Quantum squeezing amplification with a weak Kerr nonlinear oscillator
Fig. 2, panel (b-13)
Numerically simulated Wigner function $W(\alpha)$ at $t = 1600$ ns of the first cycle ($C = 1$), against $\mathrm{Re}(\alpha)$ and $\mathrm{Im}(\alpha)$; the dashed grey line is the state trajectory. Bottom row (Sim.) of printed panel (b); the map covers only the region around the state, as deposited.
Files
- Data: data.csv
- Overlay (trajectory): overlay.csv
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-14) (c-1) (c-2) (c-3) (c-4) (c-5) (c-6)
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