Kaneda 31May2007 1 Data Evgen from grid mc

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Kaneda 31/May/2007 1

Kaneda 31/May/2007 1

Data Evgen: from grid mc 12. 005640. Charybdis. Jimmy. evgen. EVNT. v 12000501_tid 005290

Data Evgen: from grid mc 12. 005640. Charybdis. Jimmy. evgen. EVNT. v 12000501_tid 005290 Simulation+digit: 12. 0. 6. 1, recon: 12. 0. 6. 5 ~20 k events (0. 5 fb-1) 005640 "charyb 2 6", # total number of dimensions"charyb 3 5000", # minimum mass "charyb 4 14000", # maximum mass "charyb 5 2", # number of partiles in remant decay "charyb 6 1", # time variation of temperature "charyb 7 1", # grey body factors "charyb 8 1" # kinematic limit 2

Leading Jet (Cone 4 Tower) 1 st 2 nd Fast Full Pt(Ge. V) 3

Leading Jet (Cone 4 Tower) 1 st 2 nd Fast Full Pt(Ge. V) 3 rd Pt(Ge. V) 4 th Pt(Ge. V) normalized to 1 fb-1 3

Fast (11. 0. 5) (use correction) Arbitrary unit Leading jet Full (12. 0. 6)

Fast (11. 0. 5) (use correction) Arbitrary unit Leading jet Full (12. 0. 6) 1 st 1 fb-1 Full (log scale) Fast 12. 0. 6(no correction? ) Full 12. 0. 6 Pt(Ge. V) 4

Leading Ele, Muo, Pho and Miss. Et Muo Ele Fast Full shoud improve selection?

Leading Ele, Muo, Pho and Miss. Et Muo Ele Fast Full shoud improve selection? Pt(Ge. V) Missing Et Pho Pt(Ge. V) normalized to 1 fb-1 Pt(Ge. V) 5

Blackhole Mass remaiingn events(1 fb-1) Fast: 13201 Full: 10238 remaiingn events(1 fb-1) Fast: 36006

Blackhole Mass remaiingn events(1 fb-1) Fast: 13201 Full: 10238 remaiingn events(1 fb-1) Fast: 36006 Full: 36915 MBH(Ge. V) this difference comes from lepton Cut Selection A: High Pt(>200 Ge. V) >3 High Pt Lepton(e or m) > 1 Selection B: High Pt Jets(>500, 400, 300 Ge. V) BH reco: using e, m and g Pt>10 Ge. V, |h|<2. 5 jet(including tau)Pt>20 Ge. V, |h|<2. 5 normalized to 1 fb-1 6

Background: J 1 -J 7 signal remaiingn events(1 fb-1) Fast: 13201 Full: 10238 remaiingn

Background: J 1 -J 7 signal remaiingn events(1 fb-1) Fast: 13201 Full: 10238 remaiingn events(1 fb-1) selection A J samples remaiingn events(1 fb-1) Fast: 0 Full: 32 Fast: 36006 Full: 36915 selection B J samples remaiingn events(1 fb-1) Fast: 64767 Full: 61125 7

Trigger events passed selection A(Signal) events passed loose selection(Signal): Jet(Pt>200 Ge. V) > 2

Trigger events passed selection A(Signal) events passed loose selection(Signal): Jet(Pt>200 Ge. V) > 2 (39428 event from 40000 events remain) each trigger name All J samples are also passed trigger such a Jet 160 8

Triggers for Black Holes ØPrevailing wisdom is the Black Holes easily pass triggers, esp.

Triggers for Black Holes ØPrevailing wisdom is the Black Holes easily pass triggers, esp. jet ones ØA preliminary look at trigger efficiencies for BH: L 1 L 2 EF Jet 160 100 100 2 jet 120 - - 99. 96 3 jet 65 99. 97 99. 89 99. 84 4 jet 50 99. 71 99. 53 99. 44 e 60 100 (EM 60) 49. 6 28. 85 g 60 100 (EM 60) 63. 7 41. 28 mu 20 i - 45. 36 40. 75 met 99. 55 (XE 50) 100 (met 10) ØBlack Holes do pass jet triggers – could “AND” all the jet triggers ØElectron/muon/gamma triggers less efficient – search for these at analysis level ØDo we need a dedicated/higher energy jet trigger? James Frost – Cambridge ATLAS 9 CSC BH Note Meeting

Multi Jets (m 1000 sample) Mass(Ge. V)(vector sum of truth particles: hard scatter(from alpgen))

Multi Jets (m 1000 sample) Mass(Ge. V)(vector sum of truth particles: hard scatter(from alpgen)) 10

check 1 Te. V-2 Te. V (loose cut) truth mass after selection MBH(Ge. V)

check 1 Te. V-2 Te. V (loose cut) truth mass after selection MBH(Ge. V) loose selection Jet(Pt>200 Ge. V) > 2 ATLFAST require MBH(ATLFAST)>3 Te. V 11

check 1 Te. V-2 Te. V truth mass after selection MBH(Ge. V) Selection B

check 1 Te. V-2 Te. V truth mass after selection MBH(Ge. V) Selection B (no events are remaining after Selection A) ATLFAST require MBH(ATLFAST)>3 Te. V 12

Atlfast Jet Eta Phi ? ? ? ? ? 13

Atlfast Jet Eta Phi ? ? ? ? ? 13