Search for New Particles at LEP
Total Page:16
File Type:pdf, Size:1020Kb
Search for New Particles at LEP S. Rosier-Lees LAPP (INPPS-CNRS) Annecy-Le-Vieux - France Abstract The LEP energy upgrade up to fi =189 GeV has allowed us to extend substantially the potential of searches for new physics. Results on searches for Higgs bosoms and supersymmetric particles obtained by the ALEPH, DELPHI, L3, and OPAL exper- iments are reported. No evidence of any signal is observed. Therefore, new limits on the Higgs boson masses as well as on the masses of the various supersymmetric particles are derived. They significantly improve those obtained either at LEPl or LEP1.5. The LEPBOO discovery potential for the neutral Higgs bosons is also shown. @ 1998 by S. Rosier-Lees. -409- . be discovered at LEP200 when running at &=200 GeV and assuming an integrated luminosity of 200 pb-’ collected by each experiment. LEP PRELIMINARY Individual Limit LEP Combined 11 Table 1: Individual and LEP combined observed and expected mass limits for the Stan- dard Model Higgs boson [3], up to fi = 183 GeV. 4 _?I: 80 82 84 86 88 90 92 94 10 80 82 84 86 88 90 92 mH(GeV/ z5 k --- HZ-Signal(mn=85GeV) 2 1.5 1 0.5 0 0 20 40 60 80 loo 0 mF(GeV) Figure 1: Mass distribution for the candidate events selected by the OPAL experiment in the searches for e+e- + HZ at center-of-mass energies up to 183 GeV [3]. I,,,I,,,,,,/,I lo 80 82 84 86 88 90 92 94. 80 82 84 86 88 90 92 94 mH(GeV/c’) mH(Ge V/c2) 2.2 The MSSM Higgs Bosons Figure 2: Average expected (dashed lines) and observed (solid lines) confidence levels, CL,, obtained In the MSSM, all SUSY particle masses, their couplings, and their production cross sec- from combining the results of the four LEP Collaborations using the four statistical methods. The tions and decay widths are predicted in terms of only six free independent parameters: intersections of the curves with the horizontal lines at 0.05 define the 95% confidence level lower rnilz (the common gaugino mass parameter at the GUT scale), me (the common mass for bounds, ezpected and observed, for the mass of the 5X4 Higgs boson. scalar fermions at the GUT scale), p (the higgsino mixing parameter), tan/3 (the ratio of the vacuum expectation values of the two Higgs doublets), mA (the mass of the neutral CP-odd Higgs boson A), and A (the trilinear coupling in the Higgs sector at the GUT scale); the renormalization group equations are used to determine the parameters at low -411- h ] Mh.a Lower Limit (GeV/c2) ] PRELIMINARY Range of ~ Lower ’ Individual Limit LEP Combined (ADLO) y#p#p h (Obs.) 70.7-74.4 78.8 (Exp.) 67.4-70.3 76.3 A (Obs.) 71.0-76.1 79.1 (ExP.) 68.4-72.0 76.3 Table 4: Individual and LEP combined mass limits for the