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1、1Introduction1.1TheHierarchyProblemofParticlePhysicsAsfarasweknow,theconstituentsofourworldexperiencefourbasictypesofinteraction.Thesearetheelectromagnetic,weak,strong,andgravitationalforces.Elaboratetheorieshavebeendevelopedforalloftheminthepastcen-tury,whi
2、chareinexcellentagreementwithallexperimentaldata.ThefirsttwoareunifiedintheelectroweaktheoryofGlashow,Salam,andWeinberg[1,2].ThestrongforceisdescribedbyQuantumChromodynamics(QCD)[3,4],andsinceitsharesmanypropertieswiththeelectroweakforce,thecommondescriptionof
3、electroweakandstronginteractionsisreferredtoastheStan-dardModel(SM).Finally,Einstein’stheoryofGeneralRelativityprovidesthetheoryofgravitation,andeventhoughitisnotaquantumtheory,itissufficienttodescribegravitationalinteractionsasfarastheyarepresentlyaccessible.
4、Nevertheless,thereareopenquestionsthatcannotbeansweredbythesetheories.Inthisbookwewillfocusononeofthem,thehierarchyprob-lemofparticle-physicsscaleswhichisassociatedwithelectroweakphysics,anddiscusshowitcanbeaddressedbyexperimentsatpresentandfuturecolliders.T
5、hestrengthsofthefundamentalforcesarecharacterizedbythreequan-tities,namely[5]theprotonmass,mp=0.983271998(38)GeV,(1.1)theFermiconstant,G=1.16639(1)×10−5GeV−2,(1.2)FNewton’sconstant,G=6.707(10)×10−39GeV−2,(1.3)Nexpressedinparticle-physicsunitswhere=c=1.Inver
6、tingthelattertwo,wehavethreedifferentfundamentalmassscales,WolfgangKilian:ElectroweakSymmetryBreaking,STMP198,1–6(2004)©Springer-VerlagNewYork,Inc.200421Introductiontheprotonmass,mp≈1GeV,(1.4)√theFermiscale,v=(2G)−1/2≈246GeV,(1.5)F−1/219thePlanckscale,MPlanck
7、=GN≈1.22×10GeV.(1.6)Allthreescalesareofimmediaterelevanceformacroscopicphysics,evenforoureverydaylife.Firstofall,theprotonsandneutronswhichmakeupatomicnucleiarecompositeparticles,andtheirmassesaredeterminednotbytheirelementaryconstituents,butbytheinherentsca
8、leofthestronginteractionswhichbindthemtogether.Sincethedominantcontributiontothemassofanyatomcomesfromitsnucleus,thestrong-interactionscale,representedbytheprotonmass,setsthemassscaleofallbodies