22 research outputs found
A Class of Exactly Solvable Pairing Models
We present three classes of exactly solvable models for fermion and boson
systems, based on the pairing interaction. These models are solvable in any
dimension. As an example we show the first results for fermion interacting with
repulsive pairing forces in a two dimensional square lattice. Inspite of the
repulsive pairing force the exact results show attractive pair correlations.Comment: 5 pages, 1 figur
Structure of the number projected BCS wave function
We study the structure of the number projected BCS (PBCS) wave function in
the particle-hole basis, displaying its similarities with coupled clusters
theory (CCT). The analysis of PBCS together with several modifications
suggested by the CCT wave function is carried out for the exactly solvable
Richardson model involving a pure pairing hamiltonian acting in a space of
equally-spaced doubly-degenerate levels. We point out the limitations of PBCS
to describe the non-superconducting regime and suggest possible avenues for
improvement.Comment: 6 pages, 4 figures. To be published in Phys. Rev.
Improvement to the Projected BCS Approximation
6 págs.; 1 fig.; XXXVIII Symposium on Nuclear Physics (Cocoyoc 2015); Open Access funded by Creative Commons Atribution Licence 3.0We consider the structure of the number projected BCS wave function in the
particle-hole basis, and use it to study several approximate treatments of pairing. The analysis
is carried out for the exactly solvable Richardson model involving a pure pairing hamiltonian
acting in a space of equally spaced doubly degenerate levels at half filling.The work was also supported in part by the Spanish MINECO under Grant No. FIS2012-34479, and in part by the US National
Science Foundation under grant # 0553127.Peer Reviewe
Pairing in 4-component fermion systems: the bulk limit of SU(4)-symmetric Hamiltonians
Fermion systems with more than two components can exhibit pairing condensates
of much more complex structure than the well-known single BCS condensate of
spin-up and spin-down fermions. In the framework of the exactly solvable SO(8)
Richardson-Gaudin model with SU(4)-symmetric Hamiltonians, we show that the BCS
approximation remains valid in the thermodynamic limit of large systems for
describing the ground state energy and the canonical and quasiparticle
excitation gaps. Correlations beyond BCS pairing give rise to a spectrum of
collective excitations, but these do not affect the bulk energy and
quasiparticle gaps.Comment: 13 pages; 2 figures; 1 tabl
A generalized Hill-Wheeler ansatz
The Hill-Wheeler ansatz for the total wave function, within the Generator Coordinate Method framework, is generalized by recourse to the theory of distributions. The ensuing approach allows one to obtain a basis that spans the collective subspace, without having to deal explicitly with the eigenvectors and eigenvalues of the overlap kernel. Applications to an exactly soluble model and anharmonic vibrations illustrate the present treatment.Facultad de Ciencias Exacta
Excited-state quantum phase transitions in the two-spin elliptic Gaudin model
10 págs.; 7 figs.We study the integrability of the two-spin elliptic Gaudin model for arbitrary values of the Hamiltonian parameters. The limit of a very large spin coupled to a small one is well described by a semiclassical approximation with just one degree of freedom. Its spectrum is divided into bands that do not overlap if certain conditions are fulfilled. In spite of the fact that there are no quantum phase transitions in each of the band heads, the bands show excited-state quantum phase transitions separating a region in which the parity symmetry is broken from another region in which time-reversal symmetry is broken. We derive analytical expressions for the critical energies in the semiclassical approximation, and confirm the results by means of exact diagonalizations for large systems. ©2016 American Physical SocietyWe acknowledge support from the Spanish Ministry of
Economy and Competitiveness through Grants No. FIS2012-
34479, No. FIS2012-35536, and from MINECO (Spain) and
FEDER (Spain) Grant No. FIS2015-63770-P.Peer Reviewe
Solving the Richardson equations close to the critical points
12 pages, 3 tables, 2 figures.--PACS nrs.: 02.30.Ik, 71.10.Li, 74.20.Fg.--Arxiv pre-print available at: http://arxiv.org/abs/math-ph/0609022We study the Richardson equations close to the critical values of the pairing
strength gc, where the occurrence of divergences precludes numerical solutions.
We derive a set of equations for determining the critical g values and the noncollapsing pair energies. Studying the behaviour of the solutions close to the
critical points, we develop a procedure to solve numerically the Richardson equations for arbitrary coupling strength.This work was supported by Spanish DGI under grant BFM2003-05316-C02-02.Peer reviewe
Many-Body Characterization of Particle-Conserving Topological Superfluids
5 págs.; 2 figs.; PACS numbers: 74.20.-z, 03.65.Vf, 74.45.+c, 74.90.+nWhat distinguishes trivial superfluids from topological superfluids in interacting many-body systems
where the number of particles is conserved? Building on a class of integrable pairing Hamiltonians, we
present a number-conserving, interacting variation of the Kitaev model, the Richardson-Gaudin-Kitaev
chain, that remains exactly solvable for periodic and antiperiodic boundary conditions. Our model allows
us to identify fermion parity switches that distinctively characterize topological superconductivity (fermion
superfluidity) in generic interacting many-body systems. Although the Majorana zero modes in this model
have only a power-law confinement, we may still define many-body Majorana operators by tuning the flux
to a fermion parity switch. We derive a closed-form expression for an interacting topological invariant and
show that the transition away from the topological phase is of third order © 2014 American Physical SocietyJ. D. and C. E. are supported by Grant No. FIS2012-
34479 of the Spanish Ministry of Economy and
Competitiveness.Peer Reviewe