{"total":19,"items":[{"citing_arxiv_id":"2606.12726","ref_index":26,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Stable, bidirectional electro-optic transduction in thin film lithium tantalate","primary_cat":"quant-ph","submitted_at":"2026-06-10T22:24:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"First demonstration of stable bidirectional microwave-optical transduction in thin-film lithium tantalate with ~1 kHz coupling rates, multi-day static-bias operation, and low added noise.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.05628","ref_index":166,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Transcranial FUS Therapy and Monitoring using Nonlinear Acoustics","primary_cat":"physics.med-ph","submitted_at":"2026-06-04T02:55:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes topology-optimized acoustic holograms and nonlinear acoustics methods for precise transcranial FUS focusing, alignment without MRI, and hydrocephalus monitoring.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03431","ref_index":15,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Epitaxial $\\mathrm{Co_2MnSi}$ with intrinsic magnetocrystalline anisotropy as a route to bias-field-free nonlinear half-metal magnonics at the nanoscale","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-06-02T10:19:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Epitaxial L2_1-ordered Co2MnSi waveguides exhibit intrinsic cubic magnetocrystalline anisotropy that suppresses first-order nonlinear instabilities over several GHz at zero bias and stabilizes low-bias Damon-Eshbach operation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.22234","ref_index":1,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Virp: neural network-accelerated prediction of physical properties in site-disordered materials","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-21T09:35:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"A pipeline samples site-disordered material configurations with 400 virtual cells when the supercell is large enough, improving computational feasibility over quasirandom or cluster expansion methods.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21286","ref_index":23,"ref_count":2,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Software Between Quantum and Machine Learning -- And Down to Pulses","primary_cat":"quant-ph","submitted_at":"2026-05-20T15:20:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Introduces a JAX-based framework for pulse-level QML with composable ansatze, end-to-end pulse optimization, and Fourier-analytic diagnostics.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.18540","ref_index":29,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Discovering Data Encoding Strategies for Quantum-Classical Neural Networks Using Monte Carlo Tree Search","primary_cat":"quant-ph","submitted_at":"2026-05-18T15:21:42+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"MCTS discovers superior data encoding circuits for QCCNNs that outperform standard encodings on medical datasets, with effective rank of feature maps serving as a performance predictor.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.18479","ref_index":3,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Spatially-Localized Second Harmonic Generation via Spin Wave Concentration in Patterned YIG Structures","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-05-18T14:32:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Patterned YIG funnel structures concentrate spin waves to enable localized second harmonic generation hundreds of micrometers from the source, verified by frequency- and spatially-resolved SNS-MOKE measurements.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13279","ref_index":79,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Robust Mutation Analysis of Quantum Programs Under Noise","primary_cat":"cs.SE","submitted_at":"2026-05-13T09:56:05+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Noise from quantum hardware simulators significantly alters mutant detection distances, making equivalent mutants harder to separate from faults, with output-distribution metrics reaching 73.03% accuracy and 74.89% F1-score under device-specific thresholds.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"qft-entangled 208 183 391 qpe 193 175 368 vqe 172 156 328 w-state 163 144 307 Total 1170 1054 2224 classical inputs provide a baseline for behavioral comparison, they do not capture the richness of quantum computation. To address this limitation, we augmented the test suites withQuantum inputstates, including entangled and superposed states generated using QuraTest [ 79]. Among QuraTest generators, we selected the UCNOT generator, which constructs parametrized quantum states based on 𝑈 and CNOT gate patterns. This choice was based on its superior mutation score and strong performance in both input diversity and output coverage, as reported in [79]. Input selection also depended on program size. For CUT with up to four qubits, we generated all"},{"citing_arxiv_id":"2605.12020","ref_index":21,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Observation