25 planarArcGeometry_m(1., 1.),
32 planarArcGeometry_m(right.planarArcGeometry_m),
33 dummy(), maxOrder_m(right.maxOrder_m), tanDelta_m(right.tanDelta_m),
34 k_m(right.k_m), Bz_m(right.Bz_m), r0_m(right.r0_m),
35 rMin_m(right.rMin_m), rMax_m(right.rMax_m), phiStart_m(right.phiStart_m),
36 phiEnd_m(right.phiEnd_m), azimuthalExtent_m(right.azimuthalExtent_m),
37 verticalExtent_m(right.verticalExtent_m), centre_m(right.centre_m),
38 endField_m(nullptr), endFieldName_m(right.endFieldName_m),
39 dfCoefficients_m(right.dfCoefficients_m)
97 double r =
std::sqrt(x * x + R[2] * R[2]);
115 if (r < rMin_m || r >
rMax_m) {
129 std::vector<double> fringeDerivatives(
maxOrder_m+1, 0.);
130 for (
size_t i = 0; i < fringeDerivatives.size(); ++i) {
137 for (
size_t n = 1;
n < zOverRVec.size(); ++
n) {
138 zOverRVec[
n] = zOverRVec[
n-1] * zOverR;
146 deltaB[1] = f2n * h * zOverRVec[
n];
153 deltaB[2] =
r0Sign_m * f2nplus1 * h * zOverRVec[
n+1];
164 dfCoefficients_m[
n+1] = std::vector<double>(dfCoefficients_m[
n].size()+1, 0);
165 for (
size_t i = 0; i < dfCoefficients_m[
n].size(); ++i) {
166 dfCoefficients_m[
n+1][i+1] = dfCoefficients_m[
n][i]/(
n+1);
168 if (
n+1 == maxOrder_m) {
171 dfCoefficients_m[
n+2] = std::vector<double>(dfCoefficients_m[
n].size()+2, 0);
172 for (
size_t i = 0; i < dfCoefficients_m[
n].size(); ++i) {
173 dfCoefficients_m[
n+2][i] = -(
k_m-
n)*(
k_m-
n)/(
n+1)*dfCoefficients_m[
n][i]/(
n+2);
175 for (
size_t i = 0; i < dfCoefficients_m[
n+1].size(); ++i) {
196 std::shared_ptr<endfieldmodel::EndFieldModel> efm
Tps< T > sqrt(const Tps< T > &x)
Square root.
virtual void visitScalingFFAMagnet(const ScalingFFAMagnet &)=0
Apply the algorithm to a scaling FFA magnet.
BGeometryBase & getGeometry() override
void initialise(PartBunchBase< double, 3 > *bunch, double &startField, double &endField) override
virtual void setElementLength(double)
Set length.
void setPhiStart(double phiStart)
bool bends() const override
PETE_TUTree< FnAbs, typename T::PETE_Expr_t > abs(const PETE_Expr< T > &l)
Abstract base class for electromagnetic fields.
virtual void setMaximumDerivative(size_t n)=0
virtual double getEndLength() const =0
Abstract base class for accelerator geometry classes.
PartBunchBase< double, 3 > * RefPartBunch_m
std::string endFieldName_m
ScalingFFAMagnet * clone() const override
void setCurvature(double)
Set curvature.
ScalingFFAMagnet(const std::string &name)
EMField & getField() override
void setEndField(endfieldmodel::EndFieldModel *endField)
PETE_TBTree< FnArcTan2, PETE_Scalar< Vektor< T1, Dim > >, typename T2::PETE_Expr_t > atan2(const Vektor< T1, Dim > &l, const PETE_Expr< T2 > &r)
PlanarArcGeometry planarArcGeometry_m
bool getFieldValue(const Vector_t &R, Vector_t &B) const
double getPhiStart() const
virtual EndFieldModel * clone() const =0
bool getFieldValueCylindrical(const Vector_t &R, Vector_t &B) const
virtual void rescale(double scaleFactor)=0
virtual double getCentreLength() const =0
void accept(BeamlineVisitor &visitor) const override
virtual double function(double x, int n) const =0
Tps< T > cos(const Tps< T > &x)
Cosine.
Tps< T > log(const Tps< T > &x)
Natural logarithm.
std::vector< std::vector< double > > dfCoefficients_m
void calculateDfCoefficients()
endfieldmodel::EndFieldModel * endField_m
Interface for a single beam element.
Tps< T > pow(const Tps< T > &x, int y)
Integer power.
Tps< T > sin(const Tps< T > &x)
Sine.
static std::shared_ptr< EndFieldModel > getEndFieldModel(std::string name)
void setAzimuthalExtent(double azimuthalExtent)
void setPhiEnd(double phiEnd)
item[EANGLE] Entrance edge counterclockwise This enables to obtain skew at each point along the magnet