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Search for MSSM Search for MSSM Particles at Particles at LEP and LEP and Interpretations Interpretations Giacomo Sguazzoni CERN –EP Division on behalf of LEP collaborations

Search for MSSM Particles at LEP and Interpretations

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Search for MSSM Particles at LEP and Interpretations. Giacomo Sguazzoni CERN –EP Division on behalf of LEP collaborations. Wish list. Primary signal searches Acoplanar leptons (sleptons) Acoplanar jets (squarks) Multi-body + missing energy. Interpretations CMSSM mSUGRA. - PowerPoint PPT Presentation

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Page 1: Search for MSSM Particles at LEP and Interpretations

Search for MSSM Search for MSSM Particles at LEP Particles at LEP

and and InterpretationsInterpretations

Giacomo SguazzoniCERN –EP Division

on behalf of LEP collaborations

Page 2: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 2

Wish listWish list Primary signal searchesPrimary signal searches

Acoplanar leptons (sleptons) Acoplanar jets (squarks) Multi-body + missing energy ...

Interpretations Interpretations CMSSM mSUGRA

LEP vs. the futureLEP vs. the future Tevatron LHC

Page 3: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 3

DisclaimerDisclaimer MSSMMSSM

R parity conservation Pair production LSP stable

(cosmology neutral and weakly interacting)

…will show LEP SUSY Working GroupLEP SUSY Working Group (preliminary!!! ) combination when available!

……all limits @ 95% Conf. levelall limits @ 95% Conf. level

ALEPH DELPHI L3 OPAL

Time-saving

Time-saving

phenomenology

phenomenology

intro™

intro™

Page 4: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 4

0

20

40

60

80

100

120

140

160

180

200

220

240

260

1 8 15 22 29 36 43 50 57 64 71 78 85 92 99 106

113

120

127

134

141

148

155

162

169

176

183

190

197

204

211

Number of scheduled days (from start-up)

inte

gra

ted

lum

ino

sit

y (

pb

-1)

Physics 93 Zo

Physics 94 Zo

Physics 95 Zo, 65-70 GeV

Physics 96 80.5 - 86 GeV

Physics 97 91 - 92 GeV

Physics 98 94.5 GeV

Physics 99 96-102GeV

Physics 00 100-104GeV

Last Value (02.11.00) : 233 pb-1

0

20

40

60

80

100

120

140

160

180

200

220

240

260

1 8 15 22 29 36 43 50 57 64 71 78 85 92 99 106

113

120

127

134

141

148

155

162

169

176

183

190

197

204

211

Number of scheduled days (from start-up)

inte

gra

ted

lum

ino

sit

y (

pb

-1)

Physics 93 Zo

Physics 94 Zo

Physics 95 Zo, 65-70 GeV

Physics 96 80.5 - 86 GeV

Physics 97 91 - 92 GeV

Physics 98 94.5 GeV

Physics 99 96-102GeV

Physics 00 100-104GeV

Last Value (02.11.00) : 233 pb-1

ECM

(GeV)

161+172

183

189

192-202

204-209

tot

Int.Lumi (pb-1)

25

63

200

254

233

775775 //experimentexperiment

2000

1999

1998

1997 1996

Good for searches: High energy High energy

up to up to ~209GeV~209GeV

High luminosityHigh luminosity ss200GeV200GeV 10pb10pb-1-1 @ @ ss208GeV208GeV

LEP2 Data sampleLEP2 Data sample

Page 5: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 5

Acoplanar e, , Acoplanar e, ,

Searching forSearching for:: sleptons

χ χ~~ ee

•Missing energy/momentum•Lepton/Tau ID

Page 6: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 6

stauR

<40-60fbTau IDM>85.9 GeV/c2

smuonR

<10-30fbM>94.2 GeV/c2

selectronR

<10-30fbHigher expected M>99.6 GeV/c2

ELEP=183-208GeV

…limits…limits

Mass LimitsM>10GeV/c2

Page 7: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 7

Searching for: squarks

Acoplanar jetsAcoplanar jets

jet

jetP miss

4321 ff χ ff χ~~ bbttee

χ χ~~

bbbbee

ν~ ν~~~ bbttee

•Multi-jets

•b-tagging

•+leptons

χ χ~~ ccttee

•Topological variables•E, P/ /

New! stop 4body decay

Page 8: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 8

Squark limitsSquark limits

M(GeV/

c2)

M STOP<M

+m c

MSBOT

MMSNEU

M STOP<M SNEU

+m b

M SBOT<M

+m b

LEP1

CDFCDFD0=56o

=56o

=68o

=0o

=0o=0o

ADLO ADLOADLO

MSTOP

=56o

=0o

NEW!

ALEPH

MSTOP

M

M STOP<M

+m b

MSTOP(GeV/c2)

ν~~ bt χ~ ct *χW~ bt χ~

bb MSBOT>92GeV/c2>77GeV/c2>95GeV/c2MSTOP>94GeV/c2

M>10GeV/c2, any

similar sensitivity for any decay channel!!!

Page 9: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 9

Stable hadronsStable hadrons

~LDET dE/dx

~LDET

kink/IP

χ)/( χ)/(T~

T~

ucucee

hadron)-t~ stable~( T~

t~

T~

T~

T~ T

~

absolute stop mass lower limit• 63 GeV/c2

(any , BR, lifetime)

PLB 488 (2000) 234

MSTOP-MLSP<5GeVlifetime!!!!

