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arXiv:2607.10415

Phase-controlled transport of Floquet-driven compact chiral photonic states

Gabriel Caceres-Aravena, Paloma Vildoso, Helena Drüeke, Rodrigo A. Vicencio

physics.opticsquant-phSubmitted Jul 11, 2026• Announced Jul 14, 2026• Revised Sep 14, 2026 (v2)
v1 · Jul 11, 2026v2 · Sep 14, 2026
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Abstract

The Aharonov-Bohm (AB) effect remains a cornerstone of fundamental and applied physics. In this work, we utilize the AB caging effect originated from an effective magnetic field induced by multiorbital interactions, creating an all flat band (FB) lattice system. Normally, FB states are known for being compact in space and having a zero tail; therefore, their mobility in a linear environment is generally understood as impossible. We propose a Floquet driving protocol in an all-FB photonic system to fully control the dynamics of localized photonic states. The modulation of the Hamiltonian along the propagation coordinate allows the translation of compact states in the direction of constructive interference, resulting in an effective stroboscopic quantum walk-like effect. We find that the traveling states exist in chiral pairs. We experimentally implement the Floquet driven protocol using femtosecond laser written photonic waveguides and demonstrate directional control of the propagation, determined by the relative phase of the input condition.

AI Summary

The paper asks whether periodic driving can translate compact localized states through an otherwise Aharonov–Bohm-caged, all-flat-band photonic lattice, with direction controlled by the input phase. It studies a diamond waveguide array whose fundamental and higher-order modes generate positive and negative hoppings, producing an effective $\pi$ flux. The protocol alternates two static configurations, each with flat-band eigenvalues $0,\pm2t$, by exchanging the central waveguides’ mode types after propagation length $Z_\pi=\pi/(2t)$. Tight-binding and Floquet calculations predict compact, dispersionless translation: equal-amplitude, in-phase and out-of-phase two-site inputs move in opposite directions. The full-period quasienergy spectrum contains a flat band and oppositely sloped linear bands. A symmetry analysis identifies counterpropagating inputs as chiral partners. The undimerized system is gapless, however, so the reported winding calculations do not establish a globally defined band-resolved topological invariant. Experiments use femtosecond-written waveguides in 70-mm glass samples at 640 nm, with $Z_\pi=16.1$ mm and up to four concatenated segments. Output images show phase-dependent opposite transport, with mean displacement approximately one lattice spacing per segment, averaged over six input positions. A participation-ratio-based leakage indicator is around 3% through three segments and around 7% after four; this is not a direct leaked-power measurement. The stated experimental limitations are fabrication asymmetries, unbalanced couplings, incomplete transfers and accumulating errors. Longer propagation may introduce further-neighbor coupling that compromises chiral symmetry and compact transport. Abrupt mode-type changes can also cause loss or imperfect conversion if the central sites are occupied during switching.

Little sign of AI-generated textOverclaimsPossible errorMissing comparison

Error found: The reported 3% and 7% 'leaking fractions' are lattice-size-normalized participation-ratio excesses, not percentages of optical power outside the intended compact state, so they do not establish corresponding leakage probabilities or transfer fidelities. The Floquet discussion declares a principal quasienergy interval of [-t,t] but subsequently describes bands reaching ±2t without distinguishing an unwrapped dispersion from the principal-branch quasienergies.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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8 pages, 3 figures