neutral h and A bosons [3]. background contamination. The 95% C.L. individual limits on the charged Higgs boson Mu*=60 GeV/c’ r-o,r+u, T+V,SC cssi: Efficiency 24% 42% 40% Expected events 9.2 30.1 99.4 Observed events ] 6 1 28 1 93 0 100 200 300 400 500 mA (GeV/c2) Table 5: Typical efficiencies and number of expected and observed events obtained by the L3 experiment in the charged Higgs boson searches at a c.m. energy of 183 GeV (141. Individual Limit (ADLO) LEP Combmed 10 11 Table 6: Individual and LEP combined mass limits for the charged Higgs bosons. mass is shown as a function of the branching ratio Br(H* + r*vT) in Fig. 4. Combining all LEP results, a lower limit on the charged Higgs boson mass of 68 GeV is established at the 95% C.L., assuming that the sum BR(H+ + r’+uT) + Br(H+ + cS) is equal to one. It represents a gain of almost 10 GeV with respect to the individual limits, Table 6. 0 20 40 60 80 loo 120 140 3 Other SUSY Particles mh (GeV/c2) The supersymmetric particles searched for at LEP2, not counting the Higgs bosons, are Figure 3: LEP combined exclusion domains (method D) in the plane (MA, tan,@ (top) or sleptons, stops, sbottoms, charginos, and neutralinos as detailed in Refs. [17] and [18]. (Mh, tan,@ (bottom) by the LEP direct searches for e+e- + hZ and hA at center-of-mass The most popular SUSY breaking mechanisms are the gravity and the gauge mediated energies up to 183 GeV assuming either a maximal mixing or no mixing [3] and [IS]. SUSY breaking models (GMSB). The results of SUSY searches at LEP are interpreted in the framework of these two models. In general, to avoid lepton and baryon number -413- -PIP- ‘cd37 $?? pa!pnls a1s s[auueqD Lwap ay$30 lsour ‘[w@s aql 03 palvduroa suo!$3as 55013 uo!pnpold a[qeuos%zal ~J!M sassaao1d a~qepyw-~[aM 0% anp are sa31nos punoL?yLnzq pea1 quamF1adxa tjasa 103 r-qd ()P-OE 30 hpOU!unl pa$%?18a$u! ue qp~ Aafj 6531~9 $8 aq$[[e azm!s .uo!pnpo1d Il’ed-M 30 asoq$ 0% .IVI!UI!S haA a1’l? sa1nlou$s 1w18!s aq$ ‘sanpzA dlluaaal pauyqo sl!unI Impw!pu! aql lsql ospz uoyam plnoqs a~ ‘8 alqvA u! u~oqs se (Aafj ()g - 09 =)~v a%%?[ 10~ ‘suo!KRJa$u! uoloqd-oM$ iEq paqwI!uIop SF pUnOI8~Xq uoymqruo~ aq$ IIF pauyqo s! ‘IOAV~ uoldal 1~pm aql uo Bmpuadap ‘Aa 01 0% z 11~023 aq+ pus ‘Ehaua aIq!s!A ~01 ‘I? pue .Qyd!~~ntu ~01 B Lq paz!1al9weqz a1e s~w@s aql 103 8uyBue1 II@ ‘I? pm sdlay &sou!umI a1otu ‘~!ur!l pz3ymau!y aql 1110131~3 a1v aa acms sa@oIodo$ palzadxa aq$ ‘a8uw (Aa=) 01 - 9 =)mv MOI aql UI .W1aua a[q!s!a aql ~101) ‘Aa ogz- = rl 103 pwe ‘z 01 p.1 -uo3 ga!q~ (6’~ - =snsw = NV) azma1agLp SS\?UI ds? ayl pue a[zysd ~sfls aql Lq moq Su@ue~ sanpzn @mu Iualagtp ~03 panFlap am sl!unf pmpFA!pu! aq~ ‘2 +!A u! UMO~S papagE acyawd u! a.nz suo!