|
1 | 1 | Dorothea |
2 | | -========== |
| 2 | +======== |
3 | 3 |
|
4 | | -.. caution:: |
5 | | - This page is currently not created, we are working on it. If you would like to contribute on this documentation, reach ` me < [email protected]>`_! |
| 4 | +*From ancient Greek, Δωροθέα: gift of God.* |
| 5 | + |
| 6 | +The purpose of *Dorothea* is to process the **PMaps** (outcome of *Irene*) and |
| 7 | +reconstruct point-like events. Therefore, all the information included in the S2 peaks |
| 8 | +is collapsed into a single x, y, and z deposition with a given E (the area under the S2 peak). |
| 9 | +Additionally, some parameters regarding the S1 and S2 peaks are provided as a tool for further selections. |
| 10 | +Last, it is worth noting that for events where more than S1 or S2 (or both) are |
| 11 | +present in the event, a point is reconstructed for each possible combination. |
| 12 | + |
| 13 | + |
| 14 | +.. _Dorothea input: |
| 15 | + |
| 16 | +Input |
| 17 | +----- |
| 18 | + |
| 19 | +* ``/Run/events`` |
| 20 | +* ``/Run/runInfo`` |
| 21 | +* ``/PMAPS/S1`` |
| 22 | +* ``/PMAPS/S1Pmt`` |
| 23 | +* ``/PMAPS/S2`` |
| 24 | +* ``/PMAPS/S2Pmt`` |
| 25 | +* ``/PMAPS/S2Si`` |
| 26 | + |
| 27 | +.. _Dorothea output: |
| 28 | + |
| 29 | +Output |
| 30 | +------ |
| 31 | + |
| 32 | + * ``/DST/Events``: summary of the reconstructed events and their main properties. Each row represents one combination of an S1 and a S2 identified under the same ``event`` but with its corresponding ``s1_peak`` and ``s2_peak`` identifier. The full list and description of the parameters in the table may be found later. |
| 33 | + * ``/Filters/s12_selector``: flag for whether an event passed the S1 and S2 selections |
| 34 | + |
| 35 | + |
| 36 | +.. _Irene config: |
| 37 | + |
| 38 | +Config |
| 39 | +------ |
| 40 | + |
| 41 | +Besides the :ref:`Common arguments to every city`, *Dorothea* has the following arguments: |
| 42 | + |
| 43 | +.. list-table:: |
| 44 | + :widths: 50 40 120 |
| 45 | + :header-rows: 1 |
| 46 | + |
| 47 | + * - **Parameter** |
| 48 | + - **Type** |
| 49 | + - **Description** |
| 50 | + |
| 51 | + * - ``drift_v`` |
| 52 | + - ``float`` |
| 53 | + - Drift velocity of the secondary electrons towards the anode. |
| 54 | + |
| 55 | + * - ``s1|s2_nmin|nmax`` |
| 56 | + - ``int`` |
| 57 | + - Lower/upper limits to the number of S1/S2 peaks per event. |
| 58 | + |
| 59 | + * - ``s1|s2_emin|emax`` |
| 60 | + - ``float`` |
| 61 | + - Lower/upper limits to the energy (integral under the peak) of each S1/S2 peak (pes). |
| 62 | + |
| 63 | + * - ``s1|s2_wmin|wmax`` |
| 64 | + - ``float`` |
| 65 | + - Lower/upper limits to the with (time over threshold) of each S1/S2 peak (ns). |
| 66 | + |
| 67 | + * - ``s1|s2_hmin|hmax`` |
| 68 | + - ``float`` |
| 69 | + - Lower/upper limits to the height (maximum amplitude) of each S1/S2 peak (pes). |
| 70 | + |
| 71 | + * - ``s1|s2_ethr`` |
| 72 | + - ``float`` |
| 73 | + - Threshold for each bin within each S1/S2 to be considered for the energy computation (pes). |
| 74 | + |
| 75 | + * - ``s2_nsipmmin|nsipmminax`` |
| 76 | + - ``int`` |
| 77 | + - Lower/upper limits to the number of SiPM sensors with a recorded signal. |
| 78 | + |
| 79 | + * - ``global_reco_params`` |
| 80 | + - ``dict`` |
| 81 | + - Set of parameters for the corona algorithm. Since the desired one is the barycenter reconstruction, the only mandatory elements in the dictionary are: |
| 82 | + |
| 83 | + * ``Qthr``: charge threshold, ignore all SiPMs with less than Qthr pes. |
| 84 | + * ``lm_radius=-1``: sets the algorithm to be the barycenter. |
| 85 | + |
| 86 | + |
| 87 | +.. _Dorothea workflow: |
| 88 | + |
| 89 | +Workflow |
| 90 | +-------- |
| 91 | + |
| 92 | +The workflow for *Dorothea* is straightforward. After a filter removing all the peaks and events not satisfying the limits provided. Then, it proceeds to perform the point-like reconstruction. Basically, this algorithm collapses the whole S2 information into a single point: |
| 93 | + |
