[2615] | 1 | #include "sopnamsp.h"
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[729] | 2 | #include "lambdaBuilder.h"
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| 3 | #include "nbconst.h"
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| 4 |
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| 5 |
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[1218] | 6 | /*!
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| 7 | \class SOPHYA::Legendre
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| 8 | generate Legendre polynomials : use in two steps :
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| 9 |
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| 10 | a) instanciate Legendre(\f$x\f$, \f$lmax\f$) ; \f$x\f$ is the value for wich Legendre polynomials will be required (usually equal to \f$\cos \theta\f$) and \f$lmax\f$ is the MAXIMUM value of the order of polynomials wich will be required in the following code (all polynomials, from \f$l=0 to lmax\f$, are computed once for all by an iterative formula).
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| 11 |
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| 12 | b) get the value of Legendre polynomial for a particular value of \f$l\f$ by calling the method getPl.
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| 13 |
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| 14 | */
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| 15 |
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| 16 |
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[729] | 17 | Legendre::Legendre(r_8 x, int_4 lmax)
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| 18 | {
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[1428] | 19 | if (fabs(x) > 1. )
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[729] | 20 | {
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| 21 | throw RangeCheckError("variable for Legendre polynomials must have modules inferior to 1" );
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| 22 | }
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| 23 | x_ = x;
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| 24 | array_init(lmax);
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| 25 | }
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[1218] | 26 |
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| 27 | /*! \fn void SOPHYA::Legendre::array_init(int_4 lmax)
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| 28 |
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| 29 | compute all \f$P_l(x,l_{max})\f$ for \f$l=1,l_{max}\f$
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| 30 | */
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[729] | 31 | void Legendre::array_init(int_4 lmax)
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| 32 | {
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| 33 | lmax_ = lmax;
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| 34 | Pl_.ReSize(lmax_+1);
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| 35 | Pl_(0)=1.;
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[2277] | 36 | if (lmax>0) Pl_(1)=x_;
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[729] | 37 | for (int k=2; k<Pl_.NElts(); k++)
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| 38 | {
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| 39 | Pl_(k) = ( (2.*k-1)*x_*Pl_(k-1)-(k-1)*Pl_(k-2) )/k;
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| 40 | }
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| 41 | }
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| 42 |
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[1756] | 43 | TriangularMatrix<r_8> LambdaLMBuilder::a_recurrence_ = TriangularMatrix<r_8>();
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| 44 | TriangularMatrix<r_8> LambdaLMBuilder::lam_fact_ = TriangularMatrix<r_8>();
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[729] | 45 | TVector<r_8>* LambdaLMBuilder::normal_l_ = NULL;
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| 46 |
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[1218] | 47 |
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| 48 |
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| 49 | /*! \class SOPHYA::LambdaLMBuilder
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| 50 |
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| 51 |
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| 52 | This class generate the coefficients :
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| 53 | \f[
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| 54 | \lambda_l^m=\sqrt{\frac{2l+1}{4\pi}\frac{(l-m)!}{(l+m)!}}
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| 55 | P_l^m(\cos{\theta})
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| 56 | \f]
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| 57 | where \f$P_l^m\f$ are the associated Legendre polynomials. The above coefficients contain the theta-dependance of spheric harmonics :
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| 58 | \f[
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| 59 | Y_{lm}(\cos{\theta})=\lambda_l^m(\cos{\theta}) e^{im\phi}.
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| 60 | \f]
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| 61 |
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| 62 | Each object has a fixed theta (radians), and maximum l and m to be calculated
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| 63 | (lmax and mmax).
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| 64 | use the class in two steps :
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| 65 | a) instanciate LambdaLMBuilder(\f$\theta\f$, \f$lmax\f$, \f$mmax\f$) ; \f$lmax\f$ and \f$mmax\f$ are MAXIMUM values for which \f$\lambda_l^m\f$ will be required in the following code (all coefficients, from \f$l=0 to lmax\f$, are computed once for all by an iterative formula).
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| 66 | b) get the values of coefficients for particular values of \f$l\f$ and \f$m\f$ by calling the method lamlm.
