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Magazine feature, apparently from New Scientist dated 30 March 2002, by physicists Gordon Kane and Edward Witten. It explains the Higgs field and electroweak symmetry breaking with a North Pole versus Africa temperature analogy, then covers LEP's hint near 115 GeV, Tevatron and LHC prospects, grand unification and supersymmetry. The scan text is noisy, with run-together words.
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HUNTING THEgSeSGS
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-ancient times. Likewise, itwas known that
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etime bythehuman eye
zB ri sibleforcertain forms ofradioactive decay,ae |(eG tp tooklate19th-century sclence. Studyingo% x Pa ’ themindetailrequired thetechnology of—— (Sy |] thelatterpartofthe20thcentury.
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physicists Gordon Kane motion, theNorthPoleisfrigidandthe
(left) and Edward Witten “ropursuetheanalogy, wemightthinkof
(above) explain why basicparticlesthattransmittheweakinter they'reconvinced thatenoleaeConeamope theHiggs particle is oflight.Inthestandard modelofparticle
justwaiting tobe buildingblocks,suchaselectronsand quar.ere Forcesbetweenparticlesaretransmitted by discovered otherparticles, suchasphotons, thecarrier
tices, thebasic particles that transmit the
knowin about light. Bycontrat, theNorth
Re PoleandtheeffectsoftheWandZparticles
30March2002NewScents«wa newscentscom 2»
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” particlesandforcesarepostulatedtodothe $jobthattheHiggsparticledoesinthestan-
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ri . sy aspectsofthestandard model,apartfrom “iiadadsaeFiche theHiggsparticle,havebeenspectacularly
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effective starting point forunified field 3 * .
theories, andstring theories, thatseektoi ¢ 4
Thesetheories areattractive butunproven. iS rOurhopeisthat,alongwithdiscovering the y
deeper eve
Thestandard model istested mostdirectly ae
byaccelerating particles toveryhighener- [au .
laboratories inEurope (CERN, andDESY in B&
Hamburg), theUS(especially SLAC inCali i bis
Japan (the KEK laboratory.
particles,thetopquark,andthetauneu- fe- ii . ‘trino,Also,numerous standard modelpre- KG eli \ dictionsfordetailsofelementary particlere- /ie i .
Large Electron Positron (LEP) acceleratorat I Ci ge a CERN.Theybehaved inaccordwiththe MMMM = q as
standardmodeltoaveryhighdegree BZ,h >»he G2 z
thetheoryplusotherexperiments.thisisaaaia4 yytyUypossible Because the standard model isaQAM Se/YYYj. mathematicaltheory thatdescribes many a /i\ Wwe
Tave alreadybeendone / ¥ Wy ‘experiments havealreadybeendone J Yi liderthatdiscoveredtheWandZparticles, MAA MMMA (CERNknew just what energy was necded
theory pus experimentsalready performed. GeV respectively them, Finally, thetests ofthestandard model
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© BP standard modeltheoryoftheHiggsparticle
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\ \\ We / theelectromagnetic andweakinteractions
j NN (Canwegofurtherandbuildaunifiedfield }| \\if . theoryofallthreestandardmodelforces?A ip) i\fh beautiflstrategyfordoingsowasproposed ip) almost30yearsagointhe“grandunified 1h) theory’ofHowardGeorgiandSheldon All \_— | Glashow,whichdrewoneatllerworkby ANY|\)eaeFr JogeshPatiandAbdusSalam,Theprecise SS Mi ste, ‘measurements performed sincethenhave
:ofthe three standard model forces are just
