Classes
struct	PreparedBrokenLineData
	data needed for the Broken Line fit procedure. More...

Typedefs
using	karimaki_circle_fit = riemannFit::CircleFit
	< Karimäki's parameters: (phi, d, k=1/R) More...

Functions
template<typename M3xN , typename M6xN , typename V4 , int n>
__host__ __device__ void	circleFit (const M3xN &hits, const M6xN &hits_ge, const V4 &fast_fit, const double bField, PreparedBrokenLineData< n > &data, karimaki_circle_fit &circle_results)
	Performs the Broken Line fit in the curved track case (that is, the fit parameters are the interceptions u and the curvature correction ). More...

template<typename M3xN , typename V4 >
__host__ __device__ void	fastFit (const M3xN &hits, V4 &result)
	A very fast helix fit. More...

template<int n>
riemannFit::HelixFit	helixFit (const riemannFit::Matrix3xNd< n > &hits, const Eigen::Matrix< float, 6, 4 > &hits_ge, const double bField)
	Helix fit by three step: -fast pre-fit (see Fast_fit() for further info); -circle fit of the hits projected in the transverse plane by Broken Line algorithm (see BL_Circle_fit() for further info); -line fit of the hits projected on the (pre-fitted) cilinder surface by Broken Line algorithm (see BL_Line_fit() for further info); Points must be passed ordered (from inner to outer layer). More...

template<typename V4 , typename M6xN , int n>
__host__ __device__ void	lineFit (const M6xN &hits_ge, const V4 &fast_fit, const double bField, const PreparedBrokenLineData< n > &data, riemannFit::LineFit &line_results)
	Performs the Broken Line fit in the straight track case (that is, the fit parameters are only the interceptions u). More...

template<int n>
__host__ __device__ riemannFit::MatrixNd< n >	matrixC_u (const riemannFit::VectorNd< n > &weights, const riemannFit::VectorNd< n > &sTotal, const riemannFit::VectorNd< n > &varBeta)
	Computes the n-by-n band matrix obtained minimizing the Broken Line's cost function w.r.t u. This is the whole matrix in the case of the line fit and the main n-by-n block in the case of the circle fit. More...

__host__ __device__ double	multScatt (const double &length, const double bField, const double radius, int layer, double slope)
	Computes the Coulomb multiple scattering variance of the planar angle. More...

template<typename M3xN , typename V4 , int n>
__host__ __device__ void	prepareBrokenLineData (const M3xN &hits, const V4 &fast_fit, const double bField, PreparedBrokenLineData< n > &results)
	Computes the data needed for the Broken Line fit procedure that are mainly common for the circle and the line fit. More...

__host__ __device__ riemannFit::Matrix2d	rotationMatrix (double slope)
	Computes the 2D rotation matrix that transforms the line y=slope*x into the line y=0. More...

__host__ __device__ void	translateKarimaki (karimaki_circle_fit &circle, double x0, double y0, riemannFit::Matrix3d &jacobian)
	Changes the Karimäki parameters (and consequently their covariance matrix) under a translation of the coordinate system, such that the old origin has coordinates (x0,y0) in the new coordinate system. The formulas are taken from Karimäki V., 1990, Effective circle fitting for particle trajectories, Nucl. Instr. and Meth. A305 (1991) 187. More...

Typedef Documentation

◆ karimaki_circle_fit

using brokenline::karimaki_circle_fit = typedef riemannFit::CircleFit

< Karimäki's parameters: (phi, d, k=1/R)

Definition at line 19 of file BrokenLine.h.

Function Documentation

◆ circleFit()

template<typename M3xN , typename M6xN , typename V4 , int n>

__host__ __device__ void brokenline::circleFit	(	const M3xN &	hits,
		const M6xN &	hits_ge,
		const V4 &	fast_fit,
		const double	bField,
		PreparedBrokenLineData< n > &	data,
		karimaki_circle_fit &	circle_results
	)

inline

Performs the Broken Line fit in the curved track case (that is, the fit parameters are the interceptions u and the curvature correction ).

Parameters

hits	hits coordinates.
hits_cov	hits covariance matrix.
fast_fit	pre-fit result in the form (X0,Y0,R,tan(theta)).
bField	magnetic field in Gev/cm/c.
data	PreparedBrokenLineData.
circle_results	struct to be filled with the results in this form: -par parameter of the line in this form: (phi, d, k); -cov covariance matrix of the fitted parameter; -chi2 value of the cost function in the minimum.

The function implements the steps 2 and 3 of the Broken Line fit with the curvature correction.
The step 2 is the least square fit, done by imposing the minimum constraint on the cost function and solving the consequent linear system. It determines the fitted parameters u and and their covariance matrix. The step 3 is the correction of the fast pre-fitted parameters for the innermost part of the track. It is first done in a comfortable coordinate system (the one in which the first hit is the origin) and then the parameters and their covariance matrix are transformed to the original coordinate system.

Definition at line 315 of file BrokenLine.h.

Referenced by helixFit().