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The Aharonov-Bohm (AB) effect remains a cornerstone of fundamental and applied physics. In this work, we utilize the AB caging effect originated from an effective magnetic field induced by multiorbital interactions, creating an all flat band (FB) lattice system. Normally, FB states are known for being compact in space and having a zero tail; therefore, their mobility in a linear environment is generally understood as impossible. We propose a Floquet driving protocol in an all-FB photonic system to fully control the dynamics of localized photonic states. The modulation of the Hamiltonian along the propagation coordinate allows the translation of compact states in the direction of constructive interference, resulting in an effective stroboscopic quantum walk-like effect. We find that the traveling states exist in chiral pairs. We experimentally implement the Floquet driven protocol using femtosecond laser written photonic waveguides and demonstrate directional control of the propagation, determined by the relative phase of the input condition.
The paper asks whether periodic driving can translate compact localized states through an otherwise Aharonov–Bohm-caged, all-flat-band photonic lattice, with direction controlled by the input phase. It studies a diamond waveguide array whose fundamental and higher-order modes generate positive and negative hoppings, producing an effective π\piπ flux.
The protocol alternates two static configurations, each with flat-band eigenvalues 0,±2t0,\pm2t0,±2t, by exchanging the central waveguides’ mode types after propagation length Zπ=π/(2t)Z_\pi=\pi/(2t)Zπ​=π/(2t). Tight-binding and Floquet calculations predict compact, dispersionless translation: equal-amplitude, in-phase and out-of-phase two-site inputs move in opposite directions. The full-period quasienergy spectrum contains a flat band and oppositely sloped linear bands. A symmetry analysis identifies counterpropagating inputs as chiral partners. The undimerized system is gapless, however, so the reported winding calculations do not establish a globally defined band-resolved topological invariant.
Experiments use femtosecond-written waveguides in 70-mm glass samples at 640 nm, with Zπ=16.1Z_\pi=16.1Zπ​=16.1 mm and up to four concatenated segments. Output images show phase-dependent opposite transport, with mean displacement approximately one lattice spacing per segment, averaged over six input positions. A participation-ratio-based leakage indicator is around 3% through three segments and around 7% after four; this is not a direct leaked-power measurement.
The stated experimental limitations are fabrication asymmetries, unbalanced couplings, incomplete transfers and accumulating errors. Longer propagation may introduce further-neighbor coupling that compromises chiral symmetry and compact transport. Abrupt mode-type changes can also cause loss or imperfect conversion if the central sites are occupied during switching.
Flat-band lattices hosting compact localized states are highly sensitive to external modulation, and the tailored design of a perturbation to imprint specific features becomes relevant. Here we show that periodic driving in the high-frequency regime transforms the all-flat-band diamond chain into one featuring two tunable quasi-flat bands and a residual flat band pinned at E=0E=0E=0. The interplay between lattice geometry and the symmetries of the driven system gives rise to drive-induced tunneling processes that redefine the interference conditions and open a controllable route to escaping Aharonov-Bohm caging. Under driving, the diamond chain effectively acquires the geometry of a dimerized lattice, exhibiting charge oscillations between opposite boundaries. This feature can be exploited to generate two-particle entanglement that is directly accessible experimentally. The resulting drive-engineered quasi-flat bands thus provide a versatile platform for manipulating quantum correlations, revealing a direct link between spectral fine structure and dynamical entanglement.
We simulate periodically driven Rydberg arrays with purely imaginary-phase driving, showing that it reshapes both internal dynamics and the structure of coupled vacuum fluctuations. In a driven Rydberg array, this interplay produces\emph{hybrid vacuum--photonic quasienergy channels}---coherent,directional modes arising from Floquet-induced modulation of theelectromagnetic local density of states (LDOS). These channels enable a coherent mapping of correlation structure far beyond the nominal dipolar range andexhibit stability characteristic of attractor-like Floquet fixed points. Using a microscopic Hamiltonian with spatiotemporally structureddipole--vacuum coupling, we derive a Floquet--Magnus expression for theeffective LDOS:ρeff(ω)=∑mJm2(A) ρ0(ω+mΩ),\rho_{\rm eff}(\omega)=\sum_m J_m^2(A)\,\rho_0(\omega+m\Omega),ρeff​(ω)=∑m​Jm2​(A)ρ0​(ω+mΩ),revealing how the drive imprints anisotropic vacuum structure.Large-scale open-system simulations confirm that this LDOS reshapingproduces long-lived, quasienergy-resolved photonic corridors, alongwhich correlation fronts propagate with direction-dependent velocities. We further show that the system's long-time behavior is well describedby an \emph{effective geometric picture}: anisotropic correlationfronts define a synthetic light cone, LDOS-induced anisotropies definean emergent spatial metric, and wavepacket bundle separation obeys ageodesic-deviation-like equation whose curvature is determined directlyfrom simulated trajectories over thousands of drive periods. We conclude with a speculative perspective: if driven matter can imprintstable geometric structure onto the vacuum LDOS, then controlled analogspacetime engineering---without material waveguides or externalphotonic scaffolds---may be achievable.
