Search for MSSM Higgs at LEP Haijun Yanggallatin.physics.lsa.umich.edu/~hyang/talks/mssm-lep.pdf ·...

39
Search for MSSM Higgs at LEP Haijun Yang University of Michigan, Ann Arbor Physics Seminar at Univ. of Michigan February 4, 2002

Transcript of Search for MSSM Higgs at LEP Haijun Yanggallatin.physics.lsa.umich.edu/~hyang/talks/mssm-lep.pdf ·...

Page 1: Search for MSSM Higgs at LEP Haijun Yanggallatin.physics.lsa.umich.edu/~hyang/talks/mssm-lep.pdf · Search for MSSM Higgs at LEP Haijun Yang University of Michigan, Ann Arbor Physics

Search for MSSM Higgs at LEP

Haijun YangUniversity of Michigan, Ann Arbor

PhysicsSeminarat Univ. of Michigan

February4, 2002

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OUTLINEL�

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� Introduction of MSSM

� Main Backgrounds

� L3 Analysis Procedure

� LEP CombinedResults

� Conclusions

HaijunYang Searchfor MSSM Higgsat LEP 1

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Intr oductionL�

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� Minimal SupersymmetricStandardModel

Two Higgsdoublets�� 5 Higgsbosons

3 neutral(h & H CP-even,A CP-odd),

2 charged Higgs.

� NeutralHiggs- Two ComplementaryProcesses

Higgsstrahlung Pair Production

e� -

e� +

γ / Z* Z

h

q�–, l+, ν–

q, l� -, ν

b, �

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HaijunYang Searchfor MSSM Higgsat LEP 2

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Intr oductionL�

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576 hZ productionis dominantat low 8:93;=<

10-3

10-2

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1

65 70 75 80 85 90 95

MA (GeV)

tanβ √s = 206 GeV

1

30

σ (hZ

) pb

σ (hA

) pb

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576 hA is dominantat large 8>93;?< .

HaijunYang Searchfor MSSM Higgsat LEP 3

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Intr oductionL�

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� Parametersof theMSSM

1. Ratioof two Higgsvacuumexpectationvalues:@(A4� �2. Massof A boson:B )3. Gauginomassparameter: C �4. Scalarfermionmass:B D5. Higgsinomassparameter: E6. Higgs-sfermiontrilinear coupling: F

� ThreeBenchmarkScenarios

B � MaximalG H F E +-,:@ � I J TeV

Minimal Mixing: No mixing in stopsectorG H F E +-,:@ � K large E

HaijunYang Searchfor MSSM Higgsat LEP 4

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Intr oductionL�

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� Higgsdecayinto LNML and OQPRO is dominant.

tan β

m h = 95 GeV B

r(h)

h → bb − h → τ + τ - h → cc h → gg

a)

tan β

m A = 80 GeV

Br(

A)

A A A A

b)

10 -3

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1 10

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− → bb − → τ + τ - → cc → gg

576 focusedon SUT V L M LWL ML and SUT V L M LXOQPYO .

HaijunYang Searchfor MSSM Higgsat LEP 5

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Main BackgroundsL�

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� Main backgroundscome from , Z Z , [ M[ ,\^] [�[ and Z \^\ etc.

HaijunYang Searchfor MSSM Higgsat LEP 6

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Data Taking in Y2kL�

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HaijunYang Searchfor MSSM Higgsat LEP 7

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Analysis ProcedureL�

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� 4-jet channel:hA V L M LWL MLPreselection`

aNeural Network`

aFinal Discriminant

Step1. Preselection:To rejectlow multiplicitybackgrounds while keepinghigh signalefficiencies(b 90%).

Step2. Neural Network: Discriminant distri-butions are combinedin a neural net-work.

Step3. Final Discriminant: Neural networkoutputs are usedto construct final dis-criminantvariable.

HaijunYang Searchfor MSSM Higgsat LEP 8

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PreselectionCutsL�

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� PreselectionCuts

1. Numberof tracks c dfe2. Numberof calorimetricclustersc g�h3. Visibleenergy: ejilk m n oqp*rts u m vwi�x4. Perpendicularimbalanceenergy y ejilg�h � n oqp*r5. Leptonenergy m k�h GeV

6. Longitudinal componentof the missing mo-mentum: z {B p|r'r s~}�� o�p|r � � � � m eji�x� Event 6 4-jet usingDURHAM algorithm

� Kinematicfit: 4-momentumconservation(4C)fit

HaijunYang Searchfor MSSM Higgsat LEP 9

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Neural NetworkL�

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� NeuralNetwork Inputs:

1. Event � �*�t�2. EventSphericity

3. EventThrust

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��� �� � B � B ) ��" �� ��� NeuralNetwork Outputs:

Threeoutputs, �?  F , �¢¡ ¡ and �7£¤£

HaijunYang Searchfor MSSM Higgsat LEP 10

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Neural Network Inputs of 4-jet ChannelL�

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HaijunYang Searchfor MSSM Higgsat LEP 11

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Final Discriminant of 4-jet ChannelL�

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� TheFinal Discriminantis definedas:·¢¸º¹ » ¼ ¸º¹ ½ �¿¾ ¼ À À " ½ �¿¾ ¼ Á.ÂÁ "

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Ó Dataagreewith MC backgrounds.Ó Efficiency is insensitive to HiggsMass.

