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arXiv:2610.38060

Coherent control and high purity single-photon emission from telecom quantum dots on metamorphic InGaAs

Beatrice Costa, Bianca Scaparra, Hubert Riedl, Gregor Koblmüller, Eugenio Zallo, Jonathan J. Finley, Lukas Hanschke, Kai Müller

cond-mat.mes-hallquant-phSubmitted Oct 27, 2026• Announced Oct 29, 2026
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Abstract

Semiconductor quantum dots emitting in the telecommunication O- and C-bands are promising candidates as single-photon sources for fiber-based quantum communication. In this work, we show how coherent quasi-resonant and phonon-assisted excitation help reveal the intrinsic optical properties of InAs quantum dots embedded in relaxed InGaAs matrices on top of metamorphic InGaAs layers for achieving emission in the telecom bands. By systematically comparing excitation schemes, we separate excitation-induced effects from intrinsic emitter properties. This allows us to observe linewidths as narrow as 21 $μ$eV, the disappearance of slow decay channels, and single-photon purity reaching second-order autocorrelation values in the order of $10^{-2}$. Photoluminescence excitation reveals higher excited states, enabling coherent control of trion transitions and the observation of Rabi-like oscillations in both telecom bands. These results confirm the promising potential of these quantum dots for applications in quantum technologies.

AI Summary

This experimental study asks how excitation-induced carrier dynamics obscure the optical properties of InAs quantum dots embedded in relaxed InGaAs on metamorphic buffers, emitting in the telecom O- and C-bands. It compares above-bandgap, wetting-layer, quasi-resonant excited-state, and longitudinal-acoustic-phonon-assisted excitation using spectroscopy, photoluminescence excitation, time-resolved emission, and Hanbury Brown–Twiss measurements at 4 K. Across 17 dots per band, quasi-resonant excitation reduces median trion linewidths from $43$ to $31\,\mu\mathrm{eV}$ in the O-band and from $63$ to $41\,\mu\mathrm{eV}$ in the C-band. The narrowest measured linewidth is $21\pm1\,\mu\mathrm{eV}$, close to the spectrometer resolution. Excitation scans on 19 dots identify discrete excited-state resonances below the wetting-layer continuum. Driving these resonances produces damped Rabi-like oscillations observable up to approximately $3\pi$ pulse area. Time-resolved measurements show suppression of delayed population and slow decay channels, although a slow component persists under phonon-assisted excitation in the illustrated C-band dot. Representative intrinsic trion lifetimes are 0.95 and 1.62 ns; excited-state relaxation times of 28 and 25 ps are comparable to the excitation pulse durations. Phonon-assisted excitation improves measured $g^{(2)}(0)$ from $0.08\pm0.03$ to $0.02\pm0.01$ in the O-band and from $0.17\pm0.02$ to $0.04\pm0.02$ in the C-band. These measurements use sub-saturation excitation, with the C-band comparison taken at different saturation fractions. Fully resonant excitation, lifetime-limited linewidths, and near-unity indistinguishability remain development targets; the paper identifies resonant protocols and microcavity integration as next steps.