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| 67 | */
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| 68 |
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| 69 |
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[729] | 70 | LambdaLMBuilder::LambdaLMBuilder(r_8 theta,int_4 lmax, int_4 mmax)
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| 71 | {
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| 72 | cth_=cos(theta);
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| 73 | sth_=sin(theta);
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| 74 | array_init(lmax, mmax);
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| 75 | }
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[1683] | 76 | LambdaLMBuilder::LambdaLMBuilder(r_8 costet, r_8 sintet,int_4 lmax, int_4 mmax)
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| 77 | {
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| 78 | cth_=costet;
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| 79 | sth_=sintet;
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| 80 | array_init(lmax, mmax);
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| 81 | }
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[729] | 82 | void LambdaLMBuilder::array_init(int lmax, int mmax)
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| 83 | {
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[2958] | 84 | updateArrayRecurrence(lmax);
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| 85 |
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[729] | 86 | lmax_=lmax;
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| 87 | mmax_=mmax;
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| 88 | r_8 bignorm2 = 1.e268; // = 1e-20*1.d288
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| 89 |
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| 90 | lambda_.ReSizeRow(lmax_+1);
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| 91 |
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| 92 | r_8 lam_mm = 1. / sqrt(4.*Pi) *bignorm2;
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| 93 |
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| 94 | for (int m=0; m<=mmax_;m++)
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| 95 | {
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| 96 |
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| 97 |
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| 98 | lambda_(m,m)= lam_mm / bignorm2;
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| 99 |
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| 100 | r_8 lam_0=0.;
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| 101 | r_8 lam_1=1. /bignorm2 ;
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| 102 | // r_8 a_rec = LWK->a_recurr(m,m);
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[1756] | 103 | r_8 a_rec = a_recurrence_(m,m);
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[729] | 104 | r_8 b_rec = 0.;
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| 105 | for (int l=m+1; l<=lmax_; l++)
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| 106 | {
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| 107 | r_8 lam_2 = (cth_*lam_1-b_rec*lam_0)*a_rec;
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| 108 | lambda_(l,m) = lam_2*lam_mm;
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| 109 | b_rec=1./a_rec;
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| 110 | // a_rec= LWK->a_recurr(l,m);
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[1756] | 111 | a_rec= a_recurrence_(l,m);
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[729] | 112 | lam_0 = lam_1;
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| 113 | lam_1 = lam_2;
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| 114 | }
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| 115 |
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| 116 | lam_mm = -lam_mm*sth_* sqrt( (2.*m+3.)/ (2.*m+2.) );
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| 117 |
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| 118 | }
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| 119 | }
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| 120 |
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[2958] | 121 | /*!
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| 122 | \brief : Specialized/optimized static function for fast spherical harmonic transform.
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| 123 | Computes bm(m) = Sum_l>=m [ lambda(l,m) * alm(l,m) ]
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| 124 | See SphericalTransformServer<T>::GenerateFromAlm(map, pixsize, alm)
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| 125 | */
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| 126 | void LambdaLMBuilder::ComputeBmFrAlm(r_8 theta,int_4 lmax, int_4 mmax,
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| 127 | const Alm<r_8>& alm, Bm< complex<r_8> >& bm)
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| 128 | {
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| 129 | updateArrayRecurrence(lmax);
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| 130 | r_8 cth = cos(theta);
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| 131 | r_8 sth = sin(theta);
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| 132 |
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| 133 | r_8 bignorm2 = 1.e268; // = 1e-20*1.d288
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| 134 |
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| 135 | r_8 lam_mm = 1. / sqrt(4.*Pi) *bignorm2;
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| 136 | r_8 lam_0, lam_1, lam_2;
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| 137 | register r_8 a_rec, b_rec;
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[729] | 138 |
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[2958] | 139 | const complex<r_8>* almp = alm.columnData(0);
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| 140 | r_8* arecp = a_recurrence_.columnData(0);
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| 141 |
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| 142 | int_4 l, m;
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| 143 |
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| 144 | for (m=0; m<=mmax;m++) {
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| 145 | //MOV^ const complex<r_8>* almp = alm.columnData(m);
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| 146 | complex<r_8>* bmp = &(bm(m));
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| 147 |
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| 148 | *bmp = (lam_mm / bignorm2)*(*almp); almp++;
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| 149 |
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| 150 | lam_0=0.;
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| 151 | lam_1=1. /bignorm2 ;
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| 152 |
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| 153 | a_rec = *arecp; arecp++; // a_recurrence_(m,m);
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| 154 | b_rec = 0.;
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| 155 | for (l=m+1; l<=lmax; l++) {
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| 156 | lam_2 = (cth*lam_1-b_rec*lam_0)*a_rec;
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| 157 |
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| 158 | //DEL lambda_(l,m) = lam_2*lam_mm;
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| 159 | *bmp += lam_2*lam_mm*(*almp); almp++;
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| 160 | b_rec=1./a_rec;
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| 161 | // a_rec= LWK->a_recurr(l,m);
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| 162 | a_rec= *arecp; arecp++; // a_recurrence_(l,m);
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| 163 | lam_0 = lam_1;
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| 164 | lam_1 = lam_2;
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| 165 | }
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| 166 | lam_mm = -lam_mm*sth* sqrt( (2.*m+3.)/ (2.*m+2.) );
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| 167 | }
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| 168 | }
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| 169 |
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| 170 | /*!
