Concept

Feigenbaum constant

The number 4.6692…, the limiting ratio between successive intervals of a period-doubling cascade. It is the same for every smooth one-humped map with a quadratic top, a universality explained by a renormalisation that rescales the map onto itself.

Named by 5 essays across one field — each of them below, with the objects they name alongside it.

Where the period doubles, and by how much the gaps shrink. The parameters at which the period doubles, with the ratio of consecutive gaps beside them.

A constant that does not care which map

The gaps between successive period doublings shrink by a factor. Measure that factor for the logistic map and you get 4.669. Measure it for a completely different map and you get 4.669, and nobody expected that.

dynamics · Period-doubling
The turning point's orbit over the bifurcation diagram, 3.55 to 4. The bifurcation diagram of the logistic map from 3.55 to 4 with the curves f(1/2), f²(1/2), … up to the 6th image drawn over it. The first two bound the attractor and the rest trace the dark lines inside it.

The dark lines are one point's orbit

Past the end of the period-doubling cascade the bifurcation diagram turns into grey bands crossed by darker curves. Every one of those curves is the orbit of a single point — the top of the hump — and the places where they meet are exactly where the bands merge, in a second cascade that runs backwards at the same rate.

dynamics · Period-doubling
Where the Rössler flow's peaks fall, as one parameter changes. Peak values of x against c from 2.5 to 6.2 for the Rössler system with a = b = 0.2: period 1, 2 and 4 at c = 2.5, 3.5 and 4, chaos beyond about 4.2, a period-3 window near 5.3.

A flow that doubles like a parabola

Otto Rössler's three equations have one nonlinear term and a single knob. Turn it and the orbit closes after one loop, then two, then four, then never — the logistic map's cascade, in a flow in three dimensions. Record each peak of the orbit against the one before and the reason appears: the points lie on a single rounded hump. The gaps between doublings shrink by ratios 3.49, 4.54, 4.59, climbing towards Feigenbaum's 4.669, and the chaos contains a period-3 window that repeats the whole cascade.

dynamics · Period-doubling
Three cascades, a sharp top, a round top and a flat top. z = 1.25: δ ≈ 3.2596; z = 2: δ ≈ 4.6692; z = 6: δ ≈ 9.2963.

One constant for each shape of top

Feigenbaum's 4.669 is the same for every smooth one-humped map — provided the hump is rounded like a parabola. Make the top flatter, like the graph of x to the fourth, and the doublings crowd together at 7.285; make it sharper, like x to the power 1.25, and they crowd at 3.260. Measured across twenty shapes of top, the constant is a smooth rising curve with 4.669 as one point on it, and the spatial constant falls as it rises.

dynamics · Period-doubling
Period doubling with nothing attracting. doubling parameters 3.0000000000, 4.0000000000, 4.1204524973, 4.1343639125, 4.1359600588, 4.1361430974, 4.1361640856.

Doubling without an attractor

Feigenbaum's 4.669 holds for every map that folds and loses area. A map that keeps area — a frictionless pendulum sampled once a swing — has no attractors at all, yet its periodic orbits double just the same: a period-1 orbit at a = 3, period 2 at a = 4, then 4.1205, 4.1344, 4.1360 and on. The intervals shrink by 8.721 each time, not 4.669, and the orbits by 4.018, not 2.503. Let the map leak a little area and the cascade starts with one constant and finishes with the other.

dynamics · Period-doubling

Named alongside it

The objects these essays reach for when they reach for this one.

Period-doublingUniversalityBifurcationRenormalisationCritical pointLogistic mapScalingArea-preserving mapAttractorChaosConvergenceDifferential equation

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