$!puo~ puno&?!yavq aql pu’e GfoIodo$ ~euB!s aq& ‘&T aq$ Aq am Aafj ~$31 0% dn [SC] sasdpm? d37 up 30 s1noquo:, uoyq3xa pamquxoa aqL .s1alammd $no pa;11w Gi1aua BU!SS!UI puz suo%daI puv/~o slaf 30 uo!+vu!quro:, awes 30 $s!suoa sam$ asaql uo spuadap a%eq~xa Iauusy>$ :X aql u! uoyDas ssom uoFmpo1d aq+ ‘“2 JOJ -WI@ Asps ‘s&7 pw saIa!$n?d J@S 09 keaap saIcnl.rvd Asps pampo1d-1!sd sno!1%t aqA ‘uo!$anpo1d-1!sd 103 uoyaas SSOJCI “!aql q>agv lou op tnq (saya1eas :X aq$ Lq LEM~UTZ pa1aAoa uo@al ayl u! :X 30 sasSem MOI 103 b~uo luvAaIa1) EX 0% &uydnoa l!ayq aSueq3 lsnf 1Ewu sla$awwvd asaql am!s ‘+ pus Wj ~03 @IB$ 10 71 uo .L~~gS~~sQuo puadap s~!ux!~ asaqL .( %U ‘ A’uL) areid aql IIF paA!Jap art? s$!uu[ 11~ saShpe 631 11” 103 pa$zw~qns ‘(Aa I N %V WP’ ‘2) s! uoFympo1d 1!‘ed-M uroq pnno&yzq papadxa aqA L@O uo!$anpo1d XT~? IunoaDa o)u~ ouyAw% aql s! y slapour 8sw3 u! aI!qti ‘(:X) ouy21~nau Isa@!1 aql s! dsq aql ‘s[apotu Bu!yv~ qIn*ejap Lq ua@ ale sasswu uo s)!ur!~ ‘71 103 uar[~~ 1aIIsurs s! xf 30 %pnpo1d 1!ed Puyea1q Asps L~!AEI~ II! reIncy.nzd III 9uycm1ary &eaM pw p1lnau aq 0% pasoddns ayl 103 uoyaas SSOJD aql ‘IwauaP u! acm!s .[pz] +JZ] Aa ggr=sJ 07 Idn d37 1~ paa1asqo s! y acm!s uo!pa)ap sadwsa puv aIqv$s SI (ds?) al3!$1vd Asps qsa)q%y aql ‘uoydurnssv S&?M sassaaold ws u10q palaadxa sluaaa 30 1aqumu aql 03 qaadsa1 I#!M ssa3xa ON sq$ u!q$!~ .salayed Asfls 103 I- = pwe sal3!$1ed prepuv~s 103 1 = ‘rz+as+7(~-) = g :payonu! s! 1aqurnu urnluenb Mau ‘t?30 uoyeAnlasuo3 aq$ ‘sdoo1 nsns bq pacmpu! suoyqo!~ +j Aa ggl o) dn sa!%aua sswu-jo-1a$ua~ ye -H+H t -a+a ~03 saqweas panp 631 ay% Aq [(“CZL t &.LH ‘FH,wJ] aweId aq$ u! su~wuop uo!snIzxa pawquro3 d3q :p aIn&J - - y..---+ i ,.“.........‘... i i... t ..- z’o .; i ,cqv luala3pp ~03 sassaao1d ms uroq sluaaa palaadxa puv sayxaygfa Iw!dQ ‘:X aql PUB :: : ;: : uolda[ yecw aql uaaM+aq ‘JV\TV ‘aaua1agtp sswu aq$ uo h1%01)s puadap saqanzas asaql.103 :: / sa!$!arl!suas aq!$ ‘uoympo1$u! aql u! pau!ydxa dpvaqs sv Gl1aua Bu~ss~ur sn[d suo$daI “’ ““- p’o 1sueIdocm Qansn uaql aw uoympo1d uo$daI 1yeas 111013Bu!spe sa@olodo) aye .alq!ssod a~anm& . aq hur (ou!Zhvq~ ad&ou@nS a1nd ‘t! 103 d~uo 71.103) 2X ou!81erl:, $sa@!I aql via 10 :X ya Sh3ap apKww ‘(dS?N) apyvd nsns $sa@+o$-$xau aq$ lou SF uo2dal 1~?1ws aq$31 ‘:X ... .. .. .. i - 9’0 ouyz1)nau $sa@!I aq$ pus s.wr+red KS 1!aq$ o$u! Kemp b~~uw~~u~op suolda1 rye~s ayL .lauuvq3-? aql u! sou!Iw~nau Bu!Suvq3xa Lq paanpo1d aq ospz uw _a suollya 1eyez~s wa1aqM ‘LIUO lauueqa-s aql u! a%eqaxa z .IO A~~&.r~oEr~r~ 8’0 L v!a spaaDo1d 4 sne$ .IS~~~S puw g suonm 1yez~ 30 uo!pnpo1d aql ‘suoy~~o~ -a+a III ‘[CT] suo!p$Dadxa ns aql q$y sq$p!~ 2 pamseacu aql30 uos! E -xedwo3 aq$ 111013 ‘Aa EP 07 dn SBSSBUI q!p~ sou!l$nau .K?IKW papnlaxa sluar.u!ladxa 6x7 2 I I .I I ..,.