test_gnumi.C
Go to the documentation of this file.
1 #include "TMath.h"
2 #include "TSystem.h"
3 #include <string>
4 #include <fstream>
5 #include <iostream>
6 #include <iomanip>
7 using namespace std;
8 
9 #include "TStyle.h"
10 #include "TCanvas.h"
11 #include "TH1D.h"
12 #include "TLorentzVector.h"
13 
14 #include "FluxDrivers/GNuMIFlux.h"
15 #include "PDG/PDGCodeList.h"
16 #include "PDG/PDGUtils.h"
17 
18 using namespace genie::flux;
19 
20 #include "FluxDrivers/GNuMIFlux.h"
21 #include "PDG/PDGCodeList.h"
22 #include "PDG/PDGUtils.h"
23 
24 // typedefs and forward declarations
26 
27 double fabserrX(double a, double b)
28 { return TMath::Abs(a-b)/TMath::Max(TMath::Abs(b),1.0e-30); }
29 
30 //////////////////////////////////////////////////////////////////////////////
31 
32 int calc_enuwgt(const fluxentry_t& fluxentry,
33  double x, double y, double z,
34  double& enu, double& wgt_xy, xypartials& partials);
35 
36 //////////////////////////////////////////////////////////////////////////////
37 
38 void test_gnumi(int mxpull = 0)
39 {
40  // mxpull: max number of entries to process 0=all, -N=until N mismatches
41 
42  // currently TFile not TChain, so better resolve to a single file
43  string fluxpatt = "";
44  fluxpatt = "$FLUXPATH/v19/fluka05_le010z185i/root/fluka05_le010z185i_1.root";
45  //fluxpatt = "$FLUXPATH/g4numi/g4fluka_le010z185i_leak_v10_0001.root";
46  //fluxpatt = "$GENIE/src/FluxDrivers/gnumi_test/*g3*.root";
47  //fluxpatt = "*g3*.root";
48  string fluxfilename(gSystem->ExpandPathName(fluxpatt.c_str()));
49 
51  gnumi->LoadBeamSimData(fluxfilename);
52  gnumi->SetGenWeighted(true); // generated entries w/ fWeight != 1.0
53 
54  const genie::PDGCodeList& pdgList = gnumi->FluxParticles();
55  int nfluxtypes = pdgList.size();
56  cout << "GNuMIFlux supplies " << nfluxtypes << " PDG particles of type: ";
57  // don't try iterators .. apparently they aren't usable in CINT
58  for (int indx=0; indx < nfluxtypes ; ++indx)
59  cout << pdgList[indx] << " ";
60  cout << endl;
61 
62  cout << "MaxEnergy " << gnumi->MaxEnergy() << endl;
63 
64  cout << "scan for max weight at NearDet" << endl;
65  //gnumi->UseFluxAtNearDetCenter();
66  gnumi->SetLengthUnits(genie::flux::GNuMIFlux::kcm);
67  gnumi->SetBeamFluxWindow(genie::flux::GNuMIFlux::kMinosNearCenter);
68  gnumi->ScanForMaxWeight();
69 
70  int npull, nxy, file_debug;
71  double xbeam, ybeam, zbeam = 103935.; // distance in cm to near "window"
72 
73  ifstream xypoints("XYPOINTS.TXT");
74 
75  xypoints >> npull >> nxy >> zbeam >> file_debug;
76 
77  TH1D* hist_ferr_enu = new TH1D("ferr_enu","ferr_enu",1000,0.0,0.000005);
78  TH1D* hist_ferr_wgt = new TH1D("ferr_wgt","ferr_wgt",1000,0.0,0.01);
79  hist_ferr_enu->Sumw2();
80  hist_ferr_wgt->Sumw2();
81  TH1D* hist_ferr_enu0 = new TH1D("ferr_enu0","ferr_enu0",1000,0.0,0.000005);
82  TH1D* hist_ferr_wgt0 = new TH1D("ferr_wgt0","ferr_wgt0",1000,0.0,0.01);
83  hist_ferr_enu0->Sumw2();
84  hist_ferr_wgt0->Sumw2();
85  gStyle->SetOptStat(111111);
86 
87  if ( mxpull > 0 && npull > mxpull ) npull = mxpull;
88 
89  for ( int ipull = 1; ipull <= npull ; ++ipull ) {
90 
91  bool genok = gnumi->GenerateNext();