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| 171 | \brief : Specialized/optimized static function for fast spherical harmonic transform.
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| 172 | */
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| 173 | void LambdaLMBuilder::ComputeBmFrAlm(r_8 theta,int_4 lmax, int_4 mmax,
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| 174 | const Alm<r_4>& alm, Bm< complex<r_4> >& bm)
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| 175 | {
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| 176 | Alm<r_8> alm8(alm.Lmax());
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| 177 | for(sa_size_t k=0; k<alm8.Size(); k++)
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| 178 | alm8(k) = complex<r_8>((r_8)alm(k).real() , (r_8)alm(k).imag());
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| 179 | Bm< complex<r_8> > bm8(bm.Mmax());
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| 180 | ComputeBmFrAlm(theta, lmax, mmax, alm8, bm8);
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| 181 | for(sa_size_t kk=-bm.Mmax(); kk<=bm.Mmax(); kk++)
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| 182 | bm(kk)= complex<r_4>((r_4)bm8(kk).real() , (r_4)bm8(kk).imag());
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| 183 | return;
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| 184 | }
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| 185 |
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| 186 |
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| 187 | /*!
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| 188 | \brief : Specialized/optimized static function for fast spherical harmonic transform.
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| 189 | Computes alm(l,m) = Sum_l>=m [ lambda(l,m) * phase(l,m) ]
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| 190 | See SphericalTransformServer<T>::carteVersAlm(SphericalMap<T>& map, nlmax, ctcut, alm)
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| 191 | */
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| 192 | void LambdaLMBuilder::ComputeAlmFrPhase(r_8 theta,int_4 lmax, int_4 mmax,
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| 193 | TVector< complex<r_8> >& phase, Alm<r_8> & alm)
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| 194 | {
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| 195 | updateArrayRecurrence(lmax);
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| 196 | r_8 cth = cos(theta);
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| 197 | r_8 sth = sin(theta);
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| 198 |
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| 199 | r_8 bignorm2 = 1.e268; // = 1e-20*1.d288
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| 200 |
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| 201 | r_8 lam_mm = 1. / sqrt(4.*Pi) *bignorm2;
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| 202 | r_8 lam_0, lam_1, lam_2;
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| 203 | register r_8 a_rec, b_rec;
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| 204 |
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| 205 | complex<r_8>* almp = alm.columnData(0);
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| 206 | r_8* arecp = a_recurrence_.columnData(0);
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| 207 |
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| 208 | int_4 l, m;
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| 209 | for (m=0; m<=mmax;m++) {
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| 210 | //MOV^ complex<r_8>* almp = alm.columnData(m);
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| 211 | complex<r_8> phi = phase(m);
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| 212 |
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| 213 | *almp += (lam_mm / bignorm2)*phi; almp++;
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| 214 |
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| 215 | lam_0=0.;
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| 216 | lam_1=1. /bignorm2 ;
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| 217 |
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| 218 | //MOV^ r_8* arecp = a_recurrence_.columnData(m);
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| 219 | a_rec = *arecp; arecp++; // a_recurrence_(m,m);
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| 220 | b_rec = 0.;
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| 221 | for (l=m+1; l<=lmax; l++) {
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| 222 | lam_2 = (cth*lam_1-b_rec*lam_0)*a_rec;
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| 223 |
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| 224 | //DEL lambda_(l,m) = lam_2*lam_mm;
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[2959] | 225 | *almp += (lam_2*lam_mm) * phi; almp++;
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[2958] | 226 |
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| 227 | b_rec=1./a_rec;
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| 228 | // a_rec= LWK->a_recurr(l,m);
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| 229 | a_rec= *arecp; arecp++; // a_recurrence_(l,m);
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| 230 | lam_0 = lam_1;
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| 231 | lam_1 = lam_2;
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| 232 | }
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| 233 | lam_mm = -lam_mm*sth* sqrt( (2.*m+3.)/ (2.*m+2.) );
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| 234 | }
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| 235 | }
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| 236 |
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| 237 | /*!