This work explores the possibility of creating and controlling unconventional nonlinearities by periodic driving, in a broad class of systems described by the nonlinear Schrödinger equation (NLSE).By means of a parent quantum many-body description, we demonstrate that such driven systems are well captured by an effective NLSE with emergent nonlinearities, which can be finely controlled by tuning the driving sequence.We first consider a general class of two-mode nonlinear systems-relevant to optical Kerr cavities, waveguides, and Bose-Einstein condensates-where we find an emergent four-wave mixing nonlinearity, which originates from pair-hopping processes in the parent quantum picture.Tuning this drive-induced nonlinearity is shown to modify the phase-space topology, which can be detected through relative population and phase measurements, and also leads to enhanced quantum properties such as spin squeezing.We then couple individual (two-mode) dimers in view of designing extended lattice models with unconventional nonlinearities and controllable pair-hopping processes.Following this general dimerization construction, we obtain an effective lattice model with drive-induced interactions, whose ground state exhibits orbital order, chiral currents, and emergent magnetic fluxes through the spontaneous breaking of time-reversal symmetry.We analyze these intriguing properties both in the weakly interacting (mean-field) regime, captured by the effective NLSE, and in the strongly correlated quantum regime.Our general approach opens a route for the engineering of unconventional optical nonlinearities in photonic devices and controllable drive-induced interactions in ultracold quantum matter.
We propose a non-Hermitian Floquet photonic lattice formed by a physical resonator coordinate and a synthetic frequency coordinate. A two-step modulation protocol realizes a chiral walk in this physical-synthetic plane, with a real synthetic flux controlling loop interference and imaginary gauge fields controlling non-reciprocal envelopes. We show that anomalous corner pairs at quasienergies zero and π/Tπ/Tπ/T exhibit three distinct layers of physics. A non-Bloch higher-order construction predicts whether the 0/π0/π0/π corner pair exists under open boundaries. The imaginary gauge fields select where the right eigenmodes accumulate. The real flux controls the local interference matrix element that determines whether the doubled-period optical response is visible. As a result, the same topological coexistence sector can be bright, skin-dark, or flux-dark in a local optical measurement. We further show that the complex gauge can tune an exceptional point of the two-period corner propagator. At this point the anomalous response keeps its doubled-period sign alternation, but its envelope becomes algebraic because of a Jordan block. These results provide a photonic route to separate topological existence, skin-selected localization, optical visibility, and defective two-period dynamics in a non-Hermitian synthetic dimension.
Aharonov-Bohm (AB) caging, a special flat-band localization mechanism, has spurred great interest in different areas of physics. AB caging can be harnessed to explore the rich and exotic physics of quantum transport in flatband systems, where geometric frustration, disorder, and correlations act in a synergetic and distinct way than that in ordinary dispersive band systems. In contrast to the ordinary Anderson localization, where disorder induces localization and prevents transport, in flat band systems disorder can induce mobility, a phenomenon dubbed inverse Anderson transition. Here, we report on the experimental realization of the AB cage using a synthetic lattice in the momentum space of ultracold atoms with tailored gauge fields, and demonstrate the geometric localization due to the flat band and the inverse Anderson transition when correlated binary disorder is added to the system. Our experimental platform in a many-body environment provides a fascinating quantum simulator where the interplay between engineered gauge fields, localization, and topological properties of flat band systems can be finely explored.
Flat bands in condensed matter systems can host emergent states of matter, from insulating states in twisted bilayer graphene to fractionalized excitations in frustrated magnets and quantum Hall materials. A key phenomenon in certain flat-band systems is Aharonov-Bohm caging, where particles become localized due to destructive interference caused by gauge fields. Here we report on the experimental realization of highly tunable flat-band models populated by strongly interacting Rydberg atoms. By employing synthetic dimensions, we engineer a flat-band rhombic lattice with twisted boundaries and explore the control of Aharonov-Bohm caging during non-equilibrium dynamics through a tunable gauge field. Microscopic measurements of Rydberg pairs reveal the interaction-driven breakdown of Aharonov-Bohm caging in the limit of strong dipolar interactions, where lattice bands mix. In the limit of weak interactions, where caging persists, we observe effective magnetism arising from the interaction-driven mixing of degenerate flat-band states. These observations offer insights into emergent phenomena in synthetic quantum materials and expand our understanding of quantum many-body physics in engineered lattice systems.