Little sign of AI-generated textIncremental

Error found: The C-band single-photon-purity comparison changes excitation from above-bandgap at 25% of saturation with 6 ps pulses to phonon-assisted at 4% with 16 ps pulses, so the measured autocorrelation improvement does not isolate the contribution of excitation scheme.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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Semiconductor quantum dots emitting in the telecommunication O- and C-bands are promising candidates as single-photon sources for fiber-based quantum communication. In this work, we show how coherent quasi-resonant and phonon-assisted excitation help reveal the intrinsic optical properties of InAs quantum dots embedded in relaxed InGaAs matrices on top of metamorphic InGaAs layers for achieving emission in the telecom bands. By systematically comparing excitation schemes, we separate excitation-induced effects from intrinsic emitter properties. This allows us to observe linewidths as narrow as 21 μμμeV, the disappearance of slow decay channels, and single-photon purity reaching second-order autocorrelation values in the order of 10−210^{-2}10−2. Photoluminescence excitation reveals higher excited states, enabling coherent control of trion transitions and the observation of Rabi-like oscillations in both telecom bands. These results confirm the promising potential of these quantum dots for applications in quantum technologies.
This experimental study asks how excitation-induced carrier dynamics obscure the optical properties of InAs quantum dots embedded in relaxed InGaAs on metamorphic buffers, emitting in the telecom O- and C-bands. It compares above-bandgap, wetting-layer, quasi-resonant excited-state, and longitudinal-acoustic-phonon-assisted excitation using spectroscopy, photoluminescence excitation, time-resolved emission, and Hanbury Brown–Twiss measurements at 4 K.
Across 17 dots per band, quasi-resonant excitation reduces median trion linewidths from 434343 to 31 μeV31\,\mu\mathrm{eV}31μeV in the O-band and from 636363 to 41 μeV41\,\mu\mathrm{eV}41μeV in the C-band. The narrowest measured linewidth is 21±1 μeV21\pm1\,\mu\mathrm{eV}21±1μeV, close to the spectrometer resolution. Excitation scans on 19 dots identify discrete excited-state resonances below the wetting-layer continuum. Driving these resonances produces damped Rabi-like oscillations observable up to approximately 3π3\pi3π pulse area. Time-resolved measurements show suppression of delayed population and slow decay channels, although a slow component persists under phonon-assisted excitation in the illustrated C-band dot. Representative intrinsic trion lifetimes are 0.95 and 1.62 ns; excited-state relaxation times of 28 and 25 ps are comparable to the excitation pulse durations.
Phonon-assisted excitation improves measured g(2)(0)g^{(2)}(0)g(2)(0) from 0.08±0.030.08\pm0.030.08±0.03 to 0.02±0.010.02\pm0.010.02±0.01 in the O-band and from 0.17±0.020.17\pm0.020.17±0.02 to 0.04±0.020.04\pm0.020.04±0.02 in the C-band. These measurements use sub-saturation excitation, with the C-band comparison taken at different saturation fractions. Fully resonant excitation, lifetime-limited linewidths, and near-unity indistinguishability remain development targets; the paper identifies resonant protocols and microcavity integration as next steps.
The role of resonant pumping schemes in improving the photon coherence is investigated on InAs/InGaAs/GaAs quantum dots (QDs) emitting in the telecom C-band. The linewidths of transitions of multiple exemplary quantum dots are determined under above-band pumping and resonance fluorescence (RF) via Fourier-transform spectroscopy and resonance scans, respectively. The average linewidth is reduced from (9.74 ± 3.3) GHz in the above-band excitation to (3.50 ± 0.39) GHz under RF underlining its superior coherence properties. Furthermore, the feasibility of coherent state preparation with a fidelity of (49.2 ± 5.8)% is demonstrated, constituting a first step toward on-demand generation of coherent, single, telecom C-band photons directly emitted by QDs. Finally, two-photon excitation of the biexciton is investigated as a resonant pumping scheme. A deconvoluted single-photon purity value of gHBT(2)(0)=0.072 ± 0.104 and a postselected degree of indistinguishability of VHOM=0.894 ± 0.109 are determined for the biexciton transition. This represents another step in demonstrating the necessary quantum optical properties for prospective applications.
Abstract Long-distance quantum communication and computation is based on the exchange of information via photons as flying qubits. In all foreseen implementations, from quantum relays and networks to remote quantum computing, the photons must be able to propagate over long distances, in silica fibers, with limited absorption and wave packet dispersion. When propagating into silica fibers, photons in the so-called telecom C-band (i.e. wavelength around 1550 nm) will experience the absolute minimum of absorption, together with a limited photon wave packet dispersion. This implies that losses of information will be minimized and additionally, the capability of the photons to quantum interfere (the so-called Hong–Ou–Mandel effect) will be negligibly affected. This motivated the search for efficient non-classical light sources in this wavelength range. In the present review, we discuss the approaches followed to red-shift the emission wavelength from the near-infrared (NIR) to telecom wavelengths. In particular, the