PartBunch.cpp

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//
// Class PartBunch
//   Particle Bunch.
//   A representation of a particle bunch as a vector of particles.
//
// Copyright (c) 2008 - 2020, Paul Scherrer Institut, Villigen PSI, Switzerland
// All rights reserved
//
// This file is part of OPAL.
//
// OPAL is free software: you can redistribute it and/or modify
// it under the terms of the GNU General Public License as published by
// the Free Software Foundation, either version 3 of the License, or
// (at your option) any later version.
//
// You should have received a copy of the GNU General Public License
// along with OPAL. If not, see <https://www.gnu.org/licenses/>.
//
#include "Algorithms/PartBunch.h"
 
#include <cfloat>
#include <memory>
#include <utility>
 
#include "FixedAlgebra/FMatrix.h"
#include "FixedAlgebra/FVector.h"
#include "Particle/ParticleBalancer.h"
 
#include "Algorithms/ListElem.h"
#include "Distribution/Distribution.h"
#include "Structure/FieldSolver.h"
#include "Utilities/GeneralClassicException.h"
 
#ifdef DBG_SCALARFIELD
    #include "Structure/FieldWriter.h"
#endif
 
//#define FIELDSTDOUT
 
PartBunch::PartBunch(const PartData *ref): // Layout is set using setSolver()
    PartBunchBase<double, 3>(new PartBunch::pbase_t(new Layout_t()), ref),
    interpolationCacheSet_m(false)
{
 
}
 
 
PartBunch::~PartBunch() {
 
}
 
// PartBunch::pbase_t* PartBunch::clone() {
//     return new pbase_t(new Layout_t());
// }
 
 
void PartBunch::initialize(FieldLayout_t *fLayout) {
    Layout_t* layout = static_cast<Layout_t*>(&getLayout());
    layout->getLayout().changeDomain(*fLayout);
}
 
 
void PartBunch::do_binaryRepart() {
    get_bounds(rmin_m, rmax_m);
 
    pbase_t* underlyingPbase =
        dynamic_cast<pbase_t*>(pbase_m.get());
 
    BinaryRepartition(*underlyingPbase);
    update();
    get_bounds(rmin_m, rmax_m);
    boundp();
}
 
 
void PartBunch::computeSelfFields(int binNumber) {
    IpplTimings::startTimer(selfFieldTimer_m);
 
    if (fs_m->getFieldSolverType() == FieldSolverType::P3M) {
        throw GeneralClassicException("PartBunch::computeSelfFields(int binNumber)", 
                            "P3M solver not available during emission");
    }
 
    rho_m = 0.0;
    Field_t imagePotential = rho_m;
 
    eg_m = Vector_t(0.0);
 
    if(fs_m->hasValidSolver()) {
        resizeMesh();
 
        this->Q *= this->dt;
        if(!interpolationCacheSet_m) {
            if(interpolationCache_m.size() < getLocalNum()) {
                interpolationCache_m.create(getLocalNum() - interpolationCache_m.size());
            } else {
                interpolationCache_m.destroy(interpolationCache_m.size() - getLocalNum(),
                                             getLocalNum(),
                                             true);
            }
            interpolationCacheSet_m = true;
            this->Q.scatter(this->rho_m, this->R, IntrplCIC_t(), interpolationCache_m);
        } else {
            this->Q.scatter(this->rho_m, IntrplCIC_t(), interpolationCache_m);
        }
 
        this->Q /= this->dt;
        this->rho_m /= getdT();
 
        double scaleFactor = 1;
        // double scaleFactor = Physics::c * getdT();
        double gammaz = getBinGamma(binNumber);
 
        double tmp2 = 1 / hr_m[0] * 1 / hr_m[1] * 1 / hr_m[2] / (scaleFactor * scaleFactor * scaleFactor) / gammaz;
        rho_m *= tmp2;
 
        Vector_t hr_scaled = hr_m * Vector_t(scaleFactor);
        hr_scaled[2] *= gammaz;
 
        imagePotential = rho_m;
 
        fs_m->solver_m->computePotential(rho_m, hr_scaled);
 
        rho_m *= hr_scaled[0] * hr_scaled[1] * hr_scaled[2];
 
        rho_m *= getCouplingConstant();
 
        eg_m = -Grad(rho_m, eg_m);
 
        eg_m *= Vector_t(gammaz / (scaleFactor), gammaz / (scaleFactor), 1.0 / (scaleFactor * gammaz));
 
