Flux qubit

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In quantum computing, flux qubits (also known as persistent current qubits) are micro-metre sized loops of superconducting metal interrupted by a number of Josephson junctions. The junction parameters are engineered during fabrication so that a persistent current will flow continuously when an external flux is applied. The computational basis states of the qubit are defined by the circulating currents which can flow either clockwise or counter-clockwise. These currents screen the applied flux limiting it to multiples of the flux quanta and give the qubit its name. When the applied flux through the loop area is close to a half integer number of flux quanta the two energy levels corresponding to the two directions of circulating current are brought close together and the loop may be operated as a Qubit.

SEM image of a 4-junction Flux Qubit Fabricated at Royal Holloway University of London.

Computational operations are performed by pulsing the qubit with microwave frequency radiation which has an energy comparable to that of the gap between the energy of the two basis states. Properly selected frequencies can put the qubit into a quantum superposition of the two basis states, subsequent pulses can manipulate the probability weighting that qubit will be measured in either of the two basis states, thus performing a computational operation.

[edit] Fabrication

Like most mesoscopic devices such as solid state qubits, single-electron transistors, quantum dots, etc., flux qubits are fabricated using techniques similar to those used in the micro-electronics industry. The devices are made on silicon wafers using electron beam lithography and metallic thin film evaporation processes. To create the Josephson junctions a technique known as shadow evaporation is normally used, this involves evaporating the source metal alternately at two angles through the lithography defined mask in the electron beam resist. This results in two overlapping layers of the superconducting metal, in between which a thin layer of insulator (normally aluminum oxide) is deposited.

[edit] Flux qubit parameters

The flux qubit is distinguished from other types of superconducting qubit such as the charge qubit or phase qubit by the coupling energy and charging energy of its junctions. In the charge qubit regime the charging energy of the junctions dominates the coupling energy, while in a flux qubit the situation is reversed and the coupling energy dominates. Typically in a flux qubit the coupling energy is 10-100 times greater than the charging energy. It is this ratio that allows the cooper pairs to flow continuously around the loop, rather than tunnel discretely across the junctions as in a charge qubit.

[edit] Readout

Like all quantum bits, Flux qubits require a suitably sensitive probe coupled to it in order to measure its state after a computation has been carried out. Such quantum probes should introduce as little back-action as possible onto the qubit during measurement. Ideally they should be decoupled during computation and then turned "on" for a short time during read-out. Read-out probes for flux qubits work by interacting with one of the qubit's macroscopic variables, such as the circulating current, the flux within the loop or the macroscopic phase of the superconductor. This interaction then changes some variable of the read-out probe which can be measured using conventional low-noise electronics. The read-out probe is typically the technology aspect that separates the research of different University groups working on flux qubits.

Prof. Mooij's group at Delft in the Netherlands^[1], along with collaborators, has pioneered flux qubit technology, and were the first to conceive, propose and implement flux qubits as they are known today. The Delft read-out scheme is based on a SQUID loop that is inductively coupled to the qubit, the qubit's state influences the critical current of the SQUID. The critical current can then be read-out using ramped measurement currents through the SQUID. Recently the group has used the plasma frequency of the SQUID as the read-out variable.

Dr. Il'ichev's group at IPHT Jena in Germany^[2] are using impedance measurement techniques based on the flux qubit influencing the resonant properties of a high qulity tank circuit, which, like the Delft group is also inductively coupled to the qubit. In this scheme the qubit's magnetic susceptibility, which is defined by its state, changes the phase angle between the current and voltage when a small A.C. signal is passed into the tank circuit.

Recently Prof. Petrashov's group at Royal Holloway ^[3] are using an Andreev interferometer probe to read out flux qubits. This read-out uses the phase influence of a superconductor on the conductance properties of a normal metal. A length of normal metal is connected at either end to either side of the qubit using superconducting leads, the phase across the qubit, which is defined by its state, is translated into the normal metal, the resistance of which is then read-out using low noise resistance measurements.

[edit] Alternative concepts

In addition to the flux qubits based on conventional Josephson junctions (JJ), i.e. 0 JJs, so called π and 0–π Josephson junctions (see Pi Josephson junction) were discussed as potential candidates for building flux-based qubits, also referred to as phase qubits. While the π junction may serve a passive phase shifter in a quiet qubit, the Josephson vortex in a 0–π junction may be used as the active part in the qubit, as was recently proposed by Goldobin et al. ^[4].

[edit] References

1. ^ University of Delft - Flux Qubit Website
2. ^ University of Jena - Flux Qubit Website
3. ^ Royal Holloway University of London - Flux Qubit Website
4. ^ Goldobin et al. Quantum tunneling of semifluxons in a 0-pi-0 long Josephson junction

• D-wave Systems, Inc - commercial effort to build a superconducting QC