searches for promptly decaying squarks and gluinos with atlas · searches for promptly decaying...
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Searches for promptly decaying squarks and gluinoswith ATLAS
J. Maurer, on behalf of the ATLAS Collaboration
SUSY2019 conference, May 20, 2019
ATLAS search program for gluinos / squarks
Signature Published in Luminosity
0` + 2-6jq
qp
p
χ01
q
χ01
q
PRD 97 (2018) 112001 36 fb−1
0` + 7-11jg
g
χ± χ02
χ∓ χ02
p
p
q q′ W±
Z
χ01
q′q W∓Z
χ01
JHEP 12 (2017) 034 36 fb−1
≥ 3bg
g
t
t
p
p
t
χ01
t
t
χ01
t
ATLAS-CONF-2018-041 80 fb−1
1` + jetsq
q
χ±1χ∓1
p
p
q′
χ01
W±
q′
χ01
W∓
PRD 96 (2017) 112010 36 fb−1
SFOS 2`q
q
χ02
χ02
p
p
q
χ01
Z
q
χ01
Z
EPJC 78 (2018) 625 36 fb−1
SS/3`b
b
χ±1
χ∓1
p
p
t
χ01
W
t
χ01
W
NEW! 139 fb−1
γ + jetsg
g
χ01
χ01
p
p
q q
G
γ
G
γ
PRD 97 (2018) 092006 36 fb−1
τ + jetsg
g
χ±1
τ
χ01 τ
p
p
q q ντ
τ
G
qq τ
τ
GPRD 99 (2019) 012009 36 fb−1
+ dedicated searches for b/t production, and g/q decays via RPV couplings
ATLAS strong production searches 2 / 16
Overall experimental sensitivity
1000 1200 1400 1600 1800 2000 2200 2400
) [GeV]g~m(
500
1000
1500
2000
2500
3000
3500
) [G
eV]
0 1χ∼m
(
0 lep. [1712.02332] 0
1χ∼q q→g~
3 b-jets [CONF-2018-041]≥ 0
1χ∼b b→g~
2 lep. SS [CONF-2018-041, 1706.03731]≥ 3 b-jets + ≥ 0
1χ∼t t→g~
0 lep. + 1 lep. [1712.02332, 1708.08232] 0
1χ∼Wq q→g~
2 lep. SS ≥ 7-11 jets + 1 lep. + ≥ 0
1χ∼WZq q→g~
[1708.02794, 1708.08232, 1706.03731]
3 lep. [1805.11381, 1706.03731]≥2 lep. OS SF + ν∼/l~ via 0
1χ∼)νν(ll/q q→g~
[1808.06358]τ 1 ≥ ν∼/τ∼ via 0
1χ∼)νν/ντ/ττ(q q→g~
[1802.03158]γ 1 ≥ 0
1χ∼ via G
~/Z)γ(q q→g~
ATLAS Preliminary
-1=13 TeV, 36.1 - 79.8 fbs
All limits at 95% CL
September 2018
)0
1χ∼)<m(
g~m(
) [GeV]q~m(
400 600 800 1000 1200 1400 1600 1800 2000
) [G
eV]
0 1χ∼m
(
500
1000
1500
2000
25000 lep. + mono-jet [1712.02332, 1711.03301] 0
1χ∼ q→ q~
0 lep. + 1 lep. [1712.02332, 1708.08232] 0
1χ∼ qW→
Lq~
[1802.03158]γ 2 ≥ 0
1χ∼ via G
~/Z)γ q(→ t~, b
~, q~
2 lep. SS≥ 7-11 jets + ≥ 0
1χ∼ qWZ→
Lq~
2 lep.≥ ν∼/l~ via 0
1χ∼)νν/ν q(ll/l→
Lq~
τ 1 ≥ ν∼/τ∼ via 0
1χ∼)νν/ντ/ττ q(→
Lq~
ATLAS Preliminary
-1=8-13 TeV, 20.3-36.1 fbs
All limits at 95% CL
c~, s~, d~
, u~ = q~
March 2018
8 TeV,[1507.05525]
)0
1χ∼)<m(
q~m(
Building block for searches: reconstructed jets + leptons + photons + EmissT , with good
resolution + rejection of misclassified objects + resilience to pile-up
ATLAS strong production searches 3 / 16
Missing transverse momentum
0 5 10 15 20 25 30 35 40
⟩µ⟨Average number of interactions
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=0.0η|=2.0η|
Electrons=0.0η|=2.0η|
γN.C. =0.0η|=2.0η|
τHadr. 1p0n3pXn
Good resolution, but non-gaussian tails.