Page 10: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 10

Topologies with ()Topologies with () γγχχχχ 111i1j ee

Search for i>1 1

radiative decays

very powerful for not-MSSM scenarios

•Single

/ /• with E, P

<40-100fb

γχχχχ 111i1 ee

<10-30fb

Page 11: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 11

2/4 fermions+(EMISS,PMISS)

2/4 fermions+(EMISS,PMISS)

searches for: charginos neutralinos

χff χff)χχ(χχ 43211j1i-

ee

ffχχχχ 1121 ee•Topological variables•E, P•multi-body

/ /

Page 12: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 12

…example of limits…example of limits

][GeV/c )M(χ 2

11 χWχ 12 χZχ

][GeV/c )M(χ 21

][GeV/c )M(χ 22

high m0 (heavy sleptons)

][GeV/c )M(χ 21

OPAL PreliminaryOPAL Preliminary

100-300fb100-200fb

Page 13: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 13

…other sparticles mass limits

LSP (not directly observable!) mass limits

Phenomenology: new topologies loop-holes?

…all results aregrinder-

dependent!!!

...extending the horizon

...extending the horizon

Page 14: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 14

Playing with CMSSMPlaying with CMSSM

small m0:

•smaller ()•light sleptons!!!

•C-MSSM•M1=5/3tan2WM2~0.5M2

•m0 for sfermions•no mixing•tan,

102 103

91

97

103

109

M2 [GeV/c2]

[GeV/c2]

LEP1

sleptons

large m0 small m0

M(

)[

GeV

/c2 ]

M2

m0=500GeV/c2

tan=2

ij

kin.limit

M2 [GeV/c2]

[GeV/c2]

m0=75GeV/c2

tan=2

Page 15: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 15

(,M2)Mass limits

(,M2)Mass limits

MGAUGINOS(,M2) mass limits M(M()=40GeV/c)=40GeV/c22

lightest chargino chargino

M(

)[

GeV

/c2 ]

lightest neutralino neutralino (LSPLSP)

tan

39.4GeV/c2

any m0

m0>500GeV/c2

tan

M(M()=100GeV/c)=100GeV/c22

93.9GeV/c2

Page 16: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 16

MSSM Higgs limit small MM22 exclusion small tantan exclusion

2222 2βcos hZh mmm

MLSP>45.6GeV/c2

m0=75GeV/c2

tan=2

M2 [GeV/c2]

[GeV/c2]

The MSSM Higgs role

The MSSM Higgs role

2

2~

log2sin2

4

t

t

m

m

Wmtm

...) ...( 22

20 Mm

Radiative corrections on the higgs mass!!

sleptons

charginos

(large m0)

Hig

gs

Hig

gs

in the corridor

1 2 5 10 tan

m0<1TeV/c2

MTOP=175GeV/c2HiggsHiggsADLO

Page 17: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 17

M

()[

GeV

/c2 ]

3rd family mixing3rd family mixing Stau mixing

chargino “holes” Robusteness checks:

mixing in sbottom, stop and stau sector (A=At=Ab=0)

only stau mixing

τχνντ~χ

tan

tan=35=-1000GeV/c2

(ISR) γγχχ

τ~ττ~τχχ χτ~τχχ

τχντχν ντ~ ντ~χχ

222

holedriven

selections τ~φ angle mix. τ~

charginosselectrons

M

()[

GeV

/c2 ]

mixing

any m0

) χ M(~) τ~ M(

INVISIBLE!

Page 18: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 18

2R 3GeV/c7)e~M(

Hig

gs

e~e~ LR

Re~

...absolute selectron mass limit

...absolute selectron mass limit

+ hole-driven selections1

2R 5GeV/c7)e~M(

chargino 2B-3B corridor

invisible!

) ν~ M(~)χ M(

ν~χ

selectrons/charginos search for to cover

small vs. M

Page 19: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 19

more constrained model complementary

benchmark!!! M()53-60GeV/c2 (A0=0) AA0 0 scan!!!scan!!!

~10GeV/c~10GeV/c22 weaker limits weaker limits

•mSUGRA•m1/2

•m0

•A0

•tan•sign(

m1/2 [GeV/c2]mSUGRAmSUGRA

tan<0

tan<0

m0[GeV/c2]

m1/

2 [G

eV/c

2 ]

m0[GeV/c2]

m1/

2 [G

eV/c

2 ]

Th

eory

exc

lud

ed

Hea

vy S

table

Sta

us

slep

tons

A0=0, MTOP=175GeV/c2

charginosneu

tral

ino-

stau

cas

cade

hig

gs

LEP1m0[GeV/c2]

ADLO preliminary

m1/2 [GeV/c2]

any Aany A00

A0=0A0=0

Page 20: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 20

SUSY paper?SUSY paper? Nice SUSY paper, will be ready for the WC*

read it! …in your relaxed moments.

*Winter Conferences

Page 21: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 21

The LEP legacyThe LEP legacy mSUGRA benchmark

LEP1

Fermilab

Fermilab

Theory exc

luded

Heavy Stable StausNeutralino-stau cascade

higgs

M(SPARTICLES) about s/2 high energy/luminosity

M0 clean environment!!!

charginos

m0[GeV/c2]

m1/

2 [G

eV/c

2 ]

Page 22: Search for MSSM Particles at LEP and Interpretations

G.Sguazzoni 22

SUSY search @ LEPSUSY search @ LEP hunting for events not compatible with SM!!! not trivial experimental task

MC simulation/detector effects/unusual topologies

ConclusionConclusion •Semileptonic candidate(26<M<31 GeV/c2)•ECM=195.6, run #50140, evt •E(tot)=45.5GeV, M(tot)=35.8GeV/c2

•E12=0 (no small angle activity)•M(miss)=147.6GeV/c2

•P(miss)=28.1GeV/c, PT(miss)=20.7GeV/c

M(hadr)=16.0GeV/c2P=8.52GeV/c