HaijunYang Searchfor MSSM Higgsat LEP 12

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Candidateof hA Ô ÕtÖÕWÕtÖÕ L×

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L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 L3 àHigh Discriminant= 0.98

àHigh B-tag= 0.6

à á â ã á ä å æ�ç�èjélèGeV

HaijunYang Searchfor MSSM Higgsat LEP 13

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SelectionResultsL×

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ALEPH DELPHI L3 OPALInte. Lumi. (ë�ìîí^ï ) 217 224 217 208

hA ð ì-ñìòìòñì ó â^ô�õöõ3÷4øData 10 5 12 11Total Background 5.5 6.5 7.8 10.34-fermionBkgd. 4.1 4.4 5.6 6.9ù ñù Bkgd. 1.4 2.1 2.2 3.4Efficiency 47% 47% 42% 48%ExpectedSignal 3.5 3.6 3.2 3.4

àThesignalefficiency andrateareshown

forá â å á ä å úwû ü ý�þ ÿ����

, with ����� � � û .

HaijunYang Searchfor MSSM Higgsat LEP 14

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Analysis ProcedureL×

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àTauchannel:hA Ô Õ ÖÕ� ��� ��

Preselection

Particle based Jet basedselection

Final Discriminant

Step1. Preselection:To rejectlow multiplicitybackgrounds while keepinghigh signalefficiencies(� 80%).

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Step3. Final Discriminant: B-tag of jets, di-jet massesareusedto constructfinal dis-criminant.

HaijunYang Searchfor MSSM Higgsat LEP 15

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Analysis ProcedureL×

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àPreselectionCuts:

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àFinal SelectionCuts:

particle-based jet-based8:9 ; <>= ?@BA C � � H 8:9 ; <>= ?@BA C � � H*�IKJMLNJMO P ��4GeV

*QIRJSLNJTO P ��4GeV*�+-,.�0/21 3 P 465VUG$ *�+-,.�0/21 3 P 465WUG4X�YZY\[]X�^_^ � E 4a` X�YZY\[bX�^c^ � E 4a`� $ P d Y&Y [ d ^_^ P ( � $ GeV � $ P d YZY [ d ^_^ P ( � $ GeV

no3-3 prongdecay no3-3 prongdecay� ^ � � Xfe ,g�hih � � $ `j ólknm X e ,.�i� j P 465VU

HaijunYang Searchfor MSSM Higgsat LEP 16

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SelectionCutsL×

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àN-1 plotsof Tauchannel

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HaijunYang Searchfor MSSM Higgsat LEP 17

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HaijunYang Searchfor MSSM Higgsat LEP 18

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HaijunYang Searchfor MSSM Higgsat LEP 19

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HaijunYang Searchfor MSSM Higgsat LEP 20

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HaijunYang Searchfor MSSM Higgsat LEP 21

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HaijunYang Searchfor MSSM Higgsat LEP 22

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HaijunYang Searchfor MSSM Higgsat LEP 23

Page 25: Search for MSSM Higgs at LEP Haijun Yanggallatin.physics.lsa.umich.edu/~hyang/talks/mssm-lep.pdf · Search for MSSM Higgs at LEP Haijun Yang University of Michigan, Ann Arbor Physics

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HaijunYang Searchfor MSSM Higgsat LEP 24

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HaijunYang Searchfor MSSM Higgsat LEP 25

Page 27: Search for MSSM Higgs at LEP Haijun Yanggallatin.physics.lsa.umich.edu/~hyang/talks/mssm-lep.pdf · Search for MSSM Higgs at LEP Haijun Yang University of Michigan, Ann Arbor Physics

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HaijunYang Searchfor MSSM Higgsat LEP 26

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3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

1

10

0 100 200 300 400 500

1

10

LEP 88-209 GeV Preliminary

mA (GeV/c2)

tanβ

Excludedby LEP�

mh� -max

MSUSY=1 TeVM2=200 GeVµ=-200 GeVmgluino=800 GeVStop mix: Xt

� =2MSUSY

� (GeV) ALEPH DELPHI L3 OPALobs.limit 90.0 90.8 83.9 80.6med.limit 92.1 90.0 88.3 86.9

ì LEP CombinedResults: 91.9/ 95.0GeV.

