Quantum squeezing amplification with a weak Kerr nonlinear oscillator
Fig. 2, panel (c-5)
Measured Wigner function $W(\alpha)$ of the squeezed vacuum state at the end of cycle $C = 5$, against $\mathrm{Re}(\alpha)$ and $\mathrm{Im}(\alpha)$. The deposited map reaches $\mathrm{Im}(\alpha) = \pm 5$; the print shows $\pm 4$.
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Provenance
This panel was computed from the authors' public data deposit (Nature Communications Source Data: https://doi.org/10.1038/s41467-025-67699-0, CC BY 4.0). The plot shown here is re-rendered for interactive viewing and analysis. See the paper for the original figure and full scientific context.
License: CC BY 4.0.
Nat. Commun. 17, 970 (2025) · DOI: 10.1038/s41467-025-67699-0
Other panels of Fig. 2: (b-1) (b-2) (b-3) (b-4) (b-5) (b-6) (b-7) (b-8) (b-9) (b-10) (b-11) (b-12) (b-13) (b-14) (c-1) (c-2) (c-3) (c-4) (c-6)
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