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np=2.77±0.05); however, note that these values are highly model dependent, since the two experimental quantities that the analysis is based upon [namely, the np total cross section at "zero" energy and the (n,p) coherent scattering length] determine only the two np scattering lengths and not the effective ranges. A better way to determine the effective ranges is to simply use the predictions from modern high-precision NN potentials which reproduce the empirical values for the scattering lengths accurately (such as the CD-Bonn potential).
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np=2.77±0.05); however, note that these values are highly model dependent, since the two experimental quantities that the analysis is based upon [namely, the np total cross section at "zero" energy and the (n,p) coherent scattering length] determine only the two np scattering lengths and not the effective ranges. A better way to determine the effective ranges is to simply use the predictions from modern high-precision NN potentials which reproduce the empirical values for the scattering lengths accurately (such as the CD-Bonn potential).
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np=2.77±0.05); however, note that these values are highly model dependent, since the two experimental quantities that the analysis is based upon [namely, the np total cross section at "zero" energy and the (n,p) coherent scattering length] determine only the two np scattering lengths and not the effective ranges. A better way to determine the effective ranges is to simply use the predictions from modern high-precision NN potentials which reproduce the empirical values for the scattering lengths accurately (such as the CD-Bonn potential).
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np=2.77±0.05); however, note that these values are highly model dependent, since the two experimental quantities that the analysis is based upon [namely, the np total cross section at "zero" energy and the (n,p) coherent scattering length] determine only the two np scattering lengths and not the effective ranges. A better way to determine the effective ranges is to simply use the predictions from modern high-precision NN potentials which reproduce the empirical values for the scattering lengths accurately (such as the CD-Bonn potential).
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n while keeping all meson parameters (including the ones for the σ's) unchanged.
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39
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note
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lab , the c.m. momentum q is larger for nn scattering as compared to pp. Both effects cause small difference in the phase shifts. Numbers listed in column "kinematics" of Table III include both effects.
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40
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85189458091
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note
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Since CD-Bonn is an OBE model, it does not include the TBE (and πγ) diagrams explicitly. Therefore, we parametrize the TBE predicted by the Bonn full model (and the πγ contributions) by adjusting the parameters of the two σ mesons of CD-Bonn such that the above charge-dependence is accurately reproduced. For more details, see Sec. IV.
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2π/4π = 13.6 instead of 14.4). These predictions are typically about 5% smaller than what was reported in Ref. [6].
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