                                                                                  {
     circle_results.qCharge = data.qCharge;
     auto& radii = data.radii;
     const auto& sTransverse = data.sTransverse;
     const auto& sTotal = data.sTotal;
     auto& zInSZplane = data.zInSZplane;
     auto& varBeta = data.varBeta;
     const double slope = -circle_results.qCharge / fast_fit(3);
     varBeta *= 1. + riemannFit::sqr(slope);  // the kink angles are projected!
 
     for (u_int i = 0; i < n; i++) {
       zInSZplane(i) = radii.block(0, i, 2, 1).norm() - fast_fit(2);
     }
 
     riemannFit::Matrix2d vMat;           // covariance matrix
     riemannFit::VectorNd<n> weightsVec;  // weights
     riemannFit::Matrix2d rotMat;         // rotation matrix point by point
     for (u_int i = 0; i < n; i++) {
       vMat(0, 0) = hits_ge.col(i)[0];               // x errors
       vMat(0, 1) = vMat(1, 0) = hits_ge.col(i)[1];  // cov_xy
       vMat(1, 1) = hits_ge.col(i)[2];               // y errors
       rotMat = rotationMatrix(-radii(0, i) / radii(1, i));
       weightsVec(i) =
           1. / ((rotMat * vMat * rotMat.transpose())(1, 1));  // compute the orthogonal weight point by point
     }
 
     riemannFit::VectorNplusONEd<n> r_uVec;
     r_uVec(n) = 0;
     for (u_int i = 0; i < n; i++) {
       r_uVec(i) = weightsVec(i) * zInSZplane(i);
     }
 
     riemannFit::MatrixNplusONEd<n> c_uMat;
     c_uMat.block(0, 0, n, n) = matrixC_u(weightsVec, sTransverse, varBeta);
     c_uMat(n, n) = 0;
     //add the border to the c_uMat matrix
     for (u_int i = 0; i < n; i++) {
       c_uMat(i, n) = 0;
       if (i > 0 && i < n - 1) {
         c_uMat(i, n) +=
             -(sTransverse(i + 1) - sTransverse(i - 1)) * (sTransverse(i + 1) - sTransverse(i - 1)) /
             (2. * varBeta(i) * (sTransverse(i + 1) - sTransverse(i)) * (sTransverse(i) - sTransverse(i - 1)));
       }
       if (i > 1) {
         c_uMat(i, n) +=
             (sTransverse(i) - sTransverse(i - 2)) / (2. * varBeta(i - 1) * (sTransverse(i) - sTransverse(i - 1)));
       }
       if (i < n - 2) {
         c_uMat(i, n) +=
             (sTransverse(i + 2) - sTransverse(i)) / (2. * varBeta(i + 1) * (sTransverse(i + 1) - sTransverse(i)));
       }
       c_uMat(n, i) = c_uMat(i, n);
       if (i > 0 && i < n - 1)
         c_uMat(n, n) += riemannFit::sqr(sTransverse(i + 1) - sTransverse(i - 1)) / (4. * varBeta(i));
     }
 
 #ifdef CPP_DUMP
     std::cout << "CU5\n" << c_uMat << std::endl;
 #endif
     riemannFit::MatrixNplusONEd<n> iMat;
     math::cholesky::invert(c_uMat, iMat);
 #ifdef CPP_DUMP
     std::cout << "I5\n" << iMat << std::endl;
 #endif
 
     riemannFit::VectorNplusONEd<n> uVec = iMat * r_uVec;  // obtain the fitted parameters by solving the linear system
 
     // compute (phi, d_ca, k) in the system in which the midpoint of the first two corrected hits is the origin...
 
     radii.block(0, 0, 2, 1) /= radii.block(0, 0, 2, 1).norm();
     radii.block(0, 1, 2, 1) /= radii.block(0, 1, 2, 1).norm();
 
     riemannFit::Vector2d dVec = hits.block(0, 0, 2, 1) + (-zInSZplane(0) + uVec(0)) * radii.block(0, 0, 2, 1);
     riemannFit::Vector2d eVec = hits.block(0, 1, 2, 1) + (-zInSZplane(1) + uVec(1)) * radii.block(0, 1, 2, 1);
     auto eMinusd = eVec - dVec;
     auto eMinusd2 = eMinusd.squaredNorm();
     auto tmp1 = 1. / eMinusd2;
     auto tmp2 = sqrt(riemannFit::sqr(fast_fit(2)) - 0.25 * eMinusd2);
 
     circle_results.par << atan2(eMinusd(1), eMinusd(0)), circle_results.qCharge * (tmp2 - fast_fit(2)),
         circle_results.qCharge * (1. / fast_fit(2) + uVec(n));
 
     tmp2 = 1. / tmp2;
 
     riemannFit::Matrix3d jacobian;
     jacobian << (radii(1, 0) * eMinusd(0) - eMinusd(1) * radii(0, 0)) * tmp1,
         (radii(1, 1) * eMinusd(0) - eMinusd(1) * radii(0, 1)) * tmp1, 0,
         circle_results.qCharge * (eMinusd(0) * radii(0, 0) + eMinusd(1) * radii(1, 0)) * tmp2,
         circle_results.qCharge * (eMinusd(0) * radii(0, 1) + eMinusd(1) * radii(1, 1)) * tmp2, 0, 0, 0,
         circle_results.qCharge;
 
     circle_results.cov << iMat(0, 0), iMat(0, 1), iMat(0, n), iMat(1, 0), iMat(1, 1), iMat(1, n), iMat(n, 0),
         iMat(n, 1), iMat(n, n);
 
     circle_results.cov = jacobian * circle_results.cov * jacobian.transpose();
 
