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Additional info for Electromagnetic Calorimeter at RHIC - Design Report
High Pt charged particles will in general deposit the energy typical of a minimum ionizing particle before exiting the rear of the calorimeter. Consequently, although the EMC will detect some of the energy from high Pt charged particles, a simple tower threshold would not be sufficient for an efficient trigger. The full energy of such particles can be recovered for the purpose of jet reconstruction and tower correction from tracking in the STAR TPC. For pp and pA interactions the "pedestal" energy deposited in a given tower by background particles from the underlying event is minimal.
V) Figure 3D-5. discrimination The rate per second per GeV of events containing_lets of a given Et for various single tower thresholds. 05). ''''i .... I .... I .... I .... 1 .... I .... 40 I .... 8- _m _u x ? o .... 0 I .... 10 | .... 20 I .... 30 Jet EL (Gev) Figure 3D-6. The efficiency as a function of jet energy for triggering on an event containing tower discrimination threshold. Data shown are for AuAu collisions at _nn = 200 GeV. 3-10 60 a jet, for a given single STAR _,_ Conceptual Design 4.
The measurement of gluon shadowing in nuclei is of particular interest since the yield of mini-jets is strongly influenced by the density of gluons at small x. Although data exist on quark shadowing in the nucleus, the degree of gluon shadowing is presently tmknown. 1For a full discussion of the STAR detector, see The STAR Conceptual Design Report, LBL PUB-5347 (1992). 2M. Gyulassy and M. Pluemmer, Phys. Lett. B243 (1990) 432. N. Wang and M. Gyulassy, Phys. Lett. 68 (1992) 1480. 4K. V. Landshoff, and J.