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Perturbative chiral nucleon–nucleon potential for the 3P0 partial wave
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Rui Peng,Songlin Lyu,Bingwei Long
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Table 2. The values taken by the counterterms in the perturbative scheme (15).
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Λ (MeV) | ${C}_{0}{{\rm{\Lambda }}}^{3}$ | ${C}_{1}{{\rm{\Lambda }}}^{3}$ | ${D}_{0}{{\rm{\Lambda }}}^{5}$ | ${C}_{2}{{\rm{\Lambda }}}^{3}$ | ${D}_{1}{{\rm{\Lambda }}}^{5}$ | ${E}_{0}{{\rm{\Lambda }}}^{7}$ |
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400.0 | 1.79 | 1.45 | −0.0330 | −0.242 | −2.87 | 3.55 | 800.0 | 15.4 | 27.1 | 32.9 | 69.1 | −12.7 | 516 | 1200.0 | 51.0 | 335 | 536 | $6.01\times {10}^{3}$ | $6.22\times {10}^{3}$ | $2.57\times {10}^{4}$ | 2400.0 | 408 | $2.70\times {10}^{4}$ | $4.80\times {10}^{4}$ | $5.35\times {10}^{6}$ | $6.48\times {10}^{6}$ | $2.29\times {10}^{7}$ |
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