Quantum Computing · Sun, Sep 27, 2026

arXiv Quantum Physics (quant-ph).

arXiv math-ph · cond-mat.quant-gas · math.MP

Effective atom-dimer bands of three-body lattice systems at strong coupling: exact critical mass ratios and a statistics-quasimomentum duality

In briefEffective atom-dimer bands of strongly coupled three-body lattice systems, with exact critical mass ratios and a statistics-quasimomentum duality

SummaryThis paper studies three particles on a square lattice with infinitely strong contact interactions, across all total quasimomenta and three statistical cases. Using a Feshbach-Schur reduction, the authors derive effective Hamiltonians with a proved first-order error bound and reduce the threshold problem to a quartic polynomial built from square-lattice two-point resistances. They give the atom-dimer band structure over the Brillouin zone and the critical mass ratio, with the exact value pi/(pi-2) at zero quasimomentum. The paper also proves two dualities relating a change of statistics to a quasimomentum shift by pi.

Mikhail V. Dolgopolov

arXiv quant-ph · cond-mat.dis-nn

Interactions Protect Periodically Driven Time Crystals Against Dephasing but Destabilise Multipolar-Driven Order

In briefInteractions help time crystals resist dephasing but disrupt order under multipolar drives

SummaryThe paper studies a disordered periodically kicked Ising model to see how interaction strength and spin coordination (grid versus ring) affect time-crystal order. For a periodic drive, stronger coupling lengthens the coherence time, whereas for random multipolar drives of order one or higher, doubling the coupling shortens it. At equal total interaction strength, a grid keeps coherence longer than a ring.

Karthikeya Machiraju, Kaustav Bhowmick

arXiv quant-ph · cs.LG

Terminal-Register Certification for Finite-Measurement Learning of Multiscale Quantum States

In briefCertifying finite-measurement learning of multiscale quantum states

SummaryThis paper studies reliable learning of pure one-dimensional quantum states from finite measurements, using an inverse binary multiscale entanglement renormalization ansatz (MERA). The authors add a noise-aware theorem that includes a calibrated total variation implementation budget in the finite-shot certificate. On a transverse field Ising ground state, an 8-qubit schedule exceeded fidelity 0.99 in all 60 held-out runs, with mean fidelity 0.996886. At 16 qubits, MERA outperformed a parameter-matched local circuit in fidelity and long-range error.

Bhvain Makwana, Kashyap Patel, Manjunath Joshi et al.

arXiv quant-ph · cs.CC

The Fully Depolarizing Noise Conjecture for Entangled Physical States: A Twenty-Year Perspective

In briefTesting a Conjecture on Entangled Qubit Noise: A Twenty-Year Review

SummaryThe author revisits a 2006 conjecture that noise acting on entangled physical qubits includes a joint fully depolarizing component, which could obstruct quantum fault tolerance. The conjecture remains open, but recent experimental advances bring it closer to empirical testing on current devices. The paper also discusses noise sensitivity and complexity in noisy intermediate-scale quantum systems, and statistical analysis of quantum advantage claims.

Gil Kalai

arXiv math-ph · math.MP · quant-ph

Minimal output entropy for the channels that add or remove a box of a Young diagram, and a Pauli principle for every permutation symmetry

In briefMinimal output entropy for box-adding or removing Young diagram channels, and a general Pauli principle

SummaryThe paper studies four covariant quantum channels connecting irreducible U(d) representations whose Young diagrams differ by one box. The authors prove that for each channel, coherent states produce outputs that majorize all others, so coherent states minimize output entropy, and they give the optimal output explicitly using hook lengths. For the two channels that keep the box, they also identify all minimizers, which need not be coherent even when pure. Applied to N particles with a given permutation symmetry, the results give sharp bounds on the spectrum of a single particle's reduced density matrix and characterize the spectra reachable by mixed states; for fermions these recover the Pauli principle and Coleman's theorem.

Robin Reuvers

arXiv cond-mat.mes-hall · physics.class-ph · quant-ph

Magnetic localization and spectral asymmetry of a charged particle at a screw dislocation

In briefMagnetic localization and spectral asymmetry of a charged particle near a screw dislocation

SummaryThe paper studies a charged particle moving outside a screw dislocation in a uniform magnetic field. Although the geometry is locally Euclidean, the global screw identification couples conserved axial and azimuthal quantities. After separating cyclic coordinates, radial motion is governed by an inverse-square term and a magnetic harmonic confining term. For nonzero field strength the reduced problem is exactly solvable, giving an equally spaced spectrum with an orientation-dependent energy shift.

Claudio Furtado, Omar Mustafa, Hassan Hassanabadi et al.

arXiv quant-ph · physics.atom-ph

How many photons can a molecule scatter before its coherence is lost?

In briefHow many light particles a molecule can scatter before losing quantum coherence

SummaryMolecular qubits trapped in optical traps can lose coherence when they scatter photons from the trapping lasers. The rate has two parts: the mean Raman scattering rate of the two qubit states, and a term proportional to the square of the difference in their Rayleigh scattering amplitudes. The paper calculates the decoherence rate in terms of the molecular polarizability components α1 and α2. It finds decoherence is suppressed at wavelengths where both are small, and identifies such wavelengths for CaF molecules.

M. R. Tarbutt

arXiv quant-ph · gr-qc · hep-th

Local Many Worlds in Spacetime: Deutsch-Hayden Descriptors and Local Wavefunctions

In briefLocal many-worlds quantum mechanics: linking Deutsch-Hayden descriptors to local wavefunctions

SummaryThe paper presents a local many-worlds formulation of quantum mechanics in spacetime, where each event has its own local wavefunction built only from its past light cone, with no global configuration-space wavefunction and no collapse. The same information is expressed in the Heisenberg picture through Deutsch-Hayden descriptors, which are compact but harder to interpret. The authors show that local wavefunctions for any N-qubit system can be constructed directly from these descriptors.

Mordecai Waegell

arXiv quant-ph · cond-mat.stat-mech

Temperature--Hamiltonian Ambiguity in Strong-Coupling Quantum Equilibrium

In briefTemperature–Hamiltonian ambiguity in strong-coupling quantum equilibrium

SummaryIn strong coupling, a subsystem's reduced equilibrium state fixes the Gibbs generator but not, by itself, the local Hamiltonian and temperature. The authors propose identifying the local Hamiltonian from physical information independent of the stationary state, after which a compatible exact reduced state determines a unique local temperature. Examples include an exactly solvable two-level-system–oscillator model and an exact bosonic model.

Jinshuang Jin