92  const fluxentry_t& fluxentry = gnumi->PassThroughInfo();
93 
94  double wgtprd_gen = gnumi->Weight();
95  double enu_gen = gnumi->Momentum().E();
96  if ( wgtprd_gen != 1.0 ) {
97  // weighted flux ... we can validate "center" values
98  // assume used kMinosNearCenter in SetBeamFluxWindow
99  double wgtprd_ntuple = fluxentry.nimpwt * fluxentry.nwtnear;
100  double enu_ntuple = fluxentry.nenergyn;
101  double ferr_enu0 = fabserrX(enu_gen,enu_ntuple);
102  double ferr_wgtprd0 = fabserrX(wgtprd_gen,wgtprd_ntuple);
103  const double eps0h = 1.0e-6; // 2.5e-5;
104  if ( ferr_enu0 > eps0h || ferr_wgtprd0 > eps0h ) {
105  hist_ferr_enu0->Fill(ferr_enu0,1.0);
106  hist_ferr_wgt0->Fill(ferr_wgtprd0,1.0);
107  }
108  const double eps0 = 2.5e-5; // 2.5e-5;
109  if ( ferr_enu0 > eps0 || ferr_wgtprd0 > eps0 ) {
110  char xenu0 = ( ferr_enu0 > eps0 ) ? '#' : ' ';
111  char xwgt0 = ( ferr_wgtprd0 > eps0 ) ? '#' : ' ';
112  cout << "Checking \"center\" energy/weight "
113  << " enu " << setw(8) << enu_gen << " " << setw(8) << enu_ntuple
114  << " err " << setw(11) << ferr_enu0 << xenu0
115  << " wgtprd " << setw(8) << wgtprd_gen << " " << setw(8) << wgtprd_ntuple
116  << " err " << setw(11) << ferr_wgtprd0 << xwgt0
117  << endl;
118  }
119 
120  }
121 
122 
123  //bool atend = gnumi->End();
124  //cout << "gnumi->GenerateNext() returned " << (genok?"true":"false")
125  // << " End() returns " << (atend?"true":"false")
126  // << endl;
127 
128  //cout << "Current entry: "
129  // << " PdgCode=" << gnumi->PdgCode()
130  // << " Weight=" << gnumi->Weight()
131  // << endl;
132  // gnumi->PrintCurrent();
133 
134  for ( int ixy = 0; ixy <= nxy ; ++ixy ) {
135  xypartials part_file, part_calc;
136  if ( file_debug ) part_file.ReadStream(xypoints);
137 
138  double enu, wgt_xy;
139  double enu_in, wgt_xy_in;
140  int ipull_in, ixy_in;
141  xypoints >> ipull_in >> ixy_in >> xbeam >> ybeam >> enu_in >> wgt_xy_in;
142  if ( ! xypoints.good() || ( ipull_in != ipull ) || ( ixy_in != ixy) ) {
143  cout << "HEY!!! XYPOINTS.TXT "
144  << " file status = " << (int)xypoints.good()
145  << " ipull " << ipull_in << " " << ipull
146  << " ixy " << ixy_in << " " << ixy
147  << endl;
148  return;
149  }
150  fluxentry.CalcEnuWgt(xbeam,ybeam,zbeam,enu,wgt_xy,part_calc);
151 
152  double ferr_enu = fabserrX(enu,enu_in);
153  double ferr_wgt_xy = fabserrX(wgt_xy,wgt_xy_in);
154  const double eps_enu = 2.5e-5; // 0.003; // 6.0e-4; // 2.5e-4; // 1.5e-5; // 1.0e-6;
155  const double eps_wgt = 2.5e-5; // 0.003; // 6.0e-4; // 2.5e-4; // 2.5e-5; //
156  if ( ferr_enu > eps_enu || ferr_wgt_xy > eps_wgt ) {
157  cout << endl;
158  char xenu = ( ferr_enu > eps_enu ) ? '#':' ';
159  char xwgt = ( ferr_wgt_xy > eps_wgt ) ? '#':' ';
160  cout << "pull " << setw(6) << ipull << " ixy " << setw(2) << ixy
161  << " enu " << setw(8) << enu << " " << setw(8) << enu_in
162  << " err " << setw(11) << ferr_enu << xenu
163  << " wgt_xy " << setw(11) << wgt_xy << " " << setw(11) << wgt_xy_in
164  << " err " << setw(11) << ferr_wgt_xy << xwgt
165  << " ptype " << setw(4) << part_file.ptype
166  << " ntype " << setw(3) << part_file.ntype << endl;
