Table: Hydrogen D(3/2) States
$\mathbf{ {\large{D}}_{3/2}}$ – states of Hydrogen
$\mathbf{3D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \beta$
$\mathbf{4D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \gamma$
$\mathbf{5D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \delta$
$\mathbf{6D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \epsilon$
$\mathbf{7D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \zeta$
$\mathbf{8D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \eta$
$\mathbf{9D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \theta$
$\mathbf{10D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \kappa$
$\mathbf{11D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \lambda$
$\mathbf{12D_{3/2}}$ $\equiv \ \ \mathbf{1S} \, + \ {\mathrm{Lyman}} \, \mu$
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