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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.

statereference GeVbaseline GeVresidual MeVconfidence
1^1S_02.9702.967-2.9high
2^1S_03.6203.626+5.8high
3^1S_04.0604.064+3.6high
1^3S_13.1003.091-8.6high
2^3S_13.6803.679-0.9high
1^3D_13.8203.818-1.7high
3^3S_14.1004.100+0.0high
2^3D_14.1904.194+4.1high
4^3S_14.4504.449-1.2medium
3^3D_14.5204.520-0.5medium
1^1P_13.5203.515-4.9high
2^1P_13.9603.956-3.8high
1^3P_03.4403.443+2.9high
2^3P_03.9203.916-3.5high
1^3P_13.5103.508-1.8high
2^3P_13.9503.953+3.2high
1^3P_23.5503.548-1.8high
2^3P_23.9803.980-0.5high
1^3F_24.0904.091+1.4medium
1^1D_23.8403.837-3.4high
2^1D_24.2104.208-2.5high
1^3D_23.8403.837-2.6high
2^3D_24.2104.208-1.8high
1^3D_33.8503.848-2.3high
2^3D_34.2204.217-3.4high
1^1F_34.0904.094+3.8medium
1^3F_34.1004.096-3.9medium
1^3F_44.0904.095+4.8medium

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_03.078-111.4+0.0+0.0+0.0+0.0+0.0-111.42.967
2^1S_03.667-41.0+0.0+0.0+0.0+0.0+0.0-41.03.626
3^1S_04.091-27.1+0.0+0.0+0.0+0.0+0.0-27.14.064
1^3S_13.066+25.6+0.0+0.0+0.0+0.0+0.0+25.63.091
2^3S_13.666+12.7+0.0+0.0+0.0+0.0+0.0+12.73.679
1^3D_13.841+0.7-42.4+23.2-19.3-3.9+0.0-22.43.818
3^3S_14.091+9.0+0.0+0.0+0.0+0.0+0.0+9.04.100
2^3D_14.210+0.6-31.2+17.2-14.0-2.7+0.0-16.24.194
4^3S_14.442+7.2+0.0+0.0+0.0+0.0+0.0+7.24.449
3^3D_14.533+0.5-25.5+13.8-11.7-2.2+0.0-13.34.520
1^1P_13.523-8.2+0.0+0.0+0.0+0.0+0.0-8.23.515
2^1P_13.963-6.4+0.0+0.0+0.0+0.0+0.0-6.43.956
1^3P_03.535+3.7-94.6+22.8-71.8-23.8+0.0-91.93.443
2^3P_03.964+2.5-52.4+14.7-37.8-12.4+0.0-47.83.916
1^3P_13.524+2.8-39.8+11.1-28.7+10.2+0.0-15.63.508
2^3P_13.963+2.2-24.9+7.3-17.6+6.0+0.0-9.43.953
1^3P_23.525+2.2+33.6-10.7+22.9-1.8+0.0+23.33.548
2^3P_23.963+1.8+22.9-7.2+15.7-1.1+0.0+16.33.980
1^3F_24.095+0.2-26.1+23.6-2.5-1.5+0.0-3.74.091
1^1D_23.838-1.9+0.0+0.0+0.0+0.0+0.0-1.93.837
2^1D_24.209-1.6+0.0+0.0+0.0+0.0+0.0-1.64.208
1^3D_23.839+0.6-13.0+7.6-5.4+3.6+0.0-1.23.837
2^3D_24.209+0.5-9.8+5.7-4.1+2.6+0.0-1.04.208
1^3D_33.839+0.6+24.0-15.0+9.0-1.0+0.0+8.63.848
2^3D_34.210+0.5+18.6-11.3+7.3-0.7+0.0+7.04.217
1^1F_34.094-0.7+0.0+0.0+0.0+0.0+0.0-0.74.094
1^3F_34.094+0.2-6.2+5.9-0.4+1.8+0.0+1.64.096
1^3F_44.095+0.2+17.8-17.4+0.4-0.6+0.0+0.04.095

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.

stateunmixed GeVmixed GeVoffdiag MeVlower-L componenthigher-L component
2^3S_13.6793.679+1.1+1.000-0.008
1^3D_13.8183.818+1.1+0.008+1.000
3^3S_14.1004.100+0.7+1.000-0.007
2^3D_14.1944.194+0.7+0.007+1.000
4^3S_14.4494.449+0.5+1.000-0.007
3^3D_14.5194.520+0.5+0.007+1.000
2^3P_23.9803.980+0.1+1.000-0.001
1^3F_24.0914.091+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.

multipletstatesreference GeVbaseline GeVresidual MeV
1D43.8413.838-2.6
2D44.2114.209-1.6
3D14.5204.520-0.5
1F44.0934.094+1.7
1P43.5233.521-2.2
2P43.9623.962-0.6
1S23.0683.060-7.2
2S23.6653.666+0.8
3S24.0904.091+0.9
4S14.4504.449-1.2

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.