Selective bound-state engineering in tripartite open quantum systems suppresses the steering volume of an untrusted party to zero while keeping trusted-party volumes finite.
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Real-time renormalization group on quantum operations produces chaotic flows in coherent-dominant regimes, and the measurement-induced PT transition belongs to the 1D Yang-Lee edge singularity universality class.
Nonnormality is an intrinsically dissipative property of Lindbladian generators that controls transient growth in open quantum dynamics and increases the cost of quantum simulations.
Optimal initial states for non-equilibrium quantum thermometry exhibit the quantum Mpemba effect and thermalize faster than most states in Markovian models.
Ultimate precision bounds for multiparameter Markovian noise metrology show average variance scaling as Ω(1/(T R²)) with Heisenberg scaling in dissipative channels R when using entangled probes and high-rank signal correlations, attainable via rapid prepare-and-measure protocols.
Undamped modes exist for any N >= 3 in Heisenberg chains with collective dissipation and are characterized via Bethe ansatz.
A landscape theory attributes wave-packet diffusion, localization, and collapse to symmetry breaking in covariance space caused by trapping potentials and bath fluctuations.
Derives a quantum Brownian motion master equation showing two thermal-like decoherence contributions for spatial superpositions along hyperbolic and circular stationary trajectories: modified field spectrum and differential time dilation.
Loss in an auxiliary cavity induces nonreciprocal excitation exchange in a three-cavity quantum battery, yielding significantly higher steady-state energy in the battery than the charger.
Thermal instabilities and noise modify quantum measurement statistics in a sensitive, nontrivial way across the weak-to-strong crossover depending on temperature, probe properties, and state selections.
Optimal cavity modulation via Krylov theory extends qubit lifetime in inhomogeneous spin ensembles by an order of magnitude over inhomogeneity and cavity losses.
A new bound based on state-Hamiltonian correlations gives the exact maximum efficiency for multi-bath thermal engines and is achievable beyond the quasistatic regime in a quantum dot model.
Open photon condensates form metastable plateaus with thermal-like fluctuations and undergo multiple non-Hermitian phase transitions via ghost attractors and exceptional points.
Derives a quantum speed limit for the OTOC decay rate by mapping scrambling to open-system decoherence bounded by system-environment coupling strength and environmental correlation functions.
Quantum trajectory algorithm achieves additive O(T + log(1/ε)) query complexity for simulating dissipative Lindbladians.
Rydberg EIT spectroscopy with linearly polarized RF fields identifies two angular momentum ladder types with opposite central EIT peak behavior, challenging SI-traceable electrometer assumptions.
Indirect measurements in quantum reservoir computing improve execution time scaling, overall performance, and memory capacity over projective measurements and classical feedback methods.
A non-equilibrium thermodynamic framework for quantum reservoir computing proves that peak predictive performance arises from spectral resonance at quantum critical points, but this maximizes informational dissipation and irreversible work, while dynamic coherence boosts capacity without extra mecha
Spin-induced noncommutativity in the Bateman oscillator yields discrete scaling covariance in amplified and damped modes, producing self-similar evolution and history-dependent non-Markovian reduced dynamics.
Modulating relative weights of interaction channels in a quantum Brownian motion model allows control over non-Markovianity, inducing transitions to Markovian regimes using Gaussian master equations.
Energy modeling and parameter optimization for cat-qubit superconducting quantum computers performing semiclassical QFT with error correction indicates an energetic advantage over classical systems for more than 26 qubits under cryogenic assumptions.
Rotational quantum tunneling of a pinned-magnetization nano-particle in a superconducting trap is protected against rest-gas decoherence by near-perfect axial symmetry and lies within experimentally accessible parameter ranges.
Two-tone driving of a superconducting qubit generates strong entanglement between two magnon modes in millimeter-sized YIG spheres containing more than 10^18 spins.
A contextual cavity QED analogue of the Stern-Gerlach experiment is proposed in which continuous phase-sensitive detection of the cavity field drives spontaneous dressed-state polarization and persistent coherent-state superpositions.
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