\( |\Delta C = 1 | \) Evolutor Class More...

#include <EvolDC1.h>

Inheritance diagram for EvolDC1:

Detailed Description

\( |\Delta C = 1 | \) Evolutor Class

This evolutor is properly written for Charm Physics studies; it is implemented for the evolution of the 8 effective Wilson coefficients (related to the 2 current x current + 4 QCD penguins + em & chromo penguins) in the Chetyrkin, Misiak and Munz basis at the NLO in \( \alpha_{strong} \); principal reference: hep-ph/9612313, hep-ph/0612329

Definition at line 24 of file EvolDC1.h.

Public Member Functions
gslpp::matrix< double >	AnomalousDimension_M (orders order, unsigned int n_u, unsigned int n_d) const
	a method returning the anomalous dimension matrix given in the Misiak basis More...

gslpp::matrix< double > &	DC1Evol (double mu, double M, orders order, schemes scheme=NDR)
	a method returning the evolutor related to the high scale \( M \) and the low scale \( \mu \) More...

	EvolDC1 (unsigned int dim, schemes scheme, orders order, const StandardModel &model)
	EvolDC1 constructor. More...

gslpp::matrix< double >	ToEffectiveBasis (gslpp::matrix< double > mat) const
	a method returning the anomalous dimension for the evolution of the effective Wilson coefficients More...

gslpp::matrix< double >	ToRescaledBasis (orders order, unsigned int n_u, unsigned int n_d) const
	a method returning the anomalous dimension in the Chetyrkin, Misiak and Munz operator basis More...

virtual	~EvolDC1 ()
	EvolDC1 destructor. More...

Public Member Functions inherited from RGEvolutor
gslpp::matrix< double > *	Evol (orders order)
	Evolution matrix set at a fixed order of QCD coupling. More...

gslpp::matrix< double > *	Evol (orders_qed order_qed)
	Evolution matrix set at a fixed order of Electroweak coupling. More...

gslpp::matrix< double > **	getEvol () const

double	getM () const
	Retrieve the upper scale of the Wilson Coefficients. More...

	RGEvolutor (unsigned int dim, schemes scheme, orders order)
	constructor More...

	RGEvolutor (unsigned int dim, schemes scheme, orders order, orders_qed order_qed)
	constructor More...

void	setEvol (const gslpp::matrix< double > &m, orders order_i)

void	setEvol (const gslpp::matrix< double > &m, orders_qed order_qed_i)

void	setEvol (unsigned int i, unsigned int j, double x, orders order_i)

void	setEvol (unsigned int i, unsigned int j, double x, orders order_i, orders_qed order_qed)

void	setM (double M)
	Sets the upper scale for the running of the Wilson Coefficients. More...

void	setMu (double mu)
	Sets the lower scale for the running of the Wilson Coefficients. More...

void	setScales (double mu, double M)
	Sets the upper and lower scale for the running of the Wilson Coefficients. More...

virtual	~RGEvolutor ()
	destructor More...

Public Member Functions inherited from WilsonTemplate< gslpp::matrix< double > >
double	getMu () const

orders	getOrder () const

orders_qed	getOrder_qed () const

schemes	getScheme () const

unsigned int	getSize () const

virtual void	resetCoefficient ()

void	setScheme (schemes scheme)

	WilsonTemplate (const WilsonTemplate< gslpp::matrix< double > > &orig)

	WilsonTemplate (unsigned int dim, schemes scheme_i, orders order_i, orders_qed order_qed_i=NO_QED)

virtual	~WilsonTemplate ()

Private Member Functions
void	DC1Evol (double mu, double M, double nf, schemes scheme)
	a void type method storing properly the magic numbers for the implementation of the evolutor More...

Private Attributes
double	a [3][10]

double	alsMZ_cache

double	b [3][10][10][10]

double	c [3][10][10][10]

double	d [3][10][10][10]

unsigned int	dim

gslpp::vector< gslpp::complex >	e

gslpp::matrix< gslpp::complex >	gg

gslpp::matrix< gslpp::complex >	h

gslpp::matrix< gslpp::complex >	js

gslpp::matrix< gslpp::complex >	jss

gslpp::matrix< gslpp::complex >	jssv

gslpp::matrix< gslpp::complex >	jv

const StandardModel &	model

double	Mz_cache

int	nd

int	nu

gslpp::matrix< gslpp::complex >	s_s

gslpp::matrix< gslpp::complex >	v

gslpp::matrix< gslpp::complex >	vi

gslpp::matrix< gslpp::complex >	vij

Additional Inherited Members
Protected Member Functions inherited from WilsonTemplate< gslpp::matrix< double > >
gslpp::matrix< double > *	Elem (orders order) const

gslpp::matrix< double > *	Elem (orders_qed order_qed) const

void	setElem (const gslpp::matrix< double > &v, orders order_i)

void	setElem (const gslpp::matrix< double > &v, orders_qed order_qed_i)

