Feigenbaum constants: Difference between revisions

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These numbers apply to a large class of [[dynamical system]]s (for example, dripping faucets to population growth).<ref name="NonlinearDynamics" />
These numbers apply to a large class of [[dynamical system]]s (for example, dripping faucets to population growth).<ref name="NonlinearDynamics" />


A simple rational approximation is {{sfrac|13|11}} × {{sfrac|17|11}} × {{sfrac|37|27}} = {{sfrac|8177|3267}}.
A simple [[rational number|rational]] approximation is {{sfrac|5|2}}, which is correct to 2 significant values. For more precision use  {{sfrac|13|11}} × {{sfrac|17|11}} × {{sfrac|37|27}} = {{sfrac|8177|3267}}, which is correct to 8 significant values.


==Properties==
==Properties==
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== Other values ==
== Other values ==
The period-3 window in the logistic map also has a period-doubling route to chaos, reaching chaos at <math>r = 3.854 077 963 591\dots</math>, and it has its own two Feigenbaum constants: <math>\delta = 55.26, \alpha = 9.277</math>.<ref>{{Cite journal |last1=Delbourgo |first1=R. |last2=Hart |first2=W. |last3=Kenny |first3=B. G. |date=1985-01-01 |title=Dependence of universal constants upon multiplication period in nonlinear maps |url=https://link.aps.org/doi/10.1103/PhysRevA.31.514 |journal=Physical Review A |language=en |volume=31 |issue=1 |pages=514–516 |doi=10.1103/PhysRevA.31.514 |pmid=9895509 |bibcode=1985PhRvA..31..514D |issn=0556-2791}}</ref><ref>{{Cite book |last=Hilborn |first=Robert C. |title=Chaos and nonlinear dynamics: an introduction for scientists and engineers |date=2000 |publisher=Oxford University Press |isbn=0-19-850723-2 |edition=2nd |location=Oxford |oclc=44737300 |page=578}}</ref>{{rp|at=Appendix F.2}}
The period-3 window in the logistic map also has a period-tripling route to chaos, reaching chaos at <math>r = 3.854 077 963 591\dots</math>, and it has its own two Feigenbaum constants: <math>\delta = 55.26, \alpha = 9.277</math>.<ref>{{Cite journal |last1=Delbourgo |first1=R. |last2=Hart |first2=W. |last3=Kenny |first3=B. G. |date=1985-01-01 |title=Dependence of universal constants upon multiplication period in nonlinear maps |url=https://link.aps.org/doi/10.1103/PhysRevA.31.514 |journal=Physical Review A |language=en |volume=31 |issue=1 |pages=514–516 |doi=10.1103/PhysRevA.31.514 |pmid=9895509 |bibcode=1985PhRvA..31..514D |issn=0556-2791|url-access=subscription }}</ref><ref>{{Cite book |last=Hilborn |first=Robert C. |title=Chaos and nonlinear dynamics: an introduction for scientists and engineers |date=2000 |publisher=Oxford University Press |isbn=0-19-850723-2 |edition=2nd |location=Oxford |oclc=44737300 |page=578}}</ref>{{rp|at=Appendix F.2}}


