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• The Higgs field does something strange: throughout the<br />

entire Universe, it takes on a uniform, non-zero value.<br />

• When the Higgs field does this, the interactions between<br />

the Higgs boson and other particles acquire their mass.<br />

• If the Higgs field didn't do this, all particles would be<br />

massless (some small technicalities that I'm glossing over).<br />

• The Standard Model of Particle Physics describes all the<br />

known properties of nature (with the exception of dark<br />

matter).<br />

• To know how the Higgs boson behaves, you have to know<br />

the Higgs boson mass (i.e. the mass is not a prediction of<br />

the theory).<br />

• The only thing you have to specify is the mass of the Higgs<br />

boson, after that, all interactions of the Standard Model<br />

are fixed, and you can make predictions to arbitrary accuracy<br />

(though it is very hard practically).<br />

• Therefore, the searches for the Higgs boson always left the<br />

mass as a free parameter.<br />

• Before July 4, 2012, the Higgs boson mass could only be in<br />

the 122 GeV to 130 GeV mass range (units where the proton<br />

mass is about 1 GeV, and the W and Z vector bosons<br />

are 80 GeV and 90 GeV, respectively). There was a small<br />

excess from the December 2011 results at 125 GeV. Many<br />

people suspected that the excess was the Higgs boson.<br />

• on July 4, 2012, the experiments showed that this excess<br />

grew substantially with the additional data that was recorded<br />

in 2012.<br />

• each experiment reached the "5 sigma" discovery threshold,<br />

which means that if there wasn't something there,<br />

it would be a fluke that would occur 1 time in 3,000,000<br />

chances.<br />

• There are two general purpose experimental collaborations<br />

at the LHC, each of which has 3000 physicists working.<br />

They are called ATLAS and CMS.<br />

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