Skip to main content

Thank you for visiting You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

Quantum engineering

Spins coupled to a persistent current

Quantum computing architectures based on hybrid systems require strong coupling and information exchange between their constituent elements. These two features have been achieved in one such hybrid setting. See Letter p.221

The development of electronic technologies based on the principles of quantum mechanics, such as quantum computing, requires coupling and integration of quantum objects of various kinds on the same electronic chip. For such integration to succeed, each object needs to be among the best in its class. On page 221 of this issue, Zhu et al.1 make progress in this direction by successfully demonstrating coupling between two quantum systems: a superconducting flux quantum bit (qubit) and an ensemble of identical, highly 'coherent' quantum spins. The authors show that the two systems exchange quanta of radiation, allowing quantum information encoded in the quanta to be reliably transferred between them. The result is relevant for quantum computing based on hybrid settings, in which the superconducting qubits would process quantum information and the spins would be used to preserve or transfer the information2.

Superconducting flux (or persistent current) qubits are loops of superconducting material interrupted by insulating barriers known as Josephson junctions. They are an excellent choice among superconducting qubits. This is because their magnetic flux, which is produced by the current circulating in the loop, couples directly to quantum magnets (atomic spins) that either exist in crystals or are artificially induced in them. In Zhu and colleagues' case, the quantum magnets are associated with the electronic spin states of atomic defects created in diamond. The two qubit states, the ground and excited states, are defined respectively by the clockwise and anticlockwise direction of a persistent current of hundreds of nanoamperes. Being a quantum, as opposed to a classical, bit, the qubit can also be in a quantum superposition of the two states — that is, it can be in the ground and excited states simultaneously. In their experiment, Zhu et al. used a qubit that has four Josephson junctions3 (Fig. 1), which allow adjustment of the energy difference between the two qubit states to match the energetic fingerprint of the diamond spins, as well as optimal operation of the qubit.

Figure 1: Quantum hybrid.

Zhu and colleagues' hybrid quantum system1 involves a slab of diamond (blue) placed on top of a superconducting circuit (grey). A persistent current (red), the direction of which can be either clockwise or anticlockwise, characterizes a tunable flux quantum bit featuring four Josephson junctions. A larger structure known as a superconducting quantum interference device (SQUID), which features two additional Josephson junctions, is used to detect the average value of the persistent current. The magnetic flux (blue arrows) generated by the persistent current couples to some of the spins (green dots) in the diamond. The spins (grey and green dots) are in the form of defects located in a plane inside the diamond slab that is separated from the flux qubit by about 1.2 micrometres. This coupling allows quantum information to be transferred from the flux qubit to the spin ensemble.

Coupling between atoms and electromagnetic fields in resonators was first studied in atomic physics because atomic energy levels in diluted gases have a sufficient lifetime for the transfer of quanta to be observed. Proposed by Tavis and Cummings4 in the 1960s, the coupling between atoms and a standing electromagnetic wave has been observed for an ensemble of atoms5 and single atoms6 in cavity quantum electrodynamics experiments, in which the photons and atoms interact in a cavity. More recently, trapping molecules above a superconducting microwave resonator has been proposed7 as a means to implement cavity quantum electrodynamics on a chip. These studies5,6,7 made use of the electric-field component of an electromagnetic field to coherently exchange photons between the field and the system under study.

Although the magnetic-field component of an electromagnetic field offers much less coupling than the electric-field analogue, magnetic two-level systems (such as the 'up' and 'down' spins in an ensemble of atoms) have much longer lifetimes than their electrical counterparts. This aspect is central to cavity quantum electrodynamics experiments in solid-state systems, which are relevant to the implementation of quantum computing on a chip but rapidly lose quantum information to the surrounding environment. Dipolar interactions between spins in such systems are a major cause of information loss because they affect the spin lifetime. But these interactions can be reduced by 'diluting' the spins in the host solid. Strong magnetic coupling between the electromagnetic field in the cavity and a spin ensemble has been demonstrated theoretically8 and experimentally (see ref. 2 for a discussion), and requires a coupling strength larger than both the cavity's photon decay rate and the rate at which the spin loses its quantum-state information.

