/dports/science/py-GPy/GPy-1.10.0/GPy/inference/latent_function_inference/ |
H A D | pep.py | 30 sigma_n = likelihood.gaussian_variance(Y_metadata) 31 if sigma_n.size >1: 45 sigma_star = sigma_n + self.alpha * (Knn - np.sum(np.square(LiUT),0)) 68 0.5*np.sum(np.square(b)) + 0.5*alpha_const_term*num_data*np.log(sigma_n) 87 dL_dthetaL += 0.5*alpha_const_term*num_data / sigma_n
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H A D | fitc.py | 28 sigma_n = likelihood.gaussian_variance(Y_metadata) 29 if sigma_n.size >1: 43 sigma_star = Knn + sigma_n - np.sum(np.square(LiUT),0)
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/dports/science/liggghts/LIGGGHTS-PUBLIC-3.8.0-26-g6e873439/src/ |
H A D | mesh_module_stress.cpp | 408 sigma_n(i) = vectorDot3D(f(i),surfNorm); in calc_total_force() 411 vectorScalarMult3D(surfNorm,sigma_n(i),temp); in calc_total_force() 417 sigma_n(i) = MathExtraLiggghts::abs(sigma_n(i)); in calc_total_force() 421 sigma_n(i) *= invSurfArea; in calc_total_force()
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H A D | mesh_module_stress.h | 135 inline double& sigma_n(int i)
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H A D | dump_mesh.cpp | 670 … vtkDoubleArray *sigma_n = static_cast<vtkDoubleArray*>(cell_attributes.back().GetPointer()); in prepare_mbSet() local 671 sigma_n->SetName("normal_stress_average"); in prepare_mbSet() 673 sigma_n->InsertNextValue(sigma_n_[iMesh]->get(iTri)); in prepare_mbSet()
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/dports/science/py-ase/ase-3.22.0/ase/test/forcefields/ |
H A D | test_rattle_linear.py | 5 sigma_me, sigma_c, sigma_n, 16 sigma = np.array([sigma_me, sigma_c, sigma_n])
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H A D | test_qmmm_acn.py | 6 sigma_me, sigma_c, sigma_n, 19 sigma = np.array([sigma_me, sigma_c, sigma_n])
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/dports/astro/py-astropy/astropy-5.0/docs/timeseries/ |
H A D | bls.rst | 66 y_\mathrm{in} = \frac{\sum_\mathrm{in} y_n/{\sigma_n}^2}{\sum_\mathrm{in} 1/{\sigma_n}^2} 68 where :math:`y_n` are the brightness measurements, :math:`\sigma_n` are the 76 y_\mathrm{out} = \frac{\sum_\mathrm{out} y_n/{\sigma_n}^2}{\sum_\mathrm{out} 1/{\sigma_n}^2} 85 -\frac{1}{2}\,\sum_\mathrm{in}\frac{(y_n-y_\mathrm{in})^2}{{\sigma_n}^2} 86 -\frac{1}{2}\,\sum_\mathrm{out}\frac{(y_n-y_\mathrm{out})^2}{{\sigma_n}^2}
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/dports/math/octave/octave-6.4.0/scripts/linear-algebra/ |
H A D | cond.m | 72 sigma_n = sigma(end); variable 73 if (sigma_1 == 0 || sigma_n == 0) 76 retval = sigma_1 / sigma_n;
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/dports/graphics/opencv/opencv-4.5.3/contrib/modules/xphoto/src/ |
H A D | inpainting_fsr.impl.hpp | 83 double sigma_n = tmp_stddev[0] / 255; in icvStandardDeviation() local 84 if (sigma_n < 0) in icvStandardDeviation() 86 sigma_n = 0; in icvStandardDeviation() 88 else if (sigma_n > 1) in icvStandardDeviation() 90 sigma_n = 1; in icvStandardDeviation() 92 return sigma_n; in icvStandardDeviation() 323 double sigma_n = icvStandardDeviation(distorted_block_2d, error_mask_2d); in icvGetTodoBlocks() local 324 sigma_n_array.at<double>( yblock_counter, xblock_counter) = sigma_n; in icvGetTodoBlocks() 327 if (sigma_n < homo_threshold) in icvGetTodoBlocks()
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/dports/science/lammps/lammps-stable_29Sep2021/doc/src/ |
H A D | fix_wall_ees.rst | 71 \sigma_{n}^5 \left(r^2-\sigma_{n}^2\right)} \right]\qquad \sigma_n 77 the particle and wall no longer interact. Also, :math:`\sigma_n` is 107 You must insure that r is always bigger than :math:`\sigma_n` for 110 position *coord* (:math:`r = \sigma_n`) or with particles penetrating 111 the wall (:math:`0 =< r < \sigma_n`) or with particles on the wrong
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/dports/math/cado-nfs/cado-nfs-f4284e2391121b2bfb97bc4880b6273c7250dc2f/sieve/ecm/ |
H A D | cofac_utils.sage | 158 sigma_n = (W - sigma_d) # u1 159 sigma2_n = sigma_n^2 # u2 165 beta_n = 4*sigma_n # u7 169 gamma = (sigma_n - sigma_d)*(sigma_n + 5*sigma_d)*(sigma2_n + 5*sigma2_d) 173 t2 = 2*V*W*sigma_n*sigma_d^3
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/dports/math/openturns/openturns-1.18/python/src/ |
H A D | GammaFactory_doc.i.in | 13 \displaystyle\Hat{k}_n= \frac{(\bar{x}_n-\Hat{\gamma}_n)^2}{(\sigma_n^X)^2}\\ 14 \displaystyle\Hat{\lambda}_n= \frac{\bar{x}_n-\Hat{\gamma}_n}{(\sigma_n^X)^2}\\
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H A D | HistogramFactory_doc.i.in | 155 h = \sigma_n \left(\frac{24 \sqrt{\pi}}{n}\right)^{\frac{1}{3}} 158 where :math:`\sigma_n^2` is the unbiaised variance of the data.
