Editing R-parity (section)

{{Short description|Discrete symmetry in certain supersymmetric models}}
'''R-parity''' is a concept in [[particle physics]]. In the [[Minimal Supersymmetric Standard Model]], [[baryon number]] and [[lepton number]] are no longer conserved by all of the [[renormalization|renormalizable]] couplings in the theory. Since baryon number and lepton number conservation have been tested very precisely, these couplings need to be very small in order not to be in conflict with experimental data. R-parity is a <math>\mathbb{Z}_2</math> symmetry acting on the Minimal Supersymmetric Standard Model (MSSM) fields that forbids these couplings and can be defined as<ref>
{{cite journal
 |last=Martin |first=S. P.
 |date=6 Sep 2011
 |title=A Supersymmetry Primer
 |arxiv=hep-ph/9709356
 |doi=10.1142/9789812839657_0001
 |journal=Advanced Series on Directions in High Energy Physics
 |volume=18
 |pages=1–98
 |isbn=978-981-02-3553-6
 |s2cid=118973381
}}</ref> 
:<math>P_\mathrm{R} = (-1)^{3B+L+2s},</math>

or, equivalently, as
:<math>P_\mathrm{R} = (-1)^{3(B-L)+2s},</math>

where {{mvar|s}} is [[Spin (physics)|spin]], {{mvar|B}} is baryon number, and {{mvar|L}} is lepton number. All Standard Model particles have R-parity of +1 while supersymmetric particles have R-parity of &minus;1.

Note that there are different forms of parity with different effects and principles, one should not confuse this parity with [[Parity (physics)|any other parity]].