SUSY searches: when dominant bkg for thesignature has no genuine Emiss
T (0`, γ, 2`):adding min ∆φ(Emiss
T , j) requirement
1
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Da
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CONF-2018-023, CONF-2018-038,CONF-2018-041, EPJC 78 (2018) 625
ATLAS strong production searches 4 / 16
Electrons, muons
10 20 30 40 50 60 70 80
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PreliminaryATLAS-1 = 13 TeV, 43.6 fbs
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[GeV]Tp
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µµZ
ID e
ffici
ency
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0.95
1
ATLAS Preliminary-1 = 13 TeV, 43.8 fbs
<2.47η-2.47<
Data: full, MC: open
Loose Medium Tight
[GeV]TE
20 40 60 80 100 120 140
Dat
a / M
C
0.85
0.9
0.95
1
1.05
EGAM-2018-006, EGAM-2018-002,EPJC 76 (2016) 292
ATLAS strong production searches 5 / 16
Taus, photons
[GeV] had-visτT
truth p
50 100 150 200 250 300 350 400 450 500
effic
ienc
y
0
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1
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Reco+Tight Tight truth 3-prong = 13 TeVs
SimulationPreliminaryATLASReco+Loose Loose
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Eve
nts
/ 3 G
eV
0.20.40.60.8
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-1 = 13 TeV, 3.2 fbs
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) [GeV]had
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Dat
a/P
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0.51
1.5
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0.6
0.7
0.8
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1.1
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γUnconverted
FixedCutLoose isolation
< 40 GeVT20 GeV < E < 2.37η < 1.37, 1.52 < η
ATLAS Preliminary-1=13 TeV, 44 fbs
10 20 30 40 50 60 70µ
0.90.95
11.05
1.1
MC
ε/D
ata
ε
SUSY searches:
0 200 400 600 800 1000 1200
Eve
nts
/ 5
0 G
eV
1
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210
310
410DataTop Quarks
ντ →W νν →Z ττ →Z
VVOther
totσ1±SM
LMg~g~
MMg~g~
HMg~g~
GMSB
ATLAS 1 = 13 TeV, 36.1 fbs
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[GeV]2τT
+m1τTm
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Data
/SM
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/ 250
GeV
2−10
1−10
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1 χ∼m
= 8000 1 χ∼ = 1000, m0
2 χ∼, ±
1 χ∼m
ATLAS-1 = 13 TeV, 36.1 fbs
pre-selectionγγ
[GeV]TH0 1000 2000 3000 4000 5000 6000 7000
Dat
a / S
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CONF-2017-029, PUB-2015-045, PRD 96 (2017) 112010, PRD 97 (2018) 092006
ATLAS strong production searches 6 / 16
Jets: energy scale / resolution
[GeV]jet
Tp
20 30 210 210×2 310 310×2
M
CR
/ da
taR
0.8
0.85
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0.95
1
1.05
1.1
1.15ATLAS Preliminary
-1 = 13 TeV, 80 fbs = 0.4 (EM+JES)R tkAnti-
+jetγ + jetee → Z + jetµµ → Z
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[GeV]jet
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EM+JES total uncertainty
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PFlow+JES total uncertainty
= 0.4R tkanti-| < 0.7η |≤0.2
ATLAS Preliminary-1 = 13 TeV, 43.6 fbs
JETM-2018-006, JETM-2018-006,CONF-2018-041, JHEP 12 (2017) 034
SUSY searches: impact on EmissT resolution,
low-pT jets, calibration of reclustered jets. . .
