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Effective Field Theory and the No-Core Shell Model

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Figure

Fig. 1. Running with the ultraviolet cutoMeV, while the continuous lines represent a fit to a linear depen-dence of 1ff for two observables:the first (0+; 0) excited state in 4He (lower panel) and the 6Liground-state energy (upper panel)
Fig. 2. Running of the energies of the first four excited states for two trapped particles at unitarity
Fig. 3. Running of the energies of the first four excited states for two-trapped particles at unitarity with a non-vanishing physical range,b/a2 = 0.15.The coupling constants are fixed so that the ground-state, and the first and second excited states given by
Fig. 4. The running of the lowest L = 0 (lower panel) and L = 1levels at LO, NLO and N2LO

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