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LDMX Software
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A deliberate mis-placement of the reconstruction magnetic field, used to quantify how well we need to know where the dipole sits before the reconstructed momentum scale is biased. More...
#include <BFieldXYZUtils.h>
Public Member Functions | |
| Acts::RotationMatrix3 | rotationMatrix () const |
| Rz(gamma) * Ry(beta) * Rx(alpha) | |
| bool | isNominal () const |
| Exact comparison on purpose: the nominal case reuses the default transforms unchanged, so an unconfigured job gets bit-for-bit the field it got before these knobs existed. | |
Public Attributes | |
| Acts::Vector3 | translation_ {Acts::Vector3::Zero()} |
| displacement of the magnet [mm] | |
| Acts::Vector3 | rotation_ {Acts::Vector3::Zero()} |
| rotation about x, y, z through pivot [rad] | |
| Acts::Vector3 | pivot_ {-DIPOLE_OFFSET, 0., 0.} |
| centre of rotation [mm], default the field-map origin | |
| double | scale_ {1.} |
| overall scaling of the field strength | |
A deliberate mis-placement of the reconstruction magnetic field, used to quantify how well we need to know where the dipole sits before the reconstructed momentum scale is biased.
The simulation is untouched.
Applied as an inverse coordinate transform at lookup time: the query point is moved back into the nominal map frame, and the returned field is rotated and rescaled on the way out.
Members are in the ACTS frame; the configuration is in the LDMX global frame, see tracking::reco::TrackingGeometryUser::bFieldDistortion().
Definition at line 63 of file BFieldXYZUtils.h.
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inline |
Exact comparison on purpose: the nominal case reuses the default transforms unchanged, so an unconfigured job gets bit-for-bit the field it got before these knobs existed.
rot * (pos - pivot) + pivot would not.
Definition at line 86 of file BFieldXYZUtils.h.
References rotation_, scale_, and translation_.
Referenced by tracking::reco::TrackingGeometryUser::loadBField().
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inline |
Rz(gamma) * Ry(beta) * Rx(alpha)
Definition at line 74 of file BFieldXYZUtils.h.
References rotation_.
Referenced by tracking::reco::TrackingGeometryUser::loadBField().
| Acts::Vector3 BFieldDistortion::pivot_ {-DIPOLE_OFFSET, 0., 0.} |
centre of rotation [mm], default the field-map origin
Definition at line 69 of file BFieldXYZUtils.h.
Referenced by tracking::reco::TrackingGeometryUser::bFieldDistortion(), and tracking::reco::TrackingGeometryUser::loadBField().
| Acts::Vector3 BFieldDistortion::rotation_ {Acts::Vector3::Zero()} |
rotation about x, y, z through pivot [rad]
Definition at line 67 of file BFieldXYZUtils.h.
Referenced by tracking::reco::TrackingGeometryUser::bFieldDistortion(), isNominal(), tracking::reco::TrackingGeometryUser::loadBField(), and rotationMatrix().
| double BFieldDistortion::scale_ {1.} |
overall scaling of the field strength
Definition at line 71 of file BFieldXYZUtils.h.
Referenced by tracking::reco::TrackingGeometryUser::bFieldDistortion(), isNominal(), and tracking::reco::TrackingGeometryUser::loadBField().
| Acts::Vector3 BFieldDistortion::translation_ {Acts::Vector3::Zero()} |
displacement of the magnet [mm]
Definition at line 65 of file BFieldXYZUtils.h.
Referenced by tracking::reco::TrackingGeometryUser::bFieldDistortion(), isNominal(), and tracking::reco::TrackingGeometryUser::loadBField().