==See also==
==See also==
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: {{OEIS el|1=A195102|2=Decimal expansion of the parameter for the biquadratic solution of the Feigenbaum-Cvitanovic equation}}
: {{OEIS el|1=A195102|2=Decimal expansion of the parameter for the biquadratic solution of the Feigenbaum-Cvitanovic equation}}
* [http://planetmath.org/feigenbaumconstant Feigenbaum constant ] – PlanetMath
* [http://planetmath.org/feigenbaumconstant Feigenbaum constant ] – PlanetMath
* Julia notebook for calculating Feigenbaum constant<ref>{{Cite web |last=Hofstätter |first=Harald |date=October 25, 2015 |title=Calculation of the Feigenbaum Constants |url=http://www.harald-hofstaetter.at/Math/Feigenbaum.html |access-date=2024-04-07 |website=www.harald-hofstaetter.at}}</ref>
* {{Cite web |last=Hofstätter |first=Harald |date=October 25, 2015 |title=Calculation of the Feigenbaum Constants |url=http://www.harald-hofstaetter.at/Math/Feigenbaum.html |access-date=2024-04-07 |website=www.harald-hofstaetter.at | type=Julia notebook for calculating Feigenbaum constant}}
* {{cite web|last=Moriarty|first=Philip|title={{mvar|δ}} – Feigenbaum Constant|url=http://www.sixtysymbols.com/videos/feigenbaum.htm|work=Sixty Symbols|publisher=[[Brady Haran]] for the [[University of Nottingham]]|author2=Bowley, Roger|year=2009}}
* {{cite web|last=Moriarty|first=Philip|title={{mvar|δ}} – Feigenbaum Constant|url=http://www.sixtysymbols.com/videos/feigenbaum.htm|work=Sixty Symbols|publisher=[[Brady Haran]] for the [[University of Nottingham]]|author2=Bowley, Roger|year=2009}}
* {{Cite thesis|type =PhD|last=Thurlby | first=Judi|date=2021|title=Rigorous calculations of renormalisation fixed points and attractors|publisher= U. Portsmouth|url=https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.840285}}
* {{Cite thesis|type=PhD|last=Thurlby|first=Judi|date=2021|title=Rigorous calculations of renormalisation fixed points and attractors|publisher=U. Portsmouth|url=https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.840285|archive-date=22 April 2022|access-date=21 March 2022|archive-url=https://web.archive.org/web/20220422223333/https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.840285|url-status=dead}}


{{Chaos theory}}
{{Chaos theory}}
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{{DEFAULTSORT:Feigenbaum Constants}}
{{DEFAULTSORT:Feigenbaum Constants}}
[[Category:Dynamical systems]]
[[Category:Dynamical systems]]
[[Category:Eponymous numbers in mathematics]]
[[Category:Mathematical constants]]
[[Category:Mathematical constants]]
[[Category:Bifurcation theory]]
[[Category:Bifurcation theory]]
[[Category:Chaos theory]]
[[Category:Chaos theory]]

Latest revision as of 22:43, 9 November 2025

Template:Short description Template:Use dmy dates Template:Infobox non-integer number

In mathematics, specifically bifurcation theory, the Feigenbaum constants Template:IPAc-en[1] Template:Mvar and Template:Mvar are two mathematical constants which both express ratios in a bifurcation diagram for a non-linear map. They are named after the physicist Mitchell J. Feigenbaum.

History

Feigenbaum originally related the first constant to the period-doubling bifurcations in the logistic map, but also showed it to hold for all one-dimensional maps with a single quadratic maximum. As a consequence of this generality, every chaotic system that corresponds to this description will bifurcate at the same rate. Feigenbaum made this discovery in 1975,[2][3] and he officially published it in 1978.[4]

The first constant

The first Feigenbaum constant or simply Feigenbaum constant[5] Template:Mvar is the limiting ratio of each bifurcation interval to the next between every period doubling, of a one-parameter map

xi+1=f(xi),

where Template:Math is a function parameterized by the bifurcation parameter Template:Mvar.

It is given by the limit:[6]

δ=limnan1an2anan1

where Template:Mvar are discrete values of Template:Mvar at the Template:Mvarth period doubling.

This gives its numerical value (sequence A006890 in the OEIS):

δ=4.669201609102990671853203820466

  • A simple rational approximation is Template:Sfrac, which is correct to 5 significant values (when rounding). For more precision use Template:Sfrac, which is correct to 7 significant values.
  • It is approximately equal to Template:Math, with an error of 0.0047 %.

Illustration

Non-linear maps

To see how this number arises, consider the real one-parameter map

f(x)=ax2.