        // If desired write E-field and potential to terminal
#ifdef FIELDSTDOUT
        // Immediate debug output:
        // Output potential and e-field along the x-, y-, and z-axes
        int mx = (int)nr_m[0];
        int mx2 = (int)nr_m[0] / 2;
        int my = (int)nr_m[1];
        int my2 = (int)nr_m[1] / 2;
        int mz = (int)nr_m[2];
        int mz2 = (int)nr_m[2] / 2;
 
        for (int i=0; i<mx; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Self Field along x axis E = " << eg_m[i][my2][mz2]
                  << ", Pot = " << rho_m[i][my2][mz2]  << endl;
 
        for (int i=0; i<my; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Self Field along y axis E = " << eg_m[mx2][i][mz2]
                  << ", Pot = " << rho_m[mx2][i][mz2]  << endl;
 
        for (int i=0; i<mz; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Self Field along z axis E = " << eg_m[mx2][my2][i]
                  << ", Pot = " << rho_m[mx2][my2][i]  << endl;
#endif
 
        Eftmp.gather(eg_m, IntrplCIC_t(), interpolationCache_m);
        //Eftmp.gather(eg_m, this->R, IntrplCIC_t());
 
        double betaC = std::sqrt(gammaz * gammaz - 1.0) / gammaz / Physics::c;
 
        Bf(0) = Bf(0) - betaC * Eftmp(1);
        Bf(1) = Bf(1) + betaC * Eftmp(0);
 
        Ef += Eftmp;
 
 
        NDIndex<3> domain = getFieldLayout().getDomain();
        Vector_t origin = rho_m.get_mesh().get_origin();
        double hz = rho_m.get_mesh().get_meshSpacing(2);
        double zshift = -(2 * origin(2) + (domain[2].first() + domain[2].last() + 1) * hz) * gammaz * scaleFactor;
 
        fs_m->solver_m->computePotential(imagePotential, hr_scaled, zshift);
 
        imagePotential *= hr_scaled[0] * hr_scaled[1] * hr_scaled[2];
 
        imagePotential *= getCouplingConstant();
 
#ifdef DBG_SCALARFIELD
        const int dumpFreq = 100;
        VField_t tmp_eg = eg_m;
 
        if ((localTrackStep_m + 1) % dumpFreq == 0) {
            FieldWriter fwriter;
            fwriter.dumpField(rho_m, "phi", "V", localTrackStep_m / dumpFreq, &imagePotential);
        }
#endif
 
        eg_m = -Grad(imagePotential, eg_m);
 
        eg_m *= Vector_t(gammaz / (scaleFactor), gammaz / (scaleFactor), 1.0 / (scaleFactor * gammaz));
 
        // If desired write E-field and potential to terminal
#ifdef FIELDSTDOUT
        // Immediate debug output:
        // Output potential and e-field along the x-, y-, and z-axes
        //int mx = (int)nr_m[0];
        //int mx2 = (int)nr_m[0] / 2;
        //int my = (int)nr_m[1];
        //int my2 = (int)nr_m[1] / 2;
        //int mz = (int)nr_m[2];
        //int mz2 = (int)nr_m[2] / 2;
 
        for (int i=0; i<mx; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Image Field along x axis E = " << eg_m[i][my2][mz2]
                  << ", Pot = " << rho_m[i][my2][mz2]  << endl;
 
        for (int i=0; i<my; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Image Field along y axis E = " << eg_m[mx2][i][mz2]
                  << ", Pot = " << rho_m[mx2][i][mz2]  << endl;
 
        for (int i=0; i<mz; i++ )
            *gmsg << "Bin " << binNumber
                  << ", Image Field along z axis E = " << eg_m[mx2][my2][i]
                  << ", Pot = " << rho_m[mx2][my2][i]  << endl;
#endif
 
#ifdef DBG_SCALARFIELD
        tmp_eg += eg_m;
        if ((localTrackStep_m + 1) % dumpFreq == 0) {
            FieldWriter fwriter;
            fwriter.dumpField(tmp_eg, "e", "V/m", localTrackStep_m / dumpFreq);
        }
#endif
 