Protected Attributes inherited from RGEvolutor
double	M

Protected Attributes inherited from WilsonTemplate< gslpp::matrix< double > >
gslpp::matrix< double > *	elem [MAXORDER_QED+1]

double	mu

orders	order

orders_qed	order_qed

schemes	scheme

unsigned int	size

Constructor & Destructor Documentation

◆ EvolDC1()

EvolDC1::EvolDC1	(	unsigned int	dim,
		schemes	scheme,
		orders	order,
		const StandardModel &	model
	)

EvolDC1 constructor.

Parameters

dim	an unsigned integer for the dimension of the evolutor
scheme	an enum "schemes" for the regularization scheme of the evolutor
order	an enum "orders" for the order of perturbation theory of the evolutor
model	an object of StandardModel class

Definition at line 14 of file EvolDC1.cpp.

:           RGEvolutor(dim_i, scheme, order), model(model),
            v(dim_i,0.), vi(dim_i,0.), js(dim_i,0.), h(dim_i,0.), gg(dim_i,0.),s_s(dim_i,0.),
            jssv(dim_i,0.), jss(dim_i,0.), jv(dim_i,0.), vij(dim_i,0.), e(dim_i,0.), dim(dim_i) 
{
    
    /* magic numbers a & b */
    
    for(int L=2; L>-1; L--){
        
    /* L=2 --> u,d,s,c (nf=4)  L=1 --> u,d,s,c,b (nf=5) L=0 --> u,d,s,c,b,t (nf=6) */
        
    nu = L;  nd = L;
    if(L == 1){nd = 3; nu = 2;} 
    if(L == 0){nd = 3; nu = 3;}
    
    // LO evolutor of the effective Wilson coefficients in the Chetyrkin, Misiak and Munz basis
    
    (ToEffectiveBasis(ToRescaledBasis(LO,nu,nd))).transpose().eigensystem(v,e);
    vi = v.inverse();
    for(unsigned int i = 0; i < dim; i++){
       a[L][i] = e(i).real();
       for (unsigned int j = 0; j < dim; j++) {
           for (unsigned int k = 0; k < dim; k++)  {
                b[L][i][j][k] = v(i, k).real() * vi(k, j).real();
               }
           }
       }
    
    // NLO evolutor of the effective Wilson coefficients in the Chetyrkin, Misiak and Munz basis
    
    gg = vi * (ToEffectiveBasis(ToRescaledBasis(NLO,nu,nd))).transpose() * v;
    double b0 = model.Beta0(6-L);
    double b1 = model.Beta1(6-L);
    for (unsigned int i = 0; i < dim; i++){
        for (unsigned int j = 0; j < dim; j++){
            s_s.assign( i, j, (b1 / b0) * (i==j) * e(i).real() - gg(i,j));    
            if(fabs(e(i).real() - e(j).real() + 2. * b0)>0.00000000001){
                h.assign( i, j, s_s(i,j) / (2. * b0 + e(i) - e(j)));
                }
            }
        }
    js = v * h * vi;
    jv = js * v;
    vij = vi * js;
    jss = v * s_s * vi;
    jssv = jss * v;        
    for (unsigned int i = 0; i < dim; i++){
        for (unsigned int j = 0; j < dim; j++){
            if(fabs(e(i).real() - e(j).real() + 2. * b0) > 0.00000000001){
                for(unsigned int k = 0; k < dim; k++){
                        c[L][i][j][k] = jv(i, k).real() * vi(k, j).real();
                        d[L][i][j][k] = -v(i, k).real() * vij(k, j).real();
                        }
                    }
            else{    
                for(unsigned int k = 0; k < dim; k++){
                   c[L][i][j][k] = (1./(2. * b0)) * jssv(i, k).real() * vi(k, j).real();
                   d[L][i][j][k] = 0.;
                   }   
                }
            }
        }
    }
}

◆ ~EvolDC1()

EvolDC1::~EvolDC1 ( )

virtual

EvolDC1 destructor.

