We study the antiferromagnetic XYZ spin chain with quenched randomness, focusing on a critical line between localized Ising magnetic phases. A previous calculation of Slagle et al., Phys. Rev. B 94, 014205 (2016), using the spectrum-bifurcation renormalization group and assuming marginal many-body localization, proposed that critical indices for Edwards-Anderson correlators vary continuously. In this work we solve the low-energy physics using an unbiased numerically exact tensor network method named the "rigorous renormalization group." We find a line of fixed points consistent with infinite-randomness phenomenology, with critical exponents for average spin correlations varying continuously. The phase boundary tunes from a free-fermion fixed point to an S3-symmetric multicritical point. For weak microscopic interactions, a self-consistent Hartree-Fock-type treatment captures much of the important physics including the varying exponents; we provide an understanding of this as a result of local correlation induced between the mean-field couplings. We then solve the problem of the locally-correlated XY spin chain with arbitrary degree of correlation and provide analytical strong-disorder renormalization group proofs of continuously varying exponents based on the survival probability of an associated classical random walk problem. This is also an example of a line of fixed points with continuously varying exponents in the equivalent disordered free-fermion chain. Finally, we conjecture that this line of fixed points also controls the critical XYZ spin chain for small interaction strength.