- /// @brief uncalibrated energy (sum of cells) in presampler in a 1x1 window in cells in eta X phi

e011 = 0,

/// @brief uncalibrated energy (sum of cells) in presampler in a 3x3 window in cells in eta X phi

e033 = 1,

/// @brief uncalibrated energy (sum of cells) in strips in a 3x2 window in cells in eta X phi

e132 = 2,

/// @brief uncalibrated energy (sum of cells) in strips in a 15x2 window in cells in eta X phi

e1152 = 3,

/// @brief transverse energy in the first sampling of the hadronic calorimeters behind the cluster calculated from ehad1

ethad1 = 4,

/// @brief ET leakage into hadronic calorimeter with exclusion of energy in CaloSampling::TileGap3

ethad = 5,

/// @brief E leakage into 1st sampling of had calo (CaloSampling::HEC0 + CaloSampling::TileBar0 + CaloSampling::TileExt0)

ehad1 = 6,

/// @brief 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 calorimet\

er cluster

f1 = 7,

/// @brief fraction of energy reconstructed in 3rd sampling

f3 = 8,

/// @brief 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

f1core = 9,

/// @brief 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 3\

x3 window around the maximum energy cell

f3core = 10,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x3 (in cell units eta X phi)

e233 = 11,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x5

e235 = 12,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 5x5

e255 = 13,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 3x7

e237 = 14,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 7x7

e277 = 15,

/// @brief uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x3

e333 = 16,

/// @brief uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x5

e335 = 17,

/// @brief uncalibrated energy (sum of cells) of the third sampling in a rectangle of size 3x7

e337 = 18,

/// @brief uncalibrated energy (sum of cells) of the middle sampling in a rectangle of size 7x7

e377 = 19,

/// @brief 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

weta1 = 20,

/// @brief 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

weta2 = 21,

/// @brief 2nd max in strips calc by summing 3 strips

e2ts1 = 22,

/// @brief energy of the cell corresponding to second energy maximum in the first sampling

e2tsts1 = 23,

/// @brief 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

fracs1 = 24,

/// @brief same as egammaParameters::weta1 but without corrections on particle impact point inside the cell

widths1 = 25,

/// @brief same as egammaParameters::weta2 but without corrections on particle impact point inside the cell

widths2 = 26,

/// @brief relative position in eta within cell in 1st sampling

poscs1 = 27,

/// @brief relative position in eta within cell in 2nd sampling

poscs2= 28,

/// @brief uncorr asymmetry in 3 strips in the 1st sampling

asy1 = 29,

/// @brief difference between shower cell and predicted track in +/- 1 cells

pos = 30,

/// @brief 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

pos7 = 31,

/// @brief barycentre in sampling 1 calculated in 3 strips

barys1 =32,

/// @brief 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

wtots1 = 33,

/// @brief energy reconstructed in the strip with the minimal value between the first and second maximum

emins1 = 34,

/// @brief energy of strip with maximal energy deposit

emaxs1 = 35,

/// @brief 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)
- r33over37allcalo = 36,
- /// @brief core energy in em calo E(core) = E0(3x3) + E1(15x2) + E2(5x5) + E3(3x5)
- ecore = 37,
- /// @brief e237/e277
- Reta = 38,
- /// @brief e233/e237
- Rphi = 39,
- /// @brief (emaxs1-e2tsts1)/(emaxs1+e2tsts1)
- Eratio = 40,
- /// @bried ethad/et
- Rhad = 41,
- /// @bried ethad1/et
- Rhad1 = 42,
- /// @bried e2tsts1-emins1
- DeltaE =43,
- ///maximum number of enums
- NumberOfShowerShapes = 44

-- YuyaKano1 - 2016-04-06

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