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| 238 | \brief : Specialized/optimized static function for fast spherical harmonic transform.
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| 239 | Computes alm(l,m) = Sum_l>=m [ lambda(l,m) * phase(l,m) ]
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| 240 | See SphericalTransformServer<T>::carteVersAlm(SphericalMap<T>& map, nlmax, ctcut, alm)
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| 241 | */
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| 242 | void LambdaLMBuilder::ComputeAlmFrPhase(r_8 theta,int_4 lmax, int_4 mmax,
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| 243 | TVector< complex<r_4> >& phase, Alm<r_4> & alm)
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| 244 | {
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[2959] | 245 | updateArrayRecurrence(lmax);
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| 246 | r_8 cth = cos(theta);
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| 247 | r_8 sth = sin(theta);
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| 248 |
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| 249 | r_8 bignorm2 = 1.e268; // = 1e-20*1.d288
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| 250 |
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| 251 | r_8 lam_mm = 1. / sqrt(4.*Pi) *bignorm2;
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| 252 | r_8 lam_0, lam_1, lam_2;
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| 253 | register r_8 a_rec, b_rec;
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| 254 | register r_4 cff;
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| 255 | complex<r_4>* almp = alm.columnData(0);
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| 256 | r_8* arecp = a_recurrence_.columnData(0);
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| 257 |
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| 258 | int_4 l, m;
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| 259 | for (m=0; m<=mmax;m++) {
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| 260 | //MOV^ complex<r_4>* almp = alm.columnData(m);
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| 261 | complex<r_4> phi = phase(m);
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| 262 |
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| 263 | cff = lam_mm / bignorm2;
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| 264 | *almp += cff*phi; almp++;
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| 265 |
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| 266 | lam_0=0.;
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| 267 | lam_1=1. /bignorm2 ;
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| 268 |
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| 269 | //MOV^ r_8* arecp = a_recurrence_.columnData(m);
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| 270 | a_rec = *arecp; arecp++; // a_recurrence_(m,m);
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| 271 | b_rec = 0.;
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| 272 | for (l=m+1; l<=lmax; l++) {
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| 273 | lam_2 = (cth*lam_1-b_rec*lam_0)*a_rec;
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| 274 |
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| 275 | //DEL lambda_(l,m) = lam_2*lam_mm;
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| 276 | cff = (lam_2*lam_mm);
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| 277 | *almp += cff * phi; almp++;
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| 278 |
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| 279 | b_rec=1./a_rec;
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| 280 | // a_rec= LWK->a_recurr(l,m);
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| 281 | a_rec= *arecp; arecp++; // a_recurrence_(l,m);
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| 282 | lam_0 = lam_1;
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| 283 | lam_1 = lam_2;
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| 284 | }
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| 285 | lam_mm = -lam_mm*sth* sqrt( (2.*m+3.)/ (2.*m+2.) );
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| 286 | }
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[2958] | 287 | }
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| 288 |
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| 289 |
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[1218] | 290 | /*! \fn void SOPHYA::LambdaLMBuilder::updateArrayRecurrence(int_4 lmax)
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| 291 |
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| 292 | compute a static array of coefficients independant from theta (common to all instances of the LambdaBuilder Class
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| 293 | */
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[729] | 294 | void LambdaLMBuilder::updateArrayRecurrence(int_4 lmax)
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| 295 | {
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[2958] | 296 | if ( (a_recurrence_.Size() > 0) && (lmax < a_recurrence_.rowNumber()) )
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| 297 | return; // Pas besoin de recalculer le tableau de recurrence
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| 298 | if (a_recurrence_.Size() > 0) {
