We discuss the problem of static chaos in spin glasses. In the case of
magnetic-field perturbation, we propose a scaling theory for the spin
-glass phase. Using the mean-field approach we argue that some pure st
ates are suppressed by the magnetic field and their free-energy cost i
s determined by the finite-temperature fixed-point exponents. In this
framework, numerical results suggest that mean-field chaos exponents a
re probably exact in finite dimensions. If we use the droplet approach
, numerical results suggest that the zero-temperature fixed-point expo
nent theta is very close to (d - 3)/2. In both approaches d = 3 is the
lower critical dimension in agreement with recent numerical simulatio
ns.