Residuals: bottomonium (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 | 9.400 | 9.393 | -6.7 | high |
2^1S_0 | 9.980 | 9.975 | -5.4 | high |
3^1S_0 | 10.340 | 10.332 | -7.6 | high |
1^3S_1 | 9.460 | 9.459 | -1.2 | high |
2^3S_1 | 10.000 | 10.004 | +4.1 | high |
1^3D_1 | 10.140 | 10.137 | -2.8 | high |
3^3S_1 | 10.350 | 10.354 | +3.5 | high |
2^3D_1 | 10.440 | 10.441 | +0.8 | high |
4^3S_1 | 10.630 | 10.633 | +2.8 | medium |
3^3D_1 | 10.700 | 10.698 | -1.7 | medium |
5^3S_1 | 10.880 | 10.875 | -5.5 | medium |
6^3S_1 | 11.100 | 11.092 | -7.7 | medium |
1^1P_1 | 9.880 | 9.881 | +0.5 | high |
2^1P_1 | 10.250 | 10.250 | -0.4 | high |
1^3P_0 | 9.850 | 9.845 | -5.2 | high |
2^3P_0 | 10.230 | 10.225 | -4.9 | high |
1^3P_1 | 9.880 | 9.875 | -5.2 | high |
2^3P_1 | 10.250 | 10.246 | -4.4 | high |
1^3P_2 | 9.900 | 9.896 | -4.3 | high |
2^3P_2 | 10.260 | 10.261 | +0.6 | high |
1^3F_2 | 10.350 | 10.350 | -0.3 | medium |
1^1D_2 | 10.150 | 10.148 | -2.3 | high |
2^1D_2 | 10.450 | 10.450 | -0.5 | high |
1^3D_2 | 10.150 | 10.147 | -3.2 | high |
2^3D_2 | 10.450 | 10.449 | -1.3 | high |
1^3D_3 | 10.160 | 10.155 | -5.4 | high |
2^3D_3 | 10.450 | 10.455 | +5.2 | high |
1^1F_3 | 10.350 | 10.354 | +4.3 | medium |
1^3F_3 | 10.350 | 10.354 | +4.3 | medium |
1^3F_4 | 10.360 | 10.358 | -2.3 | 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 | 9.452 | -58.7 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -58.7 | 9.393 |
2^1S_0 | 9.999 | -24.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -24.6 | 9.975 |
3^1S_0 | 10.350 | -17.3 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -17.3 | 10.332 |
1^3S_1 | 9.445 | +13.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +13.6 | 9.459 |
2^3S_1 | 9.998 | +6.5 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +6.5 | 10.004 |
1^3D_1 | 10.149 | +0.3 | -15.4 | +4.8 | -10.6 | -1.4 | +0.0 | -11.8 | 10.137 |
3^3S_1 | 10.349 | +4.8 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +4.8 | 10.354 |
2^3D_1 | 10.450 | +0.2 | -12.5 | +3.7 | -8.7 | -1.2 | +0.0 | -9.7 | 10.441 |
4^3S_1 | 10.629 | +4.0 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +4.0 | 10.633 |
3^3D_1 | 10.707 | +0.2 | -10.8 | +3.1 | -7.7 | -1.0 | +0.0 | -8.5 | 10.698 |
5^3S_1 | 10.871 | +3.5 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +3.5 | 10.875 |
6^3S_1 | 11.089 | +3.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | +3.2 | 11.092 |
1^1P_1 | 9.883 | -2.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -2.6 | 9.881 |
2^1P_1 | 10.252 | -2.0 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -2.0 | 10.250 |
1^3P_0 | 9.888 | +1.1 | -38.7 | +4.8 | -33.8 | -10.5 | +0.0 | -43.2 | 9.845 |
2^3P_0 | 10.254 | +0.8 | -26.1 | +3.3 | -22.8 | -7.0 | +0.0 | -28.9 | 10.225 |
1^3P_1 | 9.883 | +0.9 | -16.3 | +2.3 | -14.0 | +4.5 | +0.0 | -8.6 | 9.875 |
2^3P_1 | 10.252 | +0.7 | -11.5 | +1.6 | -9.9 | +3.1 | +0.0 | -6.1 | 10.246 |
1^3P_2 | 9.884 | +0.8 | +14.2 | -2.2 | +12.0 | -0.8 | +0.0 | +12.0 | 9.896 |
2^3P_2 | 10.252 | +0.6 | +10.3 | -1.6 | +8.7 | -0.6 | +0.0 | +8.7 | 10.261 |
1^3F_2 | 10.355 | +0.1 | -9.5 | +4.9 | -4.6 | -0.5 | +0.0 | -5.1 | 10.350 |
1^1D_2 | 10.148 | -0.7 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.7 | 10.148 |
2^1D_2 | 10.450 | -0.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.6 | 10.450 |
1^3D_2 | 10.148 | +0.2 | -4.8 | +1.6 | -3.3 | +1.4 | +0.0 | -1.7 | 10.147 |
2^3D_2 | 10.450 | +0.2 | -3.9 | +1.2 | -2.7 | +1.1 | +0.0 | -1.4 | 10.449 |
1^3D_3 | 10.149 | +0.2 | +9.2 | -3.1 | +6.1 | -0.4 | +0.0 | +6.0 | 10.155 |
2^3D_3 | 10.450 | +0.2 | +7.5 | -2.4 | +5.1 | -0.3 | +0.0 | +5.0 | 10.455 |
1^1F_3 | 10.355 | -0.3 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.3 | 10.354 |
1^3F_3 | 10.355 | +0.1 | -2.3 | +1.2 | -1.1 | +0.7 | +0.0 | -0.3 | 10.354 |
1^3F_4 | 10.355 | +0.1 | +6.7 | -3.6 | +3.2 | -0.2 | +0.0 | +3.0 | 10.358 |
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 | 10.004 | 10.004 | +0.2 | +1.000 | -0.001 |
1^3D_1 | 10.137 | 10.137 | +0.2 | +0.001 | +1.000 |
3^3S_1 | 10.354 | 10.354 | +0.0 | +1.000 | -0.000 |
2^3D_1 | 10.441 | 10.441 | +0.0 | +0.000 | +1.000 |
4^3S_1 | 10.633 | 10.633 | -0.0 | +1.000 | +0.001 |
3^3D_1 | 10.698 | 10.698 | -0.0 | -0.001 | +1.000 |
2^3P_2 | 10.261 | 10.261 | -0.0 | +1.000 | +0.000 |
1^3F_2 | 10.350 | 10.350 | -0.0 | -0.000 | +1.000 |
Mean absolute residual: 3.5 MeV. Max absolute residual: 7.7 MeV.
Spin-Averaged Diagnostics
Weighted by 2J+1 within each available (n, L) group.
| multiplet | states | reference GeV | baseline GeV | residual MeV |
|---|---|---|---|---|
1D | 4 | 10.152 | 10.148 | -3.7 |
2D | 4 | 10.448 | 10.450 | +1.5 |
3D | 1 | 10.700 | 10.698 | -1.7 |
1F | 4 | 10.353 | 10.355 | +1.4 |
1P | 4 | 9.886 | 9.882 | -3.4 |
2P | 4 | 10.252 | 10.251 | -1.3 |
1S | 2 | 9.445 | 9.442 | -2.6 |
2S | 2 | 9.995 | 9.997 | +1.7 |
3S | 2 | 10.348 | 10.348 | +0.7 |
4S | 1 | 10.630 | 10.633 | +2.8 |
5S | 1 | 10.880 | 10.875 | -5.5 |
6S | 1 | 11.100 | 11.092 | -7.7 |
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.