In typical cavity quantum electrodynamics experiments, the cavity field is a harmonic oscillator and is coupled to an ensemble of one or more two-level systems. But in their experiment, Zhu et al.1 reversed the roles of these elements: they demonstrated strong coupling between the flux qubit (a two-level system) and the ensemble of spins, which is treated as a single harmonic oscillator. The authors prepared a diamond slab with a number of nitrogen-vacancy (NV) defects located in a plane inside the diamond that is separated from the flux qubit by about 1.2 micrometres (Fig. 1). Each NV defect has three states, with the state of lowest energy being separated from the two higher-energy states owing to an internal magnetic field in the crystal (see Fig. 1c of the paper1). It is this energy-level separation that defines the ground and excited states of the ensemble of NV defects and that allows these states to be entangled with the ground and excited states of the flux qubit.

Zhu et al. used a flux qubit with an energy gap between its ground and excited states that can be tuned to have the same energy as the energy gap between the ground and excited states of the NV ensemble. In this way, the NV ensemble and qubit can be coupled and placed in an entangled state in which the qubit is in its excited state and the NV ensemble is in its ground state. This state can be reversed into a state in which the qubit is in the ground state and the ensemble is in its first excited state. This allows quantum information encoded in the qubit state to be stored in the collection of long-lived NV spins. Zhu and colleagues estimated that the number of NV defects that take part in this process is as large as 3 × 107, giving a collective qubit–NV-ensemble coupling of 70 megahertz, which is sufficiently large to split the energy of the joint state and its reverse (see Fig. 3b of the paper1). They showed that a coherent oscillation between these two states lasted for about 20 nanoseconds, and suggested ways to increase this duration.

Compared with set-ups in which a resonator is used instead of a flux qubit2, the flux qubit gives a more localized coupling. In addition, the external magnetic fields used to control the two states of the spin system alter a resonator's frequency and so affect the coupling process, which does not happen for a qubit of such small dimensions. What's more, this type of device has a larger qubit–ensemble coupling9 than devices involving resonators, and operates in a frequency range of a few gigahertz, which is practical for low-temperature experiments. Finally, a four-junction flux qubit such as that of Zhu and colleagues can be used for studies involving materials other than diamond, because it can be tuned to be in resonance with spin states over a broad energy range.


  1. 1

    Zhu, X. et al. Nature 478, 221–224 (2011).

    ADS  CAS  Article  Google Scholar 

  2. 2

    Blencowe, M. Nature 468, 44–45 (2010).

    ADS  CAS  Article  Google Scholar 

  3. 3

    Mooij, J. E. et al. Science 285, 1036–1039 (1999).

    CAS  Article  Google Scholar 

  4. 4

    Tavis, M. & Cummings, F. W. Phys. Rev. 170, 379–384 (1968).

    ADS  Article  Google Scholar 

  5. 5

    Kaluzny, Y., Goy, P., Gross, M., Raimond, J. M. & Haroche, S. Phys. Rev. Lett. 51, 1175–1178 (1983).

    ADS  CAS  Article  Google Scholar 

  6. 6

    Thompson, R. J., Rempe, G. & Kimble, H. J. Phys. Rev. Lett. 68, 1132–1135 (1992).

    ADS  CAS  Article  Google Scholar 

  7. 7

    Rabl, P. et al. Phys. Rev. Lett. 97, 033003 (2006).

    ADS  CAS  Article  Google Scholar 

  8. 8

    Imamoğlu, A. Phys. Rev. Lett. 102, 083602 (2009).

    ADS  Article  Google Scholar 

  9. 9

    Marcos, D. et al. Phys. Rev. Lett. 105, 210501 (2010).

    ADS  CAS  Article  Google Scholar 

Download references

Author information



Corresponding author

Correspondence to Irinel Chiorescu.

Rights and permissions

Reprints and Permissions

About this article

Cite this article

Chiorescu, I. Spins coupled to a persistent current. Nature 478, 195–196 (2011).

Download citation


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.


Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing