ftk studies: h hh bbbb ftk physics case meeting 11/03/05 erik brubaker university of chicago

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FTK Studies: Hhhbbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

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Page 1: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

FTK Studies: Hhhbbbb

FTK Physics Case Meeting

11/03/05

Erik Brubaker

University of Chicago

Page 2: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 2

Organization• Web page here: http

://hep.uchicago.edu/~brubaker/ftk/– Links to previous meetings– Mailing list– Information about tools, e.g. L1 response

parameterizations– Analysis code snippets, e.g. jet trigger combinatorics– Collect useful plots, results

Page 3: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 3

Topics• Hhhbbbb process, signal sample

• SHERPA multijet background sample

• Some event rates

• Next steps

Page 4: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 4

Reminder: Strategy• Making the physics case for FTK means studying

signal and background trigger rates for several processes.

• For now, quantify improvements as a function of increase in L1 rate.– In parallel, studies of FTK speed and efficiency will tell

us the magnitude of that increase.

• Use fully simulated events to parameterize the L1 jet and tau trigger response vs ATLFAST jet pT. Then various processes for physics studies can be studied using ATLFAST.

Page 5: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 5

Response parameterization• Functional form:

tried & true double Gaussian.– No pathological

behaviors– Second Gaussian

can take care of high tails (?)

• Can be modified & improved as needed.

Page 6: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 6

Double Higgs—Process• Resonant production of

lightest MSSM neutral scalar Higgs h0 through the heavier H0.

• Previous study (ATL-PHYS-97-104)– For MH=300 GeV and tan(=3, S/sqrt(B) of 5.7 can

be reached using 300 fb-1; this requires 4 jets with ET>40 GeV and ||<2.5.

– For lower integrated luminosity, more tricks are needed and jets down to 20 GeV are preferred.

– They concluded trigger rates probably prohibitive.

Page 7: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 7

Signal Sample• Contrary to last time’s claim, one can use Pythia

for resonant Hhh production.– mH = 300 GeV

– mh = 130 GeV

– Pythia reports = 2 fb• Not sure I’m working in a consistent MSSM world.

• Earlier studies used low tan (so lower mh), and ≈ 2 pb.

• Generated 10M events, so far only fast simulation.

• Should check sensitivity to mH, mh.

Page 8: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 8

Signal sample• Quite low jet pT,

especially for j4.

• Probably want multiple trigger thresholds.

Page 9: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 9

SHERPA event generator• Many of our processes have backgrounds with

four jets in the final state.– Want accurate ME description of kinematics.

• SHERPA: developed by Dresden group.– http://www.physik.tu-dresden.de/~krauss/hep/

• Generator of generators, like CompHEP etc.• Handles consistently boundary between matrix

element and parton shower emissions.• Produces unweighted events.• Not widely used, tested in ATLAS.

Page 10: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 10

SHERPA multijet sample• Unexpected distributions

of njet, jet pT.

• Expected higher <njet> for higher-order ME—opposite is true.

• PS/ME boundary is set to 50 GeV.

Page 11: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 11

SHERPA multijet sample• No obvious “turn-on” of add’l jets from ME.

Page 12: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 12

Signal & Background L1 rates• Use fast simulated signal & SHERPA samples.

– Want Pythia dijets too, but these are more complicated.

• Require at least 4 ATLFAST jets inside ||<2.8.• Find the probability for the event to have four jets

passing a 40 (60, 80, 100) GeV trigger.– Want multiple trigger thresholds as well, but that is more

complicated.

Page 13: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 13

Beginnings of an L1 rate tableSample Signal Pyth dijet SHERPA

x-section 2 pb 24.6 ub

N Events 110k 10k

Eff,#/fb-1

40 5.8%,116 0.17%, 42M

60 1.7%, 34 0.049%, 12M

80 0.64%, 13 0.022%, 5.4M

100 0.29%, 6 0.012%, 3M

Page 14: FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago

Nov 3, 2005 FTK Physics Case Meeting 14

Next steps• Get full simulation of Hhh4b.

– Check that L1 response param. matches observed rate– Work out analysis more thoroughly—need to

determine improvement from FTK relative to some “state of the art”.

• Generate large SHERPA multijet sample.

• What other background samples are needed?

• Revisit L1 response—improve as needed.