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Pointing with the IST Detectors at the vertex in p-p and Au-Au Collisions Jim Thomas

Pointing with the IST Detectors at the vertex in p-p and Au-Au Collisions Jim Thomas Lawrence Berkeley National Laboratory July 12 th , 2007. IST Pointing Resolution for B Physics.

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Pointing with the IST Detectors at the vertex in p-p and Au-Au Collisions Jim Thomas

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  1. Pointing with the IST Detectors at the vertex in p-p and Au-Au Collisions Jim Thomas Lawrence Berkeley National Laboratory July 12th, 2007

  2. IST Pointing Resolution for B Physics • At the June 29th TUP meeting, Dick Majka asked if it was possible to use the IST detectors to trigger on B physics • This requires sub-millimeter resolution from the IST system • (by assumption) the PXL layers are too slow to be part of a trigger decision • and he suggested that hand calculations could give some guidance on this matter (said with a hint in his voice …) • I have studied three cases: • TPC + SSD + IST2 + IST1 (Blue) • TPC + IST2 + IST1 (Red) • TPC + SSD + IST1 (Green)

  3. R-Phi Pointing Resolution Does Not Change (much) Figure 1: The R-Phi pointing resolution measured at the vertex for the IST detectors acting alone.

  4. Z Res at the Vertex Decreases if IST2 is Removed Figure 2: The Z resolution at 1 GeV is about 450 microns unless IST2 detector is removed from the system and then it goes up to a millimeter. The color code is TPC + SSD + IST2 + IST1 (Blue), TPC + IST2 + IST1 (Red), TPC + SSD + IST1 (Green).

  5. Efficiency Calculations (ala HW and GvB) P(good) = 1 / (1+S) where S = 2xy With a minor bit of algebra, it is easy to show that P(bad) = S / ( 1 + S ) and when S is small P(bad)  S = 2xy x is the convolution of the detector resolution and the projected track error in the ‘x’ direction, y is the convolution of the detector resolution and the projected track error in the ‘y’ direction, and  is the density of hits. The largest error dominates the sum x =  ( 2xp + 2xd ) y =  ( 2yp + 2yd ) The largest error dominates the sum

  6. Single Track Efficiency for the Systems Studied .vs. PT Efficiency Calculation Results for Central Au-Au Figure 4: The system is less efficient when the SSD is removed from the suite of detectors, as expected, but more efficient when IST2 is removed. This is a surprise. The color code is TPC + SSD + IST2 + IST1 (Blue), TPC + IST2 + IST1 (Red), TPC + SSD + IST1 (Green).

  7. A Surprise • The efficiency calculations are fairly simple when the errors are symmetric and the detector resolution is smaller than the projected track error. However, it gets complicated when the errors are asymmetric and the detector resolution is long in one dimension and the projected track error is long in the other. • The crossed terms make for low efficiencies because the largest terms dominate in the quadrature sums. • In all three cases, we assumed that the detectors were exposed to Au-Au central collision hit densities from primary tracks (without background hits or tracks). The TPC+SSD+IST2+IST1 detector combination (blue) is about 78% efficient at 1 GeV/c. • The principle source of inefficiency is IST2 because is suffers from a high number of ambiguous hits due to the 4 cm length of the strips ( 1.16 cm) in one dimension, and the asymmetric resolution of the SSD ( 650 mm) in the other.

  8. The Answer to Dick’s Question • In conclusion, the pointing resolution at the vertex for the fast detectors only (TPC+SSD+IST2+IST1) is predicted to be 200 mm by 450 mm in p-p and Au-Au. The Efficiency for Au-Au collisions is 78%. • However, the efficiency goes up to 94% if IST2 is removed from the system while the pointing resolution degrades to 200 mm by 950 mm. • So the answer to Dick’s question is that it depends upon what you want to accomplish, higher efficiency in Au-Au or better pointing resolution with the fast detectors (only) in p-p collisions.

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