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Search for New Physics in the ME T Channel at D Ø. Stelios Kesisoglou Alex Melnitchouk for the D Ø collaboration. APS-DPF 2003 Conference, Philadelphia. Gauge-Mediated SUSY. - PowerPoint PPT Presentation
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Search for New Physics in the MET Channel at DØ
Stelios Kesisoglou Alex Melnitchouk
for the DØ collaboration
APS-DPF 2003 Conference, Philadelphia
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
2
An alternative to gravity mediated SUSY: introduce new gauge fields (“messengers”) which propagate SUSY-breaking interactions and couple to ordinary and SUSY particles Phenomenology:
Gravitino is very light (<<MeV) and is LSPNLSP can be a neutralino or a sleptonNLSP lifetime is a free parameter
May yield non-prompt photons in the decay
In case of the neutralino NLSP:Final state always has two photons
Do inclusive search for MET + X
Gauge-Mediated SUSY
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
3
Previous SearchesCDF has found an intriguing event eeMET
In the GMSB framework CDF set lower limit on the neutralino mass at M(0) > 65 GeV
LEP SUSY WG
DØ PRL(80) 1998
eeMET
CDF Run 1
DØ found no high ET
diphoton+MET events and set lower limit on the neutralino mass at M(0) > 75 GeV
LEP2 recently set lower limit on 1
0 ~ 95 GeV
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
4
Data Selection ~40 pb-1 (September 2002 - January 2003) Trigger:
One EM object over the threshold ORTwo EM objects over the (lower) threshold
Off-line: events with two photonsIsolation
Shower shape consistent with photonNo matching tracks|| < 1.1 (since looking for heavy objects)
ET>20 GeV
to be above trigger turn-on: Trigger=0.98±0.02
to be able to rely on EM ID efficiency from Z decays
MET is calculated summing all calorimeter cells and corrected for EM and jet energy scales
0.150.2)(RE
0.2)(RE0.4)(RE
EM
EMTOT
EM ID = 0.85±0.06
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
5
MET Resolution Tails of MET distribution are most important (region of expected signal) Can be caused by mis-measured jets discard events in which ET is collinear with a jet
Red – EM energyRed – EM energyYellow – direction of MEYellow – direction of MET T
Blue – hadronic Blue – hadronic energyenergy
Z+jet event:Both EM have tracksMass consistent with Z
MET has the same azimuthal angle as the jet!
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
6
Backgrounds without true MET
QCD: , +j, j+j (jet is “faking” ) Drell-Yan (lost tracks)
with true MET (from )
W e & Wj ej (lost track, fake )
Z ee +X ( lost tracks )tt ee + X ( lost tracks )WW, WZ, …
Largest backgrounds
if a jet ”fakes” an isolated EM object, it’s mainly because it’s fragmented into a leading 0 and therefore its energy resolution is similar to the EM energy resolution MET resolution is similar for
, +jet, e+jet, ee, etc…
0
Quark or
gluon
hadrons
(leading particle)
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
7
Predicting Backgrounds QCD (, +j, j+j)
require at least one of the isolated EM clusters to fail the shower shape cut “QCD Sample”Assume that events in the sample with small MET are dominated by QCD use MET<20 GeV region for normalizing QCD sample
W e & Wj ej require exactly one cluster to have a track match subtract QCD contribution multiply by (1-track)/track
MET>25 >30 >35 data 3 1 0
QCD contribution 6.0 ± 0.8 2.5 ± 0.5 1.6 ± 0.4e,ej contribution
0.6 ± 0.4 0.2 ± 0.2 0.0 ± 0.2
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
8
Signal Efficiency
MET, GeV
QCD
MET, GeV
Run 2 preliminary
, TeV
, pb
Acceptance, %
ET>25
ET>30
ET>35
35 10.3 4.6 3.8 2.7
40 4.06 8.3 6.9 5.5
45 2.07 12.1 10.8 9.0
50 1.17 15.1 13.7 12.3
55 0.70 16.8 15.3 14.0
60 0.45 18.6 17.4 16.3
= 55 TeV = 45 TeV = 35 TeV
/ / /
A
AIDEMvtxtrigSUSY
09.066.0
2
Snowmass Slope E: mGMSB()
M=2; Nmess=1; tan=15; >0
( )
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
9
Upper Limit Calculation Bayesian approach
Cut on MET should depend on - for now 30 GeV is conservative
95% CL90% CL
95% CL limit
>25 >30 >35
35 10.3 3.82 3.87 4.36
40 4.06 2.11 2.12 2.14
45 2.07 1.45 1.36 1.30
50 1.17 1.16 1.07 0.95
55 0.70 1.04 0.95 0.84
60 0.45 0.94 0.85 0.72CLGeVm
CLTeV
%95@66
%95@51
01
theory
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
10
Prospects for Diphotons
Prompt decays:m(1
+) discovery up to 300 GeV with 2 fb-1
J. Qian, hep-ph/9903548
Similar model to Snowmass Slope, but tg = 2.5
Non-prompt decays:Sensitivity drops as NLSP leaves the detectorIn the limit of large lifetime we are back to jets+METIntermediate lifetime – ask for one photon plus jets plus MET
R calo
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
11
A search for the Gauge-Mediated SUSY signal was carried out in the inclusive MET + X channelMET distribution is well understood and does not have significant non-Gaussian tailsObserved MET data are in good agreement with the Standard Model predictions With 40 pb-1 neutralino mass limit has been set at 66 GeV (sensitivity approaches that in Run I) More data are being accumulated Search for non-prompt photons is underwayStay tuned - new results will be coming soon
Conclusions
Stelios Kesisoglou, Alex Melnitchouk APS-DPF
conference 2003
12
5/20/2002 6
Photon PointingPreshowers give a very precise
position measurement – fit shower axis!
ZEMVTX
EM ShowerEM4EM3EM2EM1
Central Calorimeter
EndCalorimeterSolenoid
Central Fiber Tracker
Central: R = 1.4 cm Z = 2.2 cmForward: R = 1.2 cm Z = 2.8 cm
Preshowers are still in commissioning –pointing not used now. MC estimates are
Photon Pointing
Use calorimeter and preshower detectors to reconstruct displaced vertices in MET
events