We present a model in which the cosmological constant emerges as a purely geometric effect from the four-dimensional compactification of five-dimensional Einstein-Chern-Simons gravity. The compactification of the extra dimension generates an effective cosmological constant depending on the compactification radius , the coupling parameter , and the trace of the compactified field , rather than being introduced as a free parameter. The resulting field equations are structurally equivalent to those of General Relativity with a cosmological constant, so all known vacuum solutions – Schwarzschild–de Sitter, Kerr–de Sitter, and FLRW spacetimes – remain valid. As a concrete application, we derive the Kottler (Schwarzschild–de Sitter) black hole solution. We identify two dynamical regimes. In the weak-field regime, , whose sign is controlled by , requiring fine-tuning to reproduce . In the strong-field regime, dependence on and cancels algebraically, yielding independently of the Chern-Simons coupling. This regime naturally reproduces for , without fine-tuning. The Bekenstein-Hawking entropy of the cosmological horizon gives , consistent with the Gibbons-Hawking result and admitting a direct geometric interpretation in terms of . This framework geometrically reframes the cosmological constant problem: rather than asking why is small, one asks why is large – a reformulation compatible with a large extra dimension without violating established gravitational tests.

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