     //...Translate in the system in which the first corrected hit is the origin, adding the m.s. correction...
 
     translateKarimaki(circle_results, 0.5 * eMinusd(0), 0.5 * eMinusd(1), jacobian);
     circle_results.cov(0, 0) +=
         (1 + riemannFit::sqr(slope)) * multScatt(sTotal(1) - sTotal(0), bField, fast_fit(2), 2, slope);
 
     //...And translate back to the original system
 
     translateKarimaki(circle_results, dVec(0), dVec(1), jacobian);
 
     // compute chi2
     circle_results.chi2 = 0;
     for (u_int i = 0; i < n; i++) {
       circle_results.chi2 += weightsVec(i) * riemannFit::sqr(zInSZplane(i) - uVec(i));
       if (i > 0 && i < n - 1)
         circle_results.chi2 +=
             riemannFit::sqr(uVec(i - 1) / (sTransverse(i) - sTransverse(i - 1)) -
                             uVec(i) * (sTransverse(i + 1) - sTransverse(i - 1)) /
                                 ((sTransverse(i + 1) - sTransverse(i)) * (sTransverse(i) - sTransverse(i - 1))) +
                             uVec(i + 1) / (sTransverse(i + 1) - sTransverse(i)) +
                             (sTransverse(i + 1) - sTransverse(i - 1)) * uVec(n) / 2) /
             varBeta(i);
     }
   }

◆ fastFit()

template<typename M3xN , typename V4 >

__host__ __device__ void brokenline::fastFit	(	const M3xN &	hits,
		V4 &	result
	)

inline

A very fast helix fit.

Parameters

hits	the measured hits.

Returns: (X0,Y0,R,tan(theta)).

Warning: sign of theta is (intentionally, for now) mistaken for negative charges.

Definition at line 259 of file BrokenLine.h.

References a, funct::abs(), b, HltBtagPostValidation_cff::c, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::constexpr(), riemannFit::cross2D(), ztail::d, d1, MillePedeFileConverter_cfg::e, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::hits, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::mId, dqmiodumpmetadata::n, mps_fire::result, mathSSE::sqrt(), and createJobs::tmp.

Referenced by for(), and helixFit().

                                                                         {
     constexpr uint32_t n = M3xN::ColsAtCompileTime;
 
     int mId = 1;
 
     if constexpr (n > 3) {
       riemannFit::Vector2d middle = 0.5 * (hits.block(0, n - 1, 2, 1) + hits.block(0, 0, 2, 1));
       auto d1 = (hits.block(0, n / 2, 2, 1) - middle).squaredNorm();
       auto d2 = (hits.block(0, n / 2 - 1, 2, 1) - middle).squaredNorm();
       mId = d1 < d2 ? n / 2 : n / 2 - 1;
     }
 
     const riemannFit::Vector2d a = hits.block(0, mId, 2, 1) - hits.block(0, 0, 2, 1);
     const riemannFit::Vector2d b = hits.block(0, n - 1, 2, 1) - hits.block(0, mId, 2, 1);
     const riemannFit::Vector2d c = hits.block(0, 0, 2, 1) - hits.block(0, n - 1, 2, 1);
 
     auto tmp = 0.5 / riemannFit::cross2D(c, a);
     result(0) = hits(0, 0) - (a(1) * c.squaredNorm() + c(1) * a.squaredNorm()) * tmp;
     result(1) = hits(1, 0) + (a(0) * c.squaredNorm() + c(0) * a.squaredNorm()) * tmp;
     // check Wikipedia for these formulas
 
     result(2) = sqrt(a.squaredNorm() * b.squaredNorm() * c.squaredNorm()) / (2. * std::abs(riemannFit::cross2D(b, a)));
     // Using Math Olympiad's formula R=abc/(4A)
 
     const riemannFit::Vector2d d = hits.block(0, 0, 2, 1) - result.head(2);
     const riemannFit::Vector2d e = hits.block(0, n - 1, 2, 1) - result.head(2);
 
     result(3) = result(2) * atan2(riemannFit::cross2D(d, e), d.dot(e)) / (hits(2, n - 1) - hits(2, 0));
     // ds/dz slope between last and first point
   }

◆ helixFit()

template<int n>

riemannFit::HelixFit brokenline::helixFit	(	const riemannFit::Matrix3xNd< n > &	hits,
		const Eigen::Matrix< float, 6, 4 > &	hits_ge,
		const double	bField
	)

inline

Helix fit by three step: -fast pre-fit (see Fast_fit() for further info);
-circle fit of the hits projected in the transverse plane by Broken Line algorithm (see BL_Circle_fit() for further info);
-line fit of the hits projected on the (pre-fitted) cilinder surface by Broken Line algorithm (see BL_Line_fit() for further info);
Points must be passed ordered (from inner to outer layer).