167  hist_ferr_enu->Fill(ferr_enu,1.0);
168  hist_ferr_wgt->Fill(ferr_wgt_xy,1.0);
169  }
170  //else {
171  // cout << "pull " << ipull << " ixy " << ixy
172  // << " okay ptype " << part_file.ptype << " ntype " << part_file.ntype << endl;
173  //}
174 
175  if (file_debug) {
176  int np = part_file.Compare(part_calc);
177  if (np>0) {
178  std::cout << fluxentry << endl;
179  part_file.Print();
180  part_calc.Print();
181 
182  if ( mxpull < 0 ) {
183  cout << "COUNTDOWN mismatch error count @ " << mxpull << endl;
184  mxpull += 1;
185  if ( mxpull == 0 ) {
186  cout << "REACHED LIMIT ON MISMATCHES ... exit" << endl;
187  return; // reached limit on errors, asked to stop on error
188  }
189  }
190  }
191  }
192 
193 
194  //if ( part_calc.ptype == 13 || part_calc.ptype == -13 ) {
195  // cout << "STOPPING HERE FOR INSPECTION" << endl;
196  // return;
197  //}
198 
199  } //loop over xy points for given entryƧ
200  } // loop over entries (pulls)
201 
202  TCanvas* c1 = new TCanvas("c1","all positions");
203  c1->Divide(1,2);
204  c1->cd(1);
205  gPad->SetLogy(true);
206  hist_ferr_enu->Draw();
207  c1->cd(2);
208  gPad->SetLogy(true);
209  hist_ferr_wgt->Draw();
210 
211  TCanvas* c2 = new TCanvas("c2","center weight");
212  c2->Divide(1,2);
213  c2->cd(1);
214  gPad->SetLogy(true);
215  hist_ferr_enu0->Draw();
216  c2->cd(2);
217  gPad->SetLogy(true);
218  hist_ferr_wgt0->Draw();
219 
220 }
221 
222 //////////////////////////////////////////////////////////////////////////////
223 int calc_enuwgt(const fluxentry_t& fluxentry,
224  double xpos, double ypos, double zpos,
225  double& enu, double& wgt_xy, xypartials& partials)
226 {
227 
228  // Neutrino Energy and Weigth at arbitrary point
229  // based on:
230  // NuMI-NOTE-BEAM-0109 (MINOS DocDB # 109)
231  // Title: Neutrino Beam Simulation using PAW with Weighted Monte Carlos
232  // Author: Rick Milburn
233  // Date: 1995-10-01
234 
235  // history:
236  // jzh 3/21/96 grab R.H.Milburn's weighing routine
237  // jzh 5/ 9/96 substantially modify the weighting function use dot product
238  // instead of rotation vecs to get theta get all info except
239  // det from ADAMO banks neutrino parent is in Particle.inc
240  // Add weighting factor for polarized muon decay
241  // jzh 4/17/97 convert more code to double precision because of problems
242  // with Enu>30 GeV
243  // rwh 10/ 9/08 transliterate function from f77 to C++
244 
245  // original function description:
246  // Real function for use with PAW Ntuple To transform from destination
247  // detector geometry to the unit sphere moving with decaying hadron with
248  // velocity v, BETA=v/c, etc.. For (pseudo)scalar hadrons the decays will
249  // be isotropic in this sphere so the fractional area (out of 4-pi) is the
250  // fraction of decays that hit the target. For a given target point and
251  // area, and given x-y components of decay transverse location and slope,
252  // and given decay distance from target ans given decay GAMMA and
253  // rest-frame neutrino energy, the lab energy at the target and the
254  // fractional solid angle in the rest-frame are determined.