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/dports/science/py-ase/ase-3.22.0/ase/calculators/ |
H A D | acn.py | 17 sigma_n = 3.200 variable 83 sigma = np.array([sigma_n, sigma_c, sigma_me]) 88 sigma = np.array([sigma_me, sigma_c, sigma_n])
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/dports/science/elmerfem/elmerfem-release-9.0/fem/src/modules/ |
H A D | ThermoElectricSolver.F90 | 133 REAL(KIND=dp) :: sigma_n(3,3,n),alpha_n(3,3,n), pelt_n(3,3,n), & local 147 CALL InputTensor(Material, sigma_n, isScalar,'Electric Conductivity', Element) 193 sigma(i,j) = SUM(sigma_n(i,j,:)*Basis(1:n))
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/dports/math/lidia/lidia-2.3.0+latte-patches-2014-10-04/src/number_fields/quadratic_order/ |
H A D | quadratic_number_standard.cc | 1973 xbigfloat a1, a2, a3, n, sigma_n; in get_absolute_Ln_approximation() local 2035 subtract(sigma_n, a, a3); in get_absolute_Ln_approximation() 2042 divide(n, n, sigma_n, k+6); in get_absolute_Ln_approximation() 2201 xbigfloat a1, a2, a3, n, sigma_n; in get_absolute_Ln_approximation_with_check() local 2254 subtract(sigma_n, a, a3); in get_absolute_Ln_approximation_with_check() 2261 divide(n, n, sigma_n, k+6); in get_absolute_Ln_approximation_with_check()
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H A D | qi_class_real.cc | 50 xbigfloat n, a1, a2, a3, sigma_n, l; in approx_Ln_reduce() local 87 subtract(sigma_n, a, a3); in approx_Ln_reduce() 94 divide(n, n, sigma_n, k+6); in approx_Ln_reduce()
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/dports/graphics/pfstools/pfstools-2.1.0/src/tmo/ferradans11/ |
H A D | tmo_ferradans11.cpp | 247 float sigma_n=pow(mu[k],n); in tmo_ferradans11() local 266 RGB[k].datos[d]= In/(In+sigma_n); in tmo_ferradans11()
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/dports/audio/praat/praat-6.2.03/LPC/ |
H A D | PowerCepstrum.cpp | 287 const double sigma_n = sqrt (numberOfIterations) * sigma; 288 VECsmooth_gaussian_inplace (my z.row (1), sigma_n);
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/dports/graphics/luminance-qt5/luminance-hdr-2.6.1.1/src/TonemappingOperators/ferradans11/ |
H A D | tmo_ferradans11.cpp | 366 float sigma_n = pow(mu[k], n); in tmo_ferradans11() local 384 RGB[k][i] = In / (In + sigma_n); in tmo_ferradans11()
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/dports/graphics/openfx-misc/openfx-misc-3ab0531/DenoiseSharpen/ |
H A D | DenoiseSharpen.cpp | 3128 double sigma_n[4]; in analyzeNoiseLevelsForBitDepth() local 3129 …sigma_mad(fimg, bimgmask, iwidth, iheight, b3, sigma_n, (float)c / nComponents, 1.f / nComponents); in analyzeNoiseLevelsForBitDepth() 3131 _noiseLevel[c][f]->setValue(sigma_n[f]); in analyzeNoiseLevelsForBitDepth() 3139 double sigma_n[4]; in analyzeNoiseLevelsForBitDepth() local 3140 …sigma_mad(fimg, bimgmask, iwidth, iheight, b3, sigma_n, (float)(nComponents - 1) / nComponents, 1.… in analyzeNoiseLevelsForBitDepth() 3142 _noiseLevel[3][f]->setValue(sigma_n[f]); in analyzeNoiseLevelsForBitDepth()
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/dports/science/lammps/lammps-stable_29Sep2021/src/KSPACE/ |
H A D | ewald_disp.cpp | 557 double eps_i, sigma_i, sigma_n, *bi = B = new double[7*n+7]; in init_coeffs() local 569 sigma_n = 1.0; in init_coeffs() 571 *(bi++) = sigma_n*eps_i*c[j]; sigma_n *= sigma_i; in init_coeffs()
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/dports/math/openturns/openturns-1.18/python/doc/theory/numerical_methods/ |
H A D | nataf_transformation.rst | 65 :math:`\vect{\sigma}=(\sigma_1,\dots,\sigma_n)`.
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/dports/math/deal.ii/dealii-803d21ff957e349b3799cd3ef2c840bc78734305/examples/step-42/doc/ |
H A D | intro.dox | 96 force $\sigma_n=\mathbf n \cdot (\sigma(\mathbf u) 98 body) and with zero tangential component $\mathbf \sigma_t= \sigma \mathbf n - \mathbf \sigma_n \ma…
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