qspec.mu_jj_m1  (  sc ,  lc ,  jc_l ,  jo_l ,  j_l ,  so ,  lo ,  jc_u ,  jo_u ,  j_u ,  as_sympy = False  )[source]

The reduced magnetic dipole transition matrix element $$\mu_{J_l}^{J_u}\coloneqq\langle j_{l,c}j_{l,o},J_l|| \vec{\mu}||j_{u,c}j_{u,o},J_u\rangle$$ in units of the Bohr magneton $\mu_\mathrm{B}$.

Parameters:

scsympy_quant

The spin quantum number $s_c$ of the core electron(s) of the lower and upper state.

lcsympy_quant

The orbital angular momentum quantum number $l_c$ of the core electron(s) of the lower and upper state.

jc_lsympy_quant

The total angular momentum quantum number $j_{l,c}$ of the core electron(s) of the lower state.

jo_lsympy_quant

The total angular momentum quantum number $j_{l,o}$ of the outer electron(s) of the lower state.

j_lsympy_quant

The total angular momentum quantum number $J_l$ of the lower state.

sosympy_quant

The spin quantum number $s_o$ of the outer electron(s) of the lower and upper state.

losympy_quant

The orbital angular momentum quantum number $l_o$ of the outer electron(s) of the lower and upper state.

jc_usympy_quant

The total angular momentum quantum number $j_{u,c}$ of the core electron(s) of the upper state.

jo_usympy_quant

The total angular momentum quantum number $j_{u,o}$ of the outer electron(s) of the upper state.

j_usympy_quant

The total angular momentum quantum number $J_u$ of the upper state.

as_sympybool

Return the result as a symbol (True) or as a float (False).

Returns:

outsympy_core | float

The magnetic dipole transition matrix element $\mu_{J_l}^{J_u}$ ($\mu_\mathrm{B}$).