        Eftmp.gather(eg_m, IntrplCIC_t(), interpolationCache_m);
        //Eftmp.gather(eg_m, this->R, IntrplCIC_t());
 
        Bf(0) = Bf(0) + betaC * Eftmp(1);
        Bf(1) = Bf(1) - betaC * Eftmp(0);
 
        Ef += Eftmp;
 
    }
    IpplTimings::stopTimer(selfFieldTimer_m);
}
 
void PartBunch::resizeMesh() {
    if (fs_m->getFieldSolverType() != FieldSolverType::SAAMG) {
        return;
    }
 
    double xmin = fs_m->solver_m->getXRangeMin();
    double xmax = fs_m->solver_m->getXRangeMax();
    double ymin = fs_m->solver_m->getYRangeMin();
    double ymax = fs_m->solver_m->getYRangeMax();
 
    if(xmin > rmin_m[0] || xmax < rmax_m[0] ||
       ymin > rmin_m[1] || ymax < rmax_m[1]) {
 
        for (unsigned int n = 0; n < getLocalNum(); n++) {
 
            if(R[n](0) < xmin || R[n](0) > xmax ||
               R[n](1) < ymin || R[n](1) > ymax) {
 
                // delete the particle
                INFOMSG(level2 << "destroyed particle with id=" << ID[n] << endl);
                destroy(1, n);
            }
 
        }
 
        update();
        boundp();
        get_bounds(rmin_m, rmax_m);
    }
 
    Vector_t origin = Vector_t(0.0, 0.0, 0.0);
 
    // update the mesh origin and mesh spacing hr_m
    fs_m->solver_m->resizeMesh(origin, hr_m, rmin_m, rmax_m, dh_m);
 
    getMesh().set_meshSpacing(&(hr_m[0]));
    getMesh().set_origin(origin);
 
    rho_m.initialize(getMesh(),
                     getFieldLayout(),
                     GuardCellSizes<Dimension>(1),
                     bc_m);
    eg_m.initialize(getMesh(),
                    getFieldLayout(),
                    GuardCellSizes<Dimension>(1),
                    vbc_m);
 
    update();
 
//    setGridIsFixed();
}
 
void PartBunch::computeSelfFields() {
    IpplTimings::startTimer(selfFieldTimer_m);
    rho_m = 0.0;
    eg_m = Vector_t(0.0);
 
    if(fs_m->hasValidSolver()) {
        //mesh the whole domain
        resizeMesh();
 
        //scatter charges onto grid
        this->Q *= this->dt;
        this->Q.scatter(this->rho_m, this->R, IntrplCIC_t());
        this->Q /= this->dt;
        this->rho_m /= getdT();
 
        //calculating mesh-scale factor
        double gammaz = sum(this->P)[2] / getTotalNum();
        gammaz *= gammaz;
        gammaz = std::sqrt(gammaz + 1.0);
        double scaleFactor = 1;
        // double scaleFactor = Physics::c * getdT();
        //and get meshspacings in real units [m]
        Vector_t hr_scaled = hr_m * Vector_t(scaleFactor);
        hr_scaled[2] *= gammaz;
 
        //double tmp2 = 1/hr_m[0] * 1/hr_m[1] * 1/hr_m[2] / (scaleFactor*scaleFactor*scaleFactor) / gammaz;
        double tmp2 = 1 / hr_scaled[0] * 1 / hr_scaled[1] * 1 / hr_scaled[2];
        //divide charge by a 'grid-cube' volume to get [C/m^3]
        rho_m *= tmp2;
 
        double Npoints = nr_m[0] * nr_m[1] * nr_m[2];
        rmsDensity_m = std::sqrt((1.0 /Npoints) * sum((rho_m / Physics::q_e) * (rho_m / Physics::q_e)));
 
        calcDebyeLength(); 
 
 
#ifdef DBG_SCALARFIELD
        FieldWriter fwriter;
        fwriter.dumpField(rho_m, "rho", "C/m^3", localTrackStep_m);
#endif
 
        // charge density is in rho_m
        fs_m->solver_m->computePotential(rho_m, hr_scaled);
 
