Self-Assessment Quiz: Photonic, Neutral Atom, and Other Approaches
Twenty questions on the platforms beyond superconducting and trapped ions, and why no approach has yet won. Aim for 16+.
Question 1
Neutral-atom qubits are held by:
A) Optical tweezers — focused laser beams B) RF electric fields C) Superconducting loops D) Physical cavities
Question 2
Entangling gates between neutral atoms use:
A) Rydberg blockade B) Shared motional modes C) Josephson coupling D) Photon exchange only
Question 3
The Rydberg blockade works because:
A) An excited atom shifts its neighbours' energy levels, preventing simultaneous excitation B) Atoms collide C) Photons are absorbed D) Magnetic fields align
Question 4
The distinctive advantage of neutral atoms is:
A) Reconfigurable geometry — atoms can be physically rearranged B) Fastest gates C) Room-temperature operation D) No lasers needed
Question 5
That reconfigurability makes them attractive for:
A) qLDPC codes requiring non-local stabilizers B) Surface codes only C) Classical computing D) Cryptography
Question 6
A significant neutral-atom challenge is:
A) Atom loss during operation, requiring reloading B) Fabrication variation C) Wiring heat load D) Charge noise
Question 7
Photonic qubits encode information in:
A) Photon properties such as polarization, path, or time-bin B) Atomic states C) Superconducting phase D) Electron spin
Question 8
A major photonic advantage is:
A) Room-temperature operation and natural networking B) Deterministic two-qubit gates C) Long-lived memory D) High gate rates
Question 9
The central photonic difficulty is:
A) Two-qubit gates are probabilistic without strong nonlinearity B) Photons decohere quickly C) Photons cannot be measured D) Photons are too slow
Question 10
Measurement-based / one-way quantum computing uses:
A) A large entangled cluster state consumed by adaptive measurements B) Gates only C) No entanglement D) Classical bits only
Question 11
Photonic approaches often rely on:
A) Cluster states plus fusion gates, with heavy multiplexing to overcome probabilistic success B) Deterministic CNOTs C) Ion shuttling D) Flux tuning
Question 12
Silicon spin qubits are attractive because:
A) They may leverage existing semiconductor manufacturing B) They are the fastest C) They need no cooling D) They have all-to-all connectivity
Question 13
Topological qubits aim to:
A) Encode information non-locally so local noise cannot corrupt it B) Run at room temperature C) Eliminate measurement D) Avoid entanglement
Question 14
The status of topological quantum computing is:
A) Still unproven — definitive demonstration of the required quasiparticles remains contested B) Commercially deployed C) Fully demonstrated D) Mathematically impossible
Question 15
Quantum annealing (e.g. D-Wave) is:
A) A different computational model without gate-model universality or proven speedup B) Equivalent to gate-model computing C) Faster than all classical methods D) The basis of Shor's algorithm
Question 16
True or false: One hardware platform has clearly won.
Question 17
True or false: Photonic quantum computers need no cryogenics at all.
Question 18
True or false: Neutral-atom systems have demonstrated the largest numbers of entangled logical qubits.
Question 19
Short answer. Explain why probabilistic gates are a fundamental obstacle for photonics and how the field addresses it.
Question 20
Short answer. Why has no platform won, and what would winning look like?
Answer Key
| Q | Ans | Note |
|---|---|---|
| 1 | A | Arrays of optical tweezers, each holding one atom. |
| 2 | A | Excitation to a high-lying Rydberg state produces a strong, distance-dependent interaction. |
| 3 | A | The blockade shifts the doubly-excited state out of resonance, producing a conditional phase. |
| 4 | A | Atoms are moved between operations, giving effectively programmable connectivity. |
| 5 | A | Non-local stabilizers become implementable, which is why qLDPC and neutral atoms are frequently discussed together (Ch. 23–24). |
| 6 | A | Atoms are lost from traps during operation; continuous reloading and loss-tolerant protocols are required. |
| 7 | A | Several encodings are used; dual-rail path encoding is common. |
| 8 | A | No cryogenics for the photons themselves, and photons are the natural carrier for networking. |
| 9 | A | Photons barely interact, so linear-optical two-qubit gates succeed only probabilistically. |
| 10 | A | Cluster-state computing: entangle first, then compute by measuring adaptively. |
| 11 | A | Fusion-based architectures with multiplexing to convert probabilistic success into near-deterministic operation. |
| 12 | A | The manufacturing argument — CMOS-compatible fabrication at scale. |
| 13 | A | Braiding non-Abelian anyons would give inherent protection at the hardware level. |
| 14 | A | Claims have been made and contested; the field treats it as unproven. |
| 15 | A | Annealing solves optimization heuristically; it is not gate-model universal and has no proven speedup. |
| 16 | False | Superconducting and trapped ions lead on different metrics, neutral atoms lead on logical-qubit demonstrations, and photonics and silicon have long-term structural advantages. It remains genuinely open. |
| 17 | False | The photons need none, but high-efficiency single-photon detectors typically require ~1–4 K. Photonics reduces cryogenic demands substantially rather than eliminating them. |
| 18 | True | QuEra's 2026 result — 96 logical qubits from 448 physical atoms using high-rate codes — is the largest verified logical-qubit count reported. |
| 19 | — | Photons do not interact appreciably, so with linear optics alone a two-qubit gate can only be implemented probabilistically — the KLM scheme's CNOT succeeds with probability well below 1, heralded by ancilla detection. Cascading such gates would make success probability vanish exponentially. The field's answer is multiplexing: run many probabilistic attempts in parallel and route successful outcomes forward with fast switches, converting a low per-attempt probability into near-deterministic operation at the cost of enormous component counts and stringent loss requirements. Fusion-based architectures organize this into a scalable scheme. |
| 20 | — | Because the platforms have complementary rather than comparable strengths: superconducting is fast and lithographic but wiring-limited; ions have the best fidelity but slow gates; neutral atoms have reconfigurable connectivity but suffer atom loss; photonics networks naturally but has probabilistic gates; silicon may manufacture at scale but lags in fidelity. Winning would mean demonstrating a clear path to thousands of error-corrected logical qubits — sustained below-threshold operation, logical two-qubit gates, real-time decoding, and an architecture whose scaling constraint is understood and surmountable. No platform has shown all of it. |