255  // For muon decays, correction for non-isotropic nature of decay is done.
256 
257  // Arguments:
258  // genie::flux::GNuMIFluxPassThroughInfo fluxentry :: ntuple entry info
259  // double x, y, z :: position to evaluate for (enu,wgt_xy)
260  // in *beam* frame coordinates (?units)
261  // double enu, wgt_xy :: resulting energy and weight
262  // Return:
263  // int :: error code
264  // Assumptions:
265  // Energies given in GeV
266  // Particle codes have been translated from GEANT into PDG codes
267 
268  // for now ... these _should_ come from DB
269  // but use these hard-coded values to "exactly" reproduces old code
270  const double kPIMASS = 0.13957;
271  const double kKMASS = 0.49368;
272  const double kK0MASS = 0.49767;
273  const double kMUMASS = 0.105658389;
274 
275  const int kpdg_nue = 12; // extended Geant 53
276  const int kpdg_nuebar = -12; // extended Geant 52
277  const int kpdg_numu = 14; // extended Geant 56
278  const int kpdg_numubar = -14; // extended Geant 55
279 
280  const int kpdg_muplus = -13; // Geant 5
281  const int kpdg_muminus = 13; // Geant 6
282  const int kpdg_pionplus = 211; // Geant 8
283  const int kpdg_pionminus = -211; // Geant 9
284  const int kpdg_k0long = 130; // Geant 10 ( K0=311, K0S=310 )
285  const int kpdg_k0short = 310; // Geant 16
286  const int kpdg_k0mix = 311;
287  const int kpdg_kaonplus = 321; // Geant 11
288  const int kpdg_kaonminus = -321; // Geant 12
289 
290  const double kRDET = 100.0; // set to flux per 100 cm radius
291 
292  enu = 0.0; // don't know what the final value is
293  wgt_xy = 0.0; // but set these in case we return early due to error
294 
295 
296  // in principle we should get these from the particle DB
297  // but for consistency testing use the hardcoded values
298  double parent_mass = kPIMASS;
299  switch ( fluxentry.ptype ) {
300  case kpdg_pionplus:
301  case kpdg_pionminus:
302  parent_mass = kPIMASS;
303  break;
304  case kpdg_kaonplus:
305  case kpdg_kaonminus:
306  parent_mass = kKMASS;
307  break;
308  case kpdg_k0long:
309  case kpdg_k0short:
310  case kpdg_k0mix:
311  parent_mass = kK0MASS;
312  break;
313  case kpdg_muplus:
314  case kpdg_muminus:
315  parent_mass = kMUMASS;
316  break;
317  default:
318  std::cerr << "NU_REWGT unknown particle type " << fluxentry.ptype
319  << std::endl;
320  return 1;
321  }
322 
323  double parentp2 = ( fluxentry.pdpx*fluxentry.pdpx +
324  fluxentry.pdpy*fluxentry.pdpy +
325  fluxentry.pdpz*fluxentry.pdpz );
326  double parent_energy = TMath::Sqrt( parentp2 +
327  parent_mass*parent_mass);
328  double parentp = TMath::Sqrt( parentp2 );
329 
330  double gamma = parent_energy / parent_mass;
331  double gamma_sqr = gamma * gamma;