        //do the multiplication of the grid-cube volume coming
        //from the discretization of the convolution integral.
        //this is only necessary for the FFT solver
        //FIXME: later move this scaling into FFTPoissonSolver
        if (fs_m->getFieldSolverType() == FieldSolverType::FFT ||
            fs_m->getFieldSolverType() == FieldSolverType::FFTBOX) {
            rho_m *= hr_scaled[0] * hr_scaled[1] * hr_scaled[2];
        }
 
        // the scalar potential is given back in rho_m in units
        // [C/m] = [F*V/m] and must be divided by
        // 4*pi*\epsilon_0 [F/m] resulting in [V]
        rho_m *= getCouplingConstant();
 
        //write out rho
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(rho_m, "phi", "V", localTrackStep_m);
#endif
 
        // IPPL Grad divides by hr_m [m] resulting in
        // [V/m] for the electric field
        eg_m = -Grad(rho_m, eg_m);
 
        //write out e field
#ifdef FIELDSTDOUT
        // Immediate debug output:
        // Output potential and e-field along the x-, y-, and z-axes
        int mx = (int)nr_m[0];
        int mx2 = (int)nr_m[0] / 2;
        int my = (int)nr_m[1];
        int my2 = (int)nr_m[1] / 2;
        int mz = (int)nr_m[2];
        int mz2 = (int)nr_m[2] / 2;
 
        for (int i=0; i<mx; i++ )
            *gmsg << "Field along x axis Ex = " << eg_m[i][my2][mz2] << " Pot = " << rho_m[i][my2][mz2]  << endl;
 
        for (int i=0; i<my; i++ )
            *gmsg << "Field along y axis Ey = " << eg_m[mx2][i][mz2] << " Pot = " << rho_m[mx2][i][mz2]  << endl;
 
        for (int i=0; i<mz; i++ )
            *gmsg << "Field along z axis Ez = " << eg_m[mx2][my2][i] << " Pot = " << rho_m[mx2][my2][i]  << endl;
#endif
 
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(eg_m, "e", "V/m", localTrackStep_m);
#endif
 
        // interpolate electric field at particle positions.  We reuse the
        // cached information about where the particles are relative to the
        // field, since the particles have not moved since this the most recent
        // scatter operation.
        Ef.gather(eg_m, this->R,  IntrplCIC_t());
 
        if(fs_m->getFieldSolverType() == FieldSolverType::P3M) {
            fs_m->solver_m->calculatePairForces(this,gammaz);
        }
 
        Ef = Ef * Vector_t(gammaz / (scaleFactor), gammaz / (scaleFactor), 1.0 / (scaleFactor * gammaz));
        
        double betaC = std::sqrt(gammaz * gammaz - 1.0) / gammaz / Physics::c;
 
        Bf(0) = Bf(0) - betaC * Ef(1);
        Bf(1) = Bf(1) + betaC * Ef(0);
    }
    IpplTimings::stopTimer(selfFieldTimer_m);
}
 
void PartBunch::computeSelfFields_cycl(double gamma) {
 
    IpplTimings::startTimer(selfFieldTimer_m);
 
    if (fs_m->getFieldSolverType() == FieldSolverType::P3M) {
        throw GeneralClassicException("PartBunch::computeSelfFields_cycl(double gamma)", 
                            "P3M solver not available yet for cyclotrons");
    }
 
    rho_m = 0.0;
 
    eg_m = Vector_t(0.0);
 
    if(fs_m->hasValidSolver()) {
        resizeMesh();
 
        this->Q.scatter(this->rho_m, this->R, IntrplCIC_t());
 
        Vector_t hr_scaled = hr_m ;
        hr_scaled[1] *= gamma;
 
        double tmp2 = 1.0 / (hr_scaled[0] * hr_scaled[1] * hr_scaled[2]);
        rho_m *= tmp2;
 
        double Npoints = nr_m[0] * nr_m[1] * nr_m[2];
        rmsDensity_m = std::sqrt((1.0 /Npoints) * sum((rho_m / Physics::q_e) * (rho_m / Physics::q_e)));
 
        calcDebyeLength(); 
 
        // If debug flag is set, dump scalar field (charge density 'rho') into file under ./data/
#ifdef DBG_SCALARFIELD
        FieldWriter fwriter;
        fwriter.dumpField(rho_m, "rho", "C/m^3", localTrackStep_m);
#endif
 
        fs_m->solver_m->computePotential(rho_m, hr_scaled);
 
