Residuals: charmonium (GI-style)
Model: with GI momentum-sandwiched smeared contact hyperfine (every L), fixed-sector L·S (vector+Thomas) and OGE-tensor diagonalization with GI momentum-factor sandwiches and smeared-G/S derivative kernels; GI Table II b, c, masses, ε factors, and Fig. 2 α_s(r); closed-form GI G̃(r), S̃(r), plus central Coulomb momentum sandwich A(p)G̃A(p) in the solver's native p² representation, see the GIModel package (src/ at the repository root) for the computation and GIPaper (GIPaper/src/) for the comparison layer.
Numerics: OscillatorSolver — nbasis = 24:8:80 adaptive, ΔE ≤ 0.1 MeV, beta in [0.25, 2.35] GeV (22 bracket points, refined to 0.002 GeV), 6 levels/channel.
| state | reference GeV | baseline GeV | residual MeV | confidence |
|---|---|---|---|---|
1^1S_0 | 2.970 | 2.967 | -2.9 | high |
2^1S_0 | 3.620 | 3.626 | +5.8 | high |
3^1S_0 | 4.060 | 4.064 | +3.6 | high |
1^3S_1 | 3.100 | 3.091 | -8.6 | high |
2^3S_1 | 3.680 | 3.679 | -0.9 | high |
1^3D_1 | 3.820 | 3.818 | -1.7 | high |
3^3S_1 | 4.100 | 4.100 | +0.0 | high |
2^3D_1 | 4.190 | 4.194 | +4.1 | high |
4^3S_1 | 4.450 | 4.449 | -1.2 | medium |
3^3D_1 | 4.520 | 4.520 | -0.5 | medium |
1^1P_1 | 3.520 | 3.515 | -4.9 | high |
2^1P_1 | 3.960 | 3.956 | -3.8 | high |
1^3P_0 | 3.440 | 3.443 | +2.9 | high |
2^3P_0 | 3.920 | 3.916 | -3.5 | high |
1^3P_1 | 3.510 | 3.508 | -1.8 | high |
2^3P_1 | 3.950 | 3.953 | +3.2 | high |
1^3P_2 | 3.550 | 3.548 | -1.8 | high |
2^3P_2 | 3.980 | 3.980 | -0.5 | high |
1^3F_2 | 4.090 | 4.091 | +1.4 | medium |
1^1D_2 | 3.840 | 3.837 | -3.4 | high |
2^1D_2 | 4.210 | 4.208 | -2.5 | high |
1^3D_2 | 3.840 | 3.837 | -2.6 | high |
2^3D_2 | 4.210 | 4.208 | -1.8 | high |
1^3D_3 | 3.850 | 3.848 | -2.3 | high |
2^3D_3 | 4.220 | 4.217 | -3.4 | high |
1^1F_3 | 4.090 | 4.094 | +3.8 | medium |
1^3F_3 | 4.100 | 4.096 | -3.9 | medium |
1^3F_4 | 4.090 | 4.095 | +4.8 | medium |
Contribution Breakdown (diagnostic)
The central, contact, spin-orbit, and tensor columns are operator contributions in the same fully diagonalized fixed-sector eigenstate. They are not differences from a separate central-only solve.
| state | central contribution GeV | contact MeV | L·S(vec) MeV | L·S(Thomas) MeV | L·S total MeV | tensor MeV | annihilation MeV | spin + annihilation MeV | predicted GeV |
|---|---|---|---|---|---|---|---|---|---|
1^1S_0 | 3.078 | -111.4 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -111.4 | 2.967 |
2^1S_0 | 3.667 | -41.0 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -41.0 | 3.626 |
3^1S_0 | 4.091 | -27.1 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -27.1 | 4.064 |
1^3S_1 | 3.066 | +25.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +25.6 | 3.091 |
2^3S_1 | 3.666 | +12.7 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +12.7 | 3.679 |
1^3D_1 | 3.841 | +0.7 | -42.4 | +23.2 | -19.3 | -3.9 | +0.0 | -22.4 | 3.818 |
3^3S_1 | 4.091 | +9.0 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +9.0 | 4.100 |
2^3D_1 | 4.210 | +0.6 | -31.2 | +17.2 | -14.0 | -2.7 | +0.0 | -16.2 | 4.194 |
