Corné Koks, Alexander Huck, Martijn Wubs, Nicolas Stenger
{"title":"Retrieving Bright-State Emission From Fast Blinking Quantum Emitters","authors":"Corné Koks, Alexander Huck, Martijn Wubs, Nicolas Stenger","doi":"10.1002/qute.70467","DOIUrl":"https://doi.org/10.1002/qute.70467","url":null,"abstract":"<p>To unfold their ultimate performance, a large number of photonics-based quantum technologies require reliable emitters of single photons. Emission intensity fluctuations in these single-photon emitters occur over a broad range of timescales from nanoseconds to more than several milliseconds, depending on the emitter, posing significant challenges for their future applicability. This paper focuses on quantum emitters with intensity fluctuations that occur at a rate comparable to the detection rate of the emitted light. In this regime, there is approximately one photon per bright period. Our method enables the determination of the bright-state intensity, which is otherwise unobservable through a direct time-domain measurement. This method is validated through simulations in various scenarios, and an analytical model is derived. We apply the method to measurements of both quantum emitters in hexagonal boron nitride and of <span></span><math>\u0000 <semantics>\u0000 <msup>\u0000 <mi>NV</mi>\u0000 <mo>−</mo>\u0000 </msup>\u0000 <annotation>${rm NV}^-$</annotation>\u0000 </semantics></math> centers in diamond. The gain in information about the states contributing to the emission dynamics enhances the understanding of bunching phenomena and, in particular, clarifies the influence of potential background light. This is crucial for identifying, designing, and fabricating bright single-photon emitters for applications in quantum technologies.</p>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qute.70467","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149205775","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Emergent-Coupling-Based Ansatz Evaluated on a Superconducting Quantum Processor","authors":"Alina Joch, Kevin Lively, Benedikt Fauseweh","doi":"10.1002/qute.70505","DOIUrl":"https://doi.org/10.1002/qute.70505","url":null,"abstract":"<p>The performance of the variational quantum eigensolver depends critically on the choice of ansatz. In this work, we experimentally evaluate the emergent-coupling-based ansatz (ECBA), a physically motivated variational ansatz for disordered systems. The ECBA is based on a renormalization (semi-)group approach to determine the dominant effective couplings and construct an asymptotically correct ground state. A variational layer based on the location and strength of the effective couplings then corrects the limitations of the renormalization group approach while preserving shallow circuits that capture the essential long-range entanglement structure and balance local correlations. We implement the ECBA on superconducting quantum processors and benchmark it on disordered Heisenberg chain models. Using classically pre-optimized parameters and error mitigation techniques, we study systems of up to 30 qubits and observe a relative experimental energy accuracy of 96.41% for the largest system. Furthermore, we find that the ECBA can be efficiently embedded on hardware with two-dimensional square-lattice connectivity. We compare to commonly used hardware efficient ansätze and observe that the ECBA achieves significantly higher accuracy at a similar gate count.</p>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qute.70505","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149205774","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Feng Zhang, Niladri Gomes, Joshua Aftergood, Thomas Iadecola, Yong-Xin Yao, Peter P. Orth
{"title":"Cover Feature: Sampling Noise and Optimized Measurement Distribution in Imaginary-Time Quantum Dynamics Simulations (Adv. Quantum Technol. 10/2026)","authors":"Feng Zhang, Niladri Gomes, Joshua Aftergood, Thomas Iadecola, Yong-Xin Yao, Peter P. Orth","doi":"10.1002/qute.70515","DOIUrl":"https://doi.org/10.1002/qute.70515","url":null,"abstract":"<p>In article number e70418, Yong-Xin Yao and co-workers report a variational quantum circuit architecture for simulating quantum dynamics on quantum devices. Layered quantum gates process entangled qubits through fixed-depth circuits, converging via an optimization funnel toward a ground state. The spin-chain representations at the bottom illustrate imaginary-time evolution driving a spin model toward its lowest-energy configuration with optimized measurement distribution.