Atomic physics

A route to quantum magnetism

Article metrics

The trend towards using ultracold atoms as simulators of condensed-matter and many-body phenomena is gaining momentum. These systems can now be used to simulate quantum magnetism. See Article p.307

At nanokelvin temperatures — 100 billion times closer to absolute zero than room temperature — ultracold atoms are the coldest stuff in the known Universe. At such low temperatures, these quantum gases, each consisting of hundreds to hundreds of millions of atoms, are quintessential quantum many-body systems. Unlike their more conventional solid-state cousins, nearly every property of quantum gases can be controlled1 in the laboratory with unprecedented flexibility and exquisite precision.

On page 307 of this issue, Simon et al.2 create one-dimensional chains of ultracold rubidium-87 atoms that behave as if strong magnetic interactions were present3. Their novel technique encodes the magnetic properties into the configuration, or geometry, of the atoms in each chain instead of the atoms' quantum mechanical spins as is usually the case in magnetic systems. This increases, by more than a factor of ten, the temperature at which magnetic ordering takes place (when the spatial pattern of spins becomes ordered rather than random), finally allowing quantum magnetism to be studied using ultracold atoms.

Understanding the properties of many-particle interacting systems is a crucial component of modern science. How do interactions between relatively simple components give rise to complex behaviour? How does consciousness emerge from a collection of neurons? How is the large-scale Universe organized? Why do electrons superconduct in some materials and give rise to magnetism in others? Each of these questions involves the emergence of macroscopic properties that are qualitatively distinct from the properties of the individual components.

In physics, we are interested in understanding and classifying the generic ways in which such macroscopic phenomena emerge, linking the microscopic properties of the components (including their environment) to the macroscale. This is usually the domain of condensed-matter physics, in which innumerable interacting electrons in materials give rise to complex phenomena such as superconductivity, the quantum Hall effect and magnetic ordering. Ultracold atoms provide a unique system in which to study many-body physics because the components and their environment are simple and can be nearly perfectly controlled. Indeed, many-body phenomena studied using ultracold atoms have been subjected to unprecedented quantitative comparison with many-body theories. Examples of this are the phase transition from superfluid to Mott insulator4, and a continuous transition known as the Bose–Einstein condensate–Bardeen–Cooper–Schrieffer (BEC–BCS) crossover5,6.

Magnetism is a topic of fundamental importance in condensed-matter physics, having an impact on technology (such as magnetic storage media and some visions of 'spintronic' devices7,8) as well as on concepts at the forefront of physics (such as spin liquids9). Magnetic systems cannot yet be directly studied using quantum gases because their magnetic-ordering temperatures are tens or hundreds of picokelvins (1 picokelvin is 10−12 kelvins). So far, this is too cold even for ultracold atoms.

To bypass this limitation, Simon et al.2 constructed an atomic system in which the spatial configuration of the atoms encodes the 'spin' usually associated with magnetism. They first created a rubidium-87 BEC, in which all the atoms are essentially in the same quantum state, and compressed it into a single two-dimensional (2D) plane. Next, using two independent standing waves of light, they confined the atoms into the sites of a square lattice with one atom per site. One of the two standing waves was made more intense than the other, so that the atoms could 'hop' between sites only in one-dimensional (1D) chains; such hopping is suppressed when neighbouring lattice sites are already occupied, because of the repulsive energy involved in locating two atoms on a single site (Fig. 1a).

Figure 1: The principle of Simon and colleagues' effective spin model2.
figure1

a, Two examples of a Bose–Hubbard lattice: top, energetically allowed hopping from an occupied atomic site to a neighbouring empty site; bottom, suppression of hopping between neighbouring occupied sites owing to the on-site repulsive energy U between two atoms. b, Two examples of a tilted lattice. The tilt is sufficient to overcome on-site repulsion, such that the situation in a is reversed: top, energetically allowed hopping between neighbouring occupied sites; bottom, suppression of hopping between an occupied site and a neighbouring vacant site. c, Mapping of effective spin states (arrows) into different spatial configurations. Defects denote configurations that are not associated with spins, showing that the mapping is approximate. d, Insufficient tilt. A system with an average of one atom per site will remain in this configuration, in which the spins align parallel to one another (a paramagnet). e, Excess tilt. A system with an average of one atom per site will minimize its energy by creating an alternating array of empty sites and doubly occupied sites, corresponding to an arrangement in which the spins are staggered (an antiferromagnet).

