Science1 publisher3 min readPublished
Cambridge theory paper shrinks the space where quantum advantage can hide
A Cavendish group reports in Physical Review Letters that many "magic states" buy no speedup, and that a 1945 distribution of Dirac's tells you which ones do.
The Scientist · Science desk
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What happened
- A new theoretical study led by researchers at the Cavendish Laboratory was published in Physical Review Letters.
- The study increases the set of quantum calculations known to be easy for classical computers, meaning quantum devices face a higher bar to demonstrate an advantage, and shows quantum computers are harder to make powerful than previously assumed.
- Many states that appear to be magic states and were previously assumed useful turn out to offer no quantum advantage; by identifying this class of useless magic states the team redraws the boundary between calculations that need a quantum computer and those that can be handled classically.
- To run algorithms that outperform any classical computer, qubits must be prepared in special starting configurations known as magic states, which act as computational fuel; without them a quantum computer is no better than a conventional machine.
- Dr David Arvidsson-Shukur, from the Hitachi Laboratory at the Cavendish Laboratory, said: "We're showing that magic is necessary but not sufficient to unlock quantum computers' full power. If a quantum state is not magic, you can't get a quantum advantage. But having magic alone doesn't guarantee you have one either. The picture is more nuanced and much more interesting than that."
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Why it matters
A theory group led from the Cavendish Laboratory has published a result in Physical Review Letters that enlarges the set of quantum computations known to be easy for classical machines [1][2]. That matters to anyone building hardware, because it raises the bar for demonstrating an advantage: states that look like computational fuel, and were assumed to be, can turn out to be worthless [2][3].
The standard account of where quantum speedup comes from runs through so-called magic states, special input configurations without which a quantum machine performs no better than a conventional one [4]. The Cambridge paper keeps the necessity and removes the sufficiency. "We're showing that magic is necessary but not sufficient to unlock quantum computers' full power," said Dr David Arvidsson-Shukur of the Hitachi Laboratory at the Cavendish [5]. "If a quantum state is not magic, you can't get a quantum advantage. But having magic alone doesn't guarantee you have one either" [5]. By naming the class of useless magic states, the team redraws the boundary between problems that need a quantum device and problems that do not [3].
The test they propose is the Kirkwood-Dirac distribution, a framework Paul Dirac built in Cambridge in 1945 at St John's College, extending a distribution introduced a decade earlier by MIT's John Kirkwood [6]. Its unusual feature is that the quantities behave like probabilities but may be negative [7]. The criterion is sharp in both directions: if the distribution stays positive or zero throughout a computation for a given input state, a classical computer can simulate that computation easily; if it goes negative, classical simulation becomes exponentially harder and a genuine advantage may exist [8]. That is a two-sided instrument, a certificate of classical simulability and a necessary condition for advantage in the same object [9]. Lead author J.J. Thio, a doctoral student in Crispin Barnes' group at the Cavendish and St John's, described it as "a new ingredient to the magic mix: the Kirkwood-Dirac negativity" [10].
The demonstration is the part operators should note. Thio and fellow student Rishi Goel wrote a classical simulation program that runs on a standard laptop and performs computations previously thought to require a quantum computer [11]. A laptop is not a proof of general efficiency, but it is a concrete existence result on the classical side of the line.
The account released with the paper does not specify which families of states or classes of circuits are covered, nor the scaling behaviour of the simulator, nor the size of the instances run on the laptop [12]. Those details determine how much of the current experimental programme the result touches.
What to watch: whether groups publishing advantage claims begin reporting the Kirkwood-Dirac negativity of their input states alongside fidelity and gate counts, and whether the Cambridge simulator gets pointed at circuits already advertised as beyond classical reach [8][11]. Also worth watching is how magic-state factories are specified from here, since a resource that is necessary but not sufficient is a poor unit of account for a roadmap [5].