Direct electroweakino, slepton and stop searches at CMS
Lukas Vanelderen (University of Hamburg)
- n behalf of the CMS collaboration
29.05.13, ECFA LC2013
0/21 0/21
Direct electroweakino, slepton and stop searches at CMS Lukas - - PowerPoint PPT Presentation
Direct electroweakino, slepton and stop searches at CMS Lukas Vanelderen (University of Hamburg) on behalf of the CMS collaboration 29.05.13, ECFA LC2013 0/21 0/21 Direct production of stops 1/21 CMS stop searches main challenge: small
Lukas Vanelderen (University of Hamburg)
29.05.13, ECFA LC2013
0/21 0/21
1/21
main challenge:
◮ small stop mass: large cross section but signal looks like bkg ◮ large stop mass: different kinematics, but small cross section
7 TeV results:
◮ SUS-11-030: all-hadronic channel, jets and MET, 5/fb ◮ SUS-12-009: all-hadronic channel, razor, 5/fb
8 TeV results:
◮ SUS-12-023: single-lepton channel, 9.7/fb ◮ SUS-13-003: RPV, ≥ 3 leptons, 19.5/fb ◮ SUS-13-011: single lepton channel, 19.5/fb
→ THIS TALK
2/21
◮ 1 iso e/µ, pT > 30/25 GeV ◮ 2nd lepton veto:
◮ ≥ 4 jets, pT > 30 GeV, |η| < 2.4 ◮ 1 of which is b-tagged ◮ MET > 100 GeV P1 P2 ˜ t∗ ˜ t ¯ t t ¯ b W − ˜ χ0
1
˜ χ0
1
W + b P1 P2 ˜ t∗ ˜ t ˜ χ− W − ˜ χ+ W + ¯ b ˜ χ0
1
˜ χ0
1
b
3/21
[GeV]
T
M 50 100 150 200 250 300 Entries / 30 GeV 10
2
10
3
10
4
10
5
10
6
10
Data top l 1 ll → t t W+jets rare (650/50) x1000
1χ ∼ t → t ~
Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
MT
[GeV]
miss T
E 100 150 200 250 300 350 Entries / 25 GeV 10
2
10
3
10
4
10
5
10
6
10
Data top l 1 ll → t t W+jets rare (650/50) x1000
1χ ∼ t → t ~
Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
MET
[GeV]
W T2
M 100 150 200 250 300 350 400 450 500 Entries / 25 GeV 1 10
2
10
3
10
4
10
5
10
6
10
Data top l 1 ll → t t W+jets rare (650/50) x1000
1χ ∼ t → t ~
Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
MW
T2
ratio T
H 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Entries / 0.04
10 1 10
2
10
3
10
4
10
5
10
6
10
7
10
Data top l 1 ll → t t W+jets rare (650/50) x1000
1χ ∼ t → t ~
Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
Hratio
T
) [GeV]
1
(b
T
p 50 100 150 200 250 300 350 400 Entries / 15 GeV
10 1 10
2
10
3
10
4
10
5
10
6
10
Data top l 1 ll → t t W+jets rare (650/50/0.5) x1000 ± 1 χ ∼ b → t ~Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
pT(b1)
)
1
, b l R( ∆ 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 Entries / 0.33 1 10
2
10
3
10
4
10
5
10
6
10
7
10
Data top l 1 ll → t t W+jets rare (650/50/0.5) x1000 ± 1 χ ∼ b → t ~Pre-selection
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
∆R(l, b1)
4/21
◮ MT > 120 GeV ◮ cut on BDT output,
multiple BDTs trained for particular stop scenarios:
P1 P2 ˜ t∗ ˜ t ¯ t t ¯ b W − ˜ χ0
1
˜ χ0
1
W + b P1 P2 ˜ t∗ ˜ t ˜ χ− W − ˜ χ+ W + ¯ b ˜ χ0
1
˜ χ0
1
b
m ˜
χ±
1 = m ˜
χ0
1 + x(m˜
t − m ˜ χ0
1) 2 ( l
Δ M )
100 200 300 400 500 600
ΔM = mtop
3 ( m e d i u m Δ M )
( h i g h Δ M )
(
f
h e l l t
)
t → t χ1
1 (low mass)
mt [GeV]
~
m𝛙 [GeV]
~ 1
1 ( l
Δ M )
100 200 300 400 500 600
2 (medium ΔM) 3 (high ΔM) mt [GeV]
~
m𝛙 [GeV]
~ 1
t → b χ1
+ → bW
χ1
0 (x=0.5)
ΔM = MW
x = 0.5 more BDTs for x = 0.25, 0.75
5/21
[GeV]
T
M 100 200 300 Entries / 60 GeV 1 10
2
10
3
10 Data top l 1 ll → t t W+jets rare
BDT5
1
χ ∼ t → t ~
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
MT, pass BDT5
BDT Output 0.2 0.4 0.6 Entries / 0.05 100 200 300 400 500 600 Data top l 1 ll → t t W+jets rare
BDT5
1
χ ∼ t → t ~
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
Data/MC 0.5 1 1.5 2
BDT5, MT > 120 no excess observed, we proceed with SMS interpretation...
