Is the Residual Strong Force Mediated by a Single Meson or Two Quarks?

rayveldkamp
Messages
60
Reaction score
0
In the Residual Strong Interaction, energy and momentum are exchanged not through gluons but through exchange of quarks, for example in the soft hadronic scattering of a pi + and proton. Is the interaction mediated by a single meson or by two quarks, and if the latter doesn't this violate quark confinement?

Ray
 
Physics news on Phys.org
rayveldkamp said:
In the Residual Strong Interaction, energy and momentum are exchanged not through gluons but through exchange of quarks, for example in the soft hadronic scattering of a pi + and proton. Is the interaction mediated by a single meson or by two quarks, and if the latter doesn't this violate quark confinement?

Ray


Hi,

The residual strong force is mediated by pions. Pions are the lightest possible mesons. So basically like all mesons these pions are nothing else then a quark anti-quark combination. The reason why a quarkpair is mediated is because of confinement so this phenomenon is certainly respected by the residual strong force. For example it is not possible that this interaction is mediated by one single quark because it would take an infinite amount of energy in order to make sure that this quark is single...Ofcourse then we are in trouble with renormalization and our process is not physical. So it is exactly the asymptotic freedom that makes sure that no single quark is found at low energies...

regards
marlon
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top