Curated map of Zoo entries in the Molecular family.
Entries
| Entry | Type | Status |
|---|---|---|
| molecular-qubit | qubit | demonstrated |
| nuclear-magnetic-resonance-qubit | qubit | demonstrated |
| polar-molecule-qubit | qubit | demonstrated |
Composition
- qubit: 3
Curated synthesis
“Molecular” names the physical carrier, not a common processor architecture. The useful comparison is therefore not molecule versus atom, but where each branch places addressability, interaction, and scaling cost. molecular-qubit puts design freedom into synthesis and now spans ensemble coherence, coupled dimers, optical spin control, and electrically driven single molecules, but still lacks a standard scalable initialization/readout stack; polar-molecule-qubit gains individual addressing and a native dipolar entangler by paying an assembly, cooling, and survival-detection cost; nuclear-magnetic-resonance-qubit has exceptionally mature coherent control but pays an exponential pseudo-pure-state signal penalty because it addresses ensembles rather than individual processors.
This makes experimental age a poor proxy for architectural maturity. NMR reached algorithm demonstrations first yet closed off as a scalable route; molecular spin qubits show that chemistry can engineer coherence without by itself supplying an integration stack; trapped polar molecules are the newest branch but already expose a credible two-particle gate primitive. Read the family as three different answers to the same question: which part of the quantum computer is delegated to molecular structure, and which unsolved burden remains outside the molecule?
Conceptual anchors
- coherence-time-hierarchy is the right comparison frame here, because molecular platforms compete less on raw gate speed and more on how chemical design reshapes dephasing channels and extends usable spin coherence.
- spin-orbit-coupling-for-qubit-control captures one of the central molecular design tensions: stronger ligand-field and spin-orbit structure can unlock richer control, but usually at the price of opening additional relaxation and dephasing pathways.
- divincenzo-criteria explains why this family remains strategically interesting but still immature, because synthetic tunability is strong while scalable entangling gates and qubit-specific readout remain the limiting criteria.
Family structure
- molecular-qubit is the chemistry-designed solid-state spin branch: ligand fields and molecular synthesis shape the spin Hamiltonian.
- polar-molecule-qubit is the trapped-particle branch: rotational states carry the qubit and electrically induced dipoles provide entangling interactions.
- nuclear-magnetic-resonance-qubit is the ensemble-computing branch: nuclear spins inside molecules are controlled spectroscopically, but room-temperature demonstrations use pseudo-pure ensembles rather than individually addressable pure-state qubits.
- These are genuinely different hardware models. Their shared label is molecular degrees of freedom, not a shared readout stack or scaling architecture.
Molecular platform routing table
| Branch | Logical degree of freedom | Interaction / control route | Readout model | Decisive scaling bottleneck |
|---|---|---|---|---|
| molecular-qubit | Electronic spin states engineered by ligand field, anisotropy, and hyperfine structure | Microwave, optical, or exchange-mediated electrical control; chemically coupled dimers | Ensemble EPR, optical detection, or local ESR-STM; no standard scalable readout stack | Convert chemically engineered coupling and local control into calibrated gates with repeatable initialization/readout |
| polar-molecule-qubit | Rotational and hyperfine states of individually trapped molecules | Switchable electric dipole exchange, naturally producing iSWAP-family gates; see sqrt-swap-as-universal-gate | State-selective survival detection in optical tweezers | Molecule assembly, cooling, loss, and parallel control |
| nuclear-magnetic-resonance-qubit | Nuclear spins within an ensemble of molecules | RF pulses plus intramolecular scalar -coupling | Bulk ensemble magnetization | Pseudo-pure-state signal falls exponentially and cannot support single-shot error correction |
Use this table as a routing test: chemical synthesis alone points to the first branch, individually trapped dipolar rotors to the second, and bulk spectroscopic ensembles to the third. A new molecular entry should not be merged into an existing branch merely because its carrier is a molecule.
Molecular-spin evidence ladder
The molecular-qubit branch now contains several experimental regimes that should not be collapsed into one maturity claim:
- Ensemble coherence shows that isotope, ligand, and nuclear-spin engineering can preserve a molecular electronic spin for useful times, but does not establish individual addressability.
- Coupled molecular dimers show that chemically designed interactions can outrun decoherence, but an interaction timescale is not a calibrated two-qubit-gate fidelity.
- Optically detected room-temperature control supplies a spin–optical interface and ambient operation, but currently serves sensing-style operation more directly than a scalable register.
- Single-molecule electrical control demonstrates local tuning and coherent drive on surfaces, while initialization, nondestructive readout, and repeatable multi-qubit integration remain open.
Read these as complementary rungs rather than a performance leaderboard: ensemble , single-molecule , optical contrast, and exchange times measure different parts of the processor stack. The next decisive evidence is not another isolated record but a repeatable experiment combining local initialization, coherent interaction, and qubit-specific readout in one architecture.
The three branches should remain separate in comparisons: chemistry-designed spin registers, trapped polar rotors, and ensemble NMR solve different problems and have radically different scaling limits.
NMR evidence-routing guardrail
Liquid-state NMR remains scientifically useful, but its demonstrations must be routed by what they actually establish:
- Compiled Grover and Shor experiments established that coherent pulse sequences could realize small quantum algorithms; they did not establish scalable state preparation or molecule-resolved measurement.
- The 12-spin control benchmark established unusually deep, calibrated control of an ensemble spin Hamiltonian; the pseudo-pure-state signal cost still grows exponentially with register size.
- Modern superchannel, exceptional-point, and recovery-map experiments establish NMR as a precise protocol and open-system simulation testbed; they are not renewed evidence for NMR as a scalable digital processor.
- The missing rung is an architecture with efficient pure-state initialization, single-shot qubit-specific readout, and repeatable mid-circuit feedback. No increase in pulse sophistication alone supplies that rung.
This separates control complexity from processor scalability. Route pulse design, refocusing, and protocol demonstrations toward cross-platform-moc and classical-control; keep pseudo-pure preparation, ensemble readout, and the scaling judgment in this MOC.
Cross-family boundary routing
The carrier being a molecule is enough to place these entries together, but not enough to decide where a systems comparison should continue. Route outward according to the architectural question that dominates:
| Molecular branch | Stay in this MOC when the question is… | Hand off when the question becomes… |
|---|---|---|
| polar-molecule-qubit | Rotational/hyperfine storage, switchable permanent-dipole exchange, or molecule formation and survival detection | Tweezer-array assembly is being compared through Rydberg blockade, atom rearrangement, or atom-loss handling; use neutral-atom-moc |
| nuclear-magnetic-resonance-qubit | Pseudo-pure-state preparation, scalar -coupling inside molecules, bulk readout, or the ensemble-signal scaling failure | The subject is the portable inheritance of selective pulses, refocusing, and optimal control rather than NMR as a processor; use cross-platform-moc |
| molecular-qubit | Chemical synthesis, ligand fields, anisotropy, or isotope choice engineers the spin Hamiltonian itself | A fixed host-lattice defect defines the materials platform; use color-center-moc. If emission, collection, and wavelength matching dominate instead, use spin-photon-moc |
The placement test is therefore not “does this system contain a molecule?” but “which design layer supplies the claimed advantage?” Molecular structure owns the primary note only when it supplies the encoding, interaction, or Hamiltonian engineering rather than merely hosting a control technique or optical interface.