use of metamorphic buffers (MMBs) enabled the use of highly developed InAs/GaAs systems, engineering the dots to emit single and entangled photons in the telecom C-band. The main advantage of this approach is set by the choice of the material system: being the same as state-of-the-art structures emitting in the NIR range, it opens the possibility of achieving comparable performances even at telecommunication wavelengths. Here we will discuss the current state-of-the-art in the generation of non-classical photons, comparing the properties and performances of MMB-based results with other competing quantum dot (QD) platforms. We report in particular that very low fine-structure splitting can be observed with conservative values, on average well below 10 μ eV. This allowed for the observation of post-selected entanglement fidelity higher than 0.6. Additionally, on-demand single-photon emission with g ( 0 ) 2 = 0.184 ± 0.002 was observed in addition to a very low emitter density of ≈ 10 7 cm − 2 and a decay time of τ ≈ 1.2 ns comparable to standard InAs QDs emitting in the NIR range. A final highlight on approaches to further improve the current device performances will also be reported.
Non-classical photon sources made of semiconductor quantum dots (QDs) emitting in the telecommunication C-band are crucial components for low-loss, long-distance photonic quantum communication networks. Here we designed and fabricated strain--free In0.7_{0.7}0.7​Ga0.3_{0.3}0.3​As/In0.7_{0.7}0.7​Al0.3_{0.3}0.3​As QDs grown on GaAs(111)A substrates working as single-photon emitters in the 1550 nm window. The QDs were grown via local droplet etching method in a molecular beam epitaxy environment, employing a thin In0.7_{0.7}0.7​Al0.3_{0.3}0.3​As metamorphic buffer layer with the same lattice constant of the QD material, thus allowing for a completely strain--free self-assembly of the QDs. The QDs exhibit a C3v_{3v}3v​ symmetry with a ground state emission in the 1400--1600 nm range. The exciton lifetimes of ≈\approx≈ 1.3--1.9 ns and linewidths as low as ≈\approx≈ 300 μμμeV show the good quality of the fabricated QDs. Second-order autocorrelation measurements under pulsed excitation confirmed the single-photon purity of the emitters, yielding a g(2)(0)g^{(2)}(0)g(2)(0) value of 0.141±0.0270.141 \pm 0.0270.141±0.027
We report on the experimental demonstration of triggered single-photon emission at the telecom O-band from In(Ga)As/GaAs quantum dots (QDs) grown by metal-organic vapor-phase epitaxy. Micro-photoluminescence excitation experiments allowed us to identify the p-shell excitonic states in agreement with high excitation photoluminescence on the ensemble of QDs. Hereby we drive an O-band-emitting GaAs-based QD into the p-shell states to get a triggered single photon source of high purity. Applying pulsed p-shell resonant excitation results in strong suppression of multiphoton events evidenced by the as measured value of the second-order correlation function at zero delay of 0.03 (and ~0.005 after background correction).
High Resolution Image Download MS PowerPoint Slide Entangled photons are an integral part in quantum optics experiments and a key resource in quantum imaging, quantum communication, and photonic quantum information processing. Making this resource available on-demand has been an ongoing scientific challenge with enormous progress in recent years. Of particular interest is the potential to transmit quantum information over long distances, making photons the only reliable flying qubit. Entangled photons at the telecom C-band could be directly launched into single-mode optical fibers, enabling worldwide quantum communication via existing telecommunication infrastructure. However, the on-demand generation of entangled photons at this desired wavelength window has been elusive. Here, we show a photon pair generation efficiency of 69.9 ± 3.6% in the telecom C-band by an InAs/GaAs semiconductor quantum dot on a metamorphic buffer layer. Using a robust phonon-assisted two-photon excitation scheme we measure a maximum concurrence of 91.4 ± 3.8% and a peak fidelity to the Φ + state of 95.2 ± 1.1%, verifying on-demand generation of strongly entangled photon pairs and marking an important milestone for interfacing quantum light sources with our classical fiber networks.
We demonstrate the emission of polarization-entangled photons from a single semiconductor quantum dot in the telecom C-band (1530 nm–1565 nm). To reach this telecommunication window, the well-established material system of InAs quantum dots embedded in InGaAs barriers is utilized with an additional insertion of an InGaAs metamorphic buffer to spectrally shift the system to the desired wavelengths. For the observation of polarization-entangled photon pairs, the biexciton-exciton cascade of a quantum dot displaying an intrinsically low fine-structure splitting is investigated by means of polarization-dependent cross-correlation measurements. A complete set of tomography measurements enables us to reconstruct the two-photon density matrix and therefore to calculate a corresponding fidelity f+ to the maximally entangled Bell state Ψ+ of 0.61 ± 0.07, a concurrence of 0.74 ± 0.11, a tangle of 0.55 ± 0.14, and a negativity of 0.63 ± 0.12, clearly proving the entanglement of the states. Finally, the development of the concurrence is studied in dependency of the post-selected time-gate of the emission events and the progression of the time-delay dependent fidelity to distinct Bell states is displayed.