arXiv:2610.33156
Direct tests of conformal symmetry with Rydberg atoms: assessment and proposals
Junchen Rong, Slava Rychkov
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.
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