Lipatov appears in two multibly-eponymous equations regarding this force, DGLAP and BFKL.
Lipatov appears in two multibly-eponymous equations regarding this force, DGLAP and BFKL. Entities acted on by this force can mix with its carriers to form a phase of matter which is detected by jet quenching, and which may be synthesized by the collision of ultra-relativistic heavy ions. A weaker form of this force is non-relativistically modeled by a screened Coulomb potential containing an exponential term with the product of the (*) pion mass and particle distance as an argument. That exclusively-attractive form is known as the Yukawa interaction or the "residual" form of this force, and is responsible for the stability of atomic nuclei. This force, modeled by an SU(3) gauge group, exhibits confinement, in which particles with color charge cannot be isolated due to the strength of this force. For 10 points, name this fundamental force described by QCD, in which gluons mediate interactions between quarks.
Lipatov appears in two multibly-eponymous equations regarding this force, DGLAP and BFKL.
strong interaction [or strong nuclear force; accept color force before "color," prompt after]