Residuals: isoscalar (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 | 0.520 | 0.520 | +0.0 | medium |
1^1S_0 | 0.960 | 0.960 | +0.0 | medium |
2^1S_0 | 1.440 | 1.440 | -0.0 | medium |
2^1S_0 | 1.630 | 1.630 | -0.0 | medium |
1^3S_1 | 0.780 | 0.780 | -0.1 | medium |
1^3S_1 | 1.020 | 1.020 | +0.4 | medium |
2^3S_1 | 1.460 | 1.457 | -3.4 | medium |
1^3D_1 | 1.660 | 1.664 | +4.3 | medium |
2^3S_1 | 1.690 | 1.690 | -0.4 | medium |
1^3D_1 | 1.880 | 1.879 | -1.4 | medium |
1^1P_1 | 1.220 | 1.218 | -1.5 | medium |
1^1P_1 | 1.470 | 1.473 | +3.1 | medium |
2^1P_1 | 1.780 | 1.777 | -3.1 | medium |
2^1P_1 | 2.010 | 2.008 | -2.0 | medium |
1^3P_0 | 1.090 | 1.087 | -3.1 | medium |
1^3P_0 | 1.360 | 1.355 | -5.5 | medium |
2^3P_0 | 1.780 | 1.778 | -1.8 | medium |
2^3P_0 | 1.990 | 1.986 | -4.4 | medium |
1^3P_1 | 1.240 | 1.238 | -2.5 | medium |
1^3P_1 | 1.480 | 1.480 | -0.0 | medium |
2^3P_1 | 1.820 | 1.818 | -2.0 | medium |
2^3P_1 | 2.030 | 2.027 | -2.7 | medium |
1^3P_2 | 1.280 | 1.276 | -4.4 | medium |
1^3P_2 | 1.530 | 1.532 | +1.6 | medium |
2^3P_2 | 1.820 | 1.815 | -4.6 | medium |
2^3P_2 | 2.040 | 2.042 | +2.5 | medium |
1^3F_2 | 2.050 | 2.054 | +4.4 | medium |
1^3F_2 | 2.240 | 2.243 | +2.6 | medium |
1^1D_2 | 1.680 | 1.680 | +0.5 | medium |
1^1D_2 | 1.890 | 1.893 | +3.0 | medium |
1^3D_2 | 1.700 | 1.696 | -4.3 | medium |
1^3D_2 | 1.910 | 1.904 | -5.5 | medium |
1^3D_3 | 1.680 | 1.683 | +3.1 | medium |
1^3D_3 | 1.900 | 1.897 | -3.0 | medium |
1^3G_3 | 2.370 | 2.370 | +0.3 | medium |
1^3G_3 | 2.540 | 2.542 | +1.8 | medium |
1^1F_3 | 2.030 | 2.033 | +2.8 | medium |
1^1F_3 | 2.220 | 2.223 | +2.8 | medium |
1^3F_3 | 2.050 | 2.046 | -4.0 | medium |
1^3F_3 | 2.230 | 2.234 | +4.1 | medium |
1^3F_4 | 2.010 | 2.008 | -2.4 | medium |
1^3F_4 | 2.200 | 2.202 | +2.4 | medium |
1^1G_4 | 2.330 | 2.333 | +3.2 | medium |
1^1G_4 | 2.510 | 2.507 | -3.0 | medium |
1^3G_4 | 2.340 | 2.344 | +4.3 | medium |
1^3G_4 | 2.520 | 2.517 | -2.9 | medium |
1^3G_5 | 2.300 | 2.296 | -3.6 | medium |
1^3G_5 | 2.470 | 2.475 | +4.7 | 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 | 0.764 | -614.5 | +0.0 | +0.0 | +0.0 | +0.0 | +370.9 | -243.5 | 0.520 |
