1993
DOI: 10.1103/physrevd.48.5863
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Renormalization of Hamiltonians

Abstract: Abstract. A matrix model of an asymptotically free theory with a bound state is solved using a perturbative similarity renormalization group for hamiltonians. An effective hamiltonian with a small width, calculated including the first three terms in the perturbative expansion, is projected on a small set of effective basis states. The resulting small hamiltonian matrix is diagonalized and the exact bound state energy is obtained with accuracy of order 10%. Then, a brief description and an elementary illustrati… Show more

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Cited by 488 publications
(489 citation statements)
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“…The many-body data, e.g., selected radii, are chosen in order to improve the deficient saturation behavior of chiral interactions that are used as input for nuclear many-body calculations. The first interaction optimized with this protocol is NNLO sat [26], which is able to accurately describe the ground-state energies and charge radii of 40,48 Ca at the same time. Following the same philosophy but not the same approach, Shirokov et al have produced Daejeon16, a softened chiral N N interaction that has been tuned for the description of light nuclei without explicit 3N forces [27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%
“…The many-body data, e.g., selected radii, are chosen in order to improve the deficient saturation behavior of chiral interactions that are used as input for nuclear many-body calculations. The first interaction optimized with this protocol is NNLO sat [26], which is able to accurately describe the ground-state energies and charge radii of 40,48 Ca at the same time. Following the same philosophy but not the same approach, Shirokov et al have produced Daejeon16, a softened chiral N N interaction that has been tuned for the description of light nuclei without explicit 3N forces [27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%
“…As shown by the red lines in Fig. 3(a), the further inclusion of square integrable energy-eigenstates of the 7 He nucleus (in the present calculation four 3/2 − states, of which only the first produces a substantial effect on the 2 P 3/2 resonance) compensates for missing higher 6 He excitations, leading to a much faster convergence rate. Finally, the present NCSMC calculation yields the well established 3/2 − g.s.…”
Section: The Unbound 7 He Nucleus As a Testing Groundmentioning
confidence: 74%
“…[11] is augmented by coupling fourteen (of which three 3/2 − and one 1/2 − ) NCSM eigenstates of the 5 He compound nucleus [15]. As for the 7 He nucleus in the previous section, the convergence with respect to the number of target states is now excellent. Further, the total cross section, presented in Fig.…”
Section: Three-nucleon Forces and Continuummentioning
confidence: 85%
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