The hypothesis of inflation links the birth of large-scale structure to quantum fluctuations in an accelerating curved spacetime, yet the question of directly observing the quantum nature of these fluctuations in the cosmic microwave background remains open. Wands duality states that different dynamical histories (e.g., slow-roll and ultra-slow-roll) lead to identical evolution of linear perturbations and the same power spectrum. A fundamental question arises: does this degeneracy persist at the level of actual quantum correlations between local observables?
The authors applied the continuous-variable Gaussian formalism to scalar perturbations within the framework of Friedmann expansion (described by Friedmann equations, derived from Einstein field equations). After quantizing the field and its conjugate momentum, they coarse-grained the operators in real space with a window function of radius R, constructing two spatially separated local modes. A 4×4 covariance matrix was built from two-point correlators; its symplectic eigenvalues were computed for various dual pairs, including standard slow-roll and ultra-slow-roll, as well as generalized "constant-roll" regimes with a fixed index ν. The comparison was conducted using analytical expressions and numerical integrals.
It has been found that for any pair of backgrounds connected by Wands duality (ν² = (3/2 + ε₂/2)²), the squares of the symplectic eigenvalues σ²± coincide, despite significant differences in individual elements of the covariance matrix (see Fig. 1). As a consequence, all derived quantum-information quantities—entropy of entanglement, mutual information, quantum discord, and logarithmic negativity—turn out to be identical. For instance, the mutual information between two regions separated by a distance α = d/R shows the same dependence for slow-roll and ultra-slow-roll for any α > 2(1+δ). Moreover, for generalized dual pairs with constant ν, the mutual information grows monotonically with ν, but remains indistinguishable within each pair. Logarithmic negativity is zero everywhere, indicating the absence of entanglement between the modes, yet its invariance is also rigorously proven.
The uncovered symmetry implies that any local linear entanglement witnesses built from coarse-grained fields cannot distinguish Wands-dual inflationary histories. The reason is that the duality transformation acts as a scale-independent local symplectic transformation in phase space, preserving all symplectic invariants. Thus, Wands duality extends from configuration spectra to the full quantum-information description of the Gaussian state, imposing fundamental limitations on the possibility of recovering details of the inflationary potential from measurements of such correlations.
It remains to be seen whether this symmetry persists when non-Gaussianity arising from interactions is included. It has already been shown that at the nonlinear level the duality is broken, which manifests as Wigner negativity. Another important direction is the study of phase transitions between different quasi-de Sitter regimes, where scale independence is lost and the quantum entanglement signal may become sensitive to the history.
The results are directly relevant to planned programs of cosmic Bell tests for the cosmic microwave background and to the broader problem of extracting quantum predictions from astrophysical data. They also clarify which quantum signatures are in principle observable in gravitational-wave and other correlation-based observational programs.
Next steps include the analytical calculation of corrections from non-Gaussian interactions and the construction of explicit transition models (e.g., transition from ultra-slow-roll to slow-roll) to quantify the degree of duality-symmetry breaking.
The work addresses the fundamental problem of the quantum origin of cosmological structures and raises the question of which quantum signatures are in principle observable. The discovered symmetry resonates with paradoxes of quantum gravity, such as information loss in black holes, and with the broader problem of extracting observable quantum correlations in asymptotically de Sitter spaces.
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What the work does
The authors applied the formalism of continuous Gaussian variables to scalar perturbations in the Friedmann expansion, constructed the covariance matrix for two smoothed local modes, and computed its symplectic eigenvalues for Vans-dual backgrounds. They showed that all derived quantum-information quantities (entanglement entropy, mutual information, quantum discord, logarithmic negativity) coincide for dual pairs, despite differences in the matrix elements.
Where its strength is
The work reveals an exact symplectic symmetry linking Vans duality to the conservation of all local quantum-information invariants, providing a clear criterion for the indistinguishability of inflationary histories at the level of linear perturbations.
Where it could go next
Worth trying
Why this may matter
If Vans duality holds at the level of all local quantum-information quantities, it constrains the possibility of directly observing the quantum nature of inflation through linear correlations, but opens the way to searching for violations in nonlinear or non-Gaussian regimes.
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Although the configuration variable (the perturbation itself) is indistinguishable for dual histories, the conjugate momentum behaves differently: in phase space the trajectories diverge, but a local observer measuring only unary and binary correlations will not notice it.