1^1S_0 | 0.995 | -339.8 | +0.0 | +0.0 | +0.0 | +0.0 | +304.8 | -35.0 | 0.960 |
2^1S_0 | 1.397 | -104.8 | +0.0 | +0.0 | +0.0 | +0.0 | +148.0 | +43.2 | 1.440 |
2^1S_0 | 1.653 | -76.0 | +0.0 | +0.0 | +0.0 | +0.0 | +52.7 | -23.3 | 1.630 |
1^3S_1 | 0.667 | +104.1 | +0.0 | +0.0 | +0.0 | +0.0 | +8.7 | +112.8 | 0.780 |
1^3S_1 | 0.949 | +67.9 | +0.0 | +0.0 | +0.0 | +0.0 | +3.3 | +71.2 | 1.020 |
2^3S_1 | 1.411 | +44.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.9 | +45.1 | 1.457 |
1^3D_1 | 1.700 | +3.1 | -127.5 | +98.6 | -29.0 | -9.4 | +0.0 | -35.2 | 1.664 |
2^3S_1 | 1.660 | +29.3 | +0.0 | +0.0 | +0.0 | +0.0 | +0.6 | +29.9 | 1.690 |
1^3D_1 | 1.906 | +2.0 | -101.8 | +81.1 | -20.7 | -8.3 | +0.0 | -27.0 | 1.879 |
1^1P_1 | 1.262 | -43.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -43.2 | 1.218 |
1^1P_1 | 1.500 | -26.5 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -26.5 | 1.473 |
2^1P_1 | 1.810 | -32.7 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -32.7 | 1.777 |
2^1P_1 | 2.028 | -20.1 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -20.1 | 2.008 |
1^3P_0 | 1.284 | +18.0 | -267.6 | +106.6 | -161.0 | -53.9 | +0.0 | -196.9 | 1.087 |
1^3P_0 | 1.519 | +11.5 | -211.6 | +82.1 | -129.4 | -46.8 | +0.0 | -164.7 | 1.355 |
2^3P_0 | 1.807 | +10.3 | -109.7 | +91.6 | -18.1 | -20.9 | +0.0 | -28.7 | 1.778 |
2^3P_0 | 2.025 | +6.6 | -88.8 | +60.8 | -28.0 | -18.2 | +0.0 | -39.6 | 1.986 |
1^3P_1 | 1.261 | +13.9 | -120.8 | +57.6 | -63.1 | +25.4 | +0.0 | -23.9 | 1.238 |
1^3P_1 | 1.500 | +8.9 | -93.8 | +42.9 | -50.9 | +21.6 | +0.0 | -20.4 | 1.480 |
2^3P_1 | 1.807 | +9.4 | -53.9 | +45.4 | -8.5 | +10.3 | +0.0 | +11.2 | 1.818 |
2^3P_1 | 2.027 | +6.2 | -44.4 | +29.7 | -14.7 | +9.2 | +0.0 | +0.6 | 2.027 |
1^3P_2 | 1.268 | +8.6 | +99.7 | -65.2 | +34.5 | -4.5 | -30.9 | +7.7 | 1.276 |
1^3P_2 | 1.504 | +6.1 | +78.2 | -44.9 | +33.2 | -3.8 | -7.8 | +27.7 | 1.532 |
2^3P_2 | 1.808 | +8.2 | +53.5 | -44.5 | +9.1 | -2.1 | -7.8 | +7.4 | 1.815 |
2^3P_2 | 2.028 | +5.4 | +43.9 | -29.0 | +14.9 | -1.9 | -3.7 | +14.8 | 2.042 |
1^3F_2 | 2.041 | +0.7 | -74.9 | +90.9 | +16.0 | -3.4 | +0.0 | +13.3 | 2.054 |
1^3F_2 | 2.228 | +0.5 | -60.7 | +78.1 | +17.3 | -3.1 | +0.0 | +14.7 | 2.243 |
1^1D_2 | 1.687 | -6.8 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -6.8 | 1.680 |
1^1D_2 | 1.898 | -4.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -4.6 | 1.893 |
1^3D_2 | 1.688 | +2.4 | -38.7 | +35.2 | -3.5 | +8.8 | +0.0 | +7.7 | 1.696 |
1^3D_2 | 1.898 | +1.6 | -30.9 | +27.9 | -2.9 | +7.8 | +0.0 | +6.4 | 1.904 |
1^3D_3 | 1.693 | +1.6 | +68.0 | -77.1 | -9.1 | -2.3 | +0.0 | -9.8 | 1.683 |
1^3D_3 | 1.901 | +1.2 | +55.0 | -57.8 | -2.8 | -2.0 | +0.0 | -3.6 | 1.897 |
1^3G_3 | 2.338 | +0.2 | -50.2 | +84.1 | +33.9 | -1.7 | +0.0 | +32.4 | 2.370 |
1^3G_3 | 2.510 | +0.1 | -41.3 | +74.7 | +33.5 | -1.6 | +0.0 | +32.1 | 2.542 |
1^1F_3 | 2.034 | -1.6 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -1.6 | 2.033 |
1^1F_3 | 2.224 | -1.2 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -1.2 | 2.223 |
1^3F_3 | 2.035 | +0.6 | -17.4 | +24.1 | +6.7 | +4.1 | +0.0 | +11.3 | 2.046 |
1^3F_3 | 2.224 | +0.4 | -14.2 | +20.1 | +5.9 | +3.7 | +0.0 | +10.0 | 2.234 |
1^3F_4 | 2.038 | +0.4 | +47.6 | -77.4 | -29.8 | -1.3 | +0.0 | -30.6 | 2.008 |
1^3F_4 | 2.226 | +0.3 | +39.3 | -61.9 | -22.7 | -1.2 | +0.0 | -23.5 | 2.202 |
1^1G_4 | 2.334 | -0.4 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.4 | 2.333 |
1^1G_4 | 2.507 | -0.3 | +0.0 | +0.0 | +0.0 | +0.0 | +0.0 | -0.3 | 2.507 |
1^3G_4 | 2.334 | +0.1 | -9.5 | +17.6 | +8.2 | +2.2 | +0.0 | +10.6 | 2.344 |
1^3G_4 | 2.507 | +0.1 | -7.8 | +15.3 | +7.5 | +2.1 | +0.0 | +9.7 | 2.517 |
1^3G_5 | 2.336 | +0.1 | +35.4 | -74.7 | -39.3 | -0.8 | +0.0 | -40.0 | 2.296 |
1^3G_5 | 2.509 | +0.1 | +29.5 | -62.8 | -33.3 | -0.7 | +0.0 | -33.9 | 2.475 |
Isoscalar Annihilation Mixing
Rows below use the selected isoscalar annihilation scheme. calibrated_p1 is the Fig. 5/Table III pseudoscalar control; p1/p2 are the paper Eq. (18a,b) formula modes; general_eq16 is the literal Eq. (16) block (^3S_1, ^3P_2); ideal assigns the heavier row to the s sbar channel prediction per the Table III ideal-mixing prescription.
