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| static const double | HArDCore3D::PI = boost::math::constants::pi<double>() |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_E1 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_E2 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_E3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::trigonometric_E = {trigonometric_E1, trigonometric_E2, trigonometric_E3} |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_A1 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_A2 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_A3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::trigonometric_A = {trigonometric_A1, trigonometric_A2, trigonometric_A3} |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B1_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B2_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B3_linear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::trigonometric_B_linear = {trigonometric_B1_linear, trigonometric_B2_linear, trigonometric_B3_linear} |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B1_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B2_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::trigonometric_B3_nonlinear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::trigonometric_B_nonlinear = {trigonometric_B1_nonlinear, trigonometric_B2_nonlinear, trigonometric_B3_nonlinear} |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_dtE1 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_dtE2 |
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| static YangMills::TElectricFieldType | HArDCore3D::trigonometric_dtE3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::trigonometric_dtE = {trigonometric_dtE1, trigonometric_dtE2, trigonometric_dtE3} |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f1_linear |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f2_linear |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f3_linear |
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| static YangMills::TLAForcingTermType | HArDCore3D::trigonometric_f_linear = {trigonometric_f1_linear, trigonometric_f2_linear, trigonometric_f3_linear} |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f1_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f2_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::trigonometric_f3_nonlinear |
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| static YangMills::TLAForcingTermType | HArDCore3D::trigonometric_f_nonlinear = {trigonometric_f1_nonlinear, trigonometric_f2_nonlinear, trigonometric_f3_nonlinear} |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_E1 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_E2 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_E3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::linear_E = {linear_E1, linear_E2, linear_E3} |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_A1 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_A2 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_A3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::linear_A = {linear_A1, linear_A2, linear_A3} |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B1_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B2_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B3_linear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::linear_B_linear = {linear_B1_linear, linear_B2_linear, linear_B3_linear} |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B1_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B2_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::linear_B3_nonlinear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::linear_B_nonlinear = {linear_B1_nonlinear, linear_B2_nonlinear, linear_B3_nonlinear} |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_dtE1 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_dtE2 |
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| static YangMills::TElectricFieldType | HArDCore3D::linear_dtE3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::linear_dtE = {linear_dtE1, linear_dtE2, linear_dtE3} |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f1_linear |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f2_linear |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f3_linear |
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| static YangMills::TLAForcingTermType | HArDCore3D::linear_f_linear = {linear_f1_linear, linear_f2_linear, linear_f3_linear} |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f1_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f2_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::linear_f3_nonlinear |
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| static YangMills::TLAForcingTermType | HArDCore3D::linear_f_nonlinear = {linear_f1_nonlinear, linear_f2_nonlinear, linear_f3_nonlinear} |
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| static YangMills::TElectricFieldType | HArDCore3D::const_E1 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_E2 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_E3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::const_E = {const_E1, const_E2, const_E3} |
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| static YangMills::TElectricFieldType | HArDCore3D::const_A1 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_A2 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_A3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::const_A = {const_A1, const_A2, const_A3} |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B1_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B2_linear |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B3_linear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::const_B_linear = {const_B1_linear, const_B2_linear, const_B3_linear} |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B1_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B2_nonlinear |
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| static YangMills::TMagneticFieldType | HArDCore3D::const_B3_nonlinear |
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| static YangMills::TLAMagneticFieldType | HArDCore3D::const_B_nonlinear = {const_B1_nonlinear, const_B2_nonlinear, const_B3_nonlinear} |
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| static YangMills::TElectricFieldType | HArDCore3D::const_dtE1 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_dtE2 |
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| static YangMills::TElectricFieldType | HArDCore3D::const_dtE3 |
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| static YangMills::TLAElectricFieldType | HArDCore3D::const_dtE = {const_dtE1, const_dtE2, const_dtE3} |
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| static YangMills::TForcingTermType | HArDCore3D::const_f1_linear |
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| static YangMills::TForcingTermType | HArDCore3D::const_f2_linear |
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| static YangMills::TForcingTermType | HArDCore3D::const_f3_linear |
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| static YangMills::TLAForcingTermType | HArDCore3D::const_f_linear = {const_f1_linear, const_f2_linear, const_f3_linear} |
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| static YangMills::TForcingTermType | HArDCore3D::const_f1_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::const_f2_nonlinear |
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| static YangMills::TForcingTermType | HArDCore3D::const_f3_nonlinear |
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| static YangMills::TLAForcingTermType | HArDCore3D::const_f_nonlinear = {const_f1_nonlinear, const_f2_nonlinear, const_f3_nonlinear} |
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