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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.

statereference GeVbaseline GeVresidual MeVconfidence
1^1S_09.4009.393-6.7high
2^1S_09.9809.975-5.4high
3^1S_010.34010.332-7.6high
1^3S_19.4609.459-1.2high
2^3S_110.00010.004+4.1high
1^3D_110.14010.137-2.8high
3^3S_110.35010.354+3.5high
2^3D_110.44010.441+0.8high
4^3S_110.63010.633+2.8medium
3^3D_110.70010.698-1.7medium
5^3S_110.88010.875-5.5medium
6^3S_111.10011.092-7.7medium
1^1P_19.8809.881+0.5high
2^1P_110.25010.250-0.4high
1^3P_09.8509.845-5.2high
2^3P_010.23010.225-4.9high
1^3P_19.8809.875-5.2high
2^3P_110.25010.246-4.4high
1^3P_29.9009.896-4.3high
2^3P_210.26010.261+0.6high
1^3F_210.35010.350-0.3medium
1^1D_210.15010.148-2.3high
2^1D_210.45010.450-0.5high
1^3D_210.15010.147-3.2high
2^3D_210.45010.449-1.3high
1^3D_310.16010.155-5.4high
2^3D_310.45010.455+5.2high
1^1F_310.35010.354+4.3medium
1^3F_310.35010.354+4.3medium
1^3F_410.36010.358-2.3medium

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.

statecentral contribution GeVcontact MeVL·S(vec) MeVL·S(Thomas) MeVL·S total MeVtensor MeVannihilation MeVspin + annihilation MeVpredicted GeV
1^1S_09.452-58.7+0.0+0.0+0.0+0.0+0.0-58.79.393
2^1S_09.999-24.6+0.0+0.0+0.0+0.0+0.0-24.69.975
3^1S_010.350-17.3+0.0+0.0+0.0+0.0+0.0-17.310.332
1^3S_19.445+13.6+0.0+0.0+0.0+0.0+0.0+13.69.459
2^3S_19.998+6.5+0.0+0.0+0.0+0.0+0.0+6.510.004
1^3D_110.149+0.3-15.4+4.8-10.6-1.4+0.0-11.810.137
3^3S_110.349+4.8+0.0+0.0+0.0+0.0+0.0+4.810.354
2^3D_110.450+0.2-12.5+3.7-8.7-1.2+0.0-9.710.441
4^3S_110.629+4.0+0.0+0.0+0.0+0.0+0.0+4.010.633
3^3D_110.707+0.2-10.8+3.1-7.7-1.0+0.0-8.510.698
5^3S_110.871+3.5+0.0+0.0+0.0+0.0+0.0+3.510.875
6^3S_111.089+3.2+0.0+0.0+0.0+0.0+0.0+3.211.092
1^1P_19.883-2.6+0.0+0.0+0.0+0.0+0.0-2.69.881
2^1P_110.252-2.0+0.0+0.0+0.0+0.0+0.0-2.010.250
1^3P_09.888+1.1-38.7+4.8-33.8-10.5+0.0-43.29.845
2^3P_010.254+0.8-26.1+3.3-22.8-7.0+0.0-28.910.225
1^3P_19.883+0.9-16.3+2.3-14.0+4.5+0.0-8.69.875
2^3P_110.252+0.7-11.5+1.6-9.9+3.1+0.0-6.110.246
1^3P_29.884+0.8+14.2-2.2+12.0-0.8+0.0+12.09.896
2^3P_210.252+0.6+10.3-1.6+8.7-0.6+0.0+8.710.261
1^3F_210.355+0.1-9.5+4.9-4.6-0.5+0.0-5.110.350
1^1D_210.148-0.7+0.0+0.0+0.0+0.0+0.0-0.710.148
2^1D_210.450-0.6+0.0+0.0+0.0+0.0+0.0-0.610.450
1^3D_210.148+0.2-4.8+1.6-3.3+1.4+0.0-1.710.147
2^3D_210.450+0.2-3.9+1.2-2.7+1.1+0.0-1.410.449
1^3D_310.149+0.2+9.2-3.1+6.1-0.4+0.0+6.010.155
2^3D_310.450+0.2+7.5-2.4+5.1-0.3+0.0+5.010.455
1^1F_310.355-0.3+0.0+0.0+0.0+0.0+0.0-0.310.354
1^3F_310.355+0.1-2.3+1.2-1.1+0.7+0.0-0.310.354
1^3F_410.355+0.1+6.7-3.6+3.2-0.2+0.0+3.010.358

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.

stateunmixed GeVmixed GeVoffdiag MeVlower-L componenthigher-L component
2^3S_110.00410.004+0.2+1.000-0.001
1^3D_110.13710.137+0.2+0.001+1.000
3^3S_110.35410.354+0.0+1.000-0.000
2^3D_110.44110.441+0.0+0.000+1.000
4^3S_110.63310.633-0.0+1.000+0.001
3^3D_110.69810.698-0.0-0.001+1.000
2^3P_210.26110.261-0.0+1.000+0.000
1^3F_210.35010.350-0.0-0.000+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.

multipletstatesreference GeVbaseline GeVresidual MeV
1D410.15210.148-3.7
2D410.44810.450+1.5
3D110.70010.698-1.7
1F410.35310.355+1.4
1P49.8869.882-3.4
2P410.25210.251-1.3
1S29.4459.442-2.6
2S29.9959.997+1.7
3S210.34810.348+0.7
4S110.63010.633+2.8
5S110.88010.875-5.5
6S111.10011.092-7.7

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.