332  double beta_mag = TMath::Sqrt( ( gamma_sqr - 1.0 )/gamma_sqr );
333 
334  // Get the neutrino energy in the parent decay CM
335  double enuzr = fluxentry.necm;
336  // Get angle from parent line of flight to chosen point in beam frame
337  double rad = TMath::Sqrt( (xpos-fluxentry.vx)*(xpos-fluxentry.vx) +
338  (ypos-fluxentry.vy)*(ypos-fluxentry.vy) +
339  (zpos-fluxentry.vz)*(zpos-fluxentry.vz) );
340 
341  double costh_pardet = ( fluxentry.pdpx*(xpos-fluxentry.vx) +
342  fluxentry.pdpy*(ypos-fluxentry.vy) +
343  fluxentry.pdpz*(zpos-fluxentry.vz) )
344  / ( parentp * rad);
345  if ( costh_pardet > 1.0 ) costh_pardet = 1.0;
346  if ( costh_pardet < -1.0 ) costh_pardet = -1.0;
347  double theta_pardet = TMath::ACos(costh_pardet);
348 
349  // Weighted neutrino energy in beam, approx, good for small theta
350  //RWH//double emrat = 1.0 / ( gamma * ( 1.0 - beta_mag * TMath::Cos(theta_pardet)));
351  double emrat = 1.0 / ( gamma * ( 1.0 - beta_mag * costh_pardet ));
352  enu = emrat * enuzr; // ! the energy ... normally
353 
354  // RWH-debug
355  bool debug = false;
356  if (debug) {
357  cout << setprecision(15);
358  cout << "ptype " << fluxentry.ptype << " m " << parent_mass
359  << " p " << parentp << " e " << parent_energy << " gamma " << gamma
360  << " beta " << beta_mag << endl;
361 
362  cout << " enuzr " << enuzr << " rad " << rad << " costh " << costh_pardet
363  << " theta " << theta_pardet << " emrat " << emrat
364  << " enu " << enu << endl;
365  }
366  partials.parent_mass = parent_mass;
367  partials.parentp = parentp;
368  partials.parent_energy = parent_energy;
369  partials.gamma = gamma;
370  partials.beta_mag = beta_mag;
371  partials.enuzr = enuzr;
372  partials.rad = rad;
373  partials.costh_pardet = costh_pardet;
374  partials.theta_pardet = theta_pardet;
375  partials.emrat = emrat;
376  partials.eneu = enu;
377 
378  // Get solid angle/4pi for detector element
379  double sangdet = ( kRDET*kRDET / ( (zpos-fluxentry.vz)*(zpos-fluxentry.vz)))/4.0;
380 
381  // Weight for solid angle and lorentz boost
382  wgt_xy = sangdet * ( emrat * emrat ); // ! the weight ... normally
383 
384  partials.sangdet = sangdet;
385  partials.wgt = wgt_xy;
386  partials.ptype = fluxentry.ptype; // assume already PDG
387 
388  // Done for all except polarized muon decay
389  // in which case need to modify weight
390  // (must be done in double precision)
391  if ( fluxentry.ptype == kpdg_muplus || fluxentry.ptype == kpdg_muminus) {
392  double beta[3], p_dcm_nu[4], p_nu[3], p_pcm_mp[3], partial;
393 
394  // Boost neu neutrino to mu decay CM
395  beta[0] = fluxentry.pdpx / parent_energy;
396  beta[1] = fluxentry.pdpy / parent_energy;
397  beta[2] = fluxentry.pdpz / parent_energy;
398  p_nu[0] = (xpos-fluxentry.vx)*enu/rad;
