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The presence of a nonconformally invariant term in the photon sector of the Lorentz-violating extension of Standard Model of particle physics, the "Kosteleck\'{y} term" $\mathcal{L}_K \propto (k_F)_{\alpha \beta \mu \nu} F^{\alpha \beta} F^{\m \nu}$, enables a superadiabatic amplification of magnetic vacuum fluctuations during de Sitter inflation.
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