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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.

statereference GeVbaseline GeVresidual MeVconfidence
1^1S_00.5200.520+0.0medium
1^1S_00.9600.960+0.0medium
2^1S_01.4401.440-0.0medium
2^1S_01.6301.630-0.0medium
1^3S_10.7800.780-0.1medium
1^3S_11.0201.020+0.4medium
2^3S_11.4601.457-3.4medium
1^3D_11.6601.664+4.3medium
2^3S_11.6901.690-0.4medium
1^3D_11.8801.879-1.4medium
1^1P_11.2201.218-1.5medium
1^1P_11.4701.473+3.1medium
2^1P_11.7801.777-3.1medium
2^1P_12.0102.008-2.0medium
1^3P_01.0901.087-3.1medium
1^3P_01.3601.355-5.5medium
2^3P_01.7801.778-1.8medium
2^3P_01.9901.986-4.4medium
1^3P_11.2401.238-2.5medium
1^3P_11.4801.480-0.0medium
2^3P_11.8201.818-2.0medium
2^3P_12.0302.027-2.7medium
1^3P_21.2801.276-4.4medium
1^3P_21.5301.532+1.6medium
2^3P_21.8201.815-4.6medium
2^3P_22.0402.042+2.5medium
1^3F_22.0502.054+4.4medium
1^3F_22.2402.243+2.6medium
1^1D_21.6801.680+0.5medium
1^1D_21.8901.893+3.0medium
1^3D_21.7001.696-4.3medium
1^3D_21.9101.904-5.5medium
1^3D_31.6801.683+3.1medium
1^3D_31.9001.897-3.0medium
1^3G_32.3702.370+0.3medium
1^3G_32.5402.542+1.8medium
1^1F_32.0302.033+2.8medium
1^1F_32.2202.223+2.8medium
1^3F_32.0502.046-4.0medium
1^3F_32.2302.234+4.1medium
1^3F_42.0102.008-2.4medium
1^3F_42.2002.202+2.4medium
1^1G_42.3302.333+3.2medium
1^1G_42.5102.507-3.0medium
1^3G_42.3402.344+4.3medium
1^3G_42.5202.517-2.9medium
1^3G_52.3002.296-3.6medium
1^3G_52.4702.475+4.7medium

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_00.764-614.5+0.0+0.0+0.0+0.0+370.9-243.50.520
1^1S_00.995-339.8+0.0+0.0+0.0+0.0+304.8-35.00.960
2^1S_01.397-104.8+0.0+0.0+0.0+0.0+148.0+43.21.440
2^1S_01.653-76.0+0.0+0.0+0.0+0.0+52.7-23.31.630
1^3S_10.667+104.1+0.0+0.0+0.0+0.0+8.7+112.80.780
1^3S_10.949+67.9+0.0+0.0+0.0+0.0+3.3+71.21.020
2^3S_11.411+44.2+0.0+0.0+0.0+0.0+0.9+45.11.457
1^3D_11.700+3.1-127.5+98.6-29.0-9.4+0.0-35.21.664
2^3S_11.660+29.3+0.0+0.0+0.0+0.0+0.6+29.91.690
1^3D_11.906+2.0-101.8+81.1-20.7-8.3+0.0-27.01.879
1^1P_11.262-43.2+0.0+0.0+0.0+0.0+0.0-43.21.218
1^1P_11.500-26.5+0.0+0.0+0.0+0.0+0.0-26.51.473
2^1P_11.810-32.7+0.0+0.0+0.0+0.0+0.0-32.71.777
2^1P_12.028-20.1+0.0+0.0+0.0+0.0+0.0-20.12.008
1^3P_01.284+18.0-267.6+106.6-161.0-53.9+0.0-196.91.087
1^3P_01.519+11.5-211.6+82.1-129.4-46.8+0.0-164.71.355
2^3P_01.807+10.3-109.7+91.6-18.1-20.9+0.0-28.71.778
2^3P_02.025+6.6-88.8+60.8-28.0-18.2+0.0-39.61.986
1^3P_11.261+13.9-120.8+57.6-63.1+25.4+0.0-23.91.238
1^3P_11.500+8.9-93.8+42.9-50.9+21.6+0.0-20.41.480
2^3P_11.807+9.4-53.9+45.4-8.5+10.3+0.0+11.21.818
2^3P_12.027+6.2-44.4+29.7-14.7+9.2+0.0+0.62.027
1^3P_21.268+8.6+99.7-65.2+34.5-4.5-30.9+7.71.276
1^3P_21.504+6.1+78.2-44.9+33.2-3.8-7.8+27.71.532
2^3P_21.808+8.2+53.5-44.5+9.1-2.1-7.8+7.41.815
2^3P_22.028+5.4+43.9-29.0+14.9-1.9-3.7+14.82.042
1^3F_22.041+0.7-74.9+90.9+16.0-3.4+0.0+13.32.054
1^3F_22.228+0.5-60.7+78.1+17.3-3.1+0.0+14.72.243
1^1D_21.687-6.8+0.0+0.0+0.0+0.0+0.0-6.81.680
1^1D_21.898-4.6+0.0+0.0+0.0+0.0+0.0-4.61.893
1^3D_21.688+2.4-38.7+35.2-3.5+8.8+0.0+7.71.696
1^3D_21.898+1.6-30.9+27.9-2.9+7.8+0.0+6.41.904
1^3D_31.693+1.6+68.0-77.1-9.1-2.3+0.0-9.81.683
1^3D_31.901+1.2+55.0-57.8-2.8-2.0+0.0-3.61.897
1^3G_32.338+0.2-50.2+84.1+33.9-1.7+0.0+32.42.370
1^3G_32.510+0.1-41.3+74.7+33.5-1.6+0.0+32.12.542
1^1F_32.034-1.6+0.0+0.0+0.0+0.0+0.0-1.62.033
1^1F_32.224-1.2+0.0+0.0+0.0+0.0+0.0-1.22.223
1^3F_32.035+0.6-17.4+24.1+6.7+4.1+0.0+11.32.046
1^3F_32.224+0.4-14.2+20.1+5.9+3.7+0.0+10.02.234
1^3F_42.038+0.4+47.6-77.4-29.8-1.3+0.0-30.62.008
1^3F_42.226+0.3+39.3-61.9-22.7-1.2+0.0-23.52.202
1^1G_42.334-0.4+0.0+0.0+0.0+0.0+0.0-0.42.333
1^1G_42.507-0.3+0.0+0.0+0.0+0.0+0.0-0.32.507
1^3G_42.334+0.1-9.5+17.6+8.2+2.2+0.0+10.62.344
1^3G_42.507+0.1-7.8+15.3+7.5+2.1+0.0+9.72.517
1^3G_52.336+0.1+35.4-74.7-39.3-0.8+0.0-40.02.296
1^3G_52.509+0.1+29.5-62.8-33.3-0.7+0.0-33.92.475

