Euler's decomposition of the exponential function $e^x$ partitions the power series into four subseries according to the residue modulo 4 of the summation index:
$$S_0(x) = \sum_{k=0}^{\infty} \frac{x^{4k}}{(4k)!}$$ $$S_1(x) = \sum_{k=0}^{\infty} \frac{x^{4k+1}}{(4k+1)!}$$ $$S_2(x) = \sum_{k=0}^{\infty} \frac{x^{4k+2}}{(4k+2)!}$$ $$S_3(x) = \sum_{k=0}^{\infty} \frac{x^{4k+3}}{(4k+3)!}$$Evaluating the parity sums yields the hyperbolic functions:
Their ratio defines the hyperbolic cotangent:
$$\frac{S_0(x) + S_2(x)}{S_1(x) + S_3(x)} = \coth(x)$$Evaluating the alternating differences yields the circular trigonometric functions:
Their ratio defines the circular cotangent:
$$\frac{S_0(x) - S_2(x)}{S_1(x) - S_3(x)} = \cot(x)$$We apply the identical modulo-4 partition to the Riemann zeta function $\zeta(s) = \sum_{n=1}^{\infty} n^{-s}$ for $\operatorname{Re}(s) > 1$, expressed via Hurwitz zeta functions $\zeta(s, a)$:
$$Z_1(s) = \sum_{k=0}^{\infty} (4k+1)^{-s} = 4^{-s} \zeta\left(s, \frac{1}{4}\right)$$ $$Z_2(s) = \sum_{k=0}^{\infty} (4k+2)^{-s} = 2^{-s} \sum_{m=0}^{\infty} (2m+1)^{-s} = 2^{-s} (1 - 2^{-s}) \zeta(s)$$ $$Z_3(s) = \sum_{k=0}^{\infty} (4k+3)^{-s} = 4^{-s} \zeta\left(s, \frac{3}{4}\right)$$ $$Z_0(s) = \sum_{k=1}^{\infty} (4k)^{-s} = 4^{-s} \zeta(s)$$The ratio of the odd to even parity sums cancels the transcendental component $\zeta(s)$ identically:
$$\frac{Z_1(s) + Z_3(s)}{Z_2(s) + Z_0(s)} = \frac{1 - 2^{-s}}{2^{-s}} = 2^s - 1$$where $\beta(s)$ is the Dirichlet beta function.
where $\eta(s) = (1 - 2^{1-s}) \zeta(s)$ is the Dirichlet eta function.
The ratio of the odd to even alternating differences defines the Coordinate Ratio $K(s)$:
$$K(s) = \frac{Z_1(s) - Z_3(s)}{Z_2(s) - Z_0(s)} = \frac{\beta(s)}{2^{-s} \eta(s)} = 2^s \frac{\beta(s)}{\eta(s)}$$The Coordinate Remainder $k(s)$ isolates the transcendental deviation of the alternating ratio $K(s)$ relative to the rational base scale $2^s$:
$$k(s) = K(s) - 2^s = 2^s \left( \frac{\beta(s)}{\eta(s)} - 1 \right)$$Through this partition, Euler's exponential framework and the Dirichlet series framework are revealed as dual representations of a single modulo-4 symmetry. The scalar $2^s - 1$ represents the pure geometric parity partition, while $K(s)$ and $k(s)$ govern the phase-shifted alternating spectrum.