6/21
1
P1 P2 ˜ t∗ ˜ t ¯ t t ¯ b W − ˜ χ0
1
˜ χ0
1
W + b ◮ unpolarized top ◮ results from 6 BDTs ◮ per point, use most
sensitive signal region
[GeV]
t ~
m
200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
50 100 150 200 250 300 350 400
upper limit [pb] σ
10
10
10 1 10
2
10
unpolarized top BDT analysis
1
χ ∼ t → t ~ *, t ~ t ~ → pp
)
theory
σ 1 ± Observed ( ) σ 1 ± Expected ( )
Observed (9.7 fb
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
t
= M
1χ ∼
t ~
m
W
= M
1χ ∼
t ~
m
7/21
1
P1 P2 ˜ t∗ ˜ t ˜ χ− W − ˜ χ+ W + ¯ b ˜ χ0
1
˜ χ0
1
b ◮ results from 4 BDTs ◮ per point, use most
sensitive signal region
◮ unpolarized top ◮ m ˜ χ±
1 = m ˜
χ0
1+x(m˜
t−m ˜ χ0
1)
[GeV]
t ~
m
200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
50 100 150 200 250 300 350 400
upper limit [pb] σ
10
10
10 1 10
2
10
BDT analysis
+ 1
χ ∼ b → t ~ *, t ~ t ~ → pp
)
theory
σ 1 ± Observed ( ) σ 1 ± Expected ( )
Observed (9.7 fb
1
χ ∼
+ 0.5 m
t ~
= 0.5 m
± 1
χ ∼
m
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
W
= m
1χ ∼
χ ∼
m
x=0.5
[GeV]
t ~
m
350 400 450 500 550 600 650 700 750 800
[GeV]
1
χ ∼
m
50 100 150 200 250 300 350 400
upper limit [pb] σ
10
10
10 1 10
2
10
BDT analysis
+ 1
χ ∼ b → t ~ *, t ~ t ~ → pp
)
theory
σ 1 ± Observed ( ) σ 1 ± Expected (
1
χ ∼
+ 0.75 m
t ~
= 0.25 m
± 1
χ ∼
m
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
W
= m
1χ ∼
χ ∼
m
x=0.75
8/21
◮ different scenarios tested for
χ0
1 ˜
χ±
1 coupling ◮ accomodates for different stop and ewkino mixing scenarios ◮ typical impact on limits ±20 GeV
[GeV]
t ~
m
200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
50 100 150 200 250 300 350 400 BDT analysis
1χ ∼ t → t ~ , t ~ t ~ → pp Observed (unpolarized top) Observed (right-handed top) Observed (left-handed top)
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
t
= m
1χ ∼
t ~
m
W
= m
1χ ∼
t ~
m
[GeV]
t ~
m
200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
50 100 150 200 250 300 350 400 BDT analysis
+ 1χ ∼ b → t ~ *, t ~ t ~ → pp
Observed (nominal) )
± 1χ ∼
1χ ∼ , right W
R ±χ ∼ Observed ( )
± 1χ ∼
1χ ∼ , left W
R ±χ ∼ Observed ( )
± 1χ ∼
1χ ∼ , right W
L ±χ ∼ Observed ( )
± 1χ ∼
1χ ∼ , left W
L ±χ ∼ Observed (
Ldt = 19.5 fb
∫
= 8 TeV, s CMS Preliminary
1χ ∼
+ 0.5 m
t ~
= 0.5 m
± 1χ ∼
m
W
= m
1χ ∼
χ ∼
m
9/21
10/21
◮ low cross sections compared to strong production ◮ but might dominate if squarks and gluinos are heavy ◮ CMS results from 5/fb at 7TeV:
JHEP11(2012)147, arXiv:1209.6620
◮ CMS results from 9.2/fb at 8TeV:
CMS-SUS-12-022 → THIS TALK
11/21
production of ˜ χ±
1 ˜
χ0
2, ˜
χ±
1 ˜
χ±
1 , ˜
l˜ l, ˜ χ0
2 ˜
χ0
2 ◮ w/ and w/o intermediate sparticles ◮ w/ and w/o on-shell W/Z p1 p2 ˜ χ±
1
˜ χ0
2
˜ ℓ ˜ ℓ ν ℓ ˜ χ0
1
˜ χ0
1
ℓ ℓ p1 p2 ˜ χ±
1
˜ χ0
2
W Z ˜ χ0
1
˜ χ0
1
P1 P2 ˜ χ∓ ˜ χ± ˜ ℓ ˜ ν ν ℓ ˜ χ0
1
˜ χ0
1
ν ℓ P1 P2 ˜ ℓ ˜ ℓ ℓ ˜ χ0
1
˜ χ0
1
ℓ
search in a variety of lepton + MET channels
12/21
event selection
◮ 3 iso leptons, ◮ at most 1 τhad ◮ MET > 50 GeV ◮ b-jet veto
kinematic variables
◮ Mll: mass of lepton pair
most compatible with Z,
◮ MT: transverse mass of
remaining lepton and MET search regions
◮ w/ and w/o OSSF ◮ w/ and w/o τ ◮ binned: MET, Mll, MT
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary
[GeV]
miss T
E 50 100 150 200 events / 50 GeV 1 2 3 4 5 6 7 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 1 2 3 4 5 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 0.5 1 1.5 2 2.5 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 1 2 3 4 5 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 2 4 6 8 10 12 14 16 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 0.5 1 1.5 2 2.5 3 3.5 4 4.5 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 10 20 30 40 50 60 70 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 50 100 150 200 250 300 350 400 [GeV]
miss T
E 50 100 150 200 events / 50 GeV 5 10 15 20 25
>160 GeV
T
M <75 GeV
l
M <105 GeV
l
75 GeV<M >105 GeV
l
M <160 GeV
T
120 GeV<M <120 GeV
T
M
Channels: e
±
e
±
e µ
±
e
±
e e
±
µ
±
µ µ
±
µ
±
µ Data ZZ * γ Z WZ Non-prompt Rare SM uncertainty Total bkg
with OSSF w/o τ
p1 p2 ˜ χ±
1
˜ χ0
2
˜ ℓ ˜ ℓ ν ℓ ˜ χ0
1
˜ χ0
1
ℓ ℓ p1 p2 ˜ χ±
1
˜ χ0
2
W Z ˜ χ0
1
˜ χ0
1
13/21
◮ 4 iso leptons, at most 1 τ ◮ at least one Z ◮ SR: bins in MET, NOSSF, Nτ
◮ 2 light iso leptons, SS, Z-veto ◮ SR: 120 < MET < 200, MET > 200 GeV p1 p2 ˜ χ0
2
˜ χ0
3
Z Z ˜ χ0
1
˜ χ0
1
p1 p2 ˜ χ±
1
˜ χ0
2
˜ ℓ ˜ ℓ ν ℓ ˜ χ0
1
˜ χ0
1
ℓ ℓ P1 P2 ˜ χ∓ ˜ χ± ˜ ℓ ˜ ν ν ℓ ˜ χ0
1
˜ χ0
1
ν ℓ
14/21
◮ 1 Z(ee)/Z(µµ) candidate,
|mll − mZ| < 10 GeV
◮ 1 W/Z(jj) candidate,
70 < mjj < 110 GeV
◮ SR: bins in MET
◮ 2 light iso leptons, OS ◮ Z veto, MET > 60 GeV,
MCT⊥ > 100 GeV
◮ SR: same flavor, opposite flavor p1 p2 ˜ χ0
2
˜ χ0
3
Z Z ˜ χ0
1
˜ χ0
1
p1 p2 ˜ χ±
1
˜ χ0
2
W Z ˜ χ0
1
˜ χ0
1
P1 P2 ˜ χ∓ ˜ χ± ˜ ℓ ˜ ν ν ℓ ˜ χ0
1
˜ χ0
1
ν ℓ
15/21
no excess observed, we proceed with SMS interpretation...