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.

stateschemeunmixed GeVmixed GeVshift MeV
1^1S_0calibrated_p10.1490.520+370.9
1^1S_0calibrated_p10.6550.960+304.8
2^1S_0calibrated_p11.2921.440+148.0
2^1S_0calibrated_p11.5771.630+52.7
1^3S_1general_eq160.7710.780+8.7
1^3S_1general_eq161.0171.020+3.3
2^3S_1general_eq161.4561.457+0.9
1^3D_1ideal1.6641.664+0.0
2^3S_1general_eq161.6891.690+0.6
1^3D_1ideal1.8791.879+0.0
1^1P_1ideal1.2181.218+0.0
1^1P_1ideal1.4731.473+0.0
2^1P_1ideal1.7771.777+0.0
2^1P_1ideal2.0082.008+0.0
1^3P_0ideal1.0871.087+0.0
1^3P_0ideal1.3551.355+0.0
2^3P_0ideal1.7781.778+0.0
2^3P_0ideal1.9861.986+0.0
1^3P_1ideal1.2381.238+0.0
1^3P_1ideal1.4801.480+0.0
2^3P_1ideal1.8181.818+0.0
2^3P_1ideal2.0272.027+0.0
1^3P_2general_eq161.3071.276-30.9
1^3P_2general_eq161.5391.532-7.8
2^3P_2general_eq161.8231.815-7.8
2^3P_2general_eq162.0462.042-3.7
1^3F_2ideal2.0542.054+0.0
1^3F_2ideal2.2432.243+0.0
1^1D_2ideal1.6801.680+0.0
1^1D_2ideal1.8931.893+0.0
1^3D_2ideal1.6961.696+0.0
1^3D_2ideal1.9041.904+0.0
1^3D_3ideal1.6831.683+0.0
1^3D_3ideal1.8971.897+0.0
1^3G_3ideal2.3702.370+0.0
1^3G_3ideal2.5422.542+0.0
1^1F_3ideal2.0332.033+0.0
1^1F_3ideal2.2232.223+0.0
1^3F_3ideal2.0462.046+0.0
1^3F_3ideal2.2342.234+0.0
1^3F_4ideal2.0082.008+0.0
1^3F_4ideal2.2022.202+0.0
1^1G_4ideal2.3332.333+0.0
1^1G_4ideal2.5072.507+0.0
1^3G_4ideal2.3442.344+0.0
1^3G_4ideal2.5172.517+0.0
1^3G_5ideal2.2962.296+0.0
1^3G_5ideal2.4752.475+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.

multipletstatesreference GeVbaseline GeVresidual MeV
1D81.7891.789-0.5
1F82.1262.127+1.3
1G82.4192.419+0.6
1P81.3641.363-1.0
2P81.9161.914-1.9
1S40.8600.860+0.1
2S41.5651.564-1.4

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.