HaijunYang Searchfor MSSM Higgsat LEP 27

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LEP CombinedResultsLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

1

10

0 20 40 60 80 100 120 140

1

10

LEP 88-209 GeV Preliminary

mh (GeV/c2)

tanβ

Excluded�by LEP�

TheoreticallyInaccessible

No Mixing

� No Mixing Scenarioì � � � 91.5/ 95.0GeV, for �!���"� � 1.2ì � � � 92.2/ 95.3GeV, for ���#�"� � 1.2ì 0.8 $ �!���"� $ 9.6 is excluded

HaijunYang Searchfor MSSM Higgsat LEP 28

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LEP CombinedResultsLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

� Large % Scenario

1

10

0 100 200 300 400 500

1

10

LEP 88-209 GeV Preliminary

mA& (GeV/c2)

tanβ

Excludedby LEP

Large Mu Scan

MSUSY=400 GeVM2=400 GeVµ=1 TeVmgluino=200 GeVX'

t( =-300 GeV

Unexcluded

� )+* decaysinto ,.-,0/�1�1"/ ñ 2etc.

HaijunYang Searchfor MSSM Higgsat LEP 29

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ChargedHiggs SearchLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3

3L3L3L3Lø

3Lù

3L

3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

� Three final states: hadronic,semi-leptonic andleptonic decays.

e5 -

e5 +

γ6 / Z* H-

H+

c7–, ν8–τ9s, τ: -

c, 7 ν8 τ9s–, τ: +

HaijunYang Searchfor MSSM Higgsat LEP 30

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ChargedHiggs SearchLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3

3L3L3L3Lø

3Lù

3L

3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

� ; < semi-leptonic decays.

HaijunYang Searchfor MSSM Higgsat LEP 31

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ChargedHiggs SearchLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3

3L3L3L3Lø

3Lù

3L

3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

� ; < hadronicdecays.

HaijunYang Searchfor MSSM Higgsat LEP 32

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Excessof Eventsat 68 GeVLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

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3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

� 10%of ; < decayinto = .ì Apparentexcessat 68 GeV

HaijunYang Searchfor MSSM Higgsat LEP 33

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Excessof Eventsat 68 GeVLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

ì 4.2 > excessat68 GeVfrom L3.

But ......

HaijunYang Searchfor MSSM Higgsat LEP 34

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Exclusion Limits of ChargedHiggsLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L4

3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

ì Br( ; < ? =A@ = 0.0), B C � 77.2(77.1)GeV.ì Br( ; < ? =A@ = 0.1), B C � 66.9(76.0)GeV.ì Br( ; < ? =A@ = 0.5), B C � 69.7(75.7)GeV.ì Br( ; < ? =D@ = 1.0), B C � 82.7(84.6)GeV.

HaijunYang Searchfor MSSM Higgsat LEP 35

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LEP CombinedResultsLõ

3Lö

3L3L3L3L�

3L

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

10-7

10E -6

10-5

10E -4

10-3

10E -2

10E -1

1

60 65F

70 75 80 85G

90H

mH (GeV/c2)

1-C

Lb

Observed

Expected background

Expected signal

Br(H→I τν)=0

LEP 189-209

10E -7

10-6

10E -5

10-4

10E -3

10-2

10E -1

1

60 65F

70 75J

80G

85 90H

95H

mH (GeV/c2)

1-C

Lb

Observed

Expected background

Expected signal

Br(H→I τν)=1

LEP 189-209

ì LEP CombinedDataagreewell with SM back-grounds

HaijunYang Searchfor MSSM Higgsat LEP 36

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LEP CombinedResultsLõ

3Lö

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3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L÷

3L3L3L3L3L3Lø

3Lù

3L

3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

0K

0.2K0.4K0.6K0.8K

1

60L

65L

70 75 80M

85M

90N

95N

charged Higgs mass (GeV/cO 2)P

Br(

H→

τν)

LEP 189-209 GeVQ

R S T U 78.6GeVat95%C.L..

HaijunYang Searchfor MSSM Higgsat LEP 37

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ConclusionsLV

3LW

3L3L3L3LX

3LY

3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L3LZ

3L3L3L3L[

3L\

3L]

3L3L3L 3L 3L3L3L3L3L3L 3L 3L3L3L3L3L3L3L3L3L3L3L3L3L3L3L 3L3L3L 3L3L3L 3L 3L3L3L3L3

^ Morethan200_"`ba c datawerecollectedperexper-iment in the Year2000. In total d 700 _�`ea c werecollectedabove f g poleby eachexperiment.

R No significantevidenceof MSSM neutralandchargedHiggsareobservedup to h i 209GeV.

R NeutralHiggslimits with 95%C.L.

j k U lnmporq GeV, j s U lnmporl GeVtvuxw y

is excludedfr om 0.5to 2.4

R ChargedHiggslimits with 95%C.L.

j S T U z|{no~} GeV

HaijunYang Searchfor MSSM Higgsat LEP 38