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ATLAS Offline Software
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Variables | |
| const uint16_t | AuthorUnknown =0x0 |
| for the Authors of the egamma objects | |
| const uint16_t | AuthorElectron =0x1 |
| Object Reconstructed by standard cluster-based algorithm. | |
| const uint16_t | AuthorSofte =0x2 |
| Electron reconstructed by the track-based algorithm, here for compatibility with old AOD format. | |
| const uint16_t | AuthorPhoton =0x4 |
| Object Reconstructed by standard cluster-based algorithm. | |
| const uint16_t | AuthorFwdElectron =0x8 |
| Electron reconstructed by the Forward cluster-based algorithm. | |
| const uint16_t | AuthorAmbiguous =0x10 |
| Object Reconstructed by standard cluster-based algorithm. | |
| const uint16_t | AuthorTrigElectron =0x20 |
| trigger Electrons | |
| const uint16_t | AuthorTrigPhoton =0x40 |
| trigger Photons | |
| const uint16_t | AuthorCaloTopo35 =0x80 |
| Photon reconstructed by SW CaloTopo35 seeded clusters. | |
| const uint16_t | AuthorALL = 0xFFFF |
| not an actual author, but used as default in some functions | |
| const uint32_t | BADCLUSELECTRON |
| const uint32_t | BADCLUSPHOTON |
| const uint32_t | ALLOQ = 0xFFFFFFFF |
| Enumerator | |
|---|---|
| DeadHVPS | Dead High Voltage in the EM Presampler. |
| DeadHVS1S2S3Core | Dead High Voltage in the EM strips, middle and back affecting the core of the cluster. |
| DeadHVS1S2S3Edge | Dead High Voltage in the EM strips, middle and back affecting the edge of the cluster. |
| NonNominalHVPS | Non Nominal High Voltage in the EM Presampler. |
| NonNominalHVS1S2S3 | Non Nominal High Voltage in the EM strips, middle and back. |
| MissingFEBCellCore | Missing FEB in the core of the cluster. |
| MissingFEBCellEdgePS | Missing FEB in the edge of the cluster. |
| MissingFEBCellEdgeS1 | Missing FEB in the edge of the cluster. |
| MissingFEBCellEdgeS2 | Missing FEB in the edge of the cluster. |
| MissingFEBCellEdgeS3 | Missing FEB in the edge of the cluster. |
| MaskedCellCore | Masked cell in the core of the cluster. |
| MaskedCellEdgePS | Masked presampler cell in the edge of the cluster. |
| MaskedCellEdgeS1 | Masked strip cell in the edge of the cluster. |
| MaskedCellEdgeS2 | Masked middle cell in the edge of the cluster. |
| MaskedCellEdgeS3 | Masked back cell in the edge of the cluster. |
| BadS1Core | Missing FEB or masked cell in S1 core (corresponding to the 8 strips in front of the core of the cluster) |
| SporadicNoiseLowQCore | Sporadic noisy cell in the core of the cluster. |
| SporadicNoiseLowQEdge | Sporadic noisy cell in the edge of the cluster. |
| HighQCore | High quality factor cell in the core of the cluster. |
| HighQEdge | High quality factor cell in the edge of the cluster. |
| AffectedCellCore | Affected cell in the core of the cluster. |
| AffectedCellEdgePS | Affected presampler cell in the edge of the cluster. |
| AffectedCellEdgeS1 | Affected strip cell in the edge of the cluster. |
| AffectedCellEdgeS2 | Affected middle cell in the edge of the cluster. |
| AffectedCellEdgeS3 | Affected back cell in the edge of the cluster. |
| HECHighQ | High quality factor cell in the HEC. |
| OutTime | Out of time cell. |
| LArQCleaning | Cleaning based on LArQ factor--> sum[ E(Q>4000)/E]. |
| DeadCellTileS0 | Dead cell in the Tile Calorimeter S0 affecting the hadronic leakage calculation. |
| DeadCellTileS1S2 | Dead cell in the Tile Calorimeter S1,2,3 affecting the hadronic leakage calculation. |
| HighRcell | High R_cell ----> Energy of the most energetic cell / total energy of the cluster. |
Definition at line 46 of file EgammaDefs.h.
| Enumerator | |
|---|---|
| unconverted | unconverted photon |
| singleSi | one track only, with Si hits |
| singleTRT | one track only, no Si hits (TRT only) |
| doubleSi | two tracks, both with Si hits |
| doubleTRT | two tracks, none with Si hits (TRT only) |
| doubleSiTRT | two tracks, only one with Si hits |
| NumberOfVertexConversionTypes | maximum number of types |
Definition at line 268 of file EgammaEnums.h.
| Enumerator | |
|---|---|
| electron | |
| unconvertedPhoton | |
| convertedPhoton | |
| forwardelectron | |
| NumberOfEgammaTypes | |
Definition at line 16 of file EgammaEnums.h.