\u0000\u0000 <figure>\u0000 <div><picture>\u0000 <source></source></picture><p></p>\u0000 </div>\u0000 </figure></p>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qute.70515","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149099533","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Control-Constraint-Dependent Architecture Reversal in Multilevel Quantum Batteries","authors":"Mohd Asad Siddiqui, Md Qutubuddin, Muhammed Amir","doi":"10.1002/qute.70502","DOIUrl":"https://doi.org/10.1002/qute.70502","url":null,"abstract":"<div>\u0000 \u0000 <p>For a multilevel quantum battery, the set of allowed transitions is only part of the charging problem; the control resource used to drive them is equally important. We derive two exact state-tailored instantaneous-power limits for independently addressable transition phases. Under a shared Hilbert–Schmidt norm, optimization over the initial preparation and phases selects the largest accessible Bohr gap, whereas independent per-transition amplitude bounds allow several phase-aligned currents and give an optimum set by the spectral radius of a gap-weighted transition matrix. Thus two architectures with the same spectrum, the same number of controllable transitions, and isomorphic unweighted graphs can exchange their preferred energy-labelled architecture when the experimentally specified control resource is changed; this is not an intrinsic, resource-independent ranking of battery quality. A unified laboratory constraint connects the two limits. We also obtain the resource-conditional reversal for calibrated couplings and for passive and ground-state charging, and show that the short-time ordering persists for finite times under the specified fixed continuations studied here, rather than under globally optimized finite-time control. We further construct an infinite equal-spectrum family. The comparison therefore depends on the spectrum and transition network together with state preparation and the available controls.</p>\u0000 </div>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149099526","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Chiral Transfer and Preparation of Mechanical Bell States","authors":"Xiao-Qian Wu, Yi-Fan Qiao, Peng-Bo Li","doi":"10.1002/qute.70501","DOIUrl":"https://doi.org/10.1002/qute.70501","url":null,"abstract":"<div>\u0000 \u0000 <p>Generating maximally entangled Bell states is a long-standing goal for practical quantum information processing. Mechanical resonators, as macroscopic bosonic modes with long coherence times and rich nonlinear resources, have recently been endowed with a powerful squeezing resource: two-phonon drive can be leveraged to deterministically encode qubits in the lowest squeezed–Fock states. Here, we show that this squeezed–Fock encoding not only defines a robust qubit subspace, but also provides an inherently tunable platform for generating Bell states. In this work, we propose a system of two coupled mechanical resonators. By simply modulating the squeezing parameter, the effective detuning and dissipation of a mechanical qubit can be simultaneously and precisely controlled, allowing the coupled system to dynamically evolve near exceptional points in parameter space. In post-selection protocol, we demonstrate that this enables chiral transfer between Bell states, as well as the preparation of Bell states from separable initial states, both achieving a conditional fidelity of 0.99 with no-jump success probability of <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mn>1.05</mn>\u0000 <mo>×</mo>\u0000 <msup>\u0000 <mn>10</mn>\u0000 <mrow>\u0000 <mo>−</mo>\u0000 <mn>8</mn>\u0000 </mrow>\u0000 </msup>\u0000 </mrow>\u0000 <annotation>$1.05times 10^{-8}$</annotation>\u0000 </semantics></math>. Our work establishes mechanical squeezed–Fock qubits as a promising platform for exceptional-point-based quantum control, and opens a path toward on-chip generation and chiral manipulation of macroscopic entanglement.</p>\u0000 </div>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149099530","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Syed M. Arslan, Muhammad T. Rahim, Asad Ali, Hashir Kuniyil, Saif Al-Kuwari
