christian autermann susy06 1 search for iii. phys. inst. a ... · christian autermann susy06 2...
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Christian Autermann SUSY06
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Search for RPV SUSY
Search for R-parity violating Supersymmetrywith the DØ Detector
Christian Autermann on behalf of the DØ Collaboration
Introduction to R-parity violating SUSYThree DØ searches for Rp Supersymmetry: 1. Short lived LSP in three-lepton final states2. Long lived LSP in di-muon final states3. Resonant second generation slepton production
Supported by:
III. Phys. Inst. A
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Christian Autermann SUSY06
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Search for RPV SUSY
The DØ Experiment at the Tevatron Collider
Run IIa (~1 fb-1 recorded)
Current results (~0.4 fb-1 recorded)
Muon systemToroidSolenoid
PDT’s
Liquid Argon Calorimeter
Silicon and Scintillating Fiber Tracker
pp-collider
√s = 1.96 TeV
__
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Christian Autermann SUSY06
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Search for RPV SUSY
R-Parity Violation Supersymmetry
kjiijkkjiijkkjiijkR
RMSSM
DDUDQLELLW
WWW
P
P
'''
21 λλλ ++=
+=
/
/
• Lepton number violation, ∆L=1• 27 λ’ couplings
S is the particle spin, B is the baryon number, L is the lepton number
i,j,k = 1,2,3 generation indices
R-parity violating extension of the MSSM
Chiral superfields:L: lepton doublet superfieldE: lepton singlet superfieldQ: quark doublet superfieldD: down-like quark singletλ, λ`, λ``: Yukawa couplings
• Lepton number violation, ∆L=1• Gauge symmetry enforces λijk = – λjik→ 9 λ couplings
Only one coupling is assumed to be non-zero at a time! (Stringent limits, i.e. from proton decay)
LSP no candidate for dark matter in RPV models
SLBPR
23)1( :parity-R ++−=
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Christian Autermann SUSY06
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Search for RPV SUSY
Sparticle Production at the TevatronSearch for LLE couplings• pair/associated gaugino production• production is R-parity conserving
• Each χ → 3 leptons (2 charged & 1 neutrino) via RPV01
Search for LQD coupling• R-parity violating production• s-channel: enhanced cross section• cross section σ ∝ (λ’)• Only one gaugino
• χ → 1 lepton + 2 jets via RPV
2
01
LQD_
(LLE)_
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Christian Autermann SUSY06
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Search for RPV SUSY
• Require prompt decay of χ → λ > ~ 0.01• χ is assumed to be the LSP
• Final state: 4 charged leptons & 2 neutrinos from one vertex• Analyses require 3 leptons and missing transverse energy• Three different LLE couplings are probed: λ121, λ122, λ133
01
χ → l+ l- ν01
01
Pair/associated production (LLE, prompt decay)
LLE_
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Christian Autermann SUSY06
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Search for RPV SUSY
Pair/associated production (LLE, prompt decay)Sample: 2 µ with Zo-veto
50×Signal
ττ, µµ ee, →*γ/0Z
QCD (from data)
WW, WZ, ZZ
ll+X → tt
Data
[GeV]TE0 50 100 150 200
Even
ts /
5 Ge
V
0
20
40
60
80DØ, 360 pb-1
DØ, 360 pb-1
Signal scaled by factor 50mSUGRA point:m0=1 TeV, m1/2=280 GeVtanβ=5, µ>0, A0=0
50×Signal
µµ ee, →*γ/0Z
ττ → *γ/0Z
QCD (from data)
WW, WZ, ZZ
ll+X → ttData
[GeV]eeM0 50 100 150 200
Eve
nts
/ 1
GeV
-110
1
10
210
310DØ, 360 pb-1DØ, 360 pb-1
Sample: 2 e
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
210
310
+ jet OS dataµ
+ jet LS dataµ
νµW
DØ, 360 pb-1
µµ,→
→
*
*
γ
γ
/
/
0
0
Z
Z
→
→
*
*
γ
γ
/
/
0
0
Z
Z ττ
→
→
*
*
γ
γ
/
/
0
0
Z
Z
NN output
Eve
nts
/ 0.0
5
→→
→
*
*
γ/0Z →*γ/0Z →*γ/0Z →*γ/0Z
γ/0Z →*γ/0Z →*γ/0Z →*γ/0Z
Signal
τ Identification: Neural NetDØ, 360 pb-1
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Christian Autermann SUSY06
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Search for RPV SUSY
Pair/associated production (LLE, prompt decay)
1st analysis eee or eeµ
electron pT>20 GeVelectron pT>20 GeVelectron or muon
pT>10 GeV
missing ET > 15 GeV
found events 0expected SM 0.9+0.4
-0.1±0.1
Combination of all three analyses into limits on the three channels
λ121 λ122 λ133
2nd analysis µµµ or µµe
muon pT>15 GeVmuon pT> 8 GeVmuon or electron pT>4 GeV pT>5 GeV
missing ET > 10 GeV
sum lepton pT>50 GeVadditional 2D cut (Mµµ, ET)
found events 0expected SM 0.4±0.1±0.1
3rd analysis eeτ
electron pT>10 GeVelectron pT>10 GeVtau neural net identification
pT>10 GeV
remove Z-peak Mµµ>80 GeVET/√ST>1.5 GeV1/2
found events 0expected SM 1.3±1.7±0.5
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Christian Autermann SUSY06
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Search for RPV SUSY
Pair/associated production (LLE, prompt decay)
150 200 250 300 (SUSY) NLOσ
expected limits observed121λ observed122λ observed133λ
60 80 100 120 140 160
[pb]
95%
CL
σ, N
LOσ
-110
1
DØ, 360 pb-1
=1 TeV0m>0µ=0, 0 =5, Aβtan -210×2
2
[GeV]1χ∼M ±
[GeV]1χ∼M 0
Exclusion domains121λ obs.
