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Last one before my exam tomorrow...
I was wondering. If we have B meson oscillations we can write the light/heavy eigenstates:
|B_L> = p |B^0> + q |\bar{B}^0>
|B_H> = p |B^0> - q |\bar{B}^0>
with |p|^2 + |q|^2 =1...
How can I see that:
\frac{q}{p}= -\dfrac{ \Delta m_B - (i/2) \Delta \Gamma_B}{2 [M_{12} - (i/2) \Gamma_{12}]}
??
I was wondering. If we have B meson oscillations we can write the light/heavy eigenstates:
|B_L> = p |B^0> + q |\bar{B}^0>
|B_H> = p |B^0> - q |\bar{B}^0>
with |p|^2 + |q|^2 =1...
How can I see that:
\frac{q}{p}= -\dfrac{ \Delta m_B - (i/2) \Delta \Gamma_B}{2 [M_{12} - (i/2) \Gamma_{12}]}
??
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