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Telecom Quantum Dot Keeps a Hole Spin Coherent for 21.8 Nanoseconds

Peer-reviewed measurements link a semiconductor hole spin to 1.55-micrometre photons, but this remains an interface experiment—not a network node.

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Conceptual circular grating around a quantum dot, with a hole-spin arrow linked to a 1.55-micrometre photon and a callout for 21.8-nanosecond dephasing at 20 millitesla.
Diagram: QubitWire hardware desk

Conceptual view of a hole spin in an InAs/InAlGaAs quantum dot coupled to 1.55-micrometre light through a circular Bragg grating. The reported T2* value is 21.8 ± 0.2 ns at 20 mT; this is not a device micrograph or measured plot. Image creditOriginal conceptual diagram by QubitWire hardware desk. Use with the exact honest conceptual-diagram caption; do not present as a micrograph, measurement curve, literal processor layout, network demonstration or universal coherence value. · https://qubitwire.com/editorial-standards

A Würzburg-led team has built a semiconductor interface that connects a stationary hole-spin to photons emitted directly in the telecommunications C-band. The peer-reviewed device combines an InAs/InAlGaAs quantum dot with a deterministically positioned circular Bragg grating and emits at 1.55 micrometres.

That wavelength matters because ordinary optical fibre is engineered for low-loss telecom transmission. A coherent spin can store and manipulate quantum information locally, while a photon can carry it between nodes; putting both functions in one solid-state device is a route toward networked quantum processors.

Using polarization-resolved measurements and two-photon correlations, the researchers tracked a ground-state hole spin in an in-plane magnetic field. Nature Communications reports an inhomogeneous dephasing time, T2*, of 21.8 ± 0.2 nanoseconds at the study's optimal field of 20 millitesla.

The result is not a quantum network or a fault-tolerant computer. It characterizes one interface and one selected operating point. An earlier author preprint reported 15.9 ± 1.7 nanoseconds for a pulsed measurement; that earlier value should not be treated as interchangeable with the later journal result.

The practical test is whether this platform can repeatedly create high-fidelity spin-photon and longer photon strings while preserving coherence, collection efficiency and indistinguishability. Those system-level measurements—not the wavelength or dephasing time alone—will decide whether the device can serve as a useful network node.

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