122λ obs.
133λ obs.
121λ exp.
122λ exp.
133λ exp. LEP excluded
1χ∼ ± is LSP
0
±
[GeV]1χ∼M 20 60 100 140 180 220
[GeV
]1χ∼
M
100
140
180
220
260DØ, 360 pb-1
Lower limits on χ (χ )up to 119 GeV (234 GeV)
01
±1
Interpretation within the
χ – χ mass plane01
±1
DØ,
DØ,
Accepted by Physics Letters B
mSUGRA no GUT MSSM (no relation between M1 and M2)
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Christian Autermann SUSY06
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Search for RPV SUSY
Search for neutral long lived particles (LLE)
Selection criteria: Two muons with pT > 10 GeVRequire only observation of one neutralino decay.
Pair production Decay
Specific analysis for very small λ122 coupling:→ Long lifetime of the neutralino, c·τ = O(cm), mass = O(GeV)
M1=3,5,8,10 GeV, M2=200 GeV, M3=400 GeVtanβ=10, µ=-5000, λ122<1.0Mbt=1.5 TeV, Mq=300 GeV~~ ~
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Christian Autermann SUSY06
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Search for RPV SUSY
Search for neutral long lived particles (LLE)
01
MC
Result0 data events found0.8 ± 1.1 ± 1.1 SM
events expected
Long lifetime of the neutralino leads to displaced vertex5 cm < (decay radius) < 20 cm
(χ lifetime determined by λ122)01
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Christian Autermann SUSY06
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Search for RPV SUSY
Search for neutral long lived particles (LLE)
http://www-d0.fnal.gov/Run2Physics/WWW/results/np.htm
Inspired by 3 unexpected NuTeV di-muon events
380 pb-1
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Christian Autermann SUSY06
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Search for RPV SUSY
Resonant Slepton Production via LQD
Final state: 2-muon & 2-jetThree dominant signal channels:
µχµ 01
~~→ µχµ 02
~~→ µχνµ±→ 1
~~
1. 2. 3.
→ Each channel analyzed separately→ Possible to reconstruct neutralino & slepton mass
→ Cross section limits for every channel→ Combination within mSUGRA
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Christian Autermann SUSY06
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Search for RPV SUSY
Resonant Slepton Production via LQD
m( l ) = 260 GeVm( χ ) = 100 GeV
~~
Signal reference point :
Results for this point:data SM expectation
The final selection and the results for each point depend on the neutralino and slepton masses of the point under study.
Reconstructed slepton candidate mass:
SM uncertainty
µχµ 01
~~→µχµ 0
4,3,2~~→
µχνµ±→ 2,1
~~
14 11.9±2.1±1.6
28 25.4±3.2±5.4
8 6.5±1.6±1.6
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Christian Autermann SUSY06
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Search for RPV SUSY
Resonant Slepton Production via LQD
Cross section limitInterpretation within mSUGRA(tanβ=5, µ<0, A0=0)
µχµ 01
~~→
e.g.: Exclude m( l ) < 358 GeV for λ’211=0.09DØ Run I excluded m( l ) < 280 GeV for λ’211=0.09 and m( χ )=200 GeV
Submitted to Physical Review Letters
~~ ~0
1
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Search for RPV SUSY
Conclusion
• DØ searches for R-parity violating SUSY:LLE: Pair/associated gaugino production in
tri-lepton final states (arxiv:hep-ex/0605005)
LLE: Neutral long lived particles indi-muon final states
LQD: Resonant slepton production indi-muon di-jet final states (arxiv:hep-ex/0605010)
• No excess found in the data
• Very stringent limits were set
• More than twice as much data is already recorded,new data will come in
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Search for RPV SUSY
backup
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Search for RPV SUSY
mSUGRA parameter space
tanβ=5µ<0A0=0