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| 299 | cout << " WARNING : The classes LambdaXXBuilder will be more efficient "
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| 300 | << "if instanciated with parameter lmax = maximum value of l index "
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| 301 | << "which will be needed in the whole application (arrays not "
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| 302 | << "recomputed) " << endl;
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| 303 | cout << " lmax= " << lmax << " previous instanciation with lmax= "
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| 304 | << a_recurrence_.rowNumber()-1 << endl;
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| 305 | }
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| 306 |
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[1756] | 307 | a_recurrence_.ReSizeRow(lmax+1);
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[729] | 308 | for (int m=0; m<=lmax;m++)
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| 309 | {
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[1756] | 310 | a_recurrence_(m,m) = sqrt( 2.*m +3.);
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[729] | 311 | for (int l=m+1; l<=lmax; l++)
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| 312 | {
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| 313 | r_8 fl2 = (l+1.)*(l+1.);
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[1756] | 314 | a_recurrence_(l,m)=sqrt( (4.*fl2-1.)/(fl2-m*m) );
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[729] | 315 | }
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| 316 | }
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| 317 | }
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| 318 |
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[1218] | 319 | /*! \fn void SOPHYA::LambdaLMBuilder::updateArrayLamNorm()
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[729] | 320 |
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[1218] | 321 | compute static arrays of coefficients independant from theta (common to all instances of the derived classes
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| 322 | */
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[729] | 323 | void LambdaLMBuilder::updateArrayLamNorm()
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| 324 | {
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[1756] | 325 | lam_fact_.ReSizeRow(lmax_+1);
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[729] | 326 | for(int m = 0;m<= lmax_; m++)
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| 327 | {
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| 328 | for (int l=m; l<=lmax_; l++)
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| 329 | {
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[1756] | 330 | lam_fact_(l,m) =2.*(r_8)sqrt( (2.*l+1)*(l+m)*(l-m)/(2.*l-1) );
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[729] | 331 | }
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| 332 | }
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| 333 | (*normal_l_).ReSize(lmax_+1);
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| 334 | (*normal_l_)(0)=0.;
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| 335 | (*normal_l_)(1)=0.;
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| 336 | for (int l=2; l< (*normal_l_).NElts(); l++)
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| 337 | {
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| 338 | (*normal_l_)(l) =(r_8)sqrt( 2./( (l+2)*(l+1)*l*(l-1) ) );
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| 339 | }
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| 340 | }
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| 341 |
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| 342 |
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[1218] | 343 | /*! \class SOPHYA::LambdaWXBuilder
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[729] | 344 |
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[1218] | 345 | This class generates the coefficients :
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| 346 | \f[
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| 347 | _{w}\lambda_l^m=-2\sqrt{\frac{2(l-2)!}{(l+2)!}\frac{(2l+1)}{4\pi}\frac{(l-m)!}{(l+m)!}} G^+_{lm}
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| 348 | \f]
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| 349 | \f[
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| 350 | _{x}\lambda_l^m=-2\sqrt{\frac{2(l-2)!}{(l+2)!}\frac{(2l+1)}{4\pi}\frac{(l-m)!}{(l+m)!}}G^-_{lm}
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| 351 | \f]
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| 352 | where
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| 353 | \f[G^+_{lm}(\cos{\theta})=-\left( \frac{l-m^2}{\sin^2{\theta}}+\frac{1}{2}l\left(l-1\right)\right)P_l^m(\cos{\theta})+\left(l+m\right)\frac{\cos{\theta}}{\sin^2{\theta}}P^m_{l-1}(\cos{\theta})
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| 354 | \f]
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| 355 | and
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| 356 | \f[G^-_{lm}(\cos{\theta})=\frac{m}{\sin^2{\theta}}\left(\left(l-1\right)\cos{\theta}P^m_l(\cos{\theta})-\left(l+m\right)P^m_{l-1}(\cos{\theta})\right)
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| 357 | \f]
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| 358 | \f$P_l^m\f$ are the associated Legendre polynomials.