Eve
nts
/ 10
GeV
1−10
1
10
210
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-1 = 13 TeV, 36.1 fbs
ATLAS
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Dat
a / S
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2
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510
Eve
nts
/ 25
GeV
ATLAS Preliminary-1 = 13 TeV, 79.8 fbs
1L Preselection
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Single top + Xtt
Z+jetsW+jetsDiboson
) = 1900, 1 (x50)1
0χ∼), m(g~Gtt: m(
) = 1800, 1000 (x50)1
0χ∼), m(g~Gtb: m(
0 50 100 150 200 250 300 350 400 450 500 [GeV]Σ
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1
1.5
Dat
a/S
M
With reweightingWithout reweighting
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Num
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vent
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2−10
1−10
1
10
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410
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610 1− = 13 TeV, 36.1 fbsSR-11j50-0b
ATLAS DataTotal backgroundMultijet
ql, ll→ tt + jetsν l→W
OtherpMSSM benchmark2-step benchmark
]1/2 [GeVTH / missTE
0 2 4 6 8 10 12 14 16 18
Dat
a / P
red.
00.5
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2
ATLAS strong production searches 7 / 16
Jets: flavour tagging, pile-up mitigation
Run 2 ≈ 1 interaction per mm
[GeV]T
track p1 10 210
) [m
m]
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0.1
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ATLAS = 13 TeVs
Preliminary
[GeV]T
track p1 10 210D
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7
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SUSY searches: thanks to flavour taggingand pile-up mitigation discriminants,challenging signatures with largemultiplicities can be looked into:
1
10
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410
510
610
Eve
nts
ATLAS Preliminary-1 = 13 TeV, 79.8 fbs
0L Preselection
DataTotal backgroundtt
Single top + Xtt
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) = 1900, 1 (x50)1
0χ∼), m(g~Gtt: m(
) = 1900, 1400 (x50)1
0χ∼), m(g~Gbb: m(
3 4 5 6Number of b-jets
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1.5
Dat
a/S
M
Num
ber
of E
vent
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200
1− = 13 TeV, 36.1 fbsCRW-7j50
ATLAS Data
Total background ql, ll→ tt
+ jetsν l→W Other
pMSSM benchmark
2-step benchmark
Number of Jets6 7 8 9 10 11 12 13 14
Dat
a / P
red.
00.5
11.5
2
CONF-2018-045, IDTR-2018-008,CONF-2018-041, JHEP 12 (2017) 034
ATLAS strong production searches 8 / 16
SS/3L + jets [ATLAS-CONF-2019-015]
First look at the full Run 2 dataset (139 fb−1) with this signature
Relies on ‘basic’ objects: isolated leptons, (b-tagged) jets, EmissT
benefits from the work done in the performance groups
Data acquisition: dilepton triggers + EmissT trigger (for Emiss
T > 250 GeV)
Five complementary signal regions for a coarse scan of the phase space:
SR n` nb nj met [GeV] meff [GeV] EmissT /meff SUSY
Rpv2L ≥ 2 (`±`±) ≥ 0 ≥ 6 (pT > 40 GeV) − > 2600 − g → ttχ01, χ
01 → 3q (λ′′ 6= 0)
g → qqχ01, χ
01 → qq′` (λ′ 6= 0)
g → tt∗1 , t∗1 → qq′ (λ′′ 6= 0)
Rpc2L1b ≥ 2 (`±`±) ≥ 1 ≥ 6 (pT > 40 GeV) − − > 0.25 b1 → tW χ01
Rpc2L2b ≥ 2 (`±`±) ≥ 2 ≥6 (pT > 25 GeV) > 300 > 1400 > 0.14 b1 → tW χ01
g → ttχ01
Rpc2L0b ≥ 2 (`±`±) = 0 ≥ 6 (pT > 40 GeV) > 200 > 1000 > 0.2 g → qq′WZ χ01
Rpc3LSS1b ≥ 3 (`±`±`±) ≥ 1 no cut but veto 81 < me±e± < 101 GeV > 0.14 t1 → tW±(W ∗)χ01
g
g
t
t
p
p
t
λ′′313b
d
t
b
d
b
b
χ±1
χ∓1
p
p
t
χ01
W
t
χ01
W
∗
g
g
χ±1
χ02
χ±1 χ0
2
p
p
q q W
Z
χ01
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Z
χ01
t1
t1
χ02χ±1
χ02 χ±
1
p
p
t W
W ∗
χ01
t W∓W ∗
χ01
∗
ATLAS strong production searches 9 / 16
SS/3L: prompt same-sign lepton backgrounds
WZ+jets in regions with no b-jet, ttV in regions with b-jet(s)
+ various processes with multiple t/W /Z/H: summed contribution important!