        //do the multiplication of the grid-cube volume coming
        //from the discretization of the convolution integral.
        //this is only necessary for the FFT solver
        //TODO FIXME: later move this scaling into FFTPoissonSolver
        if (fs_m->getFieldSolverType() == FieldSolverType::FFT ||
            fs_m->getFieldSolverType() == FieldSolverType::FFTBOX) {
            rho_m *= hr_scaled[0] * hr_scaled[1] * hr_scaled[2];
        }
 
        rho_m *= getCouplingConstant();
 
        // If debug flag is set, dump scalar field (potential 'phi') into file under ./data/
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(rho_m, "phi", "V", localTrackStep_m);
#endif
 
        eg_m = -Grad(rho_m, eg_m);
 
        eg_m *= Vector_t(gamma, 1.0 / gamma, gamma);
 
#ifdef FIELDSTDOUT
        // Immediate debug output:
        // Output potential and e-field along the x-, y-, and z-axes
        int mx = (int)nr_m[0];
        int mx2 = (int)nr_m[0] / 2;
        int my = (int)nr_m[1];
        int my2 = (int)nr_m[1] / 2;
        int mz = (int)nr_m[2];
        int mz2 = (int)nr_m[2] / 2;
 
        for (int i=0; i<mx; i++ )
            *gmsg << "Field along x axis Ex = " << eg_m[i][my2][mz2] << " Pot = " << rho_m[i][my2][mz2]  << endl;
 
        for (int i=0; i<my; i++ )
            *gmsg << "Field along y axis Ey = " << eg_m[mx2][i][mz2] << " Pot = " << rho_m[mx2][i][mz2]  << endl;
 
        for (int i=0; i<mz; i++ )
            *gmsg << "Field along z axis Ez = " << eg_m[mx2][my2][i] << " Pot = " << rho_m[mx2][my2][i]  << endl;
#endif
 
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(eg_m, "e", "V/m", localTrackStep_m);
#endif
 
        Ef.gather(eg_m, this->R,  IntrplCIC_t());
 
 
        
        // Relativistic E&M says gamma*v/c^2 = gamma*beta/c = sqrt(gamma*gamma-1)/c
        // but because we already transformed E_trans into the moving frame we have to
        // add 1/gamma so we are using the E_trans from the rest frame -DW
        double betaC = std::sqrt(gamma * gamma - 1.0) / gamma / Physics::c;
 
        Bf(0) =  betaC * Ef(2);
        Bf(2) = -betaC * Ef(0);
 
    }
 
    /*
    *gmsg << "gamma =" << gamma << endl;
    *gmsg << "dx,dy,dz =(" << hr_m[0] << ", " << hr_m[1] << ", " << hr_m[2] << ") [m] " << endl;
    *gmsg << "max of bunch is (" << rmax_m(0) << ", " << rmax_m(1) << ", " << rmax_m(2) << ") [m] " << endl;
    *gmsg << "min of bunch is (" << rmin_m(0) << ", " << rmin_m(1) << ", " << rmin_m(2) << ") [m] " << endl;
    */
 
    IpplTimings::stopTimer(selfFieldTimer_m);
}
 
void PartBunch::computeSelfFields_cycl(int bin) {
    IpplTimings::startTimer(selfFieldTimer_m);
 
    if (fs_m->getFieldSolverType() == FieldSolverType::P3M) {
        throw GeneralClassicException("PartBunch::computeSelfFields_cycl(int bin)", 
                            "P3M solver not available yet for cyclotrons");
    }
 
    rho_m = 0.0;
 
    eg_m = Vector_t(0.0);
 
    double gamma = getBinGamma(bin);
 
    if(fs_m->hasValidSolver()) {
        resizeMesh();
 
        this->Q.scatter(this->rho_m, this->R, IntrplCIC_t());
 
        Vector_t hr_scaled = hr_m ;
        hr_scaled[1] *= gamma;
 
        double tmp2 = 1.0 / (hr_scaled[0] * hr_scaled[1] * hr_scaled[2]);
        rho_m *= tmp2;
 
