(i,j,k).Z_i = params[m].Z_i; in setup_params()
405 (pow(paramskk(itype,jtype,jtype).Z_i,0.23) + pow(paramskk(itype,jtype,jtype).Z_j,0.23)); in operator ()()
406 … const F_FLOAT premult = (paramskk(itype,jtype,jtype).Z_i * paramskk(itype,jtype,jtype).Z_j * esq)/ in operator ()()
604 (pow(paramskk(itype,jtype,jtype).Z_i,0.23) + pow(paramskk(itype,jtype,jtype).Z_j,0.23)); in operator ()()
605 … const F_FLOAT premult = (paramskk(itype,jtype,jtype).Z_i * paramskk(itype,jtype,jtype).Z_j * esq)/ in operator ()()
|
| /dports/science/R-cran-eco/eco/src/ |
| H A D | macros.h | 55 double** Z_i; //CCAR: k x 2
|
| H A D | gibbsEM.c | 740 double **Z_i=doubleMatrix(k,2); in ecoMStepCCAR() local
765 Z_i[i][j]=params[ii].caseP.Z_i[i][j]; in ecoMStepCCAR()
766 Z_i_t[i][j]=params[ii].caseP.Z_i[j][i]; in ecoMStepCCAR()
769 matrixMul(Z_i,InvSigma,k,2,2,2,tmpk2); in ecoMStepCCAR()
797 Z_i_t[i][j]=params[ii].caseP.Z_i[j][i]; in ecoMStepCCAR()
|
| /dports/science/lammps/lammps-stable_29Sep2021/potentials/ |
| H A D | SiC.gw.zbl | 10 #E1 E2 E3 m gamma lambda3 c d h n beta lambda2 B R D lambda1 A Z_i, Z_j, ZBLcut, ZBLexpscale
|
| /dports/science/lammps/lammps-stable_29Sep2021/lib/gpu/ |
| H A D | lal_tersoff_zbl.h | 48 const double* powern, const double* Z_i, const double* Z_j,
|
| H A D | lal_tersoff_zbl.cpp | 56 const double* beta, const double* powern, const double* Z_i, in init() argument
198 dview[i].x=static_cast<numtyp>(Z_i[i]); in init()
|
| /dports/science/openkim-models/openkim-models-2021-01-28/simulator-models/Sim_LAMMPS_GWZBL_Samolyuk_2016_SiC__SM_720598599889_000/ |
| H A D | SiC.gw.zbl | 10 #E1 E2 E3 m gamma lambda3 c d h n beta lambda2 B R D lambda1 A Z_i, Z_j, ZBLcut, ZBLexpscale
|
| /dports/science/lammps/lammps-stable_29Sep2021/doc/src/ |
| H A D | pair_edip.rst | 46 …{3}(R_{ij}, R_{ik}, Z_i) = & exp{\left(\frac{\gamma}{R_{ij}-a}\right)}exp{\left(\frac{\gamma}{R_{…
47 Z_i = & \sum_{m \ne i} f(R_{im}) \qquad
|
| H A D | pair_vashishta.rst | 63 …U_{ij}^{(2)} (r) & = \frac{H_{ij}}{r^{\eta_{ij}}} + \frac{Z_i Z_j}{r}\exp(-r/\lambda_{1,ij}) - \…
128 * :math:`Z_i` (electron charge units)
162 The parameters :math:`Z_i` and :math:`Z_j` are also classified
|
| /dports/science/lammps/lammps-stable_29Sep2021/src/MANYBODY/ |
| H A D | pair_gw.h | 50 double Z_i, Z_j; member
|
| H A D | pair_tersoff.h | 52 double Z_i, Z_j; // added for TersoffZBL member
|
| H A D | pair_extep.h | 51 double Z_i, Z_j; // added for ExTePZBL member
|
| /dports/math/py-statsmodels/statsmodels-0.13.1/statsmodels/tsa/statespace/ |
| H A D | kalman_smoother.py | 1432 Z_i = get_mat('design', t_i)
1433 tmp1[:, i:i + 1] = acov @ Z_i[k_i:k_i + 1].T
1448 Z_i = get_mat('design', t_i)
1454 Z_i[k_i:k_i + 1] @ acov @ Z_j[k_j:k_j + 1].T)
|
| /dports/science/openkim-models/openkim-models-2021-01-28/model-drivers/SNAP__MD_536750310735_000/ |
| H A D | README.md | 88 Element_i Element_j zbl Z_i Z_j
92 The values of `Z_i` and `Z_j` are equal to the atomic numbers of the two atom types.
|
| H A D | README | 139 Element_i Element_j zbl Z_i Z_j
143 respectively. The values of `Z_i` and `Z_j` are equal to the atomic numbers
|
| /dports/finance/R-cran-gmm/gmm/man/ |
| H A D | tsls.Rd | 26 …de{\link{lm}} is used to regress \eqn{X_i} on the set of instruments \eqn{Z_i}. The second step a…
|
| /dports/cad/py-lcapy/lcapy-23c940f/doc/ |
| H A D | circuits.tex | 1091 gain $A_r$, input impedance, $Z_i$, and output admittance, $Y_o$.
1097 Z_i & = & Z_{11} = \frac{A_{11}}{A_{21}}, \\
1107 & = & \frac{1}{A_f} - \frac{A_{12}}{Z_i}.