Estimated with MC simulations normalized to σ(theory)
b
b
b
b
bATLAS,√
s = 13 TeV, 3.2 fb–1b
PowhegBox+Py8Sherpa v2.2PowhegBox+HerwigMC@NLO+Herwig
1
10 1
W±Z → ℓνℓℓ fid. cross section as a function of the jet multiplicity
σfid.[fb
]
0 1 2 3 ≥ 40
0.20.40.60.8
11.21.41.6
Njets
MC
/Dat
a
Arb
itrar
y U
nits
0
0.05
0.1
0.15
0.2
0.25 Simulation PreliminaryATLAS
= 13 TeVs
nominal
0µ = 2.0 µ
0µ = 0.5 µ
[GeV] eff M0 500 1000 1500 2000 2500 3000
Rat
io0.5
1
1.5
PUB-2017-005, PUB-2016-005
Uncertainties: QCD scales, matching, parton shower. . . up to 20% of total SM yield
Validation regions for WZ + 4/5 jets, and ttV
(future) challenge: how to address unknown correlations of theory uncertainties?
ATLAS strong production searches 10 / 16
SS/3L: reducible backgrounds
Fake / non-prompt leptons: estimated withmatrix method based on isolation + impactparameter + electron identification
Cha
rge
mis
iden
tific
atio
n pr
obab
ility
3−10
2−10
1−10εData misidentification probability
Tight + Fix (Tight) Medium + Fix (Tight) Medium + Fix (Tight) + BDT
ATLAS-1 = 13 TeV, 33.9 fbs
[GeV]TE
50 100 150 200 250
Dat
a / M
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Charge-flip electrons rejected with dedicateddiscriminant based on track properties,residual contribution estimated by weightingOS data by the flip rate
0
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Eve
nts
DataTotal uncertaintyFake / non-promptWZ
ZttWW, ZZ, VH, VVV
WttVV, 3t, 4ttH, ttt(W)Z, t
Charge-flip
ATLAS Preliminary-1=13 TeV, 139 fbs
> 50 GeVmiss
T2j, E≥, ±l±l
2 3 4 5 > 25 GeV)
TNumber of jets (p
0.51
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a / S
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GeV Data
Total uncertaintyFake / non-promptWZ
ZttWW, ZZ, VH, VVV
WttVV, 3t, 4ttH, ttt(W)Z, t
Charge-flip
ATLAS Preliminary-1=13 TeV, 139 fbs
> 50 GeVmiss
T2j, E≥, ±l±l
60 80 100 120 140 160 180 200 220 240
[GeV]missTE
0.51
1.5
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a / S
M 0
left figures from arXiv:1902.04655ATLAS strong production searches 11 / 16
SS/3L: results
0
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Eve
nts
DataFake / non-prompt
ZttVV, 3t, 4ttH, ttt(W)Z, t
Charge-flip
Total uncertaintyWZ
WttWW, ZZ, VH, VVV
ATLAS Preliminary-1=13 TeV, 139 fbs
> 50 GeVmiss
T3j, E≥
ee, 0b ee, 1b 2b≥ee, , 0bµe , 1bµe 2b≥, µe , 0bµµ , 1bµµ 2b≥, µµ 3l, 0b≥ 3l, 1b≥ 2b≥3l, ≥
0.51
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Charge-flip VV, 3t, 4ttH, ttt(W)Z, t Ztt
Wtt WZ WW, ZZ, VH, VVV
ATLAS Preliminary-1 = 13 TeV, 139 fbs
VRttV VRWZ4j VRWZ5j Rpc2L0b Rpc2L1b Rpc2L2b Rpc3LSS1b Rpv2L
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ATLAS strong production searches 12 / 16
SS/3L: exclusion limits for simplified models (1)
1000 1200 1400 1600 1800 2000 2200) [GeV]g~m(
500
1000
1500
2000
2500
) [G
eV]
10 χ∼m
(
)expσ1 ±Expected Limit (
)SUSYtheoryσ1 ±Observed Limit (
[arXiv:1706.03731]
-1SS/3L obs. 36 fb
) < m(Z)0
1χ∼,0
2χ∼ m(
∆
) < m(W ), 0
2χ∼,±1χ∼
m(∆
)0
1χ∼) < m(
g~m(
))/21
0χ∼) + m(
1
±χ∼) = (m(2
0χ∼))/2, m(
1
0χ∼) + m(g~) = (m(
1
±χ∼; m(1
0χ∼ qqWZ→ g~ production, g~ g~
All limits at 95% CL
-1=13 TeV, 139 fbs
Preliminary ATLAS
g
g
χ±1
χ02
χ±1 χ0
2
p
p
q q W
Z
χ01
qq W
Z
χ01
ATLAS strong production searches 13 / 16
SS/3L: exclusion limits for simplified models (2)
Versatile signature, also limits on thirdgeneration squarks, RPV scenarios. . .
600 800 1000 1200 1400 1600 1800 2000 2200) [GeV]g~m(
400
600
800
1000
1200
1400
1600
1800
2000
) [G
eV]
t~m
(
)expσ1 ±Expected Limit (
)SUSYtheoryσ1 ±Observed Limit (
[arXiv:1706.03731]
-1SS/3L obs. 36 fb
) + m
(t)
t~
) < m
(
g~m(
d b → t~
, t t~
→ g~ production, g~ g~
All limits at 95% CL
-1=13 TeV, 139 fbs
Preliminary ATLAS
g
g
t
t
p
p
t
λ′′313b
d
t
b
d
600 650 700 750 800 850 900 950 1000 1050 1100) [GeV]b
~m(
200
400
600
800
1000) [G
eV]
10 χ∼m
(
)expσ1 ±Expected Limit (
)SUSYtheoryσ1 ±Observed Limit (
[arXiv:1706.03731]
-1SS/3L obs. 36 fb
) + 100 GeV
1
0χ∼
) < m(t) + m(
b~m(
) + 100 GeV1
0χ∼) = m(
1
±χ∼, m(1
±χ∼ t→1b~
production, 1b~
1b~
All limits at 95% CL
-1=13 TeV, 139 fbs
Preliminary ATLAS
b
b
χ±1
χ∓1
p
p
t
χ01
W
t
χ01
W
∗
550 600 650 700 750 800 850 900 950) [GeV]t
~m(
3−10
2−10
1−10
1 [pb]
* B
Rσ
)1
0χ∼ m(≈)
1
±χ∼)+100 GeV ; m(1
0χ∼)=m(
2
0χ∼)-275 GeV ; m(1t
~) = m(
1
0χ∼; m(
1
0χ∼ W*→
1
±χ∼, 1
±χ∼± tW→ 1t~
production, 1t~
1t~
All limits at 95% CL
-1=13 TeV, 139 fbs
Preliminary ATLAS t~ t
~→pp
Theoretical uncertainty
Expected limit
Observed limit
σ 1±Expected
σ 2±Expected
[arXiv:1706.03731]
-1SS/3L obs. 36 fb
t1
t1
χ02χ±1
χ02 χ±
1
p
p
t W
W ∗
χ01
t W∓W ∗
χ01
∗
ATLAS strong production searches 14 / 16
Conclusion
First results for inclusive squark / gluino searches with the full Run 2 dataset
Same-sign / three leptons + jets: probing various types of (long) decay chains forgluinos and squarks
Again found no deviation from Standard Model!
More advanced techniques to be deployed in next results: stay tuned!
All ATLAS Supersymmetry Public Results
ATLAS strong production searches 15 / 16
Other highlights from ATLAS SUSY searches
General overview [G. Stark, Monday]
Third-generation squarks [J. Anders, Monday]
Compressed mass spectra [S. Sekmen, Thursday]
Public likelihood for reinterpretations [G. Stark, Thursday]
Charginos/neutralinos [D. Miller, Tuesday]
Sleptons [S. Carra, Tuesday]
R-parity violation [J. Berlingen, Thursday]
Long-lived partices [H. Otono, Thursday]
Reconstruction techniques [C. Clement, Wednesday]
Prospects with HL-LHC [A. Cervelli, Wednesday]
ATLAS strong production searches 16 / 16
SS/3L: sources of uncertainties
Rpc2L0b Rpc2L1b Rpc2L2b Rpc3LSS1b Rpv2L0
0.1
0.2
0.3
0.4
0.5
0.6
Rel
ativ
e un
cert
aint
y
ATLAS Preliminary-1 = 13 TeV, 139 fbs
Total unc. Theoretical unc.MC statistical unc. Fakes/non-prompt, Charge-flip statistical unc.Experimental unc. Fakes/non-prompt, Charge-flip systematic unc.
ATLAS strong production searches 1 / 1
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