        // If debug flag is set, dump scalar field (charge density 'rho') into file under ./data/
#ifdef DBG_SCALARFIELD
        FieldWriter fwriter;
        fwriter.dumpField(rho_m, "rho", "C/m^3", localTrackStep_m);
#endif
 
        fs_m->solver_m->computePotential(rho_m, hr_scaled);
 
        // Do the multiplication of the grid-cube volume coming from the discretization of the convolution integral.
        // This is only necessary for the FFT solver. FIXME: later move this scaling into FFTPoissonSolver
        if (fs_m->getFieldSolverType() == FieldSolverType::FFT ||
            fs_m->getFieldSolverType() == FieldSolverType::FFTBOX) {
            rho_m *= hr_scaled[0] * hr_scaled[1] * hr_scaled[2];
        }
 
        rho_m *= getCouplingConstant();
 
        // If debug flag is set, dump scalar field (potential 'phi') into file under ./data/
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(rho_m, "phi", "V", localTrackStep_m);
#endif
 
        eg_m = -Grad(rho_m, eg_m);
 
        eg_m *= Vector_t(gamma, 1.0 / gamma, gamma);
 
#ifdef FIELDSTDOUT
        // Immediate debug output:
        // Output potential and e-field along the x-, y-, and z-axes
        int mx = (int)nr_m[0];
        int mx2 = (int)nr_m[0] / 2;
        int my = (int)nr_m[1];
        int my2 = (int)nr_m[1] / 2;
        int mz = (int)nr_m[2];
        int mz2 = (int)nr_m[2] / 2;
 
        for (int i=0; i<mx; i++ )
            *gmsg << "Bin " << bin
                  << ", Field along x axis Ex = " << eg_m[i][my2][mz2]
                  << ", Pot = " << rho_m[i][my2][mz2]  << endl;
 
        for (int i=0; i<my; i++ )
            *gmsg << "Bin " << bin
                  << ", Field along y axis Ey = " << eg_m[mx2][i][mz2]
                  << ", Pot = " << rho_m[mx2][i][mz2]  << endl;
 
        for (int i=0; i<mz; i++ )
            *gmsg << "Bin " << bin
                  << ", Field along z axis Ez = " << eg_m[mx2][my2][i]
                  << ", Pot = " << rho_m[mx2][my2][i]  << endl;
#endif
 
        // If debug flag is set, dump vector field (electric field) into file under ./data/
#ifdef DBG_SCALARFIELD
        fwriter.dumpField(eg_m, "e", "V/m", localTrackStep_m);
#endif
 
        Eftmp.gather(eg_m, this->R,  IntrplCIC_t());
 
        
        
        double betaC = std::sqrt(gamma * gamma - 1.0) / gamma / Physics::c;
 
        Bf(0) = Bf(0) + betaC * Eftmp(2);
        Bf(2) = Bf(2) - betaC * Eftmp(0);
 
        Ef += Eftmp;
    }
 
    /*
    *gmsg << "gamma =" << gamma << endl;
    *gmsg << "dx,dy,dz =(" << hr_m[0] << ", " << hr_m[1] << ", " << hr_m[2] << ") [m] " << endl;
    *gmsg << "max of bunch is (" << rmax_m(0) << ", " << rmax_m(1) << ", " << rmax_m(2) << ") [m] " << endl;
    *gmsg << "min of bunch is (" << rmin_m(0) << ", " << rmin_m(1) << ", " << rmin_m(2) << ") [m] " << endl;
    */
 
 
    IpplTimings::stopTimer(selfFieldTimer_m);
}
 
 
// void PartBunch::setMesh(Mesh_t* mesh) {
//     Layout_t* layout = static_cast<Layout_t*>(&getLayout());
// //     layout->getLayout().setMesh(mesh);
// }
 
 
// void PartBunch::setFieldLayout(FieldLayout_t* fLayout) {
//     Layout_t* layout = static_cast<Layout_t*>(&getLayout());
// //     layout->getLayout().setFieldLayout(fLayout);
// //     layout->rebuild_neighbor_data();
//     layout->getLayout().changeDomain(*fLayout);
// }
 
