EFFECT OF DISORDER ON THE INTERACTING FERMI GASES IN A ONE-DIMENSIONAL OPTICAL LATTICE

Effect of Disorder on the Interacting Fermi Gases in a One-Dimensional Optical Lattice

GAO XIANLONG    M. POLINI and M. P. TOSI    B. TANATAR
Abstract

Interacting two-component Fermi gases loaded in a one-dimensional (1D) lattice and subjected to an harmonic trapping potential exhibit interesting compound phases in which fluid regions coexist with local Mott-insulator and/or band-insulator regions. Motivated by experiments on cold atoms inside disordered optical lattices, we present a theoretical study of the effects of a correlated random potential on these ground-state phases. We employ a lattice version of density-functional theory within the local-density approximation to determine the density distribution of fermions in these phases. The exchange-correlation potential is obtained from the Lieb-Wu exact solution of Fermi-Hubbard model. On-site disorder (with and without Gaussian correlations) and harmonic trap are treated as external potentials. We find that disorder has two main effects: (i) it destroys the local insulating regions if it is sufficiently strong compared with the on-site atom-atom repulsion, and (ii) it induces an anomaly in the inverse compressibility at low density from quenching of percolation. For sufficiently large disorder correlation length the enhancement in the inverse compressibility diminishes.

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Keywords: Fermi-Hubbard model; optical lattices; disorder.

1 Introduction

Disorder and interaction effects in condensed matter systems have a long and rich history. The interplay between them has been the subject of continuing interest. The notable examples range from two-dimensional electron systems with long-ranged Coulomb interactions to liquid He absorbed in various substances such as aerogel and vycor and granular superconductors. In the former system experimental and theoretical investigations reveal the crucial role played by disorder as the two-dimensional electron system undergoes a metal-insulator transition. Furthermore, thermodynamic quantities carry the signature of phase transition along with transport properties.

In recent years, cold atomic systems are being used to investigate the interplay between single-particle randomness and interaction effects with the help of optical lattices allowing access to strong coupling regimes through the depression of kinetic energy. Furthermore, the on-site interaction can be tuned either indirectly by changing the strength of the lasers that create the optical lattice or directly by means of a Feshbach resonance.

After the initial observation of superfluid to Mott insulator transition using bosonic atoms in an optical lattice and creation of disorder potentials, studies on fermionic atoms are beginning to be explored. A couple of forthcoming reviews encompass many aspects of the theory of ultracold Fermi gases.

In this work we study the interaction and disorder effects on a one-dimensional, two-component Fermi gas trapped in a harmonic confinement potential and an optical lattice. We use the lattice version of density functional theory taking advantage of the exact solution of the one-dimensional Fermi-Hubbard model. Ground-state calculations in the absence of disorder have been performed within a number of numerical techniques to identify various phases. In the present approach, the harmonic confinement potential and the disorder potential are treated as part of the Kohn-Sham potential within a local-density approximation which has an exact representation for the uniform case.

Generalizing our earlier work on the effects of uncorrelated disorder, we here study correlated disorder which depends on the correlation length as a parameter. The site occupation profiles and thermodynamic stiffness are determined to study the effects of disorder. Our motivation for considering correlated disorder comes from the experiments on Bose-Einstein condensates in optical speckle potentials where it was noted that the correlation length is several times longer than the lattice spacing.

The paper is organized as follows. In Sec. 2 we briefly outline the Fermi-Hubbard model in a harmonic potential and disorder. We then give the main ingredients of our density-functional theory approach. Section 3 presents our results on site occupations in the presence of correlated disorder. We conclude with a brief summary in Sec. 4.

2 Theory and Model

We consider a two-component Fermi gas with atoms constrained to move under harmonic confinement of strength inside a disordered optical lattice with unit lattice constant and lattice sites . The system is described by a single-band Hubbard Hamiltonian,

(1)

Here if are nearest sites and zero otherwise, is a pseudospin- label for two internal hyperfine states, is the pseudospin-resolved site occupation operator, and . The effect of disorder is simulated by the last term in Eq. (1). The above Hamiltonian without the confining potential and disorder term has been solved exactly using the Bethe Ansatz technique by Lieb and Wu. The exact solution provides us with the ground-state energy at any coupling strength and filling . In the noninteracting and unconfined limit (i.e., without the and trap terms) one recovers the Anderson model studied intensively for the Anderson localization problem. The successful creation of optical lattices to study cold atomic systems has led to renewed interest in these model systems, since the atomic systems offer a wide range of control on the various parameters.