Parameters

hits	Matrix3xNd hits coordinates in this form: \|x1\|x2\|x3\|...\|xn\| \|y1\|y2\|y3\|...\|yn\| \|z1\|z2\|z3\|...\|zn\|
hits_cov	Matrix3Nd covariance matrix in this form (()->cov()): \|(x1,x1)\|(x2,x1)\|(x3,x1)\|(x4,x1)\|.\|(y1,x1)\|(y2,x1)\|(y3,x1)\|(y4,x1)\|.\|(z1,x1)\|(z2,x1)\|(z3,x1)\|(z4,x1)\| \|(x1,x2)\|(x2,x2)\|(x3,x2)\|(x4,x2)\|.\|(y1,x2)\|(y2,x2)\|(y3,x2)\|(y4,x2)\|.\|(z1,x2)\|(z2,x2)\|(z3,x2)\|(z4,x2)\| \|(x1,x3)\|(x2,x3)\|(x3,x3)\|(x4,x3)\|.\|(y1,x3)\|(y2,x3)\|(y3,x3)\|(y4,x3)\|.\|(z1,x3)\|(z2,x3)\|(z3,x3)\|(z4,x3)\| \|(x1,x4)\|(x2,x4)\|(x3,x4)\|(x4,x4)\|.\|(y1,x4)\|(y2,x4)\|(y3,x4)\|(y4,x4)\|.\|(z1,x4)\|(z2,x4)\|(z3,x4)\|(z4,x4)\| . . . . . . . . . . . . . . . \|(x1,y1)\|(x2,y1)\|(x3,y1)\|(x4,y1)\|.\|(y1,y1)\|(y2,y1)\|(y3,x1)\|(y4,y1)\|.\|(z1,y1)\|(z2,y1)\|(z3,y1)\|(z4,y1)\| \|(x1,y2)\|(x2,y2)\|(x3,y2)\|(x4,y2)\|.\|(y1,y2)\|(y2,y2)\|(y3,x2)\|(y4,y2)\|.\|(z1,y2)\|(z2,y2)\|(z3,y2)\|(z4,y2)\| \|(x1,y3)\|(x2,y3)\|(x3,y3)\|(x4,y3)\|.\|(y1,y3)\|(y2,y3)\|(y3,x3)\|(y4,y3)\|.\|(z1,y3)\|(z2,y3)\|(z3,y3)\|(z4,y3)\| \|(x1,y4)\|(x2,y4)\|(x3,y4)\|(x4,y4)\|.\|(y1,y4)\|(y2,y4)\|(y3,x4)\|(y4,y4)\|.\|(z1,y4)\|(z2,y4)\|(z3,y4)\|(z4,y4)\| . . . . . . . . . . . . . . . \|(x1,z1)\|(x2,z1)\|(x3,z1)\|(x4,z1)\|.\|(y1,z1)\|(y2,z1)\|(y3,z1)\|(y4,z1)\|.\|(z1,z1)\|(z2,z1)\|(z3,z1)\|(z4,z1)\| \|(x1,z2)\|(x2,z2)\|(x3,z2)\|(x4,z2)\|.\|(y1,z2)\|(y2,z2)\|(y3,z2)\|(y4,z2)\|.\|(z1,z2)\|(z2,z2)\|(z3,z2)\|(z4,z2)\| \|(x1,z3)\|(x2,z3)\|(x3,z3)\|(x4,z3)\|.\|(y1,z3)\|(y2,z3)\|(y3,z3)\|(y4,z3)\|.\|(z1,z3)\|(z2,z3)\|(z3,z3)\|(z4,z3)\| \|(x1,z4)\|(x2,z4)\|(x3,z4)\|(x4,z4)\|.\|(y1,z4)\|(y2,z4)\|(y3,z4)\|(y4,z4)\|.\|(z1,z4)\|(z2,z4)\|(z3,z4)\|(z4,z4)\|
bField	magnetic field in the center of the detector in Gev/cm/c, in order to perform the p_t calculation.

Warning: see BL_Circle_fit(), BL_Line_fit() and Fast_fit() warnings.

Returns: (phi,Tip,p_t,cot(theta)),Zip), their covariance matrix and the chi2's of the circle and line fits.

Definition at line 585 of file BrokenLine.h.

References funct::abs(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::bField, riemannFit::CircleFit::chi2, riemannFit::HelixFit::chi2_circle, riemannFit::HelixFit::chi2_line, circleFit(), riemannFit::CircleFit::cov, riemannFit::HelixFit::cov, data, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::fast_fit, fastFit(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::hits, mps_splice::line, lineFit(), riemannFit::CircleFit::par, riemannFit::HelixFit::par, prepareBrokenLineData(), riemannFit::CircleFit::qCharge, riemannFit::HelixFit::qCharge, and riemannFit::sqr().

Referenced by PixelNtupletsFitter::run().

                                                             {
     riemannFit::HelixFit helix;
     riemannFit::Vector4d fast_fit;
     fastFit(hits, fast_fit);
 
     PreparedBrokenLineData<n> data;
     karimaki_circle_fit circle;
     riemannFit::LineFit line;
     riemannFit::Matrix3d jacobian;
 
     prepareBrokenLineData(hits, fast_fit, bField, data);
     lineFit(hits_ge, fast_fit, bField, data, line);
     circleFit(hits, hits_ge, fast_fit, bField, data, circle);
 
     // the circle fit gives k, but here we want p_t, so let's change the parameter and the covariance matrix
     jacobian << 1., 0, 0, 0, 1., 0, 0, 0,
         -std::abs(circle.par(2)) * bField / (riemannFit::sqr(circle.par(2)) * circle.par(2));
     circle.par(2) = bField / std::abs(circle.par(2));
     circle.cov = jacobian * circle.cov * jacobian.transpose();
 
     helix.par << circle.par, line.par;
     helix.cov = riemannFit::MatrixXd::Zero(5, 5);
     helix.cov.block(0, 0, 3, 3) = circle.cov;
     helix.cov.block(3, 3, 2, 2) = line.cov;
     helix.qCharge = circle.qCharge;
     helix.chi2_circle = circle.chi2;
     helix.chi2_line = line.chi2;
 
     return helix;
   }

◆ lineFit()

template<typename V4 , typename M6xN , int n>

__host__ __device__ void brokenline::lineFit	(	const M6xN &	hits_ge,
		const V4 &	fast_fit,
		const double	bField,
		const PreparedBrokenLineData< n > &	data,
		riemannFit::LineFit &	line_results
	)

inline

Performs the Broken Line fit in the straight track case (that is, the fit parameters are only the interceptions u).

Parameters

hits	hits coordinates.
fast_fit	pre-fit result in the form (X0,Y0,R,tan(theta)).
bField	magnetic field in Gev/cm/c.
data	PreparedBrokenLineData.
line_results	struct to be filled with the results in this form: -par parameter of the line in this form: (cot(theta), Zip); -cov covariance matrix of the fitted parameter; -chi2 value of the cost function in the minimum.

The function implements the steps 2 and 3 of the Broken Line fit without the curvature correction.
The step 2 is the least square fit, done by imposing the minimum constraint on the cost function and solving the consequent linear system. It determines the fitted parameters u and their covariance matrix. The step 3 is the correction of the fast pre-fitted parameters for the innermost part of the track. It is first done in a comfortable coordinate system (the one in which the first hit is the origin) and then the parameters and their covariance matrix are transformed to the original coordinate system.

Definition at line 464 of file BrokenLine.h.

References ALPAKA_ACCELERATOR_NAMESPACE::brokenline::bField, riemannFit::LineFit::chi2, gather_cfg::cout, riemannFit::LineFit::cov, data, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::fast_fit, mps_fire::i, l1tstage2_dqm_sourceclient-live_cfg::invert, matrixC_u(), multScatt(), dqmiodumpmetadata::n, riemannFit::LineFit::par, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::radii, rotationMatrix(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::rotMat, slope, riemannFit::sqr(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::sTotal, createJobs::tmp, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::varBeta(), w(), hltDeepSecondaryVertexTagInfosPFPuppi_cfi::weights, and ALPAKA_ACCELERATOR_NAMESPACE::brokenline::zInSZplane.

Referenced by helixFit().

                                                                            {
     const auto& radii = data.radii;
     const auto& sTotal = data.sTotal;
     const auto& zInSZplane = data.zInSZplane;
     const auto& varBeta = data.varBeta;
 
     const double slope = -data.qCharge / fast_fit(3);
     riemannFit::Matrix2d rotMat = rotationMatrix(slope);
 
     riemannFit::Matrix3d vMat = riemannFit::Matrix3d::Zero();  // covariance matrix XYZ
     riemannFit::Matrix2x3d jacobXYZtosZ =
         riemannFit::Matrix2x3d::Zero();  // jacobian for computation of the error on s (xyz -> sz)
     riemannFit::VectorNd<n> weights = riemannFit::VectorNd<n>::Zero();
     for (u_int i = 0; i < n; i++) {
       vMat(0, 0) = hits_ge.col(i)[0];               // x errors
       vMat(0, 1) = vMat(1, 0) = hits_ge.col(i)[1];  // cov_xy
       vMat(0, 2) = vMat(2, 0) = hits_ge.col(i)[3];  // cov_xz
       vMat(1, 1) = hits_ge.col(i)[2];               // y errors
       vMat(2, 1) = vMat(1, 2) = hits_ge.col(i)[4];  // cov_yz
       vMat(2, 2) = hits_ge.col(i)[5];               // z errors
       auto tmp = 1. / radii.block(0, i, 2, 1).norm();
       jacobXYZtosZ(0, 0) = radii(1, i) * tmp;
       jacobXYZtosZ(0, 1) = -radii(0, i) * tmp;
       jacobXYZtosZ(1, 2) = 1.;
       weights(i) = 1. / ((rotMat * jacobXYZtosZ * vMat * jacobXYZtosZ.transpose() * rotMat.transpose())(
                             1, 1));  // compute the orthogonal weight point by point
     }
 
     riemannFit::VectorNd<n> r_u;
     for (u_int i = 0; i < n; i++) {
       r_u(i) = weights(i) * zInSZplane(i);
     }
 #ifdef CPP_DUMP
     std::cout << "CU4\n" << matrixC_u(w, sTotal, varBeta) << std::endl;
 #endif
     riemannFit::MatrixNd<n> iMat;
     math::cholesky::invert(matrixC_u(weights, sTotal, varBeta), iMat);
 #ifdef CPP_DUMP
     std::cout << "I4\n" << iMat << std::endl;
 #endif
 
     riemannFit::VectorNd<n> uVec = iMat * r_u;  // obtain the fitted parameters by solving the linear system
 