399  p_nu[1] = (ypos-fluxentry.vy)*enu/rad;
400  p_nu[2] = (zpos-fluxentry.vz)*enu/rad;
401  partial = gamma *
402  (beta[0]*p_nu[0] + beta[1]*p_nu[1] + beta[2]*p_nu[2] );
403  partial = enu - partial/(gamma+1.0);
404  p_dcm_nu[0] = p_nu[0] - beta[0]*gamma*partial;
405  p_dcm_nu[1] = p_nu[1] - beta[1]*gamma*partial;
406  p_dcm_nu[2] = p_nu[2] - beta[2]*gamma*partial;
407  p_dcm_nu[3] = TMath::Sqrt( p_dcm_nu[0]*p_dcm_nu[0] +
408  p_dcm_nu[1]*p_dcm_nu[1] +
409  p_dcm_nu[2]*p_dcm_nu[2] );
410 
411  partials.betanu[0] = beta[0];
412  partials.betanu[1] = beta[1];
413  partials.betanu[2] = beta[2];
414  partials.p_nu[0] = p_nu[0];
415  partials.p_nu[1] = p_nu[1];
416  partials.p_nu[2] = p_nu[2];
417  partials.partial1 = partial;
418  partials.p_dcm_nu[0] = p_dcm_nu[0];
419  partials.p_dcm_nu[1] = p_dcm_nu[1];
420  partials.p_dcm_nu[2] = p_dcm_nu[2];
421  partials.p_dcm_nu[3] = p_dcm_nu[3];
422 
423  // Boost parent of mu to mu production CM
424  double particle_energy = fluxentry.ppenergy;
425  gamma = particle_energy/parent_mass;
426  beta[0] = fluxentry.ppdxdz * fluxentry.pppz / particle_energy;
427  beta[1] = fluxentry.ppdydz * fluxentry.pppz / particle_energy;
428  beta[2] = fluxentry.pppz / particle_energy;
429  partial = gamma * ( beta[0]*fluxentry.muparpx +
430  beta[1]*fluxentry.muparpy +
431  beta[2]*fluxentry.muparpz );
432  partial = fluxentry.mupare - partial/(gamma+1.0);
433  p_pcm_mp[0] = fluxentry.muparpx - beta[0]*gamma*partial;
434  p_pcm_mp[1] = fluxentry.muparpy - beta[1]*gamma*partial;
435  p_pcm_mp[2] = fluxentry.muparpz - beta[2]*gamma*partial;
436  double p_pcm = TMath::Sqrt ( p_pcm_mp[0]*p_pcm_mp[0] +
437  p_pcm_mp[1]*p_pcm_mp[1] +
438  p_pcm_mp[2]*p_pcm_mp[2] );
439 
440  //cout << " muparpxyz " << fluxentry.muparpx << " "
441  // << fluxentry.muparpy << " " << fluxentry.muparpz << endl;
442  //cout << " beta " << beta[0] << " " << beta[1] << " " << beta[2] << endl;
443  //cout << " gamma " << gamma << " partial " << partial << endl;
444  //cout << " p_pcm_mp " << p_pcm_mp[0] << " " << p_pcm_mp[1] << " " << p_pcm_mp[2] << " " << p_pcm << endl;
445  partials.muparent_px = fluxentry.muparpx;
446  partials.muparent_py = fluxentry.muparpy;
447  partials.muparent_pz = fluxentry.muparpz;
448  partials.gammamp = gamma;
449  partials.betamp[0] = beta[0];
450  partials.betamp[1] = beta[1];
451  partials.betamp[2] = beta[2];
452  partials.partial2 = partial;
453  partials.p_pcm_mp[0] = p_pcm_mp[0];
454  partials.p_pcm_mp[1] = p_pcm_mp[1];
455  partials.p_pcm_mp[2] = p_pcm_mp[2];
456  partials.p_pcm = p_pcm;
457 
458  const double eps = 1.0e-30; // ? what value to use
459  if ( p_pcm < eps || p_dcm_nu[3] < eps ) {
460  return 3; // mu missing parent info?
