Analytic representation of the probe-induced field

Derive an analytic expression for the field component V_δ generated by the coated probe in the coupled sample–probe system, rather than relying on the formal series representation used in the proof of the cloaking result.

Background

The active-cloaking analysis decomposes the probe-related field into V_δ, generated directly by the core-shell probe, and T_δ, representing the interaction between the probe and the sample. The proof of Theorem 6 establishes that both terms vanish outside the critical radius as the loss parameter δ tends to zero, thereby showing that the probe becomes effectively invisible.

Although the authors derive a formal Fourier-series representation for V_δ, its coefficients depend on the coupled density Φ and therefore incorporate sample–probe interaction information. Consequently, the representation is not an explicit analytic formula. Obtaining such a formula would clarify the field structure underlying the cloaking mechanism and potentially improve rigorous and computational analyses of more general probe configurations.

References

It should be emphasized that, unlike the case of eqref{solution-S2S3}, we do not obtain an analytic expression for eqref{Vdelta}; the expression is only formal.

Vanishing Clutter: Fast and Accurate Shape Imaging via Active Cloaking  (2608.13839 - Xiao et al., 14 Aug 2026) in Section 4.2, proof of Theorem 6