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[729] | 359 |
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[1218] | 360 | The coefficients express the theta-dependance of the \f$W_{lm}(\cos{\theta})\f$ and \f$X_{lm}(\cos{\theta})\f$ functions :
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| 361 | \f[W_{lm}(\cos{\theta}) = \sqrt{\frac{(l+2)!}{2(l-2)!}}_w\lambda_l^m(\cos{\theta})e^{im\phi}
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| 362 | \f]
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| 363 | \f[X_{lm}(\cos{\theta}) = -i\sqrt{\frac{(l+2)!}{2(l-2)!}}_x\lambda_l^m(\cos{\theta})e^{im\phi}
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| 364 | \f]
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| 365 | where \f$W_{lm}(\cos{\theta})\f$ and \f$X_{lm}(\cos{\theta})\f$ are defined as :
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| 366 |
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| 367 | \f[
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| 368 | W_{lm}(\cos{\theta})=-\frac{1}{2}\sqrt{\frac{(l+2)!}{(l-2)!}}\left(
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| 369 | _{+2}Y_l^m(\cos{\theta})+_{-2}Y_l^m(\cos{\theta})\right)
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| 370 | \f]
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| 371 | \f[X_{lm}(\cos{\theta})=-\frac{i}{2}\sqrt{\frac{(l+2)!}{(l-2)!}}\left(
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| 372 | _{+2}Y_l^m(\cos{\theta})-_{-2}Y_l^m(\cos{\theta})\right)
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| 373 | \f]
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| 374 |
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| 375 | */
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| 376 |
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| 377 |
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[729] | 378 | LambdaWXBuilder::LambdaWXBuilder(r_8 theta, int_4 lmax, int_4 mmax) : LambdaLMBuilder(theta, lmax, mmax)
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| 379 | {
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| 380 | array_init();
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| 381 | }
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| 382 |
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| 383 |
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| 384 | void LambdaWXBuilder::array_init()
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| 385 | {
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[1756] | 386 | if (lam_fact_.Size() < 1 || normal_l_ == NULL)
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[729] | 387 | {
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[1756] | 388 | // lam_fact_ = new TriangularMatrix<r_8>;
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[729] | 389 | normal_l_ = new TVector<r_8>;
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| 390 | updateArrayLamNorm();
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| 391 | }
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| 392 | else
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[1756] | 393 | if ( lmax_ > lam_fact_.rowNumber()-1 || lmax_ > (*normal_l_).NElts()-1 )
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[729] | 394 | {
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| 395 | updateArrayLamNorm();
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| 396 | }
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| 397 |
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| 398 | r_8 one_on_s2 = 1. / (sth_*sth_) ; // 1/sin^2
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| 399 | r_8 c_on_s2 = cth_*one_on_s2;
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| 400 | lamWlm_.ReSizeRow(lmax_+1);
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| 401 | lamXlm_.ReSizeRow(lmax_+1);
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| 402 |
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| 403 | // calcul des lambda
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| 404 | for(int m = 0;m<= mmax_; m++)
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| 405 | {
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| 406 | for (int l=m; l<=lmax_; l++)
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| 407 | {
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| 408 | lamWlm_(l,m) = 0.;
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| 409 | lamXlm_(l,m) = 0.;
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| 410 | }
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| 411 | }
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| 412 | for(int l = 2;l<= lmax_; l++)
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| 413 | {
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| 414 | r_8 normal_l = (*normal_l_)(l);
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| 415 | for (int m=0; m<=l; m++)
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| 416 | {
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| 417 | r_8 lam_lm1m = LambdaLMBuilder::lamlm(l-1,m);
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| 418 | r_8 lam_lm = LambdaLMBuilder::lamlm(l,m);
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[1756] | 419 | r_8 lam_fact_l_m = lam_fact_(l,m);
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[729] | 420 | r_8 a_w = 2. * (l - m*m) * one_on_s2 + l*(l-1.);
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| 421 | r_8 b_w = c_on_s2 * lam_fact_l_m;
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| 422 | r_8 a_x = 2. * cth_ * (l-1.);
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| 423 | lamWlm_(l,m) = normal_l * ( a_w * lam_lm - b_w * lam_lm1m );
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| 424 | lamXlm_(l,m) = - normal_l * m* one_on_s2* ( a_x * lam_lm - lam_fact_l_m * lam_lm1m );
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| 425 | }
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| 426 | }
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| 427 |
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| 428 | }
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| 429 |
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[1218] | 430 | /*! \class SOPHYA::LambdaPMBuilder
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[729] | 431 |
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[1218] | 432 | This class generates the coefficients
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| 433 | \f[
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| 434 | _{\pm}\lambda_l^m=2\sqrt{\frac{(l-2)!}{(l+2)!}\frac{(2l+1)}{4\pi}\frac{(l-m)!}{(l+m)!}}\left( G^+_{lm} \mp G^-_{lm}\right)
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| 435 | \f]
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| 436 | where
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| 437 | \f[G^+_{lm}(\cos{\theta})=-\left( \frac{l-m^2}{\sin^2{\theta}}+\frac{1}{2}l\left(l-1\right)\right)P_l^m(\cos{\theta})+\left(l+m\right)\frac{\cos{\theta}}{\sin^2{\theta}}P^m_{l-1}(\cos{\theta})
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| 438 | \f]
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| 439 | and
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| 440 | \f[G^-_{lm}(\cos{\theta})=\frac{m}{\sin^2{\theta}}\left(\left(l-1\right)\cos{\theta}P^m_l(\cos{\theta})-\left(l+m\right)P^m_{l-1}(\cos{\theta})\right)
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| 441 | \f]
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| 442 | and \f$P_l^m\f$ are the associated Legendre polynomials.