of Magnetically-Induced atomic transitions of the Cs 6S$_{1/2} \\rightarrow 7$P$_{3/2}$ line at 456 nm","primary_cat":"physics.atom-ph","submitted_at":"2026-05-12T12:08:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Observation of seven MI transitions (Fg=3 to Fe=5) of the Cs 456 nm line that exceed conventional transition intensities and shift by ~17 GHz at 3 kG, matching Zeeman theory predictions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"strength is almost two orders of magnitude smaller here than for the transi- tion to the 6 2P3/2 state [16, 17]. For these reasons, spectroscopic studies of the 6 2S1/2 →7 2P3/2 transition are scarce in the literature. Previous studies have focused on the observation of these transitions in nano- [18, 19] and millimeter-sized [20] vapor cells and their application for laser frequency sta- bilization [21, 22]. To study a large number closely-spaced atomic transitions split by a magnetic fields, a sub-Doppler technique is thus required. As was previously shown, using nanocell combined with derivative spec- troscopy allows one to study individual atomic transitions even in the pres- ence of a large number of Zeeman components [10]. To spectrally separate"},{"citing_arxiv_id":"2605.10471","ref_index":14,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Quantum and classical processing with photonic quantum machine learning","primary_cat":"quant-ph","submitted_at":"2026-05-11T12:34:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A programmable silicon photonic chip excited with single photons implements quantum reservoir computing for quantum state tomography, entanglement measurement via negativity, and classical tasks, with an imperfection mitigation technique that improves accuracy over the classical regime.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":": Estimation of the second-order coherence function using quantum reservoir and ensemble methods. Physical Re- view Applied24(5), 054059 (2025) [13] Huang,H.-Y.,Broughton,M.,Mohseni,M.,Bab- bush, R., Boixo, S., Neven, H., McClean, J.R.: Power of data in quantum machine learning. Na- ture Communications12(1), 2631 (2021) https: //doi.org/10.1038/s41467-021-22539-9 [14] Fujii, K., Nakajima, K.: Harnessing disordered- ensemble quantum dynamics for machine learn- ing. Physical Review Applied8(2), 024030 (2017) https://doi.org/10.1103/PhysRevApplied. 8.024030 10 [15] Gong,S.-Q.,Chen,M.-C.,Liu,H.-L.,Su,H.,Gu, Y.-C.,Tang,H.-Y.,Jia,M.-H.,Deng,Y.-H.,Wei, Q., Wang, H., Zhong, H.-S., Jiang, X., Li, L., Liu, N.-L., Lu, C."},{"citing_arxiv_id":"2605.06037","ref_index":23,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"A virtually connected probabilistic computer as a solver for higher-order, densely connected, or reconfigurable combinatorial optimisation problems","primary_cat":"cs.AR","submitted_at":"2026-05-07T11:26:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Simulations predict that a virtually connected photonic probabilistic computer solves Erdos-Renyi graph spin-glass ground states orders of magnitude faster than digital annealing units by avoiding embedding and sparsification.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"where ∆β=β i+1 −β i and ∆E=E i+1 −E i are the differences in inverse temperature and energy between neighbouring replicas, respectively. This ensures that low temperature states do not get stuck in local minima, by propagating other potentially promising states from higher temperatures. The PT algorithm is often favoured in the probabilistic computing literature [23, 24], although there is not yet a thorough understanding of when PT or SA is favourable. Nevertheless in certain cases PT has been shown to perform better, such as on Ising spin-glasses with Gaussian distributed couplings [25]. Here, we employ linear PT, where the replicas' temperatures are linearly interpolated between (βstart, βend). Similarly to SA, we perform I iterations on each replica, swapping replicas at an"},{"citing_arxiv_id":"2604.25884","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"QCalEval: Benchmarking Vision-Language Models for Quantum Calibration Plot Understanding","primary_cat":"quant-ph","submitted_at":"2026-04-28T17:28:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Introduces QCalEval benchmark showing best zero-shot VLM score of 72.3 on quantum calibration plots, with fine-tuning and in-context learning effects varying by model type.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Quantum computing systems require continuous calibration to characterize and maintain their op- erating parameters, as quantum states are sensitive to environmental perturbations. Key calibration targets, including transition frequencies, pulse amplitudes, readout settings, trapping conditions, and couplings, vary by platform and drift over time due to environmental fluctuations and hardware instabilities [1, 2, 3]. As systems scale to hundreds of qubits and beyond, the calibration burden grows combinatorially: each qubit requires dozens of characterization experiments, and the results of one calibration step can invalidate others, creating complex dependency chains [4, 5]. Similarly, results from holistic benchmarking of quantum computers can produce large amounts of data, mak-"},{"citing_arxiv_id":"2604.23431","ref_index":23,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Physics-Informed Deep Image Prior Reconstruction of In-Plane Magnetization from Scanning NV Magnetometry","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-04-25T20:00:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A physics-informed DIP method using a simple convolutional autoencoder reconstructs complex in-plane magnetization from NV magnetometry, with optimal mask orientation improving SNR by up to 3 dB.