The job is to hold one qubit's worth of information long enough to compute. The trouble is that long enough is very short.
Not every quantum system can do that job. A usable physical qubit has to clear a short checklist, the DiVincenzo criteriaThe short checklist a physical system must meet to work as a qubit: it must scale, be controllable by a few operations, and let errors be removed.: you must be able to make many of them, set them to a known starting state, keep them coherent for longer than your operations take, run a universal set of gates on them, and read them out reliably.1 Most candidate systems fail at least one, which is why only a handful of platforms, or modalities, are seriously in the race.
Figure 1: A single physical qubit, left to itself. Noise from the environment scrambles its state (decoherence): its energy drains on the T1 timescale and its phase scatters even faster on T2. This fragility is why one physical qubit is never enough.
Real hardware, real numbers
So how good are today's physical qubitsAn actual piece of qubit hardware. On its own it is fragile and makes frequent errors.? It depends entirely on the platform, and the spread is enormous.2Trapped ionsA qubit made from a single electrically charged atom held in place by electromagnetic fields and controlled with lasers. are the steady ones, holding their state for seconds. Superconducting qubitsA qubit made from tiny electrical circuits chilled to near absolute zero, where they lose all electrical resistance. are far faster to operate but twitchier, historically keeping their state for only microseconds, though that figure has climbed sharply since.3 At the accurate end, the best trapped-ion operations now clear 99.9 percent fidelity.4
Every platform is a trade between speed, stability, and how hard it is to build many of them.
The reason is decoherenceThe loss of a qubit's quantum information as it interacts with the outside world. The main reason qubits are fragile.. Left to itself, a physical qubit leaks its information into the surroundings: its energy drains away on a timescale called T1, and its delicate phase scrambles even faster, on a timescale called T2.2 That second one is the real enemy, because it costs no energy and so happens all the time. No amount of careful engineering has yet made a single physical qubit steady enough to carry a long calculation by itself.
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Ballance, C. J., Harty, T. P., Linke, N. M., Sepiol, M. A. & Lucas, D. M. “High-Fidelity Quantum Logic Gates Using Trapped-Ion Hyperfine Qubits.” Physical Review Letters117, 060504 (2016). DOI: 10.1103/PhysRevLett.117.060504. Preprint: arXiv:1512.04600.