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arXiv:2610.33156

Direct tests of conformal symmetry with Rydberg atoms: assessment and proposals

Junchen Rong, Slava Rychkov

quant-phcond-mat.quant-gashep-thphysics.atom-phSubmitted Oct 23, 2026• Announced Oct 27, 2026• 0 citations
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Abstract

We propose a direct test of conformal symmetry using Rydberg-atom arrays. By arranging the atoms on a circle and measuring equal-time two-point correlation functions, the characteristic functional form predicted by conformal field theory can be tested directly. We estimate the number of experimental snapshots required to resolve this behavior with sufficient statistical precision. We further optimize the time-dependent ramp profile of the Rabi frequency~$Ω$ and detuning~$Δ$ used to prepare the target critical state adiabatically. The optimized profile achieves higher fidelity over much shorter evolution times than those employed in previous experiments. Taken together, these results suggest that a direct experimental test of conformal symmetry is feasible with current Rydberg-atom technology.

AI Summary

The paper asks whether current Rydberg-atom arrays can directly test emergent conformal symmetry through the spatial form of critical correlators, rather than through critical exponents alone. For a periodic Ising-critical chain, the proposed observable is the equal-time correlator $\langle s_i s_j\rangle\propto[2\sin(\pi|i-j|/N)]^{-1/4}$. Its finite-size dependence tests conformal constraints beyond an infinite-system power law. The paper also discusses boundary one-point functions and state–operator correspondence, including existing experimental tests. Numerical analysis focuses on $N=24$ atoms at two points on the Ising critical line: a near-blockade point used in previous experiments and a point with onsite $\mathbb Z_2$ symmetry. Exact diagonalization finds ground-state correlators matching the CFT shape, after normalization, within approximately $4\%$ and $1\%$, respectively, even at nearest-neighbor separation. Born-rule sampling with translation averaging gives statistical errors below $2.5\%$ from $2{,}000$ snapshots. Ramp schedules are optimized in a moving 20-state low-energy subspace and validated by full symmetry-reduced Schrödinger evolution. Near blockade, a $2.5\,\mu\mathrm{s}$ ramp achieves $99.18\%$ fidelity, compared with $99.04\%$ for a previous $7\,\mu\mathrm{s}$ schedule. At the symmetric point, $1.2\,\mu\mathrm{s}$ achieves $99.90\%$. Correlator errors from imperfect preparation are approximately $4\%$ or less for the reported optimized ramps. These fidelities assume coherent dynamics. Detailed decoherence simulations are not performed; reduced atomic motion and decay are inferred from shorter durations. Detection reliability away from blockade remains unresolved, and the quantitative demonstrations are restricted to the 24-site system.

No sign of AI-generated textAI use disclosedIncrementalSmall numerics onlyStrong assumptions
Numerical simulations (exact diagonalization, ramp profile optimization) were performed using AI-generated codes, with human supervision and cross-checks.

Error found: Experimental feasibility remains conditional because the optimized ramps are validated without experimental noise, and reliable detection at P3 is explicitly unresolved. The fastest proposed preparation path requires a maximum Rabi frequency of approximately 12.05 MHz in ordinary frequency units, versus the cited experiment's 1.6 MHz, without establishing hardware compatibility. At N=24 the circular Hamiltonian's exact onsite Z2 symmetry requires Delta' approximately 1.0185, not the chosen zeta(6), so the claimed exact symmetry and associated selection rules at P3 are incorrect as written. The experimental-parameter appendix mistakenly prints a fourth power of the blockade-radius ratio where a sixth power is required to obtain its quoted interaction scale.