Definition at line 80 of file EvolDC1.cpp.

81{}

Member Function Documentation

◆ AnomalousDimension_M()

gslpp::matrix< double > EvolDC1::AnomalousDimension_M	(	orders	order,
		unsigned int	n_u,
		unsigned int	n_d
	)		const

a method returning the anomalous dimension matrix given in the Misiak basis

Parameters

order	an enum "orders" for the order of perturbation theory of the ADM
n_u	an unsigned integer for the up-type number of d.o.f.
n_d	an unsigned integer for the down-type number of d.o.f.

Returns: the ADM at the order LO/NLO in the Misiak basis

Definition at line 83 of file EvolDC1.cpp.

{
    
    /* Delta F = 1 anomalous dimension in Misiak basis, 
       ref.: M. Misiak, Nucl. Phys. B393 (1993) 23, B439 (1995) 461 (E),  
             A.J. Buras and M. Munz, Phys. Rev. D52 (1995) 186.   */  
    
    /* gamma(row, coloumn) at the LO */
    
    unsigned int nf = n_u + n_d; /*n_u/d = active type up/down flavor d.o.f.*/
  
    gslpp::matrix<double> gammaDF1(dim, dim, 0.);
   
    switch(order){
        
    case LO:
        
    gammaDF1(0,0) = -4. ;
    gammaDF1(0,1) = 8./3. ;
    
    gammaDF1(1,0) = 12.;
    
    if(nf < 5){
    gammaDF1(1,3) = 4./3.;
    gammaDF1(1,8) = -8./9.;
    gammaDF1(0,3) = -2./9.;
    gammaDF1(0,8) = -32./27.;
    }
    
    gammaDF1(2,3) = -52./3.;
    gammaDF1(2,5) = 2.;
    gammaDF1(2,8) = 8./9. + (8.*n_d)/3. - (16.*n_u)/3.;
    
    gammaDF1(3,2) = -40./9.;
    gammaDF1(3,3) = -160./9. + 4./3.*nf;
    gammaDF1(3,4) = 4./9.;
    gammaDF1(3,5) = 5./6.;
    gammaDF1(3,8) = 32./27.;
    
    gammaDF1(4,3) = -256./3.;
    gammaDF1(4,5) = 20.;
    gammaDF1(4,8) = 128./9.+(80.*n_d)/3. - (160.*n_u)/3.;
    
    gammaDF1(5,2) = -256./9.;
    gammaDF1(5,3) = -544./9. + (40./3.)*nf;
    gammaDF1(5,4) = 40./9.;
    gammaDF1(5,5) = -2./3.;
    gammaDF1(5,8) = 512./27.;
    
    gammaDF1(6,6) = 32./3. - 2.*model.Beta0(nf);   
    
    gammaDF1(7,6) = -32./9.;
    gammaDF1(7,7) = 28./3. - 2.*model.Beta0(nf);
    
    gammaDF1(8,8) = -2.*model.Beta0(nf); 
    
    gammaDF1(9,9) = -2.*model.Beta0(nf); 
    
    
    break;    
    
        case NLO:
        
    if (!(nf == 3 || nf == 4 || nf == 5 || nf == 6)){ 
                throw std::runtime_error("EvolDF1::AnomalousDimension_M(): wrong number of flavours"); 
       }
    
    /*gamma(row, coloumn) at the NLO */
    
    gammaDF1(0,0) = -145./3. + (16./9.)*nf;
    gammaDF1(0,1) = -26. + (40./27.)*nf;
    gammaDF1(1,0) = -45. + (20./3.)*nf; 
    gammaDF1(1,1) = -28./3.;
    
    if(nf < 5){
    gammaDF1(0,2) = -1412./243.;
    gammaDF1(0,3) = -1369./243.;
    gammaDF1(0,4) = 134./243.;
    gammaDF1(0,5) = -35./162.;
    gammaDF1(0,6) = -232./243.;
    gammaDF1(0,7) = +167./162.;
    gammaDF1(0,8) = -2272./729.;
            
    gammaDF1(1,2) = -416./81.;
    gammaDF1(1,3) = 1280./81.;
    gammaDF1(1,4) = 56./81.;
    gammaDF1(1,5) = 35./27.;
    gammaDF1(1,6) = 464./81.;
    gammaDF1(1,7) = 76./27.;
    gammaDF1(1,8) = 1952./243.;
    }
    