In this work we generalize our previous study on uncorrelated noise to Gaussian correlated disorder, defined as

(2)

where is the correlation length (in units of the lattice spacing, which is set to unity throughout this work) and is randomly chosen at each site from a uniform distribution in the range . Because of the following mathematical identity,

Fig. 1: (color online) The correlated disorder potential as a function of the site position for a lattice of sites. The disorder strength is . Different values of are indicated in the legend.
(3)

Eq. (2) tends smoothly to uncorrelated (i.e. white) noise in the limit . We illustrate typical behavior of over a lattice of sites in Fig. 1 for some values of . As the correlation length increases the correlated disorder potential becomes smoother with amplitude smaller than that in the uncorrelated case.

A particular set of values is a realization of disorder. Each realization defines an external potential which is the sum of a harmonic trap potential and disorder. the site-occupation functional theory (SOFT) to determine the site occupation where is the ground-state of for this particular disorder realization. The site occupation is obtained by the disorder ensemble average, . SOFT is the discrete or lattice version of the density functional theory which has been successfully applied to the present system in the absence and presence of uncorrelated disorder. In the clean limit the local-density approximation which we adopt has been shown to be reliable through extensive comparisons with accurate quantum Monte Carlo calculations . Local-density approximation based density-functional schemes for disordered systems have been employed to study the low-density compressibility anomaly in the two-dimensional metal-insulator transition (see Ref. [?, ?]) and the statistical properties of disordered quantum dots.

The total energy is a unique functional of which can be written as

(4)

where is the ground-state energy of the Hubbard Hamiltonian as obtained by Lieb and Wu. The Euler-Lagrange equation that follows from the above energy density is

(5)

where the Kohn-Sham potential is

(6)

Within the local-density approximation, exchange-correlation potential is approximated by

(7)

The above set of equations allow us to obtain the site occupations and their disorder averages .

3 Results and Discussion

Fig. 2: (color online) Site occupation as a function of site position for fermions with , , and in a lattice with sites. The four curves have been calculated for different values of disorder strength: (solid line), (circles), (triangles), and (squares).

Before we describe the effects of disorder on the trapped lattice fermions, we outline the various ground-state phases of a clean system as obtained by previous numerical studies. There are altogether five phases () controlled by the interaction strength , number of fermions , and number of lattice sites . Phase is a fluid with . In phase a Mott insulated occupies the central region of the trap with . In phase a fluid with is embedded in the Mott plateau. Phase is a band insulator with surrounded by fluid edges and embedded in the Mott plateau. Finally, in phase a band insulator in the central region of the trap coexists with fluid edges. The sketch of site occupations in these phases was given in Ref. ?.

Fig. 3: (color online) Site occupation as a function of site position for fermions with , , and in a lattice with sites. The four curves have been calculated for different values of disorder strength: (solid line), (circles), (triangles), and (squares).
Fig. 4: (color online) Site occupation as a function of site position for fermions with , , and in a lattice with sites. The five curves have been calculated for different values of disorder strength: (solid line), (solid circles), (triangles), (squares), and (empty circles).

In Fig. 2 we show the disorder-averaged site occupation for a system of fermions with in an optical lattice with sites. The interaction strength is and the trap potential is . Here we fixed the disorder correlation length to be and varied the disorder strength . The clean system is in phase . As in the case of uncorrelated disorder we find that with increasing the Mott insulating region is depleted and the site occupation profile broadens. However, the rate of depletion and broadening are smaller than the uncorrelated disorder. In other words, the Mott insulating region is more stable against the formation of a disordered fluid phase in the presence of correlated disorder.

Fig. 5: (color online) The number of consecutive sites and such that and , respectively, as a function of . The parameters are the same as in Fig. 4.
Fig. 6: (color online) The inverse compressibility (in units of ) in the presence of correlated disorder as a function of for , , , and lattice sites. The correlation length (circles), (squares), and (triangles).

In Fig. 3 we display the disorder averaged site occupation for a system with atoms keeping the rest of the parameters the same as in Fig. 2. is the critical number of atoms at which the phase transition occurs in the clean limit. For weak uncorrelated disorder a fluid phase with is induced at the center of the trap. Essentially the same behavior is observed for correlated disorder (). Sufficiently strong destroys the Mott plateau completely and the system becomes a disordered fluid with . We find that the critical disorder strength for this to happen is much larger for correlated disorder than the corresponding value of for uncorrelated disorder.

In Fig. 4 we show the site occupation for a strongly interacting system () with correlated disorder (). The disorder free system is in the phase discussed above. With increasing the band insulating region at the center of the trap is depleted. At the same time, the Mott insulating regions are also slowly destroyed. To see more clearly the rate at which the band and Mott insulating regions are destroyed, we plot in Fig. 5 the number of consecutive sites and such that and , respectively, as a function of . Comparison with the same calculation in the uncorrelated disorder case reveals the increased stability range of insulating regions for correlated disorder.

The effect of disorder on 1D fermions and in particular transitions between different phases can also be assessed through the thermodynamic properties. For this purpose we calculate the inverse compressibility defined as where is the chemical potential. In Fig. 6 we show as a function of for various values of the disorder correlation length . The phase transitions can be identified as sharp kinks in a clean system (). Uncorrelated disorder has two main effects on as discussed in our previous work. Firstly, the sharp features indicating phase transitions are smoothed out. Secondly, a large enhancement of at low density is observed. This is reminiscent of a similar behavior found in 2D electron systems. As decreases the atoms mostly occupy the deepest valleys in the disorder landscape, thus the high density regions in the system tend to become disconnected. For a given interaction strength and low the system stiffens as disorder grows. In the present situation we observe that with increasing correlation length the low density enhancement in is diminished. The basic reason for this behavior is that increasing makes the disorder potential more smooth and more shallow compared to the case. Therefore the atoms are less localized in a correlated disorder potential.

4 Concluding remarks

We have studied the one-dimensional Fermi-Hubbard model in a harmonic confinement potential and in the presence of correlated disorder. This is believed to represent cold fermionic atoms in an optical lattice created by standing laser waves. Our numerical calculations of the site occupations are based on a lattice version of density functional theory in which we make use of the exact solution of the one-dimensional Hubbard model to treat the exchange-correlation effects. Disorder affects the ground-state phases of the interacting Fermi gases confined in a harmonic potential and an optical lattice. The insulating regions appear to be stable against both uncorrelated and correlated disorder. The anomalous enhancement of the stiffness observed at low density for uncorrelated disorder decreases with increasing correlation length. We hope that our results on disorder effects will stimulate experimental investigations with cold Fermi atoms in the future.

Acknowledgements

G. X. was supported by NSF of China under Granr No. 10704066. B. T. acknowledges the support by TUBITAK (No. 106T052), TUBA and a travel grant from Julian Swchiwinger Foundation.

