| Status report TOF/T0 data in PR03 |
| Frank L. H. Wolfs | |
| University of Rochester | |
| January 17, 2003 |
| Outline |
| T0 Calibrations | |
| TOF Calibrations and Results | |
| Issues to be addressed in the next week or two. | |
| Note: all data shown here are data obtained in run 10511. This is a run with magnetic field on. |
| Software status |
| Rough energy calibration for T0 in the DB. TOF is not calibrated yet and PR01 pulse-height calibration is used to look at the current data. | |
| First rough time calibration for T0s will be implemented this weekend, | |
| T0 and TOF data are now included in the trigger trees (committed to CVS at noon on 1/16). The sum energy and multiplicities are roughly correct. | |
| Automatic calibration procedures are not automatic and in fact do not run reliably. |
| T0 calibrations |
| A first order energy calibration of the T0s is in the DB. | |
| We need to monitor the gains in the PMT, although they appear to be very stable (despite the fact that we keep turning the counters on and off). | |
| Firs order time calibrations need to be made, in order to ensure that the vertex information in the trigger trees makes sense. |
| T0 correlations |
| The multiplicity in the T0s is correlated with the multiplicities in the paddles. | |
| The correlation is similar for the N and the P side, except of the fact that the multiplicities are lower on the P side (for both paddles and T0s) compared to the N side. |
| T0 correlations |
| The sum energy in the T0s is correlated with the sum energy in the paddles. | |
| As expected, the sum energies are in general lower on the P side compared to the N side. |
| TOF Multiplicities |
| The figures show the TOF multiplicities for wall TB and wall TC. The following requirements must be satisfied: | ||
| A good pulse height in both top and bottom PMTs. | ||
| A prompt time signals in both top and bottom PMTs. | ||
| Observations are similar to those made by the SpecTrig group: the multiplicities for collision events (red) are much lower than the multiplicities for beam-gas events (blue). | ||
| TOF Energy |
| Using the last calibration parameters of PR01, we gain-matched the PMTs and reconstructed the TOF energy based on the measured pulse heights. | |
| The calibration is in terms of MIPS, but the calibration parameters depend on the average angle of incidence, which is a function of position/orientation of the walls and the field. |
| TOF Energy |
| Comparing collision events with beam-gas events we observed MIP peaks for both events. | |
| The main difference between beam-gas and collision events is the signal-to-background ratio. | |
| The background in wall TC is higher than the background in wall TB. |
| TOF Sum Energy |
| Conclusions and concerns |
| The data for both TOF and T0 look good. The critical change that was made in the RHIC operation that changed the TOF from a BLM to a good detector was the reduction in background. | |
| It will need 1 - 2 weeks before the TOF and T0 calibration procedures are finalized, and it would be bad if DV was frozen before then. Note that none of the Au - Au calibration procedures work at the moment due to changes in triggering and changes in multiplicities. | |
| Can we keep time calibrator events in the PhoHit files? We need to get more experience with how to correct the data collected on the fly. |