Inflation is the rapid expansion of the newborn Universe, when quantum fluctuations were stretched to cosmic scales. The cosmic microwave background is the fossilized light of that epoch, shadows on the wall of our cosmic cave. Alan Guth realized that inflation solves the puzzles of the Big Bang, and Edwin Hubble gave us the key — the law of expansion. But what do we see in these shadows? The quantum spectacle is more cunningly arranged than we thought.
Wands duality states: different inflation scenarios — slow-roll and ultra-slow-roll — yield the same power spectrum. The configuration variable is indistinguishable. But in phase space, the trajectories diverge: the conjugate momentum behaves differently. Imagine two puppeteers: the marionettes' arms move identically for the shadow, but their joints bend in their own way. The question arises: does the identicalness persist at the level of genuinely quantum correlations — entanglement between different regions?
In the new work, researchers showed: yes, it does. Applying the formalism of Gaussian variables to local modes, they computed the symplectic invariants. It turned out that for any dual histories, all quantum information measures — from entanglement entropy to discord — coincide. The evolution obeys the equation: $v''_k + (k^2 - z''/z) v_k = 0$, where $z''/z \approx (\nu^2-1/4)/\eta^2$. The index $\nu$ is the same for dual models — it is like a single director dictating the shadows.
This hidden symmetry means that Wands duality extends from the configuration level to the full quantum description of a Gaussian state. The duality transformation acts as a local symplectic transformation in phase space, preserving all invariants. Imagine: you are watching a shadow theatre, and the shadows remain unchanged even if the actors behind the screen perform different dances. Information about the deep dynamics is lost, and our ability to reconstruct the details of the inflationary potential from the cosmic microwave background hits a fundamental limit. This is not just a technical limitation — entanglement itself, which we used to think of as a magnifying glass, turns into a smoke screen. Here we hear an echo of the paradoxes of spacetime in quantum gravity: an observer at the event horizon cannot tell one quantum history from another — information disappears behind the scenes.
However, the symmetry is broken at the nonlinear level — where non-Gaussianity is born. Precisely these microscopic deviations from the Gaussian shadow may become the key to the puzzle. Ahead lie cosmic Bell tests for entanglement (in the spirit of the ideas of John Stewart Bell) and the analysis of phase transitions between different de Sitter regimes. Perhaps one day we will learn to read not only the shadows but also the vibrations of the curtain separating us from the quantum beginning of the expansion of the Universe. This is not just a test of inflation — it is a search for the boundaries of the very quantum description of reality.
Although the configuration variable (the perturbation itself) is indistinguishable for dual histories, the conjugate momentum behaves differently: in phase space, the trajectories diverge like two spirals of different pitch, but a local observer armed only with unary and binary correlations sees them merged into a single shadow.