     // line parameters in the system in which the first hit is the origin and with axis along SZ
     line_results.par << (uVec(1) - uVec(0)) / (sTotal(1) - sTotal(0)), uVec(0);
     auto idiff = 1. / (sTotal(1) - sTotal(0));
     line_results.cov << (iMat(0, 0) - 2 * iMat(0, 1) + iMat(1, 1)) * riemannFit::sqr(idiff) +
                             multScatt(sTotal(1) - sTotal(0), bField, fast_fit(2), 2, slope),
         (iMat(0, 1) - iMat(0, 0)) * idiff, (iMat(0, 1) - iMat(0, 0)) * idiff, iMat(0, 0);
 
     // translate to the original SZ system
     riemannFit::Matrix2d jacobian;
     jacobian(0, 0) = 1.;
     jacobian(0, 1) = 0;
     jacobian(1, 0) = -sTotal(0);
     jacobian(1, 1) = 1.;
     line_results.par(1) += -line_results.par(0) * sTotal(0);
     line_results.cov = jacobian * line_results.cov * jacobian.transpose();
 
     // rotate to the original sz system
     auto tmp = rotMat(0, 0) - line_results.par(0) * rotMat(0, 1);
     jacobian(1, 1) = 1. / tmp;
     jacobian(0, 0) = jacobian(1, 1) * jacobian(1, 1);
     jacobian(0, 1) = 0;
     jacobian(1, 0) = line_results.par(1) * rotMat(0, 1) * jacobian(0, 0);
     line_results.par(1) = line_results.par(1) * jacobian(1, 1);
     line_results.par(0) = (rotMat(0, 1) + line_results.par(0) * rotMat(0, 0)) * jacobian(1, 1);
     line_results.cov = jacobian * line_results.cov * jacobian.transpose();
 
     // compute chi2
     line_results.chi2 = 0;
     for (u_int i = 0; i < n; i++) {
       line_results.chi2 += weights(i) * riemannFit::sqr(zInSZplane(i) - uVec(i));
       if (i > 0 && i < n - 1)
         line_results.chi2 += riemannFit::sqr(uVec(i - 1) / (sTotal(i) - sTotal(i - 1)) -
                                              uVec(i) * (sTotal(i + 1) - sTotal(i - 1)) /
                                                  ((sTotal(i + 1) - sTotal(i)) * (sTotal(i) - sTotal(i - 1))) +
                                              uVec(i + 1) / (sTotal(i + 1) - sTotal(i))) /
                              varBeta(i);
     }
   }

◆ matrixC_u()

template<int n>

__host__ __device__ riemannFit::MatrixNd<n> brokenline::matrixC_u	(	const riemannFit::VectorNd< n > &	weights,
		const riemannFit::VectorNd< n > &	sTotal,
		const riemannFit::VectorNd< n > &	varBeta
	)

inline

Computes the n-by-n band matrix obtained minimizing the Broken Line's cost function w.r.t u. This is the whole matrix in the case of the line fit and the main n-by-n block in the case of the circle fit.

Parameters

weights	weights of the first part of the cost function, the one with the measurements and not the angles ({i=1}^n w*(y_i-u_i)^2).
sTotal	total distance traveled by the particle from the pre-fitted closest approach.
varBeta	kink angles' variance.

Returns: the n-by-n matrix of the linear system

Definition at line 216 of file BrokenLine.h.

References mps_fire::i, dqmiodumpmetadata::n, riemannFit::sqr(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::sTotal, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::varBeta(), and hltDeepSecondaryVertexTagInfosPFPuppi_cfi::weights.

Referenced by circleFit(), and lineFit().

                                                                                                      {
     riemannFit::MatrixNd<n> c_uMat = riemannFit::MatrixNd<n>::Zero();
     for (u_int i = 0; i < n; i++) {
       c_uMat(i, i) = weights(i);
       if (i > 1)
         c_uMat(i, i) += 1. / (varBeta(i - 1) * riemannFit::sqr(sTotal(i) - sTotal(i - 1)));
       if (i > 0 && i < n - 1)
         c_uMat(i, i) +=
             (1. / varBeta(i)) * riemannFit::sqr((sTotal(i + 1) - sTotal(i - 1)) /
                                                 ((sTotal(i + 1) - sTotal(i)) * (sTotal(i) - sTotal(i - 1))));
       if (i < n - 2)
         c_uMat(i, i) += 1. / (varBeta(i + 1) * riemannFit::sqr(sTotal(i + 1) - sTotal(i)));
 
       if (i > 0 && i < n - 1)
         c_uMat(i, i + 1) =
             1. / (varBeta(i) * (sTotal(i + 1) - sTotal(i))) *
             (-(sTotal(i + 1) - sTotal(i - 1)) / ((sTotal(i + 1) - sTotal(i)) * (sTotal(i) - sTotal(i - 1))));
       if (i < n - 2)
         c_uMat(i, i + 1) +=
             1. / (varBeta(i + 1) * (sTotal(i + 1) - sTotal(i))) *
             (-(sTotal(i + 2) - sTotal(i)) / ((sTotal(i + 2) - sTotal(i + 1)) * (sTotal(i + 1) - sTotal(i))));
 
       if (i < n - 2)
         c_uMat(i, i + 2) = 1. / (varBeta(i + 1) * (sTotal(i + 2) - sTotal(i + 1)) * (sTotal(i + 1) - sTotal(i)));
 
       c_uMat(i, i) *= 0.5;
     }
     return c_uMat + c_uMat.transpose();
   }

◆ multScatt()

__host__ __device__ double brokenline::multScatt	(	const double &	length,
		const double	bField,
		const double	radius,
		int	layer,
		double	slope
	)

inline

Computes the Coulomb multiple scattering variance of the planar angle.

Parameters

length	length of the track in the material.
bField	magnetic field in Gev/cm/c.
radius	radius of curvature (needed to evaluate p).
layer	denotes which of the four layers of the detector is the endpoint of the multiple scattered track. For example, if Layer=3, then the particle has just gone through the material between the second and the third layer.

Warning: the formula used here assumes beta=1, and so neglects the dependence of theta_0 on the mass of the particle at fixed momentum.

Returns: the variance of the planar angle ((theta_0)^2 /3).

< inverse of radiation length of the material in cm

number between 1/3 (uniform material) and 1 (thin scatterer) to be manually tuned

Definition at line 54 of file BrokenLine.h.

References funct::abs(), ALPAKA_ACCELERATOR_NAMESPACE::brokenline::bField, ALPAKA_ACCELERATOR_NAMESPACE::brokenline::constexpr(), fact, dqm-mbProfile::log, SiStripPI::min, HLT_2024v14_cff::pt2, CosmicsPD_Skims::radius, slope, and riemannFit::sqr().

Referenced by circleFit(), lineFit(), and prepareBrokenLineData().

                                                                                                {
     // limit R to 20GeV...
     auto pt2 = std::min(20., bField * radius);
     pt2 *= pt2;
     constexpr double inv_X0 = 0.06 / 16.;  
     //if(Layer==1) XXI_0=0.06/16.;
     // else XXI_0=0.06/16.;
     //XX_0*=1;
 
     constexpr double geometry_factor = 0.7;
     constexpr double fact = geometry_factor * riemannFit::sqr(13.6 / 1000.);
     return fact / (pt2 * (1. + riemannFit::sqr(slope))) * (std::abs(length) * inv_X0) *
            riemannFit::sqr(1. + 0.038 * log(std::abs(length) * inv_X0));
   }

◆ prepareBrokenLineData()

template<typename M3xN , typename V4 , int n>

__host__ __device__ void brokenline::prepareBrokenLineData	(	const M3xN &	hits,
		const V4 &	fast_fit,
		const double	bField,
		PreparedBrokenLineData< n > &	results
	)

inline

Computes the data needed for the Broken Line fit procedure that are mainly common for the circle and the line fit.

Parameters

hits	hits coordinates.
fast_fit	pre-fit result in the form (X0,Y0,R,tan(theta)).
bField	magnetic field in Gev/cm/c.
results	PreparedBrokenLineData to be filled (see description of PreparedBrokenLineData).

Definition at line 151 of file BrokenLine.h.

Referenced by helixFit(), ALPAKA_ACCELERATOR_NAMESPACE::Kernel_BLFit< N, TrackerTraits >::operator()(), and ALPAKA_ACCELERATOR_NAMESPACE::brokenline::helixFit< n >::operator()().

                                                                                             {
     riemannFit::Vector2d dVec;
     riemannFit::Vector2d eVec;
 
     int mId = 1;
 
     if constexpr (n > 3) {
       riemannFit::Vector2d middle = 0.5 * (hits.block(0, n - 1, 2, 1) + hits.block(0, 0, 2, 1));
       auto d1 = (hits.block(0, n / 2, 2, 1) - middle).squaredNorm();
       auto d2 = (hits.block(0, n / 2 - 1, 2, 1) - middle).squaredNorm();
       mId = d1 < d2 ? n / 2 : n / 2 - 1;
     }
 
     dVec = hits.block(0, mId, 2, 1) - hits.block(0, 0, 2, 1);
     eVec = hits.block(0, n - 1, 2, 1) - hits.block(0, mId, 2, 1);
     results.qCharge = riemannFit::cross2D(dVec, eVec) > 0 ? -1 : 1;
 
     const double slope = -results.qCharge / fast_fit(3);
 
     riemannFit::Matrix2d rotMat = rotationMatrix(slope);
 
     // calculate radii and s
     results.radii = hits.block(0, 0, 2, n) - fast_fit.head(2) * riemannFit::MatrixXd::Constant(1, n, 1);
     eVec = -fast_fit(2) * fast_fit.head(2) / fast_fit.head(2).norm();
     for (u_int i = 0; i < n; i++) {
       dVec = results.radii.block(0, i, 2, 1);
       results.sTransverse(i) = results.qCharge * fast_fit(2) *
                                atan2(riemannFit::cross2D(dVec, eVec), dVec.dot(eVec));  // calculates the arc length
     }
     riemannFit::VectorNd<n> zVec = hits.block(2, 0, 1, n).transpose();
 
     //calculate sTotal and zVec
     riemannFit::Matrix2xNd<n> pointsSZ = riemannFit::Matrix2xNd<n>::Zero();
     for (u_int i = 0; i < n; i++) {
       pointsSZ(0, i) = results.sTransverse(i);
       pointsSZ(1, i) = zVec(i);
       pointsSZ.block(0, i, 2, 1) = rotMat * pointsSZ.block(0, i, 2, 1);
     }
     results.sTotal = pointsSZ.block(0, 0, 1, n).transpose();
     results.zInSZplane = pointsSZ.block(1, 0, 1, n).transpose();
 
