We study families
Hn of one-dimensional (1D) quantum spin systems, where
n is the number of spins, which have a spectral gap $\ensuremath{\Delta}E$ between the ground-state and first-excited state energy that scales, asymptotically, as a constant in
n. We show that if the ground state $\ensuremath{\mid}{\ensuremath{\Omega}}_{m}⟩$ of the Hamiltonian
Hm on
m spins, where
m is an
O(1) constant, is locally the same as the ground state $\ensuremath{\mid}{\ensuremath{\Omega}}_{n}⟩$, for arbitrarily large
n, then an arbitrarily good approximation to the ground state of
Hn can be stored efficiently for all
n. We formulate a conjecture that, if true, would imply our result applies to all noncritical 1D spin systems. We also include an appendix on quasiadiabatic evolutions.