    gammaDF1(2,2) = -4468./81.;
    gammaDF1(2,3) = -29129./81. - (52./9.)*nf;
    gammaDF1(2,4) = 400./81.;
    gammaDF1(2,5) = 3493./108. - (2./9.)*nf;
    gammaDF1(2,6) = 64./81.;
    gammaDF1(2,7) = 368./27.;
    gammaDF1(2,8) = -4160./243. + (32.*n_d)/3. - (64.*n_u)/3.;
    
    gammaDF1(3,2) = -13678./243. + (368.*nf)/81.;       
    gammaDF1(3,3) = -79409./243. + (1334.*nf)/81.;
    gammaDF1(3,4) = 509./486. - (8.*nf)/81.;
    gammaDF1(3,5) = 13499./648. - (5.*nf)/27.;
    gammaDF1(3,6) = -680./243. + (32.*nf)/81;
    gammaDF1(3,7) = -427./81. - (37.*nf)/54.; 
    gammaDF1(3,8) = 784./729. - (2272.*n_d)/243. + (2912.*n_u)/243.;
            
    gammaDF1(4,2) = -244480./81. - (160./9.)*nf;
    gammaDF1(4,3) = -29648./81. - (2200./9.)*nf;
    gammaDF1(4,4) = 23116./81. + (16./9.)*nf;
    gammaDF1(4,5) = 3886./27. + (148./9.)*nf;
    gammaDF1(4,6) = -6464./81.;
    gammaDF1(4,7) = 8192./27. + 36.*nf;
    gammaDF1(4,8) = -58112./243. + (320.*n_d)/3. - (640.*n_u)/3.;
            
    gammaDF1(5,2) = 77600./243. - (1264./81.)*nf;
    gammaDF1(5,3) = -28808./243. + (164./81.)*nf;
    gammaDF1(5,4) = -20324./243. + (400./81.)*nf;
    gammaDF1(5,5) = -21211./162.+ (622./27.)*nf;
    gammaDF1(5,6) = -20096./243. - (976.*n_d)/81. + (2912.*n_u)/81.;
    gammaDF1(5,7) = -6040./81. + (220./27.)*nf;
    gammaDF1(5,8) = -22784./729. - (20704.*n_d)/243. + (28544.*n_u)/243.;
           
    gammaDF1(6,6) = 1936./9.-224./27.*nf-2.*model.Beta1(nf); 
    
    gammaDF1(7,6) = -368./9.+224./81.*nf;
    gammaDF1(7,7) = 1456./9.-61./27.*nf-2.*model.Beta1(nf);  
    
    gammaDF1(8,8) = -2.*model.Beta1(nf); 
    
    gammaDF1(9,9) = -2.*model.Beta1(nf); 
    
    break;
    
    default:
            throw std::runtime_error("EvolDF1bsg::AnomalousDimension_M(): order not implemented"); 
    }  
    return (gammaDF1);
}

◆ DC1Evol() [1/2]

void EvolDC1::DC1Evol	(	double	mu,
		double	M,
		double	nf,
		schemes	scheme
	)

private

a void type method storing properly the magic numbers for the implementation of the evolutor

Parameters

mu	a double for the low scale of the evolution
M	a double for the high scale of the evolution
nf	a double for the active number of flavors
scheme	an enum "schemes" for the regularization scheme of the evolutor

Definition at line 379 of file EvolDC1.cpp.

 {
 
    gslpp::matrix<double> resLO(dim, 0.), resNLO(dim, 0.), resNNLO(dim, 0.);
 
    int L = 6 - (int) nf;
    double alsM = model.Als(M) / 4. / M_PI;
    double alsmu = model.Als(mu) / 4. / M_PI;
    
    double eta = alsM / alsmu;
    
    for (unsigned int k = 0; k < dim; k++) {
        double etap = pow(eta, a[L][k] / 2. / model.Beta0(nf));
        for (unsigned int i = 0; i < dim; i++){
            for (unsigned int j = 0; j < dim; j++) {
                resNNLO(i, j) += 0.;
                