To create a magnetic analogue, Simon et al.2 superimposed a magnetic-field gradient on the optical lattice potential, creating an energy difference, or 'tilt', between neighbouring lattice sites. When this energy difference is large enough, it can exceed the repulsive interaction energy, allowing atoms to move from site to site. Thus, a sufficiently large tilt reverses the earlier picture: when a neighbouring site is occupied hopping is allowed (Fig. 1b), but when it is empty hopping is blocked (to conserve energy). When the tilt increases from zero, 1D chains of atoms undergo a transition from one atom per site (Fig. 1d; hopping blocked, analogous to a paramagnet) to a staggered, alternating array of empty sites and doubly occupied sites (Fig. 1e; analogous to an antiferromagnet). Here, the effective magnetism relies on repulsion between atoms, rather than the much smaller exchange interactions between the physical spin states, which normally lead to magnetism in materials. Because every aspect of this system is well understood, the authors were able to directly compare their results with the 1D quantum Ising magnetic model they sought to realize — and found spectacular agreement.

Like the Brownian motion of pollen grains suspended in water, physical systems are usually coupled to a source of random thermal motion: an environment. The successful implementation of this technique relies heavily on a second feature of ultracold atom systems: they are not well connected to such an environment. When the magnetic-field gradient tilts the lattice potential, essentially creating a hill for the atoms, one might expect the atoms to reduce their energy by all moving down the hill. Because the atoms are not linked to an environment, there is no mechanism for them to begin this downhill motion and nowhere for the excess energy to go, so instead the system remains within the subset of spatial configurations that are analogous to spins.

Simon and colleagues2 demonstrate a powerful experimental technique for creating analogues to spin systems. However, the 1D quantum Ising model is well understood from modern theoretical techniques10, and the small systems studied here can be numerically exactly solved by brute force. It is the next step that is profound: creating spin systems that are currently insoluble by known analytical or numerical techniques. For example, the extensions of this work discussed by Sachdev et al.3 would allow the simulation of 2D 'frustrated' spin systems, for some of which an exotic, ground (minimal-energy) state of matter known as a quantum spin liquid is expected9. As the complexity and control of ultracold atoms have continued to increase, it has become evident that they are not simply emulators of condensed-matter systems, but fascinating quantum many-body systems in their own right. As such, they may well exhibit behaviours that do not exist in any other physical system. Extensions of Simon and colleagues' technique2 should allow the construction of nearly arbitrary spin systems, which will be a crucial leap in that direction.

References

  1. 1

    Bloch, I., Dalibard, J. & Zwerger, W. Rev. Mod. Phys. 80, 885–964 (2008).

  2. 2

    Simon, J. et al. Nature 472, 307–312 (2011).

  3. 3

    Sachdev, S., Sengupta, K. & Girvin, S. M. Phys. Rev. B 66, 075128 (2002).

  4. 4

    Greiner, M. et al. Nature 415, 39–44 (2002).

  5. 5

    Regal, C. A., Greiner, M. & Jin, D. S. Phys. Rev. Lett. 92, 040403 (2004).

  6. 6

    Zwierlein, M. W. et al. Phys. Rev. Lett. 92, 120403 (2004).

  7. 7

    Žutić, I., Fabian, J. & Das Sarma, S. Rev. Mod. Phys. 76, 323–410 (2004).

  8. 8

    Ralph, D. C. & Stiles, M. D. J. Magn. Magn. Mater. 320, 1190–1216 (2008).

  9. 9

    Balents, L. Nature 464, 199–208 (2010).

  10. 10

    Ovchinnikov, A. A., Dmitriev, D. V., Krivnov, V. Ya. & Cheranovskii, V. O. Phys. Rev. B 68, 214406 (2003).

Download references

Author information

Correspondence to Ian B. Spielman.

Additional information

This article and the paper under discussion2 were published online on 13 April 2011.

Rights and permissions

Reprints and Permissions

About this article

Cite this article

Spielman, I. A route to quantum magnetism. Nature 472, 301–302 (2011) doi:10.1038/nature10101

Download citation

Further reading

Comments

By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.