![\"\"](\"https:\/\/www.blogs.unicamp.br\/massacritica\/wp-content\/uploads\/sites\/211\/2012\/08\/adele-parodia.jpg\" "\\"captura")
\nPar\u00f3dia que utiliza a m\u00fasica da Adele, Rolling In The Deep, como base.<\/p>\n
\nPar\u00f3dia que utiliza a m\u00fasica da Adele, Rolling In The Deep, como base.<\/p>\n
A letra:<\/p>\n
Rolling in the Higgs<\/strong><\/p>\n There\u2019s a collider under Geneva The complex scalar Chorus: Baby I have a theory to be told The particles then must all be massless Roll your vacuum to minimum potential
\nReaching new energies that we\u2019ve never achieved before
\nFinally we can see with this machine
\nA brand new data peak at 125 GeV
\nSee how gluons and vector bosons fuse
\nMuons and gamma rays emerge from something new
\nThere\u2019s a collider under Geneva
\nMaking one particle that we\u2019ve never seen before<\/p>\n
\nElusive boson
\nEscaped detection by the LEP and Tevatron
\nThe complex scalar
\nWhat is its purpose?
\nIt\u2019s got me thinking<\/p>\n
\nWe could have had a model (Particle breakthrough, at the LHC)
\nWithout a scalar field (5-sigma result, could it be the Higgs)
\nBut symmetry requires no mass (Particle breakthrough, at the LHC)
\nSo we break it, with the Higgs (5-sigma result, could it be the Higgs)<\/p>\n
\nThe standard model used to discover our quantum world
\nSU(3), U(1), SU(2)\u2019s our gauge
\nMake a transform and the equations shouldn\u2019t change<\/p>\n
\nCause mass terms vary under gauge transformation
\nThe one solution is spontaneous
\nSymmetry breaking<\/p>\n
\nBreak your SU(2) down to massless modes
\nInto mass terms of gauge bosons they go
\nFermions sink in like skiers into snow<\/em><\/p>\n