I remember reading that the background contains $q \bar{q}$ giving 4 leptons while studying the 4 lepton decay channel of Higgs boson. Since LHC is a $pp$ collider, I was wondering the source of anti-quark $\bar{q}$.

Or is it correct to say that both $q$ and $\bar{q}$ are produced simultaneously during collision?

  • $\begingroup$ Z/$\gamma$ -> q-qbar, W$\pm$ -> q-q'bar, etc $\endgroup$ – JamieBondi Mar 12 '17 at 4:35
  • $\begingroup$ The proton itself, apart from the quark content uud, has a lot of virtual q-qbar pairs and gluons propagating in the proton. $\endgroup$ – JamieBondi Mar 12 '17 at 4:43
  • $\begingroup$ @JamieBondi So can I say that there are virtual mesons present in a proton? $\endgroup$ – kg__ Mar 12 '17 at 4:50
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    $\begingroup$ Virtual quarks wouldn't form mesons/baryons. They are very energetic (in QFT jargon, they are off-shell). The coupling strength of QCD is small at high energies, so virtual quarks won't bind into bound states. $\endgroup$ – JamieBondi Mar 12 '17 at 5:00
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    $\begingroup$ It is indeed correct to say that both $q$ and $\overline{q}$ are produced during collisions. They must be produced in equal numbers to conserve baryon number. $\endgroup$ – dukwon Mar 12 '17 at 10:16

It is simple to understand if you try to write down feynman diagrams for proton proton giving a Higgs :


gluons give pairs of quark antiquark. The spectator protons will also give jets or even more gluons might be radiated because the energies are high.

The Higgs has high couplings(proportional to mass) with the top-antitop loop , and so this is dominant for two gamma decays .

Higgs to quark antiquark pairs is only limited by the mass of the Higgs. Searches are on at LHC to find the Higgs to b bbar channel.

For the general case, the gluon can generate all quark antiquark pairs that conserve energy and momentum for the interaction.


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