461  }
462  // Calc new decay angle w.r.t. (anti)spin direction
463  double costh = ( p_dcm_nu[0]*p_pcm_mp[0] +
464  p_dcm_nu[1]*p_pcm_mp[1] +
465  p_dcm_nu[2]*p_pcm_mp[2] ) /
466  ( p_dcm_nu[3]*p_pcm );
467  if ( costh > 1.0 ) costh = 1.0;
468  if ( costh < -1.0 ) costh = -1.0;
469  // Calc relative weight due to angle difference
470  double wgt_ratio = 0.0;
471  switch ( fluxentry.ntype ) {
472  case kpdg_nue:
473  case kpdg_nuebar:
474  wgt_ratio = 1.0 - costh;
475  break;
476  case kpdg_numu:
477  case kpdg_numubar:
478  double xnu = 2.0 * enuzr / kMUMASS;
479  wgt_ratio = ( (3.0-2.0*xnu ) - (1.0-2.0*xnu)*costh ) / (3.0-2.0*xnu);
480  break;
481  default:
482  return 2; // bad neutrino type
483  }
484  wgt_xy = wgt_xy * wgt_ratio;
485 
486  partials.ntype = fluxentry.ntype; // assume converted to PDG
487  partials.costhmu = costh;
488  partials.wgt_ratio = wgt_ratio;
489 
490  }
491 
492  return 0;
493 }
PYTHON x
Definition: diff.txt:3
double enu[nsteps]
TCanvas * c2
Definition: drawXsec.C:3
void SetLengthUnits(double user_units)
Set units assumed by user.
Definition: GNuMIFlux.cxx:1362
double fabserrX(double a, double b)
Definition: test_gnumi.C:27
STL namespace.
Actions and Circumstances Relevant to Incomplete Log Problem The some of the LogInfo messages issued at the end involving branch information are failing to emerge This necessitates re running the for a net loss of up to of the work done The problem can t be happening based on what the logger but it is Dave Evans worte a stand along program to issue huge bunches of messages to try to provoke a repeatable version of the bad which we could hope to debug
the ParameterSet object passed in for the configuration of a destination should be the only source that can affect the behavior of that destination This is to eliminate the dependencies of configuring a destination from multiple mostly from the defaults It suppresses possible glitches about changing the configuration file somewhere outside of a destination segament might still affect the behavior of that destination In the previous configuration for a specific the value of a certain e may come from following and have been suppressed It the configuring ParameterSet object for each destination will be required to carry a parameter list as complete as possible If a parameter still cannot be found in the ParameterSet the configuration code will go look for a hardwired default directly The model is a great simplicity comparing with the previous especially when looking for default values Another great advantage is most of the parameters now have very limited places that allows to appear Usually they can only appear at one certain level in a configuration file For in the old configuring model or in a default ParameterSet object inside of a or in a category or in a severity object This layout of multiple sources for a single parameter brings great confusion in both writing a configuration and in processing the configuration file Under the new the only allowed place for the parameter limit to appear is inside of a category which is inside of a destination object Other improvements simplify the meaning of a destination name In the old a destination name has multiple folds of meanings the e cout and cerr have the special meaning of logging messages to standard output or standard error the name also serves as the output filename if the destination is a file these names are also references to look up for detailed configurations in configuring the MessageFacility The multi purpose of the destination name might cause some unwanted behavior in either writing or parsing the configuration file To amend in the new model the destination name is now merely a name for a which might represent the literal purpose of this or just an id All other meanings of the destinations names now go into the destination ParameterSet as individual such as the type parameter and filename parameter Following is the deatiled rule for the new configuring Everything that is related with MessageFacility configuration must be wrapped in a single ParameterSet object with the name MessageFacility The MessageFacility ParameterSet object contains a series of top level parameters These parameters can be chosen a vector of string listing the name of debug enabled models Or use *to enable debug messages in all modules a vector of string a vector of string a vector of string a ParameterSet object containing the list of all destinations The destinations ParameterSet object is a combination of ParameterSet objects for individual destinations There are two types of destinations that you can insert in the destinations ParameterSet ordinary including cout
A list of PDG codes.
Definition: PDGCodeList.h:33
GENIE flux drivers.
Definition: GAstroFlux.h:117
A GENIE flux driver encapsulating the NuMI neutrino flux. It reads-in the official GNUMI neutrino flu...
