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| Content Provider | Springer Nature Link |
|---|---|
| Author | Lee, D. |
| Copyright Year | 2008 |
| Abstract | The symmetric heavy-light ansatz is a method for finding the ground state of any dilute unpolarized system of attractive two-component fermions. Operationally it can be viewed as a generalization of the Kohn-Sham equations in density functional theory applied to N -body density correlations. While the original Hamiltonian has an exact Z2 symmetry, the heavy-light ansatz breaks this symmetry by skewing the mass ratio of the two components. In the limit where one component is infinitely heavy, the many-body problem can be solved in terms of single-particle orbitals. The original Z2 symmetry is recovered by enforcing Z2 symmetry as a constraint on N -body density correlations for the two components. For the 1D, 2D, and 3D attractive Hubbard models the method is in very good agreement with exact Lanczos calculations for few-body systems at arbitrary coupling. For the 3D attractive Hubbard model there is very good agreement with lattice Monte Carlo results for many-body systems in the limit of infinite scattering length. |
| Starting Page | 171 |
| Ending Page | 187 |
| Page Count | 17 |
| File Format | |
| ISSN | 14346001 |
| Journal | The European Physical Journal A - Hadrons and Nuclei |
| Volume Number | 35 |
| Issue Number | 2 |
| e-ISSN | 1434601X |
| Language | English |
| Publisher | Società Italiana di Fisica |
| Publisher Date | 2008-03-07 |
| Publisher Place | Bologna |
| Access Restriction | One Nation One Subscription (ONOS) |
| Subject Keyword | Nuclear Physics, Heavy Ions, Hadrons Elementary Particles and Nuclei Nuclear Fusion |
| Content Type | Text |
| Resource Type | Article |
| Subject | Nuclear and High Energy Physics |
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