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Integrable pairing models in nuclear and mesoscopic physics

Integrable pairing models in nuclear and mesoscopic physics. Cooper pairs and BCS (1956-1957) Richardson exact solution (1963). Ultrasmall superconducting grains (1999). SU(2) Richarson-Gaudin models (2000).

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Integrable pairing models in nuclear and mesoscopic physics

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  1. Integrable pairing models in nuclear and mesoscopic physics • Cooper pairs and BCS (1956-1957) • Richardson exact solution (1963). • Ultrasmall superconducting grains (1999). • SU(2) Richarson-Gaudin models (2000). • Cooper pairs and pairing correlations from the exact solution. BCS-BEC crossover in cold atoms (2005) and in atomic nuclei (2007). • Generalized Richardson-Gaudin Models for r>1 (2006-2009). Exact solution of the T=0,1 p-n pairing model. 3-color pairing.

  2. The Cooper Problem Problem : A pair of electrons with an attractive interaction on top of an inert Fermi sea.

  3. “Bound” pair for arbitrary small attractive interaction. The FS is unstable against the formation of these pairs

  4. Bardeen-Cooper-Schrieffer

  5. BCS in Nuclear Structure

  6. Richardson’s Exact Solution

  7. Exact Solution of the BCS Model Eigenvalue equation: Ansatz for the eigenstates (generalized Cooper ansatz)

  8. Richardson equations Properties: This is a set of M nonlinear coupled equations with M unknowns (E). The first and second terms correspond to the equations for the one pair system. The third term contains the many body correlations and the exchange symmetry. The pair energies are either real or complex conjugated pairs. There are as many independent solutions as states in the Hilbert space. The solutions can be classified in the weak coupling limit (g0).

  9. 154Sm

  10. Pair energies E for a system of 200 equidistant levels at half filling

  11. Recovery of the Richardson solution: Ultrasmall superconducting grains • A fundamental question posed by P.W. Anderson in J. Phys. Chem. Solids 11 (1959) 26 : • “at what particle size will superconductivity actually disappear?” • Since d~Vol-1Anderson argued that for a sufficiently small metallic particle, there will be a critical size d ~bulkat which superconductivity must disappear. • This condition arises for grains at the nanometer scale. • Main motivation from the revival of this old question came from the works:  • D.C. Ralph, C. T. Black y M. Tinkham, • PRL’s 74 (1995) 3421 ; 76 (1996) 688 ; 78 (1997) 4087.

  12. The model used to study metallic grains is the reduced BCS Hamiltonian in a discrete basis: Single particles are assumed equally spaced where  is the total number of levels given by the Debye frequency D and the level spacing d as

  13. PBCS study of ultrasmall grains: D. Braun y J. von Delft. PRL 81 (1998)47

  14. Condensation energy for even and odd grains PBCS versus Exact J. Dukelsky and G. Sierra, PRL 83, 172 (1999)

  15. Exact study of the effect of level statistics in ultrasmall superconducting grains. (Randomly spaced levels) G. Sierra, JD, G.G. Dussel, J. von Delft and F. Braun. PRB 61(2000) R11890

  16. Richardson-Gaudin Models • JD, C. Esebbag and P. Schuck, PRL 87, 066403 (2001). • Combine the Richardson’s exact solution of the Pairing Model and the integrable Gaudin Magnet • Based on the rank 1 pair algebra of su(2) for fermions or su(1,1) for bosons Pair realization Two-level realization [Only su(2)] Finite center of mass momentum realization(FFLO) Spin realization[Only su(2)]. Bosonization for large S

  17. Construction of the Integrals of Motion • The most general combination of linear and quadratic generators, with the restriction of being hermitian and number conserving, is • The integrability condition leads to • These are the same conditions encountered by Gaudin (J. de Phys. 37 (1976) 1087) in a spin model known as the Gaudin magnet.

  18. Gaudin (1976) found three solutions • Rational Model • Richardson equations • Eigenvalues • Hamiltonianos

  19. Some models derived from RG • BCS Hamiltonian (Fermion and Boson) • Generalized Pairing Hamiltonians (Fermion and Bosons) • Central Spin Model • Gaudin magnets (spin glass models) • Lipkin Model • Two-level boson models (IBM, molecular, Josephson, etc..) • Atom-molecule Hamiltonians (Feshbach resonances) • Generalized Jaynes-Cummings models, • Breached superconductivity. LOFF and breached LOFF states. • Px + i Py pairing. Review: J.D., S. Pittel and G. Sierra, Rev. Mod. Phys. 76, 643 (2004). G. Ortiz, R. Somma, JD, S. Rombouts, Nucl. Phys. B 707 (2005) 421.