Definition: GNuMIFlux.h:217
double Weight(void)
returns the flux neutrino weight (if any)
Definition: GNuMIFlux.h:234
double y
double MaxEnergy(void)
declare the max flux neutrino energy that can be generated (for init. purposes)
Definition: GNuMIFlux.h:231
virtual void LoadBeamSimData(const std::vector< std::string > &filenames, const std::string &det_loc)
Definition: GNuMIFlux.cxx:640
const double e
genie::flux::GNuMIFluxPassThroughInfo fluxentry_t
Definition: test_gnumi.C:25
const GNuMIFluxPassThroughInfo & PassThroughInfo(void)
GNuMIFluxPassThroughInfo.
Definition: GNuMIFlux.h:252
const double a
double z
int CalcEnuWgt(const TLorentzVector &xyz, double &enu, double &wgt_xy) const
Definition: GNuMIFlux.cxx:1885
const PDGCodeList & FluxParticles(void)
declare list of flux neutrinos that can be generated (for init. purposes)
Definition: GNuMIFlux.h:230
bool GenerateNext(void)
generate the next flux neutrino (return false in err)
Definition: GNuMIFlux.cxx:295
the ParameterSet object passed in for the configuration of a destination should be the only source that can affect the behavior of that destination This is to eliminate the dependencies of configuring a destination from multiple mostly from the defaults It suppresses possible glitches about changing the configuration file somewhere outside of a destination segament might still affect the behavior of that destination In the previous configuration for a specific the value of a certain e may come from following and have been suppressed It the configuring ParameterSet object for each destination will be required to carry a parameter list as complete as possible If a parameter still cannot be found in the ParameterSet the configuration code will go look for a hardwired default directly The model is a great simplicity comparing with the previous especially when looking for default values Another great advantage is most of the parameters now have very limited places that allows to appear Usually they can only appear at one certain level in a configuration file For in the old configuring model or in a default ParameterSet object inside of a or in a category or in a severity object This layout of multiple sources for a single parameter brings great confusion in both writing a configuration and in processing the configuration file Under the new the only allowed place for the parameter limit to appear is inside of a category which is inside of a destination object Other improvements simplify the meaning of a destination name In the old a destination name has multiple folds of meanings the e cout and cerr have the special meaning of logging messages to standard output or standard error the name also serves as the output filename if the destination is a file these names are also references to look up for detailed configurations in configuring the MessageFacility The multi purpose of the destination name might cause some unwanted behavior in either writing or parsing the configuration file To amend in the new model the destination name is now merely a name for a which might represent the literal purpose of this or just an id All other meanings of the destinations names now go into the destination ParameterSet as individual such as the type parameter and filename parameter Following is the deatiled rule for the new configuring Everything that is related with MessageFacility configuration must be wrapped in a single ParameterSet object with the name MessageFacility The MessageFacility ParameterSet object contains a series of top level parameters These parameters can be chosen a vector of string listing the name of debug enabled models Or use *to enable debug messages in all modules a vector of string a vector of string a vector of string a ParameterSet object containing the list of all destinations The destinations ParameterSet object is a combination of ParameterSet objects for individual destinations There are two types of destinations that you can insert in the destinations ParameterSet ordinary including cerr
void Print(const Option_t *opt="") const
Definition: GNuMIFlux.cxx:1626
static const double rad
Definition: Units.h:165
const TLorentzVector & Momentum(void)
returns the flux neutrino 4-momentum
Definition: GNuMIFlux.h:235
void ScanForMaxWeight(void)
scan for max flux weight (before generating unweighted flux neutrinos)
Definition: GNuMIFlux.cxx:836
void test_gnumi(int mxpull=0)
Definition: test_gnumi.C:38
int calc_enuwgt(const fluxentry_t &fluxentry, double x, double y, double z, double &enu, double &wgt_xy, xypartials &partials)
Definition: test_gnumi.C:223
void SetGenWeighted(bool genwgt=false)
toggle whether GenerateNext() returns weight=1 flux (initial default false)
Definition: GNuMIFlux.h:292