DetailedBalance: Difference between revisions
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-M_f & \mu & M_i | -M_f & \mu & M_i | ||
\end{array} \right)</math> | \end{array} \right)</math> | ||
Using the orthogonality condition: <math>\sum_{m_1 m_2} | |||
\left( \begin{array}{lll} | |||
j_1 & j_2 & j_3 \\ | |||
m_1 & m_2 & m_3 | |||
\end{array} \right) | |||
\left( \begin{array}{lll} | |||
j_1 & j_2 & j_3 \\ | |||
m_1 & m_2 & m_3 | |||
\end{array} \right)=\dfrac{\delta_{j_3 j'_3}\delta_{m_3 m'_3}}{2j_3+1}</math> | |||
Which leads us to our final result: <math>B(T_{\lambda}; i \rightarrow f)= \dfrac{(f|| T_{\lambda}|| i)^2}{2J_i+1}</math> | |||
It is obvious that this result does not depend on <math>M_i</math> |
Revision as of 16:27, 12 April 2010
Consider a transition from between two states of the nucleus with spins and , respectively. The transition probability is proportional to the squared matrix element where is a hermitian tensor operator of rank responsible for the process. Define the reduced transition probability
as a sum of squared matrix elements over final projections and operator projections .
a) Express in terms of the reduced matrix element and show that it does not depend on the initial projection .
b) Establish the detailed balance between the reduced transition probabilities of the direct , and inverse processes.
SOLUTION:
a) According to the Wigner-Eckert theorem, the entire dependence of the matrix element of a tensor operator on the magnetic quantum numbers is concentrated in the vector coupling coefficients,
We obtain the rate by squaring this and summing over and
Using the orthogonality condition:
Which leads us to our final result:
It is obvious that this result does not depend on