                if(fabs(e(i).real() - e(j).real() + 2. * model.Beta0(nf))>0.000000000001)  {
                    resNLO(i, j) += c[L][i][j][k] * etap * alsmu;
                    resNLO(i, j) += d[L][i][j][k] * etap * alsM;
                }
                else{
                    resNLO(i, j) += - c[L][i][j][k] * etap * alsmu * log(eta);    
                }        
                resLO(i, j) += b[L][i][j][k] * etap;
            }
        }
    }
    
    switch(order) {
        case NNLO:
            *elem[NNLO] = 0.;
        case NLO:
            *elem[NLO] = (*elem[LO]) * resNLO + (*elem[NLO]) * resLO;
        case LO:
            *elem[LO] = (*elem[LO]) * resLO;
            break;
        case FULLNNLO:
        case FULLNLO:
        default:
            throw std::runtime_error("Error in EvolDC1::DC1Evol()");
    } 
    
  }

◆ DC1Evol() [2/2]

gslpp::matrix< double > & EvolDC1::DC1Evol	(	double	mu,
		double	M,
		orders	order,
		schemes	scheme = `NDR`
	)

a method returning the evolutor related to the high scale \( M \) and the low scale \( \mu \)

Parameters

mu	a double for the low scale of the evolution
M	a double for the high scale of the evolution
order	an enum "orders" for the order of perturbation theory of the evolutor
scheme	an enum "schemes" for the regularization scheme of the evolutor

Returns: the evolutor \( U (\mu , M) \)

Definition at line 334 of file EvolDC1.cpp.

{
    switch (scheme) {
        case NDR:
            break;
        case LRI:
        case HV:
        default:
            std::stringstream out;
            out << scheme;
            throw std::runtime_error("EvolDC1::Df1EvolDC1(): scheme " + out.str() + " not implemented "); 
    }
 
    double alsMZ = model.getAlsMz();
    double Mz = model.getMz();
    if(alsMZ == alsMZ_cache && Mz == Mz_cache) {
        if (mu == this->mu && M == this->M && scheme == this->scheme)
            return (*Evol(order));        
    }
    alsMZ_cache = alsMZ;
    Mz_cache = Mz;
 
    if (M < mu) {
        std::stringstream out;
        out << "M = " << M << " < mu = " << mu;
        throw out.str();
    }
 
    setScales(mu, M); // also assign evol to identity
 
    double m_down = mu;
    double m_up = model.AboveTh(m_down);
    double nf = model.Nf(m_down);
    
    while (m_up < M) {
        DC1Evol(m_down, m_up, nf, scheme);
        m_down = m_up;
        m_up = model.AboveTh(m_down);
        nf += 1.;
    }
    DC1Evol(m_down, M, nf, scheme);
    return (*Evol(order));
    
    }

◆ ToEffectiveBasis()

gslpp::matrix< double > EvolDC1::ToEffectiveBasis ( gslpp::matrix< double > mat ) const

a method returning the anomalous dimension for the evolution of the effective Wilson coefficients

Parameters

mat	a temporary variable of gslpp::matrix type

Returns: the ADM at the order LO/NLO for the effective Wilson coefficients

Definition at line 304 of file EvolDC1.cpp.

{
    
    gslpp::matrix<double> y(dim, 0.);
    
    y(0,0) = 1.;
    y(1,1) = 1.;
    y(2,2) = 1.;
    y(3,3) = 1.;
    y(4,4) = 1.;
    y(5,5) = 1.;
    y(6,6) = 1.;
    y(7,7) = 1.;
    y(8,8) = 1.;
    y(9,9) = 1.;
    
    y(6,2) = -1./3.;
    y(6,3) = -4./9.;
    y(6,4) = -20./3.;
    y(6,5) = -80./9.;
    
    y(7,2) = 1.;
    y(7,3) = -1./6.;
    y(7,4) = 20.;
    y(7,5) = -10./3.;
    
    return( (y.inverse()).transpose() * mat * y.transpose() );
    
}

◆ ToRescaledBasis()

gslpp::matrix< double > EvolDC1::ToRescaledBasis	(	orders	order,
		unsigned int	n_u,
		unsigned int	n_d
	)		const

a method returning the anomalous dimension in the Chetyrkin, Misiak and Munz operator basis

Parameters

order	an enum "orders" for the order of perturbation theory of the evolutor
n_u	an unsigned integer for the up-type number of d.o.f.
n_d	an unsigned integer for the down-type number of d.o.f.

Returns: the ADM at the order LO/NLO in the Chetyrkin, Misiak and Munz basis

Definition at line 225 of file EvolDC1.cpp.

