  All higher-spin s >= 1/2 Ising spin glasses are studied by
renormalization-group theory in spatial dimension d=3. The s-sequence of global
phase diagrams, the chaos Lyapunov exponent, and the spin-glass runaway
exponent are calculated. It is found that, in d=3, a finite-temperature
spin-glass phase occurs for all spin values, including the continuum limit of s
\rightarrow \infty. The phase diagrams, with increasing spin s, saturate to a
limit value. The spin-glass phase, for all s, exhibits chaotic behavior under
rescalings, with the calculated Lyapunov exponent of \lambda = 1.93 and runaway
exponent of y_R=0.24, showing simultaneous strong-chaos and strong-coupling
behaviors. The ferromagnetic-spinglass-antiferromagnetic phase transitions
occurring around p_t = 0.37 and 0.63 are unaffected by s, confirming the
percolative nature of this phase transition.