References

References

  • 1. See for instance, E. Abrahams, S.V. Kravchenko, and M.P. Sarachik, Rev. Mod. Phys. 73, 251 (2001); B.L. Altshuler, D.L. Maslov, and V.M. Pudalov, Physica E 9, 209 (2001).
  • 2. J.D. Reppy, J. Low Temp. Phys. 87, 205 (1992); B. Fåk, O. Plantevin, H.R. Glyde, and N. Mulders, Phys. Rev. Lett. 85, 3886 (2000), and references therein.
  • 3. R. Fazio and H. van der Zant, Phys. Rep. 355, 235 (2001).
  • 4. A. Punnoose and A.M. Finkel’stein, Science 310, 289 (2005); A.A. Shashkin, S. Anissimova, M.R. Sakr, S.V. Kravchenko, V.T. Dolgopolov, and T.M. Klapwijk, Phys. Rev. Lett. 96, 036403 (2006).
  • 5. J.P. Eisenstein, L.N. Pfeiffer, and K.W. West, Phys. Rev. Lett. 68, 674 (1992); S. Ilani, A. Yacoby, D. Mahalu, and H. Shtrikman, ibid. 84, 3133 (2000); S.C. Dultz and H.W. Jiang, ibid. 84, 4689 (2000).
  • 6. B. Tanatar, A.L. Subaşı, K. Esfarjani, and S.M. Fazeli, Int. J. Mod. Phys. B 21, 2134 (2007).
  • 7. J.E. Lye, L. Fallani, M. Modugno, D.S. Wiersma, C. Fort, and M. Inguscio, Phys. Rev. Lett. 95, 070401 (2005); D. Clément, A.F. Varón, M. Hugbart, J.A. Retter, P. Bouyer, L. Sanchez-Palencia, D.M. Gangardt, G.V. Shlyapnikov, and A. Aspect, ibid. 95, 170409 (2005); C. Fort, L. Fallani, V. Guarrera, J.E. Lye, M. Modugno, D.S. Wiersma, and M. Inguscio, ibid. 95, 170410 (2005); for a review see V. Ahufinger, L. Sanchez-Palencia, A. Kantian, A. Sanpera, and M. Lewenstein, Phys. Rev. A 72, 063616 (2005).
  • 8. J.I. Cirac and P. Zoller, Science 301, 176 (2003).
  • 9. D. Clement, P. Bouyer, A. Aspect, and L. Sanchez-Palencia, Phys. Rev. A: 77, 033631 (2008); Y.P. Chen et al., e-print arXiv:0710.5187, to be published in Phys. Rev. A.
  • 10. M. Greiner, O. Mandel, T. Esslinger, T.W. Hänsch, and I. Bloch, Nature 415, 39 (2002).
  • 11. T. Schulte, S. Drenkelforth, J. Kruse, W. Ertmer, J. Arlt, K. Sacha, J. Zakrzewski, and M. Lewenstein, Phys. Rev. Lett. 95, 170411 (2005).
  • 12. H. Moritz, T. Stöferle, K. Günter, M. Köhl, and T. Esslinger, Phys. Rev. Lett. 94, 210401 (2005).
  • 13. W. Hofstetter, C.I. Cirac, P. Zoller, E. Demmler, and M.D. Lukin, Phys. Rev. Lett. 89, 220407 (2002); S. Trebst, U. Schollwök, M. Troyer, and P. Zoller, Phys. Rev. Lett. 96, 250402 (2006).
  • 14. I. Bloch, J. Dalibard, and W. Zwerger, arXiv:0704.3011v2, to be published in Rev. Mod. Phys.; L. Giorgini, L.P. Pitaevskii, and S. Stringari, e-print arXiv:0706.3360v2, to be published in Rev. Mod. Phys.
  • 15. K. Schönhammer, O. Gunnarsson, and R.M. Noack, Phys. Rev. B 52, 2504 (1995); N.A. Lima, M.F. Silva, L.N. Oliveira, and K. Capelle, Phys. Rev. Lett. 90, 146402 (2003).
  • 16. E.H. Lieb and F.Y. Wu, Phys. Rev. Lett. 20, 1445 (1968).
  • 17. M. Rigol, A. Muramatsu, G.G. Batrouni, and R.T. Scalettar, Phys. Rev. Lett. 91, 130403 (2003); M. Rigol and A. Muramatsu, Phys. Rev. A 69, 053612 (2004); Opt. Commun. 243, 33 (2004); X.-J. Liu, P.D. Drummond, and H. Hu, Phys. Rev. Lett. 94, 136406 (2005); V.L. Campo, Jr. and K. Capelle, Phys. Rev. Lett. 72, 061602 (2005).
  • 18. Gao Xianlong, M. Polini, M.P. Tosi, V.L. Campo, Jr., K. Capelle, and M. Rigol, Phys. Rev. B 73, 165120 (2006).
  • 19. Gao Xianlong, M. Polini, B. Tanatar, and M.P. Tosi, Phys. Rev. B 73, 161103 (2006).
  • 20. P.W. Anderson, Phys. Rev. 109, 1492 (1958).
  • 21. J. Shi and X.C. Xie, Phys. Rev. Lett. 88, 086401 (2002).
  • 22. K. Hirose, F. Zhou, and N.S. Wingreen, Phys. Rev. B 63, 075301 (2001); K. Hirose and N.S. Wingreen, ibid. 65, 193305 (2002); H. Jiang, D. Ullmo, W. Yang, and H.U. Baranger, ibid. 69, 235326 (2004); E. Räsänen and M. Aichinger, ibid. 72, 045352 (2005).
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