4^3S_1 | 4.442 | +7.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +7.2 | 4.449 |
3^3D_1 | 4.533 | +0.5 | -25.5 | +13.8 | -11.7 | -2.2 | +0.0 | -13.3 | 4.520 |
1^1P_1 | 3.523 | -8.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -8.2 | 3.515 |
2^1P_1 | 3.963 | -6.4 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -6.4 | 3.956 |
1^3P_0 | 3.535 | +3.7 | -94.6 | +22.8 | -71.8 | -23.8 | +0.0 | -91.9 | 3.443 |
2^3P_0 | 3.964 | +2.5 | -52.4 | +14.7 | -37.8 | -12.4 | +0.0 | -47.8 | 3.916 |
1^3P_1 | 3.524 | +2.8 | -39.8 | +11.1 | -28.7 | +10.2 | +0.0 | -15.6 | 3.508 |
2^3P_1 | 3.963 | +2.2 | -24.9 | +7.3 | -17.6 | +6.0 | +0.0 | -9.4 | 3.953 |
1^3P_2 | 3.525 | +2.2 | +33.6 | -10.7 | +22.9 | -1.8 | +0.0 | +23.3 | 3.548 |
2^3P_2 | 3.963 | +1.8 | +22.9 | -7.2 | +15.7 | -1.1 | +0.0 | +16.3 | 3.980 |
1^3F_2 | 4.095 | +0.2 | -26.1 | +23.6 | -2.5 | -1.5 | +0.0 | -3.7 | 4.091 |
1^1D_2 | 3.838 | -1.9 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -1.9 | 3.837 |
2^1D_2 | 4.209 | -1.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -1.6 | 4.208 |
1^3D_2 | 3.839 | +0.6 | -13.0 | +7.6 | -5.4 | +3.6 | +0.0 | -1.2 | 3.837 |
2^3D_2 | 4.209 | +0.5 | -9.8 | +5.7 | -4.1 | +2.6 | +0.0 | -1.0 | 4.208 |
1^3D_3 | 3.839 | +0.6 | +24.0 | -15.0 | +9.0 | -1.0 | +0.0 | +8.6 | 3.848 |
2^3D_3 | 4.210 | +0.5 | +18.6 | -11.3 | +7.3 | -0.7 | +0.0 | +7.0 | 4.217 |
1^1F_3 | 4.094 | -0.7 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.7 | 4.094 |
1^3F_3 | 4.094 | +0.2 | -6.2 | +5.9 | -0.4 | +1.8 | +0.0 | +1.6 | 4.096 |
1^3F_4 | 4.095 | +0.2 | +17.8 | -17.4 | +0.4 | -0.6 | +0.0 | +0.0 | 4.095 |
Same-J Tensor Mixing
Rows below use the mixed eigenvalues from triplet L=J-1 / L=J+1 tensor blocks. Components are ordered as lower-L/higher-L in the unmixed basis.
| state | unmixed GeV | mixed GeV | offdiag MeV | lower-L component | higher-L component |
|---|---|---|---|---|---|
2^3S_1 | 3.679 | 3.679 | +1.1 | +1.000 | -0.008 |
1^3D_1 | 3.818 | 3.818 | +1.1 | +0.008 | +1.000 |
3^3S_1 | 4.100 | 4.100 | +0.7 | +1.000 | -0.007 |
2^3D_1 | 4.194 | 4.194 | +0.7 | +0.007 | +1.000 |
4^3S_1 | 4.449 | 4.449 | +0.5 | +1.000 | -0.007 |
3^3D_1 | 4.519 | 4.520 | +0.5 | +0.007 | +1.000 |
2^3P_2 | 3.980 | 3.980 | +0.1 | +1.000 | -0.001 |
1^3F_2 | 4.091 | 4.091 | +0.1 | +0.001 | +1.000 |
Mean absolute residual: 2.9 MeV. Max absolute residual: 8.6 MeV.
Spin-Averaged Diagnostics
Weighted by 2J+1 within each available (n, L) group.
| multiplet | states | reference GeV | baseline GeV | residual MeV |
|---|---|---|---|---|
1D | 4 | 3.841 | 3.838 | -2.6 |
2D | 4 | 4.211 | 4.209 | -1.6 |
3D | 1 | 4.520 | 4.520 | -0.5 |
1F | 4 | 4.093 | 4.094 | +1.7 |
1P | 4 | 3.523 | 3.521 | -2.2 |
2P | 4 | 3.962 | 3.962 | -0.6 |
1S | 2 | 3.068 | 3.060 | -7.2 |
2S | 2 | 3.665 | 3.666 | +0.8 |
3S | 2 | 4.090 | 4.091 | +0.9 |
4S | 1 | 4.450 | 4.449 | -1.2 |
The spin-independent central path is the current GI reproduction candidate. Remaining heavy-quarkonium residuals should be read mainly as spin-dependent/operator-ordering and extraction-audit targets.