Weak ascending epochs #
Deterministic epoch characterizations assume EpochsFinite, which eliminates
the empty-set value of sInf. Weak epochs retain ties at the running maximum.
The next weak ascending epoch after the epoch s (junk 0 if none).
Equations
Instances For
All epochs exist (the walk returns to each running-maximum level or above).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The number of times u in the cycle [τ_i, τ_{i+1}) with gap < a below the epoch value:
the cycle visit count V_i(a).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The epochs are strictly increasing when finite.
Finiteness makes the epoch sequence strictly increasing.
Every weak epoch attains the running maximum, including time zero.
At an epoch the running maximum is attained: reflGap ω (τ_i) = 0 and the epochs are exactly
the zeros of reflGap (ties are weak records).
The number of epochs u ∈ [1,k] is the last cycle index: τ_H ≤ k < τ_{H+1}.
Inside a cycle the running maximum remains equal to the initial epoch value.
(Deterministic stopped decomposition) With H = weakLadderCount ω k and a > 0:
Σ_{i<H} V_i(a) - 1 ≤ bandCount ω k a ≤ Σ_{i ≤ H} V_i(a).