We present a Pfaffian formula for projection and symmetry restoration for wave functions of the general Bogoliubov form, including quasiparticle excited states and linear combinations of them. This solves a long-standing problem in calculating states of good symmetry, arising from the sign ambiguity of the commonly used determinant formula. A simple example is given of projecting a good particle number and angular momentum from a Bogoliubov wave function in the Fock space of a single j-shellThis work was supported in part by the U.S. Department of Energy under Grant No. DE-FG02- 00ER41132, and by the National Science Foundation under Grant No. PHY-0835543. The work of L. M. R. was supported by MICINN (Spain) under Grants No. FPA2009-08958, ...
AbstractWe present new formulae for the matrix elements of one-body and two-body physical operators,...
We present the numerical code $$\textsf {TAURUS}_{\textsf {vap}}$$ that solves the variation after p...
We present new formulae for the matrix elements of one-body and two-body physical operators, which a...
In this Letter, we present a new expression for the overlaps of wave functions in Hartree-Fock-Bogol...
International audienceBackground: Many quantal many-body methods that aim at the description of self...
The restoration of particle number and angular momentum symmetry using projection operators has been...
We consider symmetry-projected Hartree-Fock trial wave functions in constrained-path Monte Carlo (CP...
In the present work, projection methods employed to restore the spontaneously broken symmetry in the...
Projected Hartree–Fock (PHF) theory can restore important symmetries to broken symmetry wave functio...
Given elementary inter-nucleon interactions,the resolution of the A-body Schrödinger equation gives ...
AbstractOverlap between Hartree–Fock–Bogoliubov (HFB) vacua is very important in the beyond mean-fie...
The mean-field approximation based on effective interactions or density functionals plays a pivotal ...
Background: State-of-the-art multi-reference energy density functional calculations require the comp...
The numerical solution of the recently formulated number-projected Hartree-Fock-Bogoliubov equations...
Slater determinants provide a convenient basis for expanding many-electron wave functions. In second...
AbstractWe present new formulae for the matrix elements of one-body and two-body physical operators,...
We present the numerical code $$\textsf {TAURUS}_{\textsf {vap}}$$ that solves the variation after p...
We present new formulae for the matrix elements of one-body and two-body physical operators, which a...
In this Letter, we present a new expression for the overlaps of wave functions in Hartree-Fock-Bogol...
International audienceBackground: Many quantal many-body methods that aim at the description of self...
The restoration of particle number and angular momentum symmetry using projection operators has been...
We consider symmetry-projected Hartree-Fock trial wave functions in constrained-path Monte Carlo (CP...
In the present work, projection methods employed to restore the spontaneously broken symmetry in the...
Projected Hartree–Fock (PHF) theory can restore important symmetries to broken symmetry wave functio...
Given elementary inter-nucleon interactions,the resolution of the A-body Schrödinger equation gives ...
AbstractOverlap between Hartree–Fock–Bogoliubov (HFB) vacua is very important in the beyond mean-fie...
The mean-field approximation based on effective interactions or density functionals plays a pivotal ...
Background: State-of-the-art multi-reference energy density functional calculations require the comp...
The numerical solution of the recently formulated number-projected Hartree-Fock-Bogoliubov equations...
Slater determinants provide a convenient basis for expanding many-electron wave functions. In second...
AbstractWe present new formulae for the matrix elements of one-body and two-body physical operators,...
We present the numerical code $$\textsf {TAURUS}_{\textsf {vap}}$$ that solves the variation after p...
We present new formulae for the matrix elements of one-body and two-body physical operators, which a...