Extended Data Fig. 4: Hyperfine structure energy levels of HD+ in the two relevant rovibrational levels. | Nature Physics

Extended Data Fig. 4: Hyperfine structure energy levels of HD+ in the two relevant rovibrational levels.

From: Test of charged baryon interaction with high-resolution vibrational spectroscopy of molecular hydrogen ions

Extended Data Fig. 4

Shown are the values \({E}_{{{{\rm{spin}}}},p}^{({{{\rm{theor}}}})}/h\) for the ground vibrational level (v = 0, N = 0) (left) and \({E}_{{{{\rm{spin}}}},q}^{({{{\rm{theor}}}})}/h\) for the excited vibrational level \(({v}^{{\prime} }=5,{N}^{{\prime} }=1)\) (right) of the \({}^{2}{\Sigma }_{g}^{+}\) ground electronic state. The vertical axis is broken for better visualization. The numbers next to the arrows indicate the line numbers i(p, q), where p (q) denotes the particular lower (upper) spin state. In this work, line 12 and line 21 were measured. G1 refers to the sum of electron and proton spin, G2 to the sum of G1 and deuteron spin, and F to the sum of G2 and rotational angular momentum N. The ground rovibrational level has zero rotational angular momentum, N = 0, giving rise to 4 spin states with total angular momentum F = 0, 1, 2. The upper rovibrational level \(({v}^{{\prime} }=5,\,{N}^{{\prime} }=1)\) has 10 spin states, having values \({F}^{{\prime} }=0,\,1,\,2,\,3\). For both studied lines 12 and 21, the lower and upper hyperfine states have the same particle spin coupling \({G}_{1}={G}_{1}^{{\prime} }\) and \({G}_{2}={G}_{2}^{{\prime} }\). The line 12 measured here is analogous to line 12 in ref. 3 and to line 12 in ref. 4. The line 21 is analogous to line 16 in ref. 3. Spin states with total angular momentum F are (2F + 1)-fold degenerate in zero magnetic field. We denote the lines and corresponding transition frequencies in zero external fields by fline i. i indicates the position in the list {fspin,i} of the spin frequency values of all spin components in ascending order.

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