Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation

Dynamical description of low energy fission is, in our full microscopic approach, decomposed in two steps. In the first step we generate the Potential Energy Surface (PES) of the compound system we want to describe with the Hartree-Fock-Bogoliubov (HFB) method with a Gogny interaction. The second st...

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Main Authors: Verrière Marc, Dubray Noël, Schunck Nicolas, Regnier David, Dossantos-Uzarralde Pierre
Format: Article
Language:English
Published: EDP Sciences 2017-01-01
Series:EPJ Web of Conferences
Online Access:https://doi.org/10.1051/epjconf/201714604034
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spelling doaj-f40d2bee41224b53808008ca61e4e9aa2021-08-02T13:40:59ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011460403410.1051/epjconf/201714604034epjconf-nd2016_04034Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equationVerrière Marc0Dubray Noël1Schunck Nicolas2Regnier David3Dossantos-Uzarralde Pierre4CEA, DAM, DIFCEA, DAM, DIFNuclear and Chemical Science Division, Lawrence Livermore National LaboratoryCEA, DAM, DIFCEA, DAM, DIFDynamical description of low energy fission is, in our full microscopic approach, decomposed in two steps. In the first step we generate the Potential Energy Surface (PES) of the compound system we want to describe with the Hartree-Fock-Bogoliubov (HFB) method with a Gogny interaction. The second step uses the Time Dependent Generator Coordinate Method (TDGCM) with the Gaussian Overlap Approximation (GOA). The GOA holds in two assumptions: the overlap matrix between HFB states has a gaussian shape (with respect to the difference between coordinates of states in deformation space); and the expectation value of the collective hamiltonian between these states can be expanded up to order two, leading in this case to a Schrödinger-like equation. In this work we replace TDGCM+GOA in the second step of our approach by an exact treatment of the TDGCM. The main equation of this method is the time-dependent Hill-Wheeler equation and involves two objects: the overlap matrix and the collective hamiltonian. We first calculate these matrices on a PES. Then, we build an “exact TDGCM” solver using a finite element method and a Crank-Nicolson scheme. In this talk, we will present the time-dependent Hill-Wheeler equation and discretization schemes (in time and deformation space). The analytic calculation of overlap matrix and collective hamiltonian will be detailed. Finally, first results with an exact treatment of the TDGCM will be discussed.https://doi.org/10.1051/epjconf/201714604034
collection DOAJ
language English
format Article
sources DOAJ
author Verrière Marc
Dubray Noël
Schunck Nicolas
Regnier David
Dossantos-Uzarralde Pierre
spellingShingle Verrière Marc
Dubray Noël
Schunck Nicolas
Regnier David
Dossantos-Uzarralde Pierre
Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
EPJ Web of Conferences
author_facet Verrière Marc
Dubray Noël
Schunck Nicolas
Regnier David
Dossantos-Uzarralde Pierre
author_sort Verrière Marc
title Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
title_short Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
title_full Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
title_fullStr Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
title_full_unstemmed Fission description: First steps towards a full resolution of the time-dependent Hill-Wheeler equation
title_sort fission description: first steps towards a full resolution of the time-dependent hill-wheeler equation
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2017-01-01
description Dynamical description of low energy fission is, in our full microscopic approach, decomposed in two steps. In the first step we generate the Potential Energy Surface (PES) of the compound system we want to describe with the Hartree-Fock-Bogoliubov (HFB) method with a Gogny interaction. The second step uses the Time Dependent Generator Coordinate Method (TDGCM) with the Gaussian Overlap Approximation (GOA). The GOA holds in two assumptions: the overlap matrix between HFB states has a gaussian shape (with respect to the difference between coordinates of states in deformation space); and the expectation value of the collective hamiltonian between these states can be expanded up to order two, leading in this case to a Schrödinger-like equation. In this work we replace TDGCM+GOA in the second step of our approach by an exact treatment of the TDGCM. The main equation of this method is the time-dependent Hill-Wheeler equation and involves two objects: the overlap matrix and the collective hamiltonian. We first calculate these matrices on a PES. Then, we build an “exact TDGCM” solver using a finite element method and a Crank-Nicolson scheme. In this talk, we will present the time-dependent Hill-Wheeler equation and discretization schemes (in time and deformation space). The analytic calculation of overlap matrix and collective hamiltonian will be detailed. Finally, first results with an exact treatment of the TDGCM will be discussed.
url https://doi.org/10.1051/epjconf/201714604034
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