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In supersymmetric extension to the Standard Model of physics, a sfermion is a hypothetical spin-0 superpartner particle (sparticle) of its associated fermion. Each particle has a superpartner with spin that differs by 1/2. Fermions in the SM have spin-1/2 and therefore sfermions have spin 0.

The name 'sfermion' was formed by the general rule of prefixing an 's' to the name of its superpartner, denoting that it is a scalar particle with spin 0. For instance, the electron's superpartner is the selectron and the top quark's superpartner is the stop squark.

One corollary from supersymmetry is that sparticles have the same gauge numbers as their SM partners. This means that sparticle–particle pairs have the same color charge, weak isospin charge, and hypercharge (and consequently electric charge). Unbroken supersymmetry also implies that sparticle–particle pairs have the same mass. This is evidently not the case, since these sparticles would have already been detected. Thus, sparticles must have different masses from the particle partners and supersymmetry is said to be broken.

Contents

Fundamental sfermionsEdit

SquarksEdit

Squarks are the superpartners of quarks. These include the sup squark, sdown squark, scharm squark, sstrange squark, stop squark, and sbottom squark.

Squarks
Squark Symbol Associated quark Symbol
First generation
Sup squark   Up quark  
Sdown squark   Down quark  
Second generation
Scharm squark   Charm quark  
Sstrange squark   Strange quark  
Third generation
Stop squark   Top quark  
Sbottom squark   Bottom quark  

SleptonsEdit

Sleptons are the superpartners of leptons. These include the selectron, smuon, stau, and the sneutrinos.

Sleptons
Slepton Symbol Associated lepton Symbol
First generation
Selectron   Electron  
Selectron sneutrino   Electron neutrino  
Second generation
Smuon   Muon  
Smuon sneutrino   Muon neutrino  
Third generation
Stauon   Tauon  
Stauon sneutrino   Tauon neutrino  

See alsoEdit

ReferencesEdit

  • Martin, Stephen, P. (2011). "A Supersymmetry Primer". Advanced Series on Directions in High Energy Physics: 1–98. arXiv:hep-ph/9709356. doi:10.1142/9789812839657_0001.