| 94 | + * The *x* and *y* position are determined via a charge-weighted average. This makes use of the so-called ``corona`` `algorithm <https://github.com/next-exp/IC/blob/8be75c65aa2e452eae4ce2e51494a58eab18a0d4/invisible_cities/reco/xy_algorithms.py#L61>`_, with the proper configuration to apply the barycenter computation. |
| 95 | + * The *z* coordinate is derived from the time difference between the maximum amplitude of the S1 and S2 considered, corrected by the drift velocity. |
| 96 | + * The energy is the integral under the S2 of those bins above the threshold. |
| 97 | + |
| 98 | + Besides, the reconstruction yields a set of useful values regarding the peaks that are also provided in the final table: |
| 99 | + |
| 100 | + .. list-table:: |
| 101 | + :widths: 50 40 120 |
| 102 | + :header-rows: 1 |
| 103 | + |
| 104 | + * - **Parameter** |
| 105 | + - **Type** |
| 106 | + - **Description** |
| 107 | + |
| 108 | + * - ``event`` |
| 109 | + - ``int`` |
| 110 | + - Event ID. As an event can have several S1 and S2 combinations, each one representing one row, this number identifies all the reconstructed points within the same original waveform. |
| 111 | + |
| 112 | + * - ``time`` |
| 113 | + - ``float`` |
| 114 | + - Timestamp of the event. |
| 115 | + |
| 116 | + * - ``s1_peak`` |
| 117 | + - ``int`` |
| 118 | + - S1 ID. It identifies the S1 within an event. |
| 119 | + |
| 120 | + * - ``s2_peak`` |
| 121 | + - ``int`` |
| 122 | + - S2 ID. It identifies the S2 within an event. |
| 123 | + |
| 124 | + * - ``nS1`` |
| 125 | + - ``int`` |
| 126 | + - Number of S1 present in the event. |
| 127 | + * - ``nS2`` |
| 128 | + - ``int`` |
| 129 | + - Number of S2 present in the event. |
| 130 | + |
| 131 | + * - ``S1w`` |
| 132 | + - ``float`` |
| 133 | + - S1 time over threshold (ns). |
| 134 | + |
| 135 | + * - ``s1h`` |
| 136 | + - ``float`` |
| 137 | + - S1 maximum amplitude (pes). |
| 138 | + |
| 139 | + * - ``S1e`` |
| 140 | + - ``float`` |
| 141 | + - S1 PMT- and time-summed amplitude over threshold (pes). |
| 142 | + |
| 143 | + * - ``S1t`` |
| 144 | + - ``float`` |
| 145 | + - Waveform time at maximum S1 amplitude (ns). |
| 146 | + |
| 147 | + * - ``S2w`` |
| 148 | + - ``float`` |
| 149 | + - S2 time over threshold (ns). |
| 150 | + |
| 151 | + * - ``s2h`` |
| 152 | + - ``float`` |
| 153 | + - S2 maximum amplitude (pes). |
| 154 | + |
| 155 | + * - ``S2e`` |
| 156 | + - ``float`` |
| 157 | + - S2 PMT- and time-summed amplitude over threshold (pes). |
| 158 | + |
| 159 | + * - ``S2t`` |
| 160 | + - ``float`` |
| 161 | + - Waveform time at maximum S2 amplitude (ns). |
| 162 | + |
| 163 | + * - ``S2q`` |
| 164 | + - ``float`` |
| 165 | + - S2 SiPM- and time-summed amplitude over threshold (pes). |
| 166 | + |
| 167 | + * - ``Nsipm`` |
| 168 | + - ``int`` |
| 169 | + - Number of SiPMs with signal over threshold. |
| 170 | + |
| 171 | + * - ``DT`` |
| 172 | + - ``float`` |
| 173 | + - Drift Time —i.e., time difference between the corresponding S1 and S2— (:math:`\mu s`). |
| 174 | + |
| 175 | + * - ``Z`` |
| 176 | + - ``float`` |
| 177 | + - Reconstructed z position coordinate —i.e., the DT times the drift velocity— (mm). |
| 178 | + |
| 179 | + * - ``Zrms`` |
| 180 | + - ``float`` |
| 181 | + - Standard deviation of the PMT signal in the z coordinate (mm). |
| 182 | + |
| 183 | + * - ``X`` |
| 184 | + - ``float`` |
| 185 | + - Reconstructed x position coordinate using the barycenter algorithm (mm). |
| 186 | + |
| 187 | + * - ``Y`` |
| 188 | + - ``float`` |
| 189 | + - Reconstructed y position coordinate using the barycenter algorithm (mm). |
| 190 | + |
| 191 | + * - ``R`` |
| 192 | + - ``float`` |
| 193 | + - Reconstructed radial coordinate, :math:`r^2=x^2+y^2` (mm). |
| 194 | + |
| 195 | + * - ``Phi`` |
| 196 | + - ``float`` |
| 197 | + - Reconstructed azimuthal coordinate, :math:`\phi=\arctan(y/x)` (rad). |
| 198 | + |
| 199 | + * - ``Xrms`` |
| 200 | + - ``float`` |
| 201 | + - Standard deviation of the PMT signal in the x coordinate (mm). |
| 202 | + |
| 203 | + * - ``Yrms`` |
| 204 | + - ``float`` |
| 205 | + - Standard deviation of the PMT signal in the y coordinate (mm). |
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