In spin-glass systems, frustration can be adjusted continuously and
considerably, without changing the antiferromagnetic bond probability p, by
using locally correlated quenched randomness, as we demonstrate here on
hypercubic lattices and hierarchical lattices. Such overfrustrated and
underfrustrated Ising systems on hierarchical lattices in d=3 and 2 are
studied. With the removal of just 51 % of frustration, a spin-glass phase
occurs in d=2. With the addition of just 33 % frustration, the spin-glass phase
disappears in d=3. Sequences of 18 different phase diagrams for different
levels of frustration are calculated in both dimensions. In general,
frustration lowers the spin-glass ordering temperature. At low temperatures,
increased frustration favors the spin-glass phase (before it disappears) over
the ferromagnetic phase and symmetrically the antiferromagnetic phase. When any
amount, including infinitesimal, frustration is introduced, the chaotic
rescaling of local interactions occurs in the spin-glass phase. Chaos increases
with increasing frustration, as seen from the increased positive value of the
calculated Lyapunov exponent λ, starting from λ=0 when
frustration is absent. The calculated runaway exponent yR of the
renormalization-group flows decreases with increasing frustration to yR=0
when the spin-glass phase disappears. From our calculations of entropy and
specific heat curves in d=3, it is seen that frustration lowers in temperature
the onset of both long- and short-range order in spin-glass phases, but is more
effective on the former. From calculations of the entropy as a function of
antiferromagnetic bond concentration p, it is seen that the ground-state and
low-temperature entropy already mostly sets in within the ferromagnetic and
antiferromagnetic phases, before the spin-glass phase is reached.Comment: Published version, 18 phase diagrams, 12 figures, 10 page