The cold dark matter paradigm has been posited as the standard explanation for the non-Keplerian behavior of galaxy rotation curves, where for galaxies satisfying the Tully-Fisher relation, the mass of the dark matter halo from a large class of universal dark matter profiles ought to roughly increase linearly with radial distance at large distances, $m(r) sim r/nG$ ($G$ is the gravitational constant and $n$ is a dimensionless parameter which depends on the amount of baryonic matter $M$ within the galaxy). Despite numerous advances in modeling galaxy formation and evolution, a scientific consensus on the origin of the observed dependence of the dimensionless parameter $n = (GMa_{0})^{-1/2}$ on the mass of baryonic matter $M$ within the galaxy (the Tully-Fisher relation), and the connection of the cosmological constant $Lambda$ to the parameter $a_{0} sim (Lambda/3)^{1/2}$ remains elusive. Here, we show that Einstein Field Equations can be remolded into $ abla_{ u}mathcal{K}^{ u}_{,,mu} = 8pi GMPsi^{*}mathcal{D}_{mu}Psi$, where $mathcal{K}_{mu u}$ is a complex Hermitian tensor, $mathcal{D}_{mu}$ is a covariant derivative and $Psi$ is a complex-valued function. This avails a novel constraint, $ abla_{mu} abla_{ u}mathcal{K}^{mu u} = 0$ not necessarily available in Einsteins General Relativity. In the weak-field regime, we can readily reproduce the Tully-Fisher relation using the usual charge-less pressure-less fluid. Moreover, our approach is equivalent to a Ginzburg-Landau theory of $n$ bosons, where the order parameter is normalized as $int_{0}^{1/a_{0}} dr,4pi r^2Psi^*Psi = n$ and $1/a_{0} sim (Lambda/3)^{-1/2}$ is the cut-off length scale comparable to the size of the de Sitter universe. Our investigations provide a framework that reproduces the mass-asymptotic speed relation in galaxies within the cold dark matter paradigm.
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