B What happens when particles collide with their anti-particles?

  • B
  • Thread starter Thread starter teachmemorepls
  • Start date Start date
teachmemorepls
Messages
1
Reaction score
0
What will happen when a particle collide with other particles' anti-self? For example, down quark with anti-up quark , up quark with positron etc
 
Physics news on Phys.org
It will scatter somehow. You can think of all kinds of elastic and inelastic collisions compatible with the conservation laws. If something is not forbidden by conservation laws, it will happen with some probability. Perhaps I don't understand right your question, but there's nothing special about anti-particles. They just undergo elastic or inelastic reactions as particles.
 
  • Like
Likes bhobba
Most mesons are a combination of a quark and an anti-quark.
 
You can see this in the decay of the charged and neutral pion decays.
The decay of the neutral pion is basically a matter-antimatter annihilation process that can be seen through the decay equation:
π0 -> γ + γ
The annihilation occurs because neutral pions always have a quark and an antiquark from the same flavor.
But you can't see this annihilation process in charged pions where the flavors are different
π± -> π0 + e± + electron neutrino/antineutrino
 
Garlic said:
π± -> π0 + e± + electron neutrino/antineutrino
That is an extremely rare decay (about 10 decays in a billion). The most common decay is ##\pi^+ \to \mu^+ \nu## and ##\pi^- \to \mu^- \bar\nu## (probability of more than 99.98%).

Free quarks do not exist, you cannot "collide" quarks. You can have them in the same meson, with implications discussed above.
 
  • Like
Likes vanhees71 and Garlic
Thread 'Why is there such a difference between the total cross-section data? (simulation vs. experiment)'
Well, I'm simulating a neutron-proton scattering phase shift. The equation that I solve numerically is the Phase function method and is $$ \frac{d}{dr}[\delta_{i+1}] = \frac{2\mu}{\hbar^2}\frac{V(r)}{k^2}\sin(kr + \delta_i)$$ ##\delta_i## is the phase shift for triplet and singlet state, ##\mu## is the reduced mass for neutron-proton, ##k=\sqrt{2\mu E_{cm}/\hbar^2}## is the wave number and ##V(r)## is the potential of interaction like Yukawa, Wood-Saxon, Square well potential, etc. I first...
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