| Enumerator | |
|---|---|
| e011 | uncalibrated energy (sum of cells) in presampler in a 1x1 window in cells in eta X phi |
| e033 | uncalibrated energy (sum of cells) in presampler in a 3x3 window in cells in eta X phi |
| e132 | uncalibrated energy (sum of cells) in strips in a 3x2 window in cells in eta X phi |
| e1152 | uncalibrated energy (sum of cells) in strips in a 15x2 window in cells in eta X phi |
| ethad1 | transverse energy in the first sampling of the hadronic calorimeters behind the cluster calculated from ehad1 |
| ethad | ET leakage into hadronic calorimeter with exclusion of energy in CaloSampling::TileGap3. |
| ehad1 | E leakage into 1st sampling of had calo (CaloSampling::HEC0 + CaloSampling::TileBar0 + CaloSampling::TileExt0) |
| f1 | E1/E = fraction of energy reconstructed in the first sampling, where E1 is energy in all strips belonging to the cluster and E is the total energy reconstructed in the electromagnetic calorimeter cluster. |
| f3 | fraction of energy reconstructed in 3rd sampling |
| f1core | E1(3x1)/E = fraction of the energy reconstructed in the first longitudinal compartment of the electromagnetic calorimeter, where E1(3x1) the energy reconstructed in +/-3 strips in eta, centered around the maximum energy strip and E is the energy reconstructed in the electromagnetic calorimeter. |
| f3core | E3(3x3)/E fraction of the energy reconstructed in the third compartment of the electromagnetic calorimeter, where E3(3x3), energy in the back sampling, is the sum of the energy contained in a 3x3 window around the maximum energy cell. |
| e233 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x3 (in cell units eta X phi) |
| e235 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x5 |
| e255 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 5x5 |
| e237 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x7 |
| e277 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 7x7 |
| e333 | uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x3 |
| e335 | uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x5 |
| e337 | uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x7 |
| e377 | uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 7x7 |
| weta1 | shower width using +/-3 strips around the one with the maximal energy deposit: w3 strips = sqrt{sum(Ei)x(i-imax)^2/sum(Ei)}, where i is the number of the strip and imax the strip number of the most energetic one |
| weta2 | the lateral width is calculated with a window of 3x5 cells using the energy weighted sum over all cells, which depends on the particle impact point inside the cell: weta2 = sqrt(sum Ei x eta^2)/(sum Ei) -((sum Ei x eta)/(sum Ei))^2, where Ei is the energy of the i-th cell |
| e2ts1 | 2nd max in strips calc by summing 3 strips |
| e2tsts1 | energy of the cell corresponding to second energy maximum in the first sampling |
| fracs1 | shower shape in the shower core : [E(+/-3)-E(+/-1)]/E(+/-1), where E(+/-n) is the energy in ± n strips around the strip with highest energy |
| widths1 | same as egammaParameters::weta1 but without corrections on particle impact point inside the cell |
| widths2 | same as egammaParameters::weta2 but without corrections on particle impact point inside the cell |
| poscs1 | relative position in eta within cell in 1st sampling |
| poscs2 | relative position in eta within cell in 2nd sampling |
| asy1 | uncorr asymmetry in 3 strips in the 1st sampling |
| pos | difference between shower cell and predicted track in +/- 1 cells |
| pos7 | Difference between the track and the shower positions: sum_{i=i_m-7}^{i=i_m+7}E_i x (i-i_m) / sum_{i=i_m-7}^{i=i_m+7}E_i, The difference between the track and the shower positions measured in units of distance between the strips, where i_m is the impact cell for the track reconstructed in the inner detector and E_i is the energy reconstructed in the i-th cell in the eta direction for constant phi given by the track parameters. |
| barys1 | barycentre in sampling 1 calculated in 3 strips |
| wtots1 | shower width is determined in a window detaxdphi = 0,0625 ×~0,2, corresponding typically to 20 strips in eta : wtot1=sqrt{sum Ei x ( i-imax)^2 / sum Ei}, where i is the strip number and imax the strip number of the first local maximum |
| emins1 | energy reconstructed in the strip with the minimal value between the first and second maximum |
| emaxs1 | energy of strip with maximal energy deposit |
| r33over37allcalo | 1-ratio of energy in 3x3 over 3x7 cells; E(3x3) = E0(1x1) + E1(3x1) + E2(3x3) + E3(3x3); E(3x7) = E0(3x3) + E1(15x3) + E2(3x7) + E3(3x7) |
| ecore | core energy in em calo E(core) = E0(3x3) + E1(15x2) + E2(5x5) + E3(3x5) |
| Reta | e237/e277 |
| Rphi | e233/e237 |
| Eratio | (emaxs1-e2tsts1)/(emaxs1+e2tsts1) |
| Rhad | ethad/et |
| Rhad1 | ethad1/et |
| DeltaE | e2tsts1-emins1 |
| NumberOfShowerShapes | maximum number of enums |
Definition at line 27 of file EgammaEnums.h.
Definition at line 173 of file EgammaEnums.h.
Definition at line 239 of file EgammaEnums.h.
| const uint32_t xAOD::EgammaParameters::ALLOQ = 0xFFFFFFFF |
Definition at line 133 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorALL = 0xFFFF |
not an actual author, but used as default in some functions
Definition at line 40 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorAmbiguous =0x10 |
Object Reconstructed by standard cluster-based algorithm.
Ambiguous ==> can be either Electron or Photon
Definition at line 32 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorCaloTopo35 =0x80 |
Photon reconstructed by SW CaloTopo35 seeded clusters.
Definition at line 38 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorElectron =0x1 |
Object Reconstructed by standard cluster-based algorithm.
Surely not Photon ==> Electron
Definition at line 24 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorFwdElectron =0x8 |
Electron reconstructed by the Forward cluster-based algorithm.
Definition at line 30 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorPhoton =0x4 |
Object Reconstructed by standard cluster-based algorithm.
Surely not Electron ==> Photon
Definition at line 28 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorSofte =0x2 |
Electron reconstructed by the track-based algorithm, here for compatibility with old AOD format.
Definition at line 26 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorTrigElectron =0x20 |
trigger Electrons
Definition at line 34 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorTrigPhoton =0x40 |
trigger Photons
Definition at line 36 of file EgammaDefs.h.
| const uint16_t xAOD::EgammaParameters::AuthorUnknown =0x0 |
| const uint32_t xAOD::EgammaParameters::BADCLUSELECTRON |
Definition at line 116 of file EgammaDefs.h.
| const uint32_t xAOD::EgammaParameters::BADCLUSPHOTON |
Definition at line 124 of file EgammaDefs.h.