1111 A_{12} = \encp{\frac{1}{A_f} - A_r} Z_i.
1115 A_{11} = A_{12} Y_o = \encp{\frac{1}{A_f} - A_r} Z_i Y_o.
1119 A_{21} = \frac{A_{11}}{Z_i} = \encp{\frac{1}{A_f} - A_r} Y_o.
|
| /dports/misc/openmvg/openMVG-2.0/docs/sphinx/rst/openMVG/cameras/ |
| H A D | cameras.rst | 72 Z_i\\
|
| /dports/science/py-cirq-aqt/Cirq-0.12.0/docs/tutorials/educators/ |
| H A D | qaoa_ising.ipynb | 246 "E = -\\sum_{\\langle i,j \\rangle} Z_i Z_j - \\sum_i h_i Z_i,\n",
274 … \\prod_{\\langle i,j\\rangle}e^{-i\\pi\\gamma Z_iZ_j/2} \\prod_i e^{-i\\pi \\gamma h_i Z_i/2}.\n",
441 …"Now that we know how to implement both $Z_i Z_j$ and $Z_i$, we can implement the full $U(\\gamma,…
459 …"The Ising Model is particularly simple because the nearest-neighbor interaction $Z_i Z_j$ is alre…
1321 …so that instead of $\\exp(i\\pi \\gamma Z_i Z_j/2)$ for that edge you would have $\\exp(i\\pi \\ga…
1357 …"The Ising Model with transverse field replaces the $\\sum h_i Z_i$ term with a $\\sum h_i X_i$ te…
|
| /dports/science/py-cirq-ionq/Cirq-0.13.1/docs/tutorials/educators/ |
| H A D | qaoa_ising.ipynb | 246 "E = -\\sum_{\\langle i,j \\rangle} Z_i Z_j - \\sum_i h_i Z_i,\n",
274 … \\prod_{\\langle i,j\\rangle}e^{-i\\pi\\gamma Z_iZ_j/2} \\prod_i e^{-i\\pi \\gamma h_i Z_i/2}.\n",
441 …"Now that we know how to implement both $Z_i Z_j$ and $Z_i$, we can implement the full $U(\\gamma,…
459 …"The Ising Model is particularly simple because the nearest-neighbor interaction $Z_i Z_j$ is alre…
1321 …so that instead of $\\exp(i\\pi \\gamma Z_i Z_j/2)$ for that edge you would have $\\exp(i\\pi \\ga…
1357 …"The Ising Model with transverse field replaces the $\\sum h_i Z_i$ term with a $\\sum h_i X_i$ te…
|
| /dports/science/py-cirq-pasqal/Cirq-0.13.1/docs/tutorials/educators/ |
| H A D | qaoa_ising.ipynb | 246 "E = -\\sum_{\\langle i,j \\rangle} Z_i Z_j - \\sum_i h_i Z_i,\n",
274 … \\prod_{\\langle i,j\\rangle}e^{-i\\pi\\gamma Z_iZ_j/2} \\prod_i e^{-i\\pi \\gamma h_i Z_i/2}.\n",
441 …"Now that we know how to implement both $Z_i Z_j$ and $Z_i$, we can implement the full $U(\\gamma,…
459 …"The Ising Model is particularly simple because the nearest-neighbor interaction $Z_i Z_j$ is alre…
1321 …so that instead of $\\exp(i\\pi \\gamma Z_i Z_j/2)$ for that edge you would have $\\exp(i\\pi \\ga…
1357 …"The Ising Model with transverse field replaces the $\\sum h_i Z_i$ term with a $\\sum h_i X_i$ te…
|
| /dports/science/py-cirq-core/Cirq-0.13.1/docs/tutorials/educators/ |
| H A D | qaoa_ising.ipynb | 246 "E = -\\sum_{\\langle i,j \\rangle} Z_i Z_j - \\sum_i h_i Z_i,\n",
274 … \\prod_{\\langle i,j\\rangle}e^{-i\\pi\\gamma Z_iZ_j/2} \\prod_i e^{-i\\pi \\gamma h_i Z_i/2}.\n",
441 …"Now that we know how to implement both $Z_i Z_j$ and $Z_i$, we can implement the full $U(\\gamma,…
459 …"The Ising Model is particularly simple because the nearest-neighbor interaction $Z_i Z_j$ is alre…
1321 …so that instead of $\\exp(i\\pi \\gamma Z_i Z_j/2)$ for that edge you would have $\\exp(i\\pi \\ga…
1357 …"The Ising Model with transverse field replaces the $\\sum h_i Z_i$ term with a $\\sum h_i X_i$ te…
|
| /dports/science/py-cirq-google/Cirq-0.13.0/docs/tutorials/educators/ |
| H A D | qaoa_ising.ipynb | 246 "E = -\\sum_{\\langle i,j \\rangle} Z_i Z_j - \\sum_i h_i Z_i,\n",
274 … \\prod_{\\langle i,j\\rangle}e^{-i\\pi\\gamma Z_iZ_j/2} \\prod_i e^{-i\\pi \\gamma h_i Z_i/2}.\n",
441 …"Now that we know how to implement both $Z_i Z_j$ and $Z_i$, we can implement the full $U(\\gamma,…
459 …"The Ising Model is particularly simple because the nearest-neighbor interaction $Z_i Z_j$ is alre…
1321 …so that instead of $\\exp(i\\pi \\gamma Z_i Z_j/2)$ for that edge you would have $\\exp(i\\pi \\ga…
1357 …"The Ising Model with transverse field replaces the $\\sum h_i Z_i$ term with a $\\sum h_i X_i$ te…
|