Semiconducting MOC

Curated map of Zoo entries in the Semiconducting family.

Entries

Entry	Type	Status
aeon-qubit	qubit	active
exchange-only-qubit	qubit	active
hole-spin-qubit	qubit	demonstrated
hybrid-qubit	qubit	demonstrated
kane-qubit	qubit	demonstrated
rx-qubit	qubit	demonstrated
semiconductor-charge-qubit	qubit	demonstrated
silicon-spin-qubit	qubit	demonstrated
loss-divincenzo-qubit	qubit	demonstrated
singlet-triplet-qubit	qubit	active
spin-qubit	qubit	demonstrated

Composition

• qubit: 11

Conceptual anchors

• exchange-interaction-in-quantum-dots is the core coupling primitive for loss-divincenzo-qubit, singlet-triplet-qubit, exchange-only-qubit, aeon-qubit, and rx-qubit.
• decoherence-free-subspace separates the encoded-spin branch from the simpler one- and two-spin modalities.
• charge-noise-sweet-spot is the right cross-cutting lens for AEON, singlet-triplet, and other detuning-sensitive devices.
• spin-orbit-coupling-for-qubit-control marks the main fork between electron-spin designs that need synthetic field gradients and hole-spin designs that get all-electrical control natively.

Control surfaces

• loss-divincenzo-qubit, spin-qubit, and silicon-spin-qubit are the coherence-first baseline: local spin states, exchange for two-qubit logic, and extra engineering for fast single-qubit drive.
• singlet-triplet-qubit, exchange-only-qubit, rx-qubit, and aeon-qubit are the encoded-exchange branch, trading simpler state definitions for symmetry protection, exchange-only control, or sweet-spot operation.
• semiconductor-charge-qubit and hybrid-qubit sit on the charge-admixed edge of the family, where stronger electrical control is bought by re-exposing the device to detuning noise.
• hole-spin-qubit is the high-SOC branch: faster and cleaner electrical drive, but with charge-noise sensitivity moved back into the center of the design problem.

Family structure

• loss-divincenzo-qubit is the minimal single-spin + exchange proposal.
• singlet-triplet-qubit, exchange-only-qubit, rx-qubit, and aeon-qubit are best read as a local progression in how much symmetry structure is added to tame exchange control.
• kane-qubit is the donor-spin branch: same semiconductor ambition, but with atomically placed dopants instead of lithographic dots as the qubit-defining resource.
• spin-qubit and silicon-spin-qubit should stay as broad modality overviews, not absorb the encoded-spin subfamily.
• For the semiconductor descendants that cross into Josephson-circuit territory, see super-semi-moc.