     //calculate varBeta
     results.varBeta(0) = results.varBeta(n - 1) = 0;
     for (u_int i = 1; i < n - 1; i++) {
       results.varBeta(i) = multScatt(results.sTotal(i + 1) - results.sTotal(i), bField, fast_fit(2), i + 2, slope) +
                            multScatt(results.sTotal(i) - results.sTotal(i - 1), bField, fast_fit(2), i + 1, slope);
     }
   }

◆ rotationMatrix()

__host__ __device__ riemannFit::Matrix2d brokenline::rotationMatrix ( double slope )

inline

Computes the 2D rotation matrix that transforms the line y=slope*x into the line y=0.

Parameters

slope tangent of the angle of rotation.

Returns: 2D rotation matrix.

Definition at line 78 of file BrokenLine.h.

References makeMuonMisalignmentScenario::rot, slope, riemannFit::sqr(), and mathSSE::sqrt().

Referenced by circleFit(), lineFit(), and prepareBrokenLineData().

                                                                              {
     riemannFit::Matrix2d rot;
     rot(0, 0) = 1. / sqrt(1. + riemannFit::sqr(slope));
     rot(0, 1) = slope * rot(0, 0);
     rot(1, 0) = -rot(0, 1);
     rot(1, 1) = rot(0, 0);
     return rot;
   }

◆ translateKarimaki()

__host__ __device__ void brokenline::translateKarimaki	(	karimaki_circle_fit &	circle,
		double	x0,
		double	y0,
		riemannFit::Matrix3d &	jacobian
	)

inline

Changes the Karimäki parameters (and consequently their covariance matrix) under a translation of the coordinate system, such that the old origin has coordinates (x0,y0) in the new coordinate system. The formulas are taken from Karimäki V., 1990, Effective circle fitting for particle trajectories, Nucl. Instr. and Meth. A305 (1991) 187.

Parameters

circle	circle fit in the old coordinate system. circle.par(0) is phi, circle.par(1) is d and circle.par(2) is rho.
x0	x coordinate of the translation vector.
y0	y coordinate of the translation vector.
jacobian	passed by reference in order to save stack.

Definition at line 98 of file BrokenLine.h.

References funct::cos(), l1tSlwPFPuppiJets_cfi::cosPhi, riemannFit::CircleFit::cov, amptDefaultParameters_cff::mu, riemannFit::CircleFit::par, funct::sin(), l1tSlwPFPuppiJets_cfi::sinPhi, riemannFit::sqr(), mathSSE::sqrt(), and protons_cff::xi.

Referenced by circleFit().

                                                                                   {
     // Avoid multiple access to the circle.par vector.
     using scalar = std::remove_reference<decltype(circle.par(0))>::type;
     scalar phi = circle.par(0);
     scalar dee = circle.par(1);
     scalar rho = circle.par(2);
 
     // Avoid repeated trig. computations
     scalar sinPhi = sin(phi);
     scalar cosPhi = cos(phi);
 
     // Intermediate computations for the circle parameters
     scalar deltaPara = x0 * cosPhi + y0 * sinPhi;
     scalar deltaOrth = x0 * sinPhi - y0 * cosPhi + dee;
     scalar tempSmallU = 1 + rho * dee;
     scalar tempC = -rho * y0 + tempSmallU * cosPhi;
     scalar tempB = rho * x0 + tempSmallU * sinPhi;
     scalar tempA = 2. * deltaOrth + rho * (riemannFit::sqr(deltaOrth) + riemannFit::sqr(deltaPara));
     scalar tempU = sqrt(1. + rho * tempA);
 
     // Intermediate computations for the error matrix transform
     scalar xi = 1. / (riemannFit::sqr(tempB) + riemannFit::sqr(tempC));
     scalar tempV = 1. + rho * deltaOrth;
     scalar lambda = (0.5 * tempA) / (riemannFit::sqr(1. + tempU) * tempU);
     scalar mu = 1. / (tempU * (1. + tempU)) + rho * lambda;
     scalar zeta = riemannFit::sqr(deltaOrth) + riemannFit::sqr(deltaPara);
     jacobian << xi * tempSmallU * tempV, -xi * riemannFit::sqr(rho) * deltaOrth, xi * deltaPara,
         2. * mu * tempSmallU * deltaPara, 2. * mu * tempV, mu * zeta - lambda * tempA, 0, 0, 1.;
 
     // translated circle parameters
     // phi
     circle.par(0) = atan2(tempB, tempC);
     // d
     circle.par(1) = tempA / (1 + tempU);
     // rho after translation. It is invariant, so noop
     // circle.par(2)= rho;
 
     // translated error matrix
     circle.cov = jacobian * circle.cov * jacobian.transpose();
   }

Classes

Typedefs

Functions

Typedef Documentation

◆ karimaki_circle_fit

Function Documentation

◆ circleFit()

◆ fastFit()

◆ helixFit()

◆ lineFit()

◆ matrixC_u()

◆ multScatt()

◆ prepareBrokenLineData()

◆ rotationMatrix()

◆ translateKarimaki()