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
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 spin control; proposed resonator and spin-photon interfaces | Ensemble control remains common; single-molecule readout is emerging | No standard scalable two-qubit coupling and readout stack yet |
| 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.
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.