16/21
1 ˜
2, intermediate ˜
flavor democratic
◮ 3-lepton and SS di-lepton ◮ “flavor democratic” ◮ m ˜ χ±
1 = m ˜
χ0
2
◮ m˜ l = m ˜ χ0
1 + x(m ˜
χ0
2 − m ˜
χ0
1)
p1 p2 ˜ χ±
1
˜ χ0
2
˜ ℓ ˜ ℓ ν ℓ ˜ χ0
1
˜ χ0
1
ℓ ℓ
flavor democratic, x = 0.5
[GeV]
2
χ ∼
=m
± 1
χ ∼
m
100 200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
100 200 300 400 500 600
[fb] σ 95% CL upper limit on
1 10
2
10
3
10
1χ ∼
> m
± 1χ ∼
= m
2χ ∼
m
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± l Observed 3
theoryσ 1 ± l Expected 3
2
χ ∼
± 1
χ ∼ → pp
τ
ν τ ∼ ,
µ
ν µ ∼ ,
e
ν e ~ →
± 1
χ ∼ τ τ ∼ , µ µ ∼ , e e ~ →
2
χ ∼ ) = 0.5
+
l ~ →
2
χ ∼ ( Br
1χ ∼
+ 0.5m
± 1χ ∼
= 0.5m
l ~
m
flavor democratic, x = 0.95
[GeV]
2
χ ∼
=m
± 1
χ ∼
m
100 200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
100 200 300 400 500 600
[fb] σ 95% CL upper limit on
1 10
2
10
3
10
1χ ∼
> m
± 1χ ∼
= m
2χ ∼
m
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± +SS l Observed 3 σ 1 ± +SS l Expecteded 3
l Observed 3 Observed SS only
2
χ ∼
± 1
χ ∼ → pp
τ
ν τ ∼ ,
µ
ν µ ∼ ,
e
ν e ~ →
± 1
χ ∼ τ τ ∼ , µ µ ∼ , e e ~ →
2
χ ∼ ) = 0.5
+
l ~ →
2
χ ∼ ( Br
1χ ∼
+ 0.95m
± 1χ ∼
= 0.05m
l ~
m
17/21
1 ˜
2, intermediate ˜
◮ 3-lepton and SS di-lepton ◮ m ˜ χ±
1 = m ˜
χ0
2
◮ m˜ l = m ˜ χ0
1 + x(m ˜
χ0
2 − m ˜
χ0
1)
p1 p2 ˜ χ±
1
˜ χ0
2
˜ ℓ ˜ ℓ ν ℓ ˜ χ0
1
˜ χ0
1
ℓ ℓ
τ-enriched, x = 0.5
[GeV]
2
χ ∼
=m
± 1
χ ∼
m
100 200 300 400 500 600 700 800
[GeV]
1
χ ∼
m
100 200 300 400 500 600
[fb] σ 95% CL upper limit on
1 10
2
10
3
10
1χ ∼
> m
± 1χ ∼
= m
2χ ∼
m
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± +SS l Observed 3 σ 1 ± +SS l Expecteded 3
2
χ ∼
± 1
χ ∼ → pp
τ
ν τ ∼ →
± 1
χ ∼ τ τ ∼ , µ µ ∼ , e e ~ →
2
χ ∼ ) = 1
+
l ~ →
2
χ ∼ ( Br
1χ ∼
+ 0.5m
± 1χ ∼
= 0.5m
l ~
m
τ-dominated, x = 0.5
[GeV]
2
χ ∼
=m
± 1
χ ∼
m
100 150 200 250 300 350
[GeV]
1
χ ∼
m
50 100 150 200 250
[fb] σ 95% CL upper limit on
10
2
10
3
10
4
10
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± l Observed 3
theoryσ 1 ± l Expected 3
2
χ ∼
± 1
χ ∼ → pp
τ
ν τ ∼ →
± 1
χ ∼ τ τ ∼ →
2
χ ∼
1χ ∼
+ 0.5m
± 1χ ∼
= 0.5m
l ~
m
18/21
1 ˜
2, on-shell W, Z
◮ 3-lepton and Z(ll) + W/Z(jj) ◮ m ˜ χ±
1 = m ˜
χ0
2
p1 p2 ˜ χ±
1
˜ χ0
2
W Z ˜ χ0
1
˜ χ0
1
[GeV]
2
χ ∼
=m
± 1
χ ∼
m
100 150 200 250 300 350 400
[GeV]
1
χ ∼
m
50 100 150 200
[fb] σ 95% CL upper limit on
2
10
3
10
Z
< m
1χ ∼
χ ∼
m
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± l +3 j 2 l Observed 2 σ 1 ± l 2j+3 l Expecteded 2
l Observed 3
j 2 l Observed 2
± 1
χ ∼
2
χ ∼ → pp
1
χ ∼ Z →
2
χ ∼
1
χ ∼ W →
± 1
χ ∼
◮ SS P1 P2 ˜ ℓ ˜ ℓ ℓ ˜ χ0
1
˜ χ0
1
ℓ
[GeV]
l ~
m
100 150 200 250 300
[GeV]
1
χ ∼
m
50 100 150 200
[fb] σ 95% CL upper limit on
1 10
2
10
= 9.2 fb
int
= 8 TeV, L s CMS Preliminary 95% C.L. CLs NLO Exclusions
theoryσ 1 ± Observed σ 1 ± Expecteded
L
µ ∼
L
µ ∼ ,
L
e ~
L
e ~ → pp ) = 1
1
χ ∼ l →
L
l ~ ( Br
19/21
20/21
Latest CMS stop results in SUS-13-008:
◮ 1-lepton + MET channel ◮ multitude of search regions dedicated to different stop scenarios ◮ no excess observed, exclusion scenarios up to 650 GeV ◮ but, compressed scenarios stay under the radar
Latest CMS ewk susy results in SUS-12-022:
◮ variety of channels cover many production/decay topologies ◮ no hints of SUSY
◮ but, compressed scenarios stay under the radar
21/21