Axion Decay Width: Mass 10^-6 eV, Primakoff Effect

  • Thread starter Thread starter florian101
  • Start date Start date
  • Tags Tags
    Decay Width
florian101
Messages
11
Reaction score
0
hello
I would like to know the frequency width of a decaying axion
Lets say the axion has a mass of 10^-6 eV and it decays via the primakoff effect within a B field into one photon. Because there is only one photon in the final state I would assume that the photon frequency is quite narrow but what actually defines the width of the signal?
thanks
florian
 
Last edited:
Physics news on Phys.org
Spectrum of incoming axions, I think? Primakoff effect is just a fancy name for scattering, a+Z -> gamma+Z. Final frequency should be exactly computable if we know initial energy and scattering angle, simply using conservation of energy & momentum (since all particles are stable).
 
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