theHiggsparticle weighs lessthanabout THERE |SVERY tighttomakegrandunificationwork200GeV,andlessthanabout160GeVwith ] Buttheresacatch:grandunificationonlyhighconfidence. Dietexperiments have GOOD INDIRECT snakessenseithestandardmodelconcept
swept through roughlyhalfoftheexpected EVIDENCE, ANDA.ofthetiggsparticiisright.Soeitherthisis
orendprobablyaaFotgoalof0a HINT OFDIRECT tiicecoupingstrengthshowninthePare piri rec 2g MIDI: =see
Howfarhas experiment current reached? nature onunwary physicist.reetepenentlboundontgs THATHIGGS "Anirsnoteonlyxe,orgrand particlemassisthattisatteat 1138Gev, PARTICLES DOEXIST’ unificationtowork,oneatsoneedsto assumesumingthevalidityofthestandardmodel supersymmetry. Toexplainsupersymmetry‘Thismeasurement wasmadebytheextra-present,thehighestenerglesintheworldare_propelyisasubjectforanotherarticle.But ordinarily successful LPcollider which also attained atthe Tevatron collider atFermilab, inbrlf, supersymmetry isanenrichment
Carried outmany ofthemost accurate which recently resumed operation afteranofElnstln’s theory ofspecial relativity to
Standard model ets. When thefinalstageofupgradetoprovidemoreIntenseparticleincludequantumvariableinthestructureof LEPwasbuilt wasexpected tosearch for beams, Ifitperforms asplanned, itwillbespace-time. Itrelates thequarks andelectrons
Higgs particles uptoanenergy ofabout 108 abletodiscover Higgs particles uptoabout tothe particles thattransmitthe ores. ItpreGeVBystrainingeverythingtothelimit,LEP180GeVwithinseveralyears,andhopefully dietsnewparticles,partnersfortheparticlesengineerswereabletooperatethemachine confirmorexcludeby2004thehintfromLEP._wealeadyknow,thatshouldbediscoveredatbeyond itsdesign, making itpossible to Beyond theTevatron, thenextbigstepinthe Tevatron andLHCandfuture facilities
search fortheHiggs upto113.5GeV. energy willcome withthecommissioning suchasalinea electron collider. Itoffers aFamous,intheclosingstageoftheLEPoftheLargeHadronCollider(LHC)atCERN,windowtograndunification andbeyond
programme,ahintwasfoundofadiscovery scheduledfor2006,Itisexpectedtohavethattotheevenmoreambitiousstring bftheHiggs particle with amass ofvery roughly seven timesthe energyoftheTevatrontheory,whichmayunifygravityalongwith neatly118GeV.Unfortunately, LEPdidnotandconsiderably moreintenseparticlebeams.theotherforces.Supersymmetry affectsthe {gite have theenergy andintensity toestab- TheLHC willcoverthewholerangeofHiggs_detallsofsearchesforHiggsparticlesbutnot ishthisconclusively orruleitout.Sowewillparticlemasses upto200GeVand{farbeyond, thegeneralidea.hvetoawait future experiments. ndshould findtheHiggs particle, orwhat- Ifsupersymmetry 1sdiscovered, itwill
“Thus themotivation forproving the everdoesthejobthatItssupposed todo, putphysics onanewlevel. ItwillenableexistenceofHiggsparticlesIsassongorwhetheritsthestandardmodeltheoryofexperimenters tomakemanyimportantandStrongerthanever,andthereIsverygoodtheHiggsparticlethatprovestobecomector excitingmeasurements andgiveaboostto
tvidence, that theydoinfactexst.JustasFindingandstudyingtheHiggsparticleanddeeperinsightsbeyondthat. a direct observation ofthetopquarkremained exploring thestandard model atyethigherelusiveuntilfalitieswithsuficientenergyenergiesmakesanexcitingmission.AndtheGordonKaneiatheUniversoMichigan,
and intensitywereavallable,soItsnowforpropertiesoftheHiggsparticlewilpoint10.janarbor Higgs particles. fewdevelopments. There lsagood chance Edward witen sate Intute forAdvancedWhereillthenextresultscomefom?AtthattheLH,andpossiblytheTevatron,willStd,Princeton,NewJersey