{"title":"One-Sided Device-Independent Quantum Key Distribution Over Noisy Metropolitan Links: Noise Thresholds and Purification-Assisted Recovery","authors":"Syed M. Arslan, Muhammad T. Rahim, Asad Ali, Hashir Kuniyil, Saif Al-Kuwari","doi":"10.1002/qute.70503","DOIUrl":"https://doi.org/10.1002/qute.70503","url":null,"abstract":"<div>\u0000 \u0000 <p>One-sided device-independent quantum key distribution (1SDI-QKD) offers a practical middle ground between fully device-independent protocols and standard QKD, achieving security with detection efficiencies as low as 50.1% on the untrusted side. However, prior analyzes assumed idealized channels. This work extends the 1SDI-QKD framework to amplitude damping, dephasing, and depolarizing noise. Results reveal a clear noise hierarchy: dephasing tolerates the most noise before security is lost (<span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msub>\u0000 <mi>p</mi>\u0000 <mtext>crit</mtext>\u0000 </msub>\u0000 <mo>≈</mo>\u0000 <mn>0.50</mn>\u0000 </mrow>\u0000 <annotation>$p_{text{crit}} approx 0.50$</annotation>\u0000 </semantics></math> vs. 0.449 and 0.220 respectively), while depolarizing noise imposes the most stringent detection efficiency requirements, exceeding 97% at 20% noise where amplitude damping requires 76%. Security is lost while substantial entanglement remains (<span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mi>C</mi>\u0000 <mo>≈</mo>\u0000 <mn>0.67</mn>\u0000 </mrow>\u0000 <annotation>$C approx 0.67$</annotation>\u0000 </semantics></math>–0.74), demonstrating that steering violation, not merely entanglement, determines 1SDI-QKD security. Integrating the BBPSSW purification protocol shows that it functions primarily as a range-extension mechanism: five rounds extend dephasing-limited operation from 10 to 36 km at 90% detection efficiency. Accounting for both the <span></span><math>\u0000 <semantics>\u0000 <msup>\u0000 <mn>2</mn>\u0000 <mi>n</mi>\u0000 </msup>\u0000 <annotation>$2^n$</annotation>\u0000 </semantics></math> pair cost and the cumulative success probability, the effective rate peaks at <span></span><math>\u0000 <semantics>\u0000 <msup>\u0000 <mn>10</mn>\u0000 <mrow>\u0000 <mo>−</mo>\u0000 <mn>3</mn>\u0000 </mrow>\u0000 </msup>\u0000 <annotation>$ 10^{-3}$</annotation>\u0000 </semantics></math> bits per initial pair for dephasing but only <span></span><math>\u0000 <semantics>\u0000 <msup>\u0000 <mn>10</mn>\u0000 <mrow>\u0000 <mo>−</mo>\u0000 <mn>6</mn>\u0000 </mrow>\u0000 </msup>\u0000 <annotation>$ 10^{-6}$</annotation>\u0000 </semantics></math> for amplitude damping and depolarizing noise, identifying phase noise limited links as the regime where purification is worthwhile.</p>\u0000 </div>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149099529","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Emergence of Quasi-Two-Dimensional Superconductivity in W-Doped Bulk Noncentrosymmetric 3\u0000 \u0000 R\u0000 $R$\u0000 -\u0000 \u0000 \u0000 TaSe\u0000 2\u0000 \u0000 ${rm TaSe}_2$","authors":"P. Manna, R. P. Singh","doi":"10.1002/qute.70500","DOIUrl":"https://doi.org/10.1002/qute.70500","url":null,"abstract":"<div>\u0000 \u0000 <p>Noncentrosymmetric transition-metal dichalcogenides offer a rich environment for the study of unconventional superconducting phenomena. Here, we present a comprehensive analysis of single-crystalline W-doped 3<span></span><math>\u0000 <semantics>\u0000 <mi>R</mi>\u0000 <annotation>$R$</annotation>\u0000 </semantics></math>-<span></span><math>\u0000 <semantics>\u0000 <msub>\u0000 <mi>TaSe</mi>\u0000 <mn>2</mn>\u0000 </msub>\u0000 <annotation>${rm TaSe}_2$</annotation>\u0000 </semantics></math>, revealing weakly coupled anisotropic unconventional superconductivity at <span></span><math>\u0000 <semantics>\u0000 <msub>\u0000 <mi>T</mi>\u0000 <mi>c</mi>\u0000 </msub>\u0000 <annotation>$T_c$</annotation>\u0000 </semantics></math> = 2.82(2) K, with an in-plane upper critical field exceeding the Pauli limit by 1.7 times. The angular dependence of the upper critical field, along with the observation of a Berezinskii–Kosterlitz–Thouless transition, reveals quasi-two-dimensional superconductivity. Crucially, magnetotransport reveals a distinct two-fold rotational symmetry within the superconducting state under in-plane fields, breaking the underlying three-fold lattice symmetry. These findings establish W-doped <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mn>3</mn>\u0000 <mi>R</mi>\u0000 <msub>\u0000 <mtext>-TaSe</mtext>\u0000 <mn>2</mn>\u0000 </msub>\u0000 </mrow>\u0000 <annotation>$3Rtext{-TaSe}_2$</annotation>\u0000 </semantics></math> as a bulk model system for exploring intrinsic low-dimensional superconductivity and broken rotational symmetry, thus opening new directions for future quantum technologies.</p>\u0000 </div>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"9 10","pages":""},"PeriodicalIF":4.3,"publicationDate":"2026-10-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149099525","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}