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Figure 5: The demonstration of ogc for this reaction with respect to the energy in the center of mass frame(¢ = 0).

Figure 5 The demonstration of ogc for this reaction with respect to the energy in the center of mass frame(¢ = 0).

Related Figures (6)

Figure 1: One loop correction to the scattering amplitude of the nuclear interaction. The solid black lines depict the alpha particles and the dark circles depict the nuclear interactions regardless of the Coulomb interaction in the center of mass frame.
Figure 1: One loop correction to the scattering amplitude of the nuclear interaction. The solid black lines depict the alpha particles and the dark circles depict the nuclear interactions regardless of the Coulomb interaction in the center of mass frame.
Figure 2: The integral equation of the Feynman diagrams of this interaction that demon- strate Coulomb propagator as an infinite sum. The solid black lines depict the alpha particles and the dashed lines demonstrate the photon exchange between the two alpha particles and the shaded bubble demonstrate the Coulomb interaction between the two alpha particles.
Figure 2: The integral equation of the Feynman diagrams of this interaction that demon- strate Coulomb propagator as an infinite sum. The solid black lines depict the alpha particles and the dashed lines demonstrate the photon exchange between the two alpha particles and the shaded bubble demonstrate the Coulomb interaction between the two alpha particles.
Figure 3: s-wave phase shifts at NLO and NNLO and comparison with experimental data (28, 29, 30, 31].
Figure 3: s-wave phase shifts at NLO and NNLO and comparison with experimental data (28, 29, 30, 31].
Figure 4: The demonstration of oc for this reaction with respect to the energy in the center of mass frame(é = 0). T-matrixes are calculated by considering the halo Effective Field Theory for this scattering at low energy. The relation for the differential cross section is [23]
Figure 4: The demonstration of oc for this reaction with respect to the energy in the center of mass frame(é = 0). T-matrixes are calculated by considering the halo Effective Field Theory for this scattering at low energy. The relation for the differential cross section is [23]
Figure 6: The demonstration of o; for this reaction with respect to the energy in the center of mass frame(é = 0).
Figure 6: The demonstration of o; for this reaction with respect to the energy in the center of mass frame(é = 0).
Table 1: Comparison between results by considering the coulomb and short range interaction and the total cross section.
Table 1: Comparison between results by considering the coulomb and short range interaction and the total cross section.
Related topics:
PhysicsScattering TheoryElastic ScatteringHaloMott scattering
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