  20. The Structure of the Cooper pairs in BCS-BEC rs : Interparticle distance ,  : Size of the “Cooper” pair Quasibound molecules Pair resonaces + Free fermions+ Quasibound molecules Pair resonances

  21. Thermodynamic limit of the Richardson equations J.M. Roman, G. Sierra and JD, Nucl. Phys. B 634 (2002) 483. V, N, G=g / V and =N / V Using an electrostatic analogy and assuming that extremes of the arc are 2+2i , the Richardson equations transform into the BCS equations Gap Number The equation for the arc  is,

  22. Leggett model (1980)for a uniform 3D system. The divergency of the gap equation can be cured with Scattering length The Leggett model describes the BCS-BEC crossover in terms of a single parameter . The resulting equations can be integrated (Papenbrock and Bertsch PRC 59, 2052 (1999))

  23. Evolution of the chemical potential and the gap along the crossover

  24. What is a Cooper pair in the superfluid is medium? G. Ortiz and JD, Phys. Rev. A 72, 043611 (2005) “Cooper” pair wavefunction • From MF BCS: • From pair correlations: • From Exact wavefuction: • E real and <0, bound eigenstate of a zero range interaction parametrized by a. • E complex and R (E) < 0, quasibound molecule. • E complex and R (E) > 0, molecular resonance. • E Real and >0 free two particle state.

  25. BCS-BEC Crossover diagram f pairs with Re(E) >0 1-f unpaired, E real >0 f=1 Re(E)<0 • = -1, f = 0.35 (BCS) • = 0, f = 0.87 (BCS) • = 0.37, f = 1 (BCS-P) • = 0.55, f = 1 (P-BEC) • = 1,2, f=1 (BEC) f=1 some Re(E)>0 others Re(E) <0

  26. “Cooper” pair wave function Weak coupling BCS Strong coupling BCS BEC

  27. Sizes and Fraction of the condensate

  28. Nature 454, 739-743 (2008) Cooper wavefunction in the BEC region A spectroscopic pair size can be defined from the threshold energy of the pair dissociation spectrum as

  29. Application to Samarium isotopes G.G. Dussel, S. Pittel, J. Dukelsky and P. Sarriguren, PRC 76, 011302 (2007) • Z = 62 , 80  N 96 • Selfconsistent Skyrme (SLy4) Hartree-Fock plus BCS in 11 harmonic oscillator shells (40 to 48 pairs in 286 double degenerate levels). • The strength of the pairing force is chosen to reproduce the experimental pairing gaps in 154Sm (n=0.98 MeV, p= 0.94 MeV) • gn=0.106 MeV and gp=0.117 MeV. A dependence g=G0/A is assumed for the isotope chain.

  30. Correlations Energies

  31. Fraction of the condensate in mesoscopic systems From the exact solution f is the fraction of pair energies whose distance in the complex plane to nearest single particle energy is larger than the mean level spacing.

  32. Exactly Solvable RG models for simple Lie algebras Cartan classification of Lie algebras

  33. Exactly Solvable Pairing Hamiltonians 1) SU(2), Rank 1 algebra 2) SO(5), Rank 2 algebra J. Dukelsky, V. G. Gueorguiev, P. Van Isacker, S. Dimitrova, B. Errea y S. Lerma H. PRL 96 (2006) 072503. 3) SO(6), Rank 3 algebra B. Errea, J. Dukelsky and G. Ortiz, PRA 79 05160 (2009) 4) SO(8), Rank 4 algebra S. Lerma H., B. Errea, J. Dukelsky and W. Satula. PRL 99, 032501 (2007).

  34. 3-color Pairing Phase diagram Breached, Unbreached configurations L=500, N=150, P=(NG-NB)/(NG+NB)

  35. 3-color Pairing Density profiles Occupation probabilities

  36. The exact solution

  37. T=0,1 Pairing Odd-Even Pair effect as a signal of quartet correlations 200 levels, g=-0.2

  38. Summary • From the analysis of the exact BCS wavefunction we proposed a new view to the nature of the Cooper pairs in the BCS-BEC crossover. • Alternative definition of the fraction of the condensate. Consistent with the change of sign of the chemical potential. • For finite system, PBCS improves significantly over BCS but it is still far from the exact solution. Typically, PBCS misses ~ 1 MeV in binding energy. • The T=0,1 pairing model could be a benchmark model to study different approximations dealing with alpha correlations, clusterization and condensation. It can also describe spin 3/2 cold atom models where this physics could be explored. • The SO(6) pairing model describes color superconductivity and exotic phases with two condensates. • SP(6) RG model: A deformed-superfluid benchmark model for nuclear structure?

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