Mapping separation power Klaus Gtzen GSI Darmstadt PID

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Mapping separation power Klaus Götzen GSI Darmstadt PID TAG Meeting 15. Feb. 2007 K.

Mapping separation power Klaus Götzen GSI Darmstadt PID TAG Meeting 15. Feb. 2007 K. Götzen PID TAG Meeting – EVO – 15. 02. 08

Central Problem • Problem: – What is necessary PID quality for PANDA, i. e.

Central Problem • Problem: – What is necessary PID quality for PANDA, i. e. what minimal set of PID detectors is needed? . . . or to be more exact: – How much separation power do we need in which phase space region to reach our physics goals? • Answering implies: 1. How good is separation over phase space? 2. Where is significant kinematic signal/background overlap? K. Götzen PID TAG Meeting – EVO – 15. 02. 08 2

PID information • Attempt to answer question No 1. • At the moment: almost

PID information • Attempt to answer question No 1. • At the moment: almost no reco‘d PID info from Full Sim • Consider parametrized PID info in Fast Sim from det‘s – – – Barrel DIRC ( C) Endcap DIRC ( C) Forward RICH ( C) Straw Tube Tracker (d. E/dx) Micro Vertex Detector (d. E/dx) Barrel TOF (m 2) tcb tcd tcr des dem mt • Dataset: 200 k isotropic ( , p) single track events of every particle type (e, , , K, p) 0° < < 180° 0. 15 Ge. V/c < p < 8 Ge. V/c K. Götzen PID TAG Meeting – EVO – 15. 02. 08 3

Quality check C barrel DIRC endcap DIRC p [Ge. V/c 2] K. Götzen forward

Quality check C barrel DIRC endcap DIRC p [Ge. V/c 2] K. Götzen forward RICH p [Ge. V/c 2] d. E/dx p [Ge. V/c 2] STT C MVD p [Ge. V/c 2] PID TAG Meeting – EVO – 15. 02. 08 p [Ge. V/c 2] m 2 C TOF p [Ge. V/c 2] 4

Method • Divide 2 -D p, region into bins • for every bin &

Method • Divide 2 -D p, region into bins • for every bin & every 2 PID hypothesis (only ‚neighbours‘, i. e. : e- / -K / K-p) – plot the 2 distributions – determine mean values i and RMS ri for both hypothesis (e. g. and K) – separation power (number sigmas) is estimated as – colorize a 2 -D map according to n K. Götzen PID TAG Meeting – EVO – 15. 02. 08 5

Example 1 Barrel DIRC K |p-2. 0|<0. 1 [Ge. V] | -2|<0. 2 K

Example 1 Barrel DIRC K |p-2. 0|<0. 1 [Ge. V] | -2|<0. 2 K C K = 0. 7955 r. K = 0. 00288 K. Götzen |p-1. 0|<0. 1 [Ge. V] | -2|<0. 2 Barrel DIRC = 0. 8218 r = 0. 00239 (not really gauss‘sch) C K = 0. 7071 r. K = 0. 01436 PID TAG Meeting – EVO – 15. 02. 08 = 0. 8147 r = 0. 00238 6

Example 2 |p-4. 0|<0. 1 [Ge. V] | -2|<0. 2 Barrel DIRC K |p-0.

Example 2 |p-4. 0|<0. 1 [Ge. V] | -2|<0. 2 Barrel DIRC K |p-0. 3|<0. 1 [Ge. V] | -2|<0. 2 STT K C K = 0. 817 r. K = 0. 00243 K. Götzen = 0. 823 r = 0. 00239 d. E/dx = 4. 02 r = 0. 976 PID TAG Meeting – EVO – 15. 02. 08 K = 12. 94 r. K = 6. 015 7

p [Ge. V] Separation e - mu 6 6 6 5 5 5 4

p [Ge. V] Separation e - mu 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 [deg] p [Ge. V] 0 K. Götzen [deg] 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 [deg] PID TAG Meeting – EVO – 15. 02. 08 [deg] 8

p [Ge. V] Separation mu - pi 6 6 6 5 5 5 4

p [Ge. V] Separation mu - pi 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 p [Ge. V] [deg] K. Götzen [deg] 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 [deg] PID TAG Meeting – EVO – 15. 02. 08 [deg] 9

p [Ge. V] Separation pi - K 6 6 6 5 5 5 4

p [Ge. V] Separation pi - K 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 p [Ge. V] [deg] K. Götzen [deg] 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 [deg] PID TAG Meeting – EVO – 15. 02. 08 [deg] 10

p [Ge. V] Separation K - p 6 6 6 5 5 5 4

p [Ge. V] Separation K - p 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 p [Ge. V] [deg] K. Götzen [deg] 6 6 6 5 5 5 4 4 4 3 3 3 2 2 2 1 1 1 0 0 0 [deg] PID TAG Meeting – EVO – 15. 02. 08 [deg] 11

Overall performance Combined n given by expression Of course, there are still some flaws,

Overall performance Combined n given by expression Of course, there are still some flaws, but this is the preliminary separation power map! K. Götzen PID TAG Meeting – EVO – 15. 02. 08 12

Signal / Background overlap • How does this now apply to our physics cases?

Signal / Background overlap • How does this now apply to our physics cases? • Compare the following: • Evt. Gen: Kaon p- distributions of benchmark channel, e. g. at different pbar momenta (1. 432, 5. 0, 10. 0, 15. 0 Ge. V/c) • DPM Gen: Pion p- distribution at same energies • Determine kinematic overlap regions and look how good separation power is there K. Götzen PID TAG Meeting – EVO – 15. 02. 08 13

p = 5. 0 Ge. V/c p = 1. 432 Ge. V/c ppbar =

p = 5. 0 Ge. V/c p = 1. 432 Ge. V/c ppbar = 1. 432 / 5. 0 Ge. V/c K. Götzen , bkg K, signal product of histo‘s (overlap) PID TAG Meeting – EVO – 15. 02. 08 14

p = 15. 0 Ge. V/c p = 10. 0 Ge. V/c ppbar =

p = 15. 0 Ge. V/c p = 10. 0 Ge. V/c ppbar = 10. 0 / 15. 0 Ge. V/c K. Götzen , bkg K, signal product of histo‘s (overlap) PID TAG Meeting – EVO – 15. 02. 08 15

Combining information K. Götzen PID TAG Meeting – EVO – 15. 02. 08 16

Combining information K. Götzen PID TAG Meeting – EVO – 15. 02. 08 16

Combining information @ 1. 432 Ge. V/c K. Götzen PID TAG Meeting – EVO

Combining information @ 1. 432 Ge. V/c K. Götzen PID TAG Meeting – EVO – 15. 02. 08 17

Combining information @ 15. 0 Ge. V/c K. Götzen PID TAG Meeting – EVO

Combining information @ 15. 0 Ge. V/c K. Götzen PID TAG Meeting – EVO – 15. 02. 08 18

Combining information problem here? @ 15. 0 Ge. V/c K. Götzen PID TAG Meeting

Combining information problem here? @ 15. 0 Ge. V/c K. Götzen PID TAG Meeting – EVO – 15. 02. 08 19

Summary • Task: Recommendation for minimum set of PID detectors • Attempt to determine

Summary • Task: Recommendation for minimum set of PID detectors • Attempt to determine – Separation power p- dependent – Regions, where it‘s acctually needed • Limitations – Information based on parametrizations only – No EMC informations so far – Dsitributions are not gaussian does our definition of sep. power make sense here – Due to finite granularity (bin width) artifacts in the map – Is the estimate for the total n , tot correct? K. Götzen PID TAG Meeting – EVO – 15. 02. 08 20