{
    
    /* matrix entries for the anomalous dimension in the Chetyrkin, Misiak and Munz basis,
       ref. hep-ph/9711280v1, hep-ph/0504194 */
    
    gslpp::matrix<double> mat(dim, 0.);
    gslpp::matrix<double> mat1(dim, 0.);
    unsigned int nf = n_u + n_d;
    double z3 = gsl_sf_zeta_int(3);
    
    mat1(0,6) = - 13454./2187. + 44./2187.*nf;
    mat1(1,6) = 20644./729. - 88./729.*nf;
    mat1(2,6) = 119456./729. + 5440./729.*n_d -21776./729.*n_u;
    mat1(3,6) = - 202990./2187. + 32./729.*n_d*n_d + n_d*(16888./2187. + 64./729.*n_u)
                - 17132./2187.*n_u + 32./729.*n_u*n_u;
    mat1(4,6) = 530240./243. + 300928./729.*n_d - 461120./729.*n_u;
    mat1(5,6) = - 1112344./729. + 5432./729.*n_d*n_d + n_d*(419440./2187. - 
                2744./729.*n_u) + 143392./2187.*n_u - 8176./729.*n_u*n_u;
    
    mat1(0,7) = 25759./5832. + 431./5832.*nf;
    mat1(1,7) = 9733./486. - 917./972.*nf;
    mat1(2,7) = 82873./243. - 3361./243.*nf;
    mat1(3,7) = - 570773./2916. - 253./486.*n_d*n_d +n_d*(-40091./5832. - 
                253./243.*n_u) - 40091./5832.*n_u - 253./486.*n_u*n_u;
    mat1(4,7) = 838684./81. - 14.*n_d*n_d + n_d*(129074./243. - 28.*n_u) + 
                129074./243.*n_u - 14.*n_u*n_u;
    mat1(5,7) = - 923522./243. - 6031./486.*n_d*n_d + n_d*(-13247./1458. - 6031./243.*n_u)
                -13247./1458.*n_u - 6031./486.*n_u*n_u;
    
    mat1(0,8) = - 22357278./19683. + 14440./6561.*n_d + 144688./6561.*n_u + 6976./243.*z3;
    mat1(1,8) = - 200848./6561. - 23696./2187.*n_d + 30736./2187.*n_u - 3584./81.*z3;
    mat1(2,8) = - 1524104./6561. - 176./27.*n_d*n_d + 352./27.*n_u*n_u +
                n_d*(257564./2187. + 176./27.*n_u - 128./3.*z3) - 256./81.*z3 + 
                n_u*(-382984./2187. + 256./3.*z3); 
    mat1(3,8) = 1535926./19683. + 1984./2187.*n_d*n_d - 5792./2187.*n_u*n_u +
                n_d*(-256901./6561. - 3808./2187.*n_u - 2720./81.*z3) - 
                5056./243.*z3 + n_u*(34942./6561. + 1600./81.*z3);
    mat1(4,8) = - 31433600./6561. - 2912./27.*n_d*n_d + 5824./27.*n_u*n_u +
                n_d*(- 3786616./2187. + 2912./27.*n_u - 1280./3.*z3) -
                4096./81.*z3 + n_u*(7525520./2187. + 2560./3.*z3);
    mat1(5,8) = - 48510784./19683. -51296./2187.*n_d*n_d + 54976./2187.*n_u*n_u +
                n_u*(-11231648./6561. - 22016./81.*z3) + n_d*(340984./6561. + 
                3680./2187.*n_u - 8192./81.*z3) - 80896./243.*z3;
     
    
    switch(order){
        case(NLO): 
            mat = AnomalousDimension_M(NLO, n_u, n_d);
            for (int i=0; i<6; i++){
                for (unsigned int j=6; j<dim; j++){
                    mat(i,j) = mat1(i,j);
                }
            }
            for (unsigned int i=6; i<dim; i++){
                for (unsigned int j=6; j<dim; j++){
                    mat(i,j) = mat(i,j) + 2. * (i==j) * model.Beta1(nf);
                }
            }
            return (mat);
        case(LO):
            mat = AnomalousDimension_M(LO, n_u, n_d);
            for (int i=0; i<6; i++){
                for (unsigned int j=6; j<dim; j++){
                    mat(i,j) = AnomalousDimension_M(NLO, n_u, n_d)(i,j);
                }
            }
            for (unsigned int i=6; i<dim; i++){
                for (unsigned int j=6; j<dim; j++){
                    mat(i,j) = mat(i,j) + 2. * (i==j) * model.Beta0(nf);
                }
            }
            return (mat);
        default:
            throw std::runtime_error("change to rescaled operator basis: order not implemented"); 
    }
    
