scholarly journals The similarity renormalization group for three-body interactions in one dimension

2011 ◽  
Vol 47 (10) ◽  
Author(s):  
O. Åkerlund ◽  
E. J. Lindgren ◽  
J. Bergsten ◽  
B. Grevholm ◽  
P. Lerner ◽  
...  
2019 ◽  
Vol 69 (1) ◽  
pp. 307-362 ◽  
Author(s):  
S. Ragnar Stroberg ◽  
Heiko Hergert ◽  
Scott K. Bogner ◽  
Jason D. Holt

The nuclear shell model has perhaps been the most important conceptual and computational paradigm for the understanding of the structure of atomic nuclei. While the shell model has been used predominantly in a phenomenological context, there have been efforts stretching back more than half a century to derive shell model parameters based on a realistic interaction between nucleons. More recently, several ab initio many-body methods—in particular, many-body perturbation theory, the no-core shell model, the in-medium similarity renormalization group, and coupled-cluster theory—have developed the capability to provide effective shell model Hamiltonians. We provide an update on the status of these methods and investigate the connections between them and their potential strengths and weaknesses, with a particular focus on the in-medium similarity renormalization group approach. Three-body forces are demonstrated to be important for understanding the modifications needed in phenomenological treatments. We then review some applications of these methods to comparisons with recent experimental measurements, and conclude with some remaining challenges in ab initio shell model theory.


2021 ◽  
Vol 103 (4) ◽  
Author(s):  
M. Heinz ◽  
A. Tichai ◽  
J. Hoppe ◽  
K. Hebeler ◽  
A. Schwenk

2017 ◽  
Vol 96 (3) ◽  
Author(s):  
N. M. Parzuchowski ◽  
S. R. Stroberg ◽  
P. Navrátil ◽  
H. Hergert ◽  
S. K. Bogner

Author(s):  
Lucas Happ ◽  
Matthias Zimmermann ◽  
Maxim A Efremov

Abstract We study a heavy-heavy-light three-body system confined to one space dimension in the regime where an excited state in the heavy-light subsystems becomes weakly bound. The associated two-body system is characterized by (i) the structure of the weakly-bound excited heavy-light state and (ii) the presence of deeply-bound heavy-light states. The consequences of these aspects for the behavior of the three-body system are analyzed. We find a strong indication for universal behavior of both three-body binding energies and wave functions for different weakly-bound excited states in the heavy-light subsystems.


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