Advanced quantum technologies最新文献

A discrete ‘Quantum Memory Matrix’ lattice (central orange cell) symbolizes Planck-scale quantum memory units imprinting and retrieving local quantum fields. The circuit diagram below, featuring controlled-Ry, Ry, and CSWAP gates, illustrates the fully unitary QMM imprint–retrieval primitive that underpins enhanced error suppression and hybrid quantum-classical learning on NISQ devices. More in article number 2500262, Florian Neukart and co-workers.

The cover picture shows a controlled SWAP test quantum circuit with several state copies, and bitstrings (e.g., 0000, 1001, 1111) as measurement results. These bitstrings correspond to probabilities to simultaneously estimate traces of the 2nd to nth power traces of reduced density matrices via a single circuit, applied to entanglement measure computation. More in article number 2500376, Ming Li and co-workers.

A scheme is proposed to realize strong photon blockade (PB) effect in cavity magnomechanical system by incorporating a magnon parametric amplification (MPA). By analyzing the theoretical model of this system, it is found that the introduction of MPA not only increases additional transition pathways but also facilitates destructive interference between different transition paths, leading to a significantly enhanced unconventional photon blockade (UPB). This research demonstrates that PB is highly sensitive to phase and driving strength, and the optimized parameter relationships provide effective guidance for achieving quantum correlation. Furthermore, these conditions are closely related to the strength of the magnon-photon coupling, indicating the significant impact of the system's nonlinear characteristics on the photon–photon correlations. This work not only deepens the understanding of quantum interference in hybrid cavity systems but also provides a viable route toward realizing high-purity single-photon sources in magnomechanical platforms.

Symmetry breaking is commonly employed to optimize the functionalities of cavities, such as the single-wavelength resonance, directional output, or high quality-factor (Q). Due to the mutual influence and restriction of these performance metrics, it is a great challenge to realize high-Q multiple-wavelength resonances with each wavelength's emission being directional and distinguished. Here, a non-circular inner and circular outer (NICO) cavity is proposed, and dual-wavelength resonant modes with different in-plane emission directions for the two wavelengths are realized. More importantly, the Q of the two modes in the NICO cavity remains unchanged (100%) compared to the fully circular cavity. To gradually change the inner ellipse shape to the outer-circle shape, only the coordinates (not the refractive index) are transformed. This transformation makes the cavity easy to fabricate in the experiment. Both the band-gap confinement effect of the outer circle layers and the gradual change from the inner ellipse shape to the outer-circle shape significantly halt the Q-spoiling phenomena. Solutions of increasing refractive index differences and further breaking symmetry are provided to improve the Q factors (as high as 10¹³) and narrow the emission divergence angles (by approximately twice), as well as increase the splitting wavelengths (by ≈6 times).

Enhancing and controlling optomechanically induced higher-order sideband generation is essential to achieve high-sensitivity sensing. This study theoretically explores the amplified charge-dependent generation of optical second-order sidebands (OSS) within a cavity optomechanical system, facilitated by an atomic ensemble. Findings reveal that the presence of an atomic ensemble not only enhances OSS generation but also shows a more pronounced charge dependence in the output OSS spectrum compared to a single optomechanical cavity system. This enhancement inspires to explore charge measurements with higher sensitivity. The results demonstrate that the sensitivity of charge measurement can be elevated by over four orders of magnitude when additional atomic ensembles are incorporated. The proposed scheme presents a promising approach for charge measurement and holds significant potential for applications in quantum sensing.

2D ferromagnetic (FM) semiconductors/half-metals offer promising prospects for quantum information technologies in miniature devices. However, the low Curie temperature (T_C) severely limits their application in spintronic devices. Here, two stable FM transition metal chalcogenides, Ti₃S₂X₂ (X = Se, Te) monolayers, based on first-principles calculations are presented. It is found that the Ti₃S₂Se₂ monolayer is a bipolar magnetic semiconductor with an indirect bandgap of 0.094 eV, while Ti₃S₂Te₂ exhibits be FM half-metallic feature. Notably, the T_Cs of Ti₃S₂Se₂ monolayer and Ti₃S₂Te₂ monolayer are 641 and 408 K, respectively, much higher than room temperature. Moreover, the T_Cs and electronic properties of both Ti₃S₂X₂ (X = Se, Te) monolayers can be modulated by applying biaxial strains. These promising properties make Ti₃S₂X₂ (X = Se, Te) monolayers ideal candidates for 2D spintronic devices.

Periodically driving a quantum many-body system can drastically change its properties, leading to exotic non-equilibrium states of matter without a static analog. In this scenario, parametric resonances and the complexity of an interacting many-body system are pivotal in establishing non-equilibrium states. A Floquet-engineered transverse field Ising model for the controlled propagation in one dimension of spin waves is reported. The underlying mechanisms behind the proposal rely on high-frequency drivings using characteristic parametric resonances of the spin lattice. Many-body resonances modulating spin-spin exchange or individual spin gaps inhibit interactions between spins thus proving a mechanism for controlling spin-wave propagation and a quantum switch. The schemes may be implemented in circuit QED with direct applications in coupling–decoupling schemes for system-reservoir interaction and routing in quantum networks.

Quantum secret sharing (QSS) plays a crucial role in quantum cryptography as a privacy preserving scheme. Designing an efficient QSS protocol requires addressing three key challenges: 1) dynamic agent membership (handling agents joining or leaving during execution), 2) adversarial resilience (ensuring robustness against dishonest agents), and 3) practical optimization (improving computational and communication efficiency while minimizing implementation cost). In this paper, a verifiable dynamic $��(�t�,�n�)�$ threshold QSS (VDQSS) protocol with authentication capability is proposed. The protocol employs single particles for both authentication and share distribution, combining homogeneous linear recursion (HLR) with mutually unbiased bases (MUBs) to reconstruct multiple secrets. This approach significantly enhances security while reducing protocol complexity. The correctness and practicality of the protocol are validated through experimental simulations. Analytical results demonstrate its robustness against common attacks, providing reliable security guarantees for quantum communications. Compared to existing QSS protocols, the protocol offers enhanced simplicity and practical applicability.