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.13444","ref_index":20,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Nonlocal photonic time crystals: Infinite momentum bandgaps with minimal modulation speed and strength","primary_cat":"physics.optics","submitted_at":"2026-04-15T03:48:45+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Spatial nonlocality in Lorentz-dispersive media enables infinite-extent momentum bandgaps in photonic time crystals at arbitrarily low modulation speed and strength.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.11690","ref_index":29,"ref_count":2,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Geometry-controlled magnon-polaritons of double magnetic films in planar cavities","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-04-13T16:31:31+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Derives two-film scattering theory for planar cavity magnonics that enables geometry-controlled bright-channel enhancement and symmetry-breaking effects on mode visibility.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Bridges, X. L. Fan, D. S. Xue, C.-M. Hu, Interferometric control of magnon-induced nearly perfect absorption in cavity magnonics, Nat. Commun. 12 (2021) 1933.doi:10.1038/s41467-021-22171-7. [28] J. M. Lee, M.-J. Hwang, H.-W. Lee, Topological magnon-photon in- teraction for cavity magnonics, Commun. Phys. 6 (2023) 194.doi: 10.1038/s42005-023-01316-8. [29] S. Mart 'ınez-Losa del Rinc 'on, I. Gimeno, J. P 'erez-Bail'on, V . Rollano, F. Luis, D. Zueco, M. J. Mart 'ınez-P'erez, Measuring the magnon-photon coupling in shaped ferromagnets: tuning of the resonance frequency, Phys. Rev. Appl. 19 (2023) 014002.doi:10.1103/PhysRevApplied. 19.014002. [30] Y . Cao, P. Yan, H. Huebl, S. T. B. Goennenwein, G. E."},{"citing_arxiv_id":"2604.06869","ref_index":21,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Telecom C-band single-photon sources with a semiconductor-dielectric microresonator","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-04-08T09:31:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Hybrid semiconductor-dielectric microresonator with quantum dot delivers 11% end-to-end efficiency for polarized telecom C-band single photons.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"and height of the QDs also vary, leading to variations in their emission wavelength in the range from 1350 to 1570 nm. High-resolution cross-sectional transmission electron microscopy (TEM) images of individual QDs emitting around 1550 nm show a lateral dimensionsLof 30 nm and a heightsHof 5-6 nm. The estimated density of such QDs is in the mid of 10 8 cm-2, as reported in [21, 44]. After growth by MBE, periodically arranged pillars with diameters ranging from 1 to 5µm were fabricated using photolithography and reactive ion-plasma etching. Then a high-performance thin DBR was fabricated by ion-assisted reactive magnetron sputtering to finish the SPSs. The deposited structure consisted of a 40-nm Si layer followed by two pairs of Si/SiO 2."},{"citing_arxiv_id":"2503.16785","ref_index":16,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Milliwatt-level UV generation using sidewall poled lithium niobate","primary_cat":"physics.optics","submitted_at":"2025-03-21T01:44:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Sidewall poled TFLN waveguides achieve 4.2 mW UV output at 390 nm with record efficiency and low propagation loss.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2406.17995","ref_index":53,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Managing Classical Processing Requirements for Quantum Error Correction","primary_cat":"quant-ph","submitted_at":"2024-06-26T00:50:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A two-level decoder scheduling framework reduces classical processing requirements for quantum error correction by 10-40% on fault-tolerant benchmarks by managing bursty workloads as shared resources.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1906.10328","ref_index":5,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Direct-Write Ion Beam Irradiated Josephson Junctions","primary_cat":"cond-mat.supr-con","submitted_at":"2019-06-25T05:41:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Focused helium ion beam creates controllable, highly uniform SNS and SIS Josephson junctions in YBCO films, with arrays showing no appreciable variation in electrical properties.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}