Abstract The configuration space of spin-glasses is characterized by the existence of quasi-degenerate equilibrium states separated by barriers, Δ( T ). A temperature cycling protocol enables us to extract the temperature dependence of a specific barrier . We determine ϖΔ( T )/ϖ T vs T , and ϖΔ( T )/ϖ T vs Δ for barriers between 25 T g and 35 T g at temperatures 8, 9, 9.5 and 10 K ( T g = 10.4 K) for Ag:Mn (2.6 at%). We find, in the range of temperature investigated and within experimental accuracy, that ϖΔ( T )/ϖ T depends only on the particular value of Δ( T ) and not on the temperature. dΔ( T )/d T r can be fitted using all the data points to either a power law ( a Δ 6 ) or an exponential [α exp(βΔ)], where r = T / T g . Integration leads to a divergence of Δ( T ) at temperature T ∗ (integration constant) as the temperature decreases, characteristic of the particular barrier considered. The existence of aging effects at all temperatures below T g in the whole range of accessible times impliesa continuous distribution of barrier heights at any temperature. Hence, at any temperature below T g there are diverging barriers, associated with a distribution of T ∗ with an upper cutoff value of T g . Said another way, as the temperature is lowered to T g , the first divergence of a barrier occurs, separating phase space into two (or more) regimes. States separated by divergent barriers are the “pure states”. As the temperature is lowered, a continuous series of barrier divergences breaks up phase space into ever smaller regions, creating an ever increasing number of pure states. Between these divergent barriers, barriers of finite height exist. Those between 25 T g and 35 T g are responsible for the dynamics accessible to us in our experiments. We interpret the time decay of the thermoremanent magnetization, M TRM ( t ), at times t much larger than the waiting time, t w , as a measure of the correlation of the spin-glass state at t with the field cooled state. Using the concept of ultrametricity, this enables us to extract the branching ratio of the “tree” into which the spin-glass states are organized from a plot of log M TRM ( t ) vs log t , for t a t w . Experiements times t up to to 5540 min (4 days!) exhibits a linear waiting time of 10.2 min and measurement times t up to 5 540 min (4 days!) exhibit a linear relationship between log M TRM ( t ) and log t . Within the approximations made, this implies a constant branching ratio for the ultrametric tree, at least within the (small) range of overlaps q accessible to us because of our experimental time window. These conclusions suggest that our dynamical measurements can be interpreted within the mean-field picture for spin-glasses.
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