Nuclear Structure: Hindrance Factor Explained

  • Thread starter Thread starter rgshankar76
  • Start date Start date
  • Tags Tags
    Nuclear Structure
rgshankar76
Messages
12
Reaction score
0
What is hindrance factor?
What does it indicate? If the Hindrance is very high? If its low?

For eg. 103Rh (39.76 keV) E3 transition has got hindrance factor of ~400.
What does this mean.

The Hindrance is calculated using

Theoretical Lambda(E3) / Exptl. Lambda (E3)
Lambda(E3) -- > E3 Transition probablity.

Theoretical value obtained frm the single particle estimates.
Weisskopf or Moszowski single particle estimates.
for E3 : 34(A^2) (E^7)

exptl : 0.693 / [(t1/2) (1+Total ICC)]
Total ICC - total conversion coefficient
 
Physics news on Phys.org
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