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

Comments
Comments welcome, 30 pages, 14 figures

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We propose a direct test of conformal symmetry using Rydberg-atom arrays. By arranging the atoms on a circle and measuring equal-time two-point correlation functions, the characteristic functional form predicted by conformal field theory can be tested directly. We estimate the number of experimental snapshots required to resolve this behavior with sufficient statistical precision. We further optimize the time-dependent ramp profile of the Rabi frequency~ΩΩΩ and detuning~ΔΔΔ used to prepare the target critical state adiabatically. The optimized profile achieves higher fidelity over much shorter evolution times than those employed in previous experiments. Taken together, these results suggest that a direct experimental test of conformal symmetry is feasible with current Rydberg-atom technology.
The paper asks whether current Rydberg-atom arrays can directly test emergent conformal symmetry through the spatial form of critical correlators, rather than through critical exponents alone. For a periodic Ising-critical chain, the proposed observable is the equal-time correlator ⟨sisj⟩∝[2sin⁡(π∣i−j∣/N)]−1/4\langle s_i s_j\rangle\propto[2\sin(\pi|i-j|/N)]^{-1/4}⟨si​sj​⟩∝[2sin(π∣i−j∣/N)]−1/4. Its finite-size dependence tests conformal constraints beyond an infinite-system power law. The paper also discusses boundary one-point functions and state–operator correspondence, including existing experimental tests.
Numerical analysis focuses on N=24N=24N=24 atoms at two points on the Ising critical line: a near-blockade point used in previous experiments and a point with onsite Z2\mathbb Z_2Z2​ symmetry. Exact diagonalization finds ground-state correlators matching the CFT shape, after normalization, within approximately 4%4\%4% and 1%1\%1%, respectively, even at nearest-neighbor separation. Born-rule sampling with translation averaging gives statistical errors below 2.5%2.5\%2.5% from 2,0002{,}0002,000 snapshots.
Ramp schedules are optimized in a moving 20-state low-energy subspace and validated by full symmetry-reduced Schrödinger evolution. Near blockade, a 2.5 μs2.5\,\mu\mathrm{s}2.5μs ramp achieves 99.18%99.18\%99.18% fidelity, compared with 99.04%99.04\%99.04% for a previous 7 μs7\,\mu\mathrm{s}7μs schedule. At the symmetric point, 1.2 μs1.2\,\mu\mathrm{s}1.2μs achieves 99.90%99.90\%99.90%. Correlator errors from imperfect preparation are approximately 4%4\%4% or less for the reported optimized ramps.
These fidelities assume coherent dynamics. Detailed decoherence simulations are not performed; reduced atomic motion and decay are inferred from shorter durations. Detection reliability away from blockade remains unresolved, and the quantitative demonstrations are restricted to the 24-site system.
Preparation of a so-called circular state in a Rydberg atom where the projection of the electron angular momentum takes its maximum value is challenging due to the required amount of angular momentum transfer. Currently available protocols for circular state preparation are either accurate but slow or fast but error prone. Here we show how to use quantum optimal control theory to derive pulse shapes that realize fast and accurate circularization of a Rydberg atom. In particular, we present a theoretical proposal for optimized radio-frequency pulses that achieve high fidelity in the shortest possible time, given current experimental limitations on peak amplitudes and spectral bandwidth. We also discuss the fundamental quantum speed limit for circularization of a Rydberg atom when lifting these constraints.
Conformal field theories (CFTs) feature prominently in high-energy physics, statistical mechanics, and condensed matter. For example, CFTs govern emergent universal properties of systems tuned to quantum phase transitions, including their entanglement, correlations, and low-energy excitation spectra. Much of the rich structure predicted by CFTs nevertheless remains unobserved in experiment. Here we directly observe the energy excitation spectra of emergent CFTs at quantum phase transitions -- recovering universal energy ratios characteristic of the underlying field theories. Specifically, we develop and implement a modulation technique to resolve a Rydberg chain's finite-size spectra, variably tuned to quantum phase transitions described by either Ising or tricritical Ising CFTs. We also employ local control to distinguish parities of excitations under reflection and, in the tricritical Ising chain, to induce transitions between distinct CFT spectra associated with changing boundary conditions. By utilizing a variant of the modulation technique, we furthermore study the dynamical structure factor of the critical system, which is closely related to the correlation of an underlying Ising conformal field. Our work not only probes the emergence of CFT features in a quantum simulator, but also provides a technique for diagnosing a priori unknown universality classes in future experiments.
We propose a test of conformal invariance in critical phenomena based on the study of a two-point correlation function in the presence of a boundary. This two-point function can be studied using X-ray or neutron scattering in the conditions of total reflection (so-called grazing scattering). The conformal Ward identity in momentum space is here expressed as a differential constraint on the scattering cross-section, as a function of the momentum transfer and the scattering angle. Experimental verification using X-rays and binary alloys appears well within the existing techniques, while feasibility for neutron scattering requires further study. This would be the first direct experimental test of conformal invariance in critical phenomena, a symmetry widely assumed but never directly verified.
Rydberg atom arrays are powerful platforms for studying quantum many-body systems. We consider the Rydberg-Ising Hamiltonian in a ring geometry and numerically study ensembles of states generated by random global pulse sequences subject to hardware constraints and fixed evolution times. We compare the statistical properties of such states with those of Haar-random states within the relevant lattice symmetry sector. In the strong-interaction regime (short interatomic distance), the dynamics is governed by an effective blockade that restricts Hilbert-space exploration and limits entanglement growth. In this regime, level-spacing statistics of the entanglement spectrum are close to random-matrix predictions, while the distribution of measurement probabilities deviates from Porter-Thomas behavior. For weaker interactions (larger interatomic distance), the system approaches Haar-like statistics at long times, as reflected in entanglement entropy, entanglement-spectrum statistics, and the distribution of measurement probabilities. At intermediate interactions, this behavior is observed on experimentally relevant timescales. Motivated by this observation, we investigate whether individual target states can be efficiently prepared using quantum optimal control in this regime. Employing target states drawn from an ensemble with a broad entropy distribution, we observe high fidelities (infidelities between 10^-5 and 3 x 10^-2 for nine spins). Within this ensemble, the fidelity decreases with the entanglement entropy of the target state, indicating that highly entangled targets are more difficult to prepare under the considered finite-time control constraints.
Rydberg chains provide an appealing platform for probing conformal field theories (CFTs) that capture universal behavior in a myriad of physical settings. Focusing on a Rydberg chain at the Ising transition separating charge density wave and disordered phases, we establish a detailed link between microscopics and low-energy physics emerging at criticality. We first construct lattice incarnations of primary fields in the underlying Ising CFT including chiral fermions, a nontrivial task given that the Rydberg chain Hamiltonian does not admit an exact fermionization. With this dictionary in hand, we compute correlations of microscopic Rydberg operators, paying special attention to finite, open chains of immediate experimental relevance. We further develop a method to quantify how second-neighbor Rydberg interactions tune the sign and strength of four-fermion couplings in the Ising CFT. Finally, we determine how the Ising fields evolve when four-fermion couplings drive an instability to Ising tricriticality. Our results pave the way to a thorough experimental characterization of Ising criticality in Rydberg arrays, and can inform the design of novel higher-dimensional phases based on coupled critical chains.