Pion Constituents: Nucleon & Antinucleon Explained

  • Thread starter Thread starter ruchika
  • Start date Start date
  • Tags Tags
    Pions
ruchika
Messages
3
Reaction score
0
The nucleon and antinucleon are each about seven times more massive than the pion How is it conceivable that the pion could be a combination of nucleon and antinucleon
 
Physics news on Phys.org
You are exactly correct, the pion is not made up of a nucleon and an antinucleon. The pion is a meson and is composed of a quark and an antiquark. In the case of a pion, it is made up of up and down (anti)quarks. Whether it is a positive, negative or neutral (electric) charged pion determines whether the up or down (or a linear combination) is quark or antiquark.

You should consider picking up Griffiths "Introduction to Elementary Particles." It is an excellent book.
 
What is conceivable, is to describe the nucleon as a chiral soliton in a pionic field, where the scalar and pseudoscalar Goldstone meson are treated as if elementary. Please note that this is a (convenient, powerful, elegant, appealing ?) model which neither ignores its own approximations (those fields are not fundamental) nor can not be at least partially justified from a more fundamental point of view. In particular, it attempts to treat spontaneous chiral symmetry breaking effectively.
 
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}...

Similar threads

Back
Top