Communication: Random phase approximation renormalized many-body perturbation theory

2013 ◽  
Vol 139 (17) ◽  
pp. 171103 ◽  
Author(s):  
Jefferson E. Bates ◽  
Filipp Furche
2006 ◽  
Vol 05 (04) ◽  
pp. 945-956
Author(s):  
GEETHA GOPAKUMAR ◽  
CHIRANJIB SUR ◽  
BHANU PRATAP DAS ◽  
RAJAT K. CHAUDHURI ◽  
DEBASHIS MUKHERJEE ◽  
...  

The connections between the Random Phase Approximation (RPA) and Many-Body Perturbation Theory (MBPT) and its all order generalization, the Coupled-Cluster Theory (CCT), have been explored. Explicit expressions have been derived for the electric dipole amplitudes for allowed and forbidden transitions induced by the parity non-conserving neutral weak interaction. The Goldstone diagrams associated with the RPA terms in both cases are shown to arise in MBPT and CCT, and the numerical verification of this relationship is made for the allowed electric dipole transitions.


2020 ◽  
Vol 9 ◽  
pp. 211
Author(s):  
O. Civitarese

The nuclear structure physics of double beta decay transitions is reviewed starting from the consideration of fundamental symmetries of the nuclear many body problem. The problems found in the use of the Quasiparticle Random Phase Approximation (QRPA) and related approximations, in dealing with the calculation of nuclear double beta decay observables, are understood in terms of the mixing between isospin collective and intrinsic variables.


2019 ◽  
Vol 16 (1) ◽  
pp. 427-442 ◽  
Author(s):  
Marcin Modrzejewski ◽  
Sirous Yourdkhani ◽  
Jiří Klimeš

2021 ◽  
Vol 17 (2) ◽  
pp. 804-817
Author(s):  
Marcin Modrzejewski ◽  
Sirous Yourdkhani ◽  
Szymon Śmiga ◽  
Jiří Klimeš

Open Physics ◽  
2009 ◽  
Vol 7 (4) ◽  
Author(s):  
Željana Bonačić Lošić ◽  
Paško Županović

AbstractThe dielectric response is considered within models of a one-band metal, a two-band insulator and a two-band metal using the semi-classical approximation. Corresponding dielectric functions are found. The dielectric function of two-band metal is found to be the interpolation between the Sellmeyer and Lorenz-Lorentz expressions, respectively. The frequencies of the collective modes are identified as the zeroes of the dielectric functions. The correspondence between the semi-classical approach used in this paper and the many-body calculation within the random-phase approximation is established.


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