| state | scheme | unmixed GeV | mixed GeV | shift MeV |
|---|---|---|---|---|
1^1S_0 | calibrated_p1 | 0.149 | 0.520 | +370.9 |
1^1S_0 | calibrated_p1 | 0.655 | 0.960 | +304.8 |
2^1S_0 | calibrated_p1 | 1.292 | 1.440 | +148.0 |
2^1S_0 | calibrated_p1 | 1.577 | 1.630 | +52.7 |
1^3S_1 | general_eq16 | 0.771 | 0.780 | +8.7 |
1^3S_1 | general_eq16 | 1.017 | 1.020 | +3.3 |
2^3S_1 | general_eq16 | 1.456 | 1.457 | +0.9 |
1^3D_1 | ideal | 1.664 | 1.664 | +0.0 |
2^3S_1 | general_eq16 | 1.689 | 1.690 | +0.6 |
1^3D_1 | ideal | 1.879 | 1.879 | +0.0 |
1^1P_1 | ideal | 1.218 | 1.218 | +0.0 |
1^1P_1 | ideal | 1.473 | 1.473 | +0.0 |
2^1P_1 | ideal | 1.777 | 1.777 | +0.0 |
2^1P_1 | ideal | 2.008 | 2.008 | +0.0 |
1^3P_0 | ideal | 1.087 | 1.087 | +0.0 |
1^3P_0 | ideal | 1.355 | 1.355 | +0.0 |
2^3P_0 | ideal | 1.778 | 1.778 | +0.0 |
2^3P_0 | ideal | 1.986 | 1.986 | +0.0 |
1^3P_1 | ideal | 1.238 | 1.238 | +0.0 |
1^3P_1 | ideal | 1.480 | 1.480 | +0.0 |
2^3P_1 | ideal | 1.818 | 1.818 | +0.0 |
2^3P_1 | ideal | 2.027 | 2.027 | +0.0 |
1^3P_2 | general_eq16 | 1.307 | 1.276 | -30.9 |
1^3P_2 | general_eq16 | 1.539 | 1.532 | -7.8 |
2^3P_2 | general_eq16 | 1.823 | 1.815 | -7.8 |
2^3P_2 | general_eq16 | 2.046 | 2.042 | -3.7 |
1^3F_2 | ideal | 2.054 | 2.054 | +0.0 |
1^3F_2 | ideal | 2.243 | 2.243 | +0.0 |
1^1D_2 | ideal | 1.680 | 1.680 | +0.0 |
1^1D_2 | ideal | 1.893 | 1.893 | +0.0 |
1^3D_2 | ideal | 1.696 | 1.696 | +0.0 |
1^3D_2 | ideal | 1.904 | 1.904 | +0.0 |
1^3D_3 | ideal | 1.683 | 1.683 | +0.0 |
1^3D_3 | ideal | 1.897 | 1.897 | +0.0 |
1^3G_3 | ideal | 2.370 | 2.370 | +0.0 |
1^3G_3 | ideal | 2.542 | 2.542 | +0.0 |
1^1F_3 | ideal | 2.033 | 2.033 | +0.0 |
1^1F_3 | ideal | 2.223 | 2.223 | +0.0 |
1^3F_3 | ideal | 2.046 | 2.046 | +0.0 |
1^3F_3 | ideal | 2.234 | 2.234 | +0.0 |
1^3F_4 | ideal | 2.008 | 2.008 | +0.0 |
1^3F_4 | ideal | 2.202 | 2.202 | +0.0 |
1^1G_4 | ideal | 2.333 | 2.333 | +0.0 |
1^1G_4 | ideal | 2.507 | 2.507 | +0.0 |
1^3G_4 | ideal | 2.344 | 2.344 | +0.0 |
1^3G_4 | ideal | 2.517 | 2.517 | +0.0 |
1^3G_5 | ideal | 2.296 | 2.296 | +0.0 |
1^3G_5 | ideal | 2.475 | 2.475 | +0.0 |
Mean absolute residual: 2.6 MeV. Max absolute residual: 5.5 MeV.
Spin-Averaged Diagnostics
Weighted by 2J+1 within each available (n, L) group.
| multiplet | states | reference GeV | baseline GeV | residual MeV |
|---|---|---|---|---|
1D | 8 | 1.789 | 1.789 | -0.5 |
1F | 8 | 2.126 | 2.127 | +1.3 |
1G | 8 | 2.419 | 2.419 | +0.6 |
1P | 8 | 1.364 | 1.363 | -1.0 |
2P | 8 | 1.916 | 1.914 | -1.9 |
1S | 4 | 0.860 | 0.860 | +0.1 |
2S | 4 | 1.565 | 1.564 | -1.4 |
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.