We propose a novel approach for optimizing topological quantum devices: instead of merely isolating qubits from environmental noise, we engineer the environment to actively suppress decoherence. For a Majorana qubit in a topological superconducting wire, the exponentially small energy splitting provides protection against local perturbations but renders it highly susceptible to pure dephasing from low-frequency environmental noise. We show that coupling via a parity-conserving operator () to a bosonic environment yields a dephasing rate , where is the environmental noise power at the qubit splitting frequency. In the experimentally relevant regime where (with mK), the noise power scales as , leading to a dephasing rate . This exposes a fundamental challenge: the dephasing rate diverges as for a standard environment, e.g., a 1D system with linear dispersion where is constant. We overcome this by designing environments with a suppressed density of states following . This creates an ``inverse Purcell effect’’ that yields a temperature-independent suppression factor . For , the engineered dephasing rate decreases exponentially with wire length, , meaning longer wires provide better coherence protection. This provides a quantitative design principle where environmental engineering transforms detrimental noise into a tool for coherence stabilization, while respecting fermion parity superselection rules.

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