next up previous
Next: The Naive Zeeman Splitting Up: Derivations and Computations Previous: The Hamiltonian in terms


The Size of the B field Terms in Atoms

In the equation

\begin{displaymath}\bgroup\color{black}{-\hbar^2\over{2\mu}}\nabla^2\psi
+ {e\o...
...{B}\right)^2\right]\psi
= \left(E + e \phi\right)\psi. \egroup\end{displaymath}

the second term divided by \bgroup\color{black}$(e^2/a_0)$\egroup

\begin{displaymath}\bgroup\color{black} {e\over{2\mu c}}\vec{B}\cdot\vec{L} / (e...
...
\sim {e\over{2\mu c}}B\left(m\hbar\right) / (e^2/a_0) \egroup\end{displaymath}


\begin{displaymath}\bgroup\color{black} = m{\alpha eBa_0\over 2} / \left(e^2/a_0\right)
= m{\alpha a_0^2\over {2 e}} B \egroup\end{displaymath}


\begin{displaymath}\bgroup\color{black} = mB{ \left(0.5\times 10^{-8}\mbox{ cm}\...
...{10}\right) }}
= m{B\over {5\times 10^9\mbox{ gauss}}} \egroup\end{displaymath}


\begin{displaymath}\bgroup\color{black}\left(\alpha = {e^2\over {\hbar c}} \qquad a_0={\hbar\over{\alpha m c}}\right)\egroup\end{displaymath}

divide the second term by the third:

\begin{displaymath}\bgroup\color{black} \sim {B^2 a^2_0 {e^2\over{8mc^2}}
\over {{e\over{2\mu c}}B\hbar}}
= \alpha {a^2_0\over{4 e}} B \egroup\end{displaymath}


\begin{displaymath}\bgroup\color{black} = { \left(0.5\times 10^{6}\right)^2
\o...
...mes 10^{10}\right) }}
= {B\over{10^{10}\mbox{ gauss}}} \egroup\end{displaymath}



James Branson
2001-09-17