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| 443 | The coefficients express the theta-dependance of the spin-2 spherical harmonics :
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| 444 | \f[_{\pm2}Y_l^m(\cos{\theta})=_\pm\lambda_l^m(\cos{\theta})e^{im\phi}
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| 445 | \f]
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| 446 | */
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| 447 |
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[729] | 448 | LambdaPMBuilder::LambdaPMBuilder(r_8 theta, int_4 lmax, int_4 mmax) : LambdaLMBuilder(theta, lmax, mmax)
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| 449 | {
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| 450 | array_init();
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| 451 | }
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| 452 |
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| 453 |
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| 454 | void LambdaPMBuilder::array_init()
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| 455 | {
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[1756] | 456 | if (lam_fact_.Size() < 1 || normal_l_ == NULL)
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[729] | 457 | {
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[1756] | 458 | // lam_fact_ = new TriangularMatrix<r_8>;
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[729] | 459 | normal_l_ = new TVector<r_8>;
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| 460 | updateArrayLamNorm();
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| 461 | }
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| 462 | else
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[1756] | 463 | if ( lmax_ > lam_fact_.rowNumber()-1 || lmax_ > (*normal_l_).NElts()-1 )
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[729] | 464 | {
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| 465 | updateArrayLamNorm();
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| 466 | }
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| 467 |
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| 468 | r_8 one_on_s2 = 1. / (sth_*sth_) ;
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| 469 | r_8 c_on_s2 = cth_*one_on_s2;
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| 470 | lamPlm_.ReSizeRow(lmax_+1);
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| 471 | lamMlm_.ReSizeRow(lmax_+1);
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| 472 |
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| 473 | // calcul des lambda
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| 474 | for(int m = 0;m<= mmax_; m++)
|
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| 475 | {
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| 476 | for (int l=m; l<=lmax_; l++)
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| 477 | {
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| 478 | lamPlm_(l,m) = 0.;
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| 479 | lamMlm_(l,m) = 0.;
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| 480 | }
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| 481 | }
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| 482 |
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| 483 | for(int l = 2;l<= lmax_; l++)
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| 484 | {
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| 485 | r_8 normal_l = (*normal_l_)(l);
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| 486 | for (int m=0; m<=l; m++)
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| 487 | {
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| 488 | r_8 lam_lm1m = LambdaLMBuilder::lamlm(l-1,m);
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| 489 | r_8 lam_lm = LambdaLMBuilder::lamlm(l,m);
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[1756] | 490 | r_8 lam_fact_l_m = lam_fact_(l,m);
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[729] | 491 | r_8 a_w = 2. * (l - m*m) * one_on_s2 + l*(l-1.);
|
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| 492 | r_8 f_w = lam_fact_l_m/(sth_*sth_);
|
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| 493 | r_8 c_w = 2*m*(l-1.) * c_on_s2;
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| 494 |
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| 495 | lamPlm_(l,m) = normal_l * ( -(a_w+c_w) * lam_lm + f_w*( cth_ + m) * lam_lm1m )/Rac2;
|
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| 496 | lamMlm_(l,m) = normal_l * ( -(a_w-c_w) * lam_lm + f_w*( cth_ - m) * lam_lm1m )/Rac2;
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| 497 | }
|
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| 498 | }
|
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| 499 |
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| 500 | }
|
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| 501 |
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| 502 |
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