}

Member Data Documentation

◆ a

double EvolDC1::a[3][10]

private

Parameters

a	array of double for the magic numbers of the evolutor ( LO evolution )
b	array of double for the magic numbers of the evolutor ( LO evolution )
c	array of double for the magic numbers of the evolutor ( NLO evolution, associated to \( \alpha_{strong}(\mu) \) )
d	array of double for the magic numbers of the evolutor ( NLO evolution, associated to \( \alpha_{strong}(M) \) )

Definition at line 82 of file EvolDC1.h.

◆ alsMZ_cache

double EvolDC1::alsMZ_cache

private

Definition at line 95 of file EvolDC1.h.

◆ b

double EvolDC1::b[3][10][10][10]

private

Definition at line 82 of file EvolDC1.h.

◆ c

double EvolDC1::c[3][10][10][10]

private

Definition at line 82 of file EvolDC1.h.

◆ d

double EvolDC1::d[3][10][10][10]

private

Definition at line 82 of file EvolDC1.h.

◆ dim

unsigned int EvolDC1::dim

private

Definition at line 94 of file EvolDC1.h.

◆ e

gslpp::vector<gslpp::complex> EvolDC1::e

private

Definition at line 93 of file EvolDC1.h.

◆ gg

gslpp::matrix<gslpp::complex> EvolDC1::gg

private

Definition at line 92 of file EvolDC1.h.

◆ h

gslpp::matrix<gslpp::complex> EvolDC1::h

private

Definition at line 92 of file EvolDC1.h.

◆ js

gslpp::matrix<gslpp::complex> EvolDC1::js

private

Definition at line 92 of file EvolDC1.h.

◆ jss

gslpp::matrix<gslpp::complex> EvolDC1::jss

private

Definition at line 92 of file EvolDC1.h.

◆ jssv

gslpp::matrix<gslpp::complex> EvolDC1::jssv

private

Definition at line 92 of file EvolDC1.h.

◆ jv

gslpp::matrix<gslpp::complex> EvolDC1::jv

private

Definition at line 92 of file EvolDC1.h.

◆ model

const StandardModel& EvolDC1::model

private

Definition at line 83 of file EvolDC1.h.

◆ Mz_cache

double EvolDC1::Mz_cache

private

Definition at line 96 of file EvolDC1.h.

◆ nd

int EvolDC1::nd

private

Definition at line 75 of file EvolDC1.h.

◆ nu

int EvolDC1::nu

private

Parameters

nu	an unsigned integer for the up-type number of d.o.f.
nu	an unsigned integer for the down-type number of d.o.f.

Definition at line 75 of file EvolDC1.h.

◆ s_s

gslpp::matrix<gslpp::complex> EvolDC1::s_s

private

Definition at line 92 of file EvolDC1.h.

◆ v

gslpp::matrix<gslpp::complex> EvolDC1::v

private

Definition at line 92 of file EvolDC1.h.

◆ vi

gslpp::matrix<gslpp::complex> EvolDC1::vi

private

Definition at line 92 of file EvolDC1.h.

◆ vij

gslpp::matrix<gslpp::complex> EvolDC1::vij

private

Definition at line 92 of file EvolDC1.h.

The documentation for this class was generated from the following files:

Detailed Description

Public Member Functions

Private Member Functions

Private Attributes

Additional Inherited Members

Constructor & Destructor Documentation

◆ EvolDC1()

◆ ~EvolDC1()

Member Function Documentation

◆ AnomalousDimension_M()

◆ DC1Evol() [1/2]

◆ DC1Evol() [2/2]

◆ ToEffectiveBasis()

◆ ToRescaledBasis()

Member Data Documentation

◆ a

◆ alsMZ_cache

◆ b

◆ c

◆ d

◆ dim

◆ e

◆ gg

◆ h

◆ js

◆ jss

◆ jssv

◆ jv

◆ model

◆ Mz_cache

◆ nd

◆ nu

◆ s_s

◆ v

◆ vi

◆ vij