 
FieldLayout_t &PartBunch::getFieldLayout() {
    Layout_t* layout = static_cast<Layout_t*>(&getLayout());
    return dynamic_cast<FieldLayout_t &>(layout->getLayout().getFieldLayout());
}
 
void PartBunch::setBCAllPeriodic() {
    for (int i = 0; i < 2 * 3; ++i) {
 
        if (Ippl::getNodes()>1) {
            bc_m[i] = new ParallelInterpolationFace<double, Dimension, Mesh_t, Center_t>(i);
            //std periodic boundary conditions for gradient computations etc.
            vbc_m[i] = new ParallelPeriodicFace<Vector_t, Dimension, Mesh_t, Center_t>(i);
        }
        else {
            bc_m[i] = new InterpolationFace<double, Dimension, Mesh_t, Center_t>(i);
            //std periodic boundary conditions for gradient computations etc.
            vbc_m[i] = new PeriodicFace<Vector_t, Dimension, Mesh_t, Center_t>(i);
        }
        getBConds()[i] =  ParticlePeriodicBCond;
    }
    dcBeam_m=true;
    INFOMSG(level3 << "BC set all periodic" << endl);
}
 
void PartBunch::setBCAllOpen() {
    for (int i = 0; i < 2 * 3; ++i) {
        bc_m[i] = new ZeroFace<double, 3, Mesh_t, Center_t>(i);
        vbc_m[i] = new ZeroFace<Vector_t, 3, Mesh_t, Center_t>(i);
        getBConds()[i] = ParticleNoBCond;
    }
    dcBeam_m=false;
    INFOMSG(level3 << "BC set for normal Beam" << endl);
}
 
void PartBunch::setBCForDCBeam() {
    for (int i = 0; i < 2 * 3; ++ i) {
        if (i >= 4) {
            if (Ippl::getNodes() > 1) {
                bc_m[i] = new ParallelPeriodicFace<double, 3, Mesh_t, Center_t>(i);
                vbc_m[i] = new ParallelPeriodicFace<Vector_t, 3, Mesh_t, Center_t>(i);
            } else {
                bc_m[i] = new PeriodicFace<double, 3, Mesh_t, Center_t>(i);
                vbc_m[i] = new PeriodicFace<Vector_t, 3, Mesh_t, Center_t>(i);
            }
 
            getBConds()[i] = ParticlePeriodicBCond;
        } else {
            bc_m[i] = new ZeroFace<double, 3, Mesh_t, Center_t>(i);
            vbc_m[i] = new ZeroFace<Vector_t, 3, Mesh_t, Center_t>(i);
            getBConds()[i] = ParticleNoBCond;
        }
    }
    dcBeam_m=true;
    INFOMSG(level3 << "BC set for DC-Beam, longitudinal periodic" << endl);
}
 
 
void PartBunch::updateDomainLength(Vektor<int, 3>& grid) {
    NDIndex<3> domain = getFieldLayout().getDomain();
    for (unsigned int i = 0; i < Dimension; i++)
        grid[i] = domain[i].length();
}
 
 
void PartBunch::updateFields(const Vector_t& /*hr*/, const Vector_t& origin) {
    getMesh().set_meshSpacing(&(hr_m[0]));
    getMesh().set_origin(origin);
    rho_m.initialize(getMesh(),
                     getFieldLayout(),
                     GuardCellSizes<Dimension>(1),
                     bc_m);
    eg_m.initialize(getMesh(),
                    getFieldLayout(),
                    GuardCellSizes<Dimension>(1),
                    vbc_m);
}
 
inline
PartBunch::VectorPair_t PartBunch::getEExtrema() {
    const Vector_t maxE = max(eg_m);
    //      const double maxL = max(dot(eg_m,eg_m));
    const Vector_t minE = min(eg_m);
    // INFOMSG("MaxE= " << maxE << " MinE= " << minE << endl);
    return VectorPair_t(maxE, minE);
}
 
 
inline
void PartBunch::resetInterpolationCache(bool clearCache) {
    interpolationCacheSet_m = false;
    if(clearCache) {
        interpolationCache_m.destroy(interpolationCache_m.size(), 0, true);
    }
}
 
void PartBunch::swap(unsigned int i, unsigned int j) {
 
    // FIXME
    PartBunchBase<double, 3>::swap(i, j);
 
    if (interpolationCacheSet_m)
        std::swap(interpolationCache_m[i], interpolationCache_m[j]);
}
 
 
Inform &PartBunch::print(Inform &os) {
    return PartBunchBase<double, 3>::print(os);
}