Here Template:Mvar is the bifurcation parameter, Template:Mvar is the variable. The values of Template:Mvar for which the period doubles (e.g. the largest value for Template:Mvar with no period-2 orbit, or the largest Template:Mvar with no period-4 orbit), are Template:Math, Template:Math etc. These are tabulated below:[7]

Template:Mvar Period Bifurcation parameter (Template:Mvar) Ratio Template:Math
1 2 0.75
2 4 1.25
3 8 Template:Val 4.2337
4 16 Template:Val 4.5515
5 32 Template:Val 4.6458
6 64 Template:Val 4.6639
7 128 Template:Val 4.6682
8 256 Template:Val 4.6689

The ratio in the last column converges to the first Feigenbaum constant. The same number arises for the logistic map

f(x)=ax(1x)

with real parameter Template:Mvar and variable Template:Mvar. Tabulating the bifurcation values again:[8]

Template:Mvar Period Bifurcation parameter (Template:Mvar) Ratio Template:Math
1 2 3
2 4 Template:Val
3 8 Template:Val 4.7514
4 16 Template:Val 4.6562
5 32 Template:Val 4.6683
6 64 Template:Val 4.6686
7 128 Template:Val 4.6680
8 256 Template:Val 4.6768

Fractals

File:Mandelbrot zoom.gif
Self-similarity in the Mandelbrot set shown by zooming in on a round feature while panning in the negative-Template:Mvar direction. The display center pans from (−1, 0) to (−1.31, 0) while the view magnifies from 0.5 × 0.5 to 0.12 × 0.12 to approximate the Feigenbaum ratio.

In the case of the Mandelbrot set for complex quadratic polynomial

f(z)=z2+c

the Feigenbaum constant is the limiting ratio between the diameters of successive circles on the real axis in the complex plane (see animation on the right).

Template:Mvar Period = Template:Math Bifurcation parameter (Template:Mvar) Ratio =cn1cn2cncn1
1 2 Template:Val
2 4 Template:Val
3 8 Template:Val 4.2337
4 16 Template:Val 4.5515
5 32 Template:Val 4.6459
6 64 Template:Val 4.6639
7 128 Template:Val 4.6668
8 256 Template:Val 4.6740
9 512 Template:Val 4.6596
10 1024 Template:Val 4.6750
... ... ... ...
Template:Math Template:Val...

Bifurcation parameter is a root point of period-Template:Math component. This series converges to the Feigenbaum point Template:Mvar = −1.401155...... The ratio in the last column converges to the first Feigenbaum constant.

File:Feigenbaum Julia set.png
Julia set for the Feigenbaum point

Other maps also reproduce this ratio; in this sense the Feigenbaum constant in bifurcation theory is analogous to [[Pi (number)|Template:Pi]] in geometry and Template:Math in calculus.

The second constant

The second Feigenbaum constant or Feigenbaum reduction parameter[5] Template:Mvar is given by (sequence A006891 in the OEIS):

α=2.502907875095892822283902873218

It is the ratio between the width of a tine and the width of one of its two subtines (except the tine closest to the fold). A negative sign is applied to Template:Mvar when the ratio between the lower subtine and the width of the tine is measured.[9]

These numbers apply to a large class of dynamical systems (for example, dripping faucets to population growth).[9]

A simple rational approximation is Template:Sfrac, which is correct to 2 significant values. For more precision use Template:Sfrac × Template:Sfrac × Template:Sfrac = Template:Sfrac, which is correct to 8 significant values.

Properties

Both numbers are believed to be transcendental, although they have not been proven to be so.[10] In fact, there is no known proof that either constant is even irrational.

The first proof of the universality of the Feigenbaum constants was carried out by Oscar Lanford—with computer-assistance—in 1982[11] (with a small correction by Jean-Pierre Eckmann and Peter Wittwer of the University of Geneva in 1987[12]). Over the years, non-numerical methods were discovered for different parts of the proof, aiding Mikhail Lyubich in producing the first complete non-numerical proof.[13]

Other values

The period-3 window in the logistic map also has a period-tripling route to chaos, reaching chaos at r=3.854077963591, and it has its own two Feigenbaum constants: δ=55.26,α=9.277.[14][15]Template:Rp

See also

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Notes

Template:Reflist

References

  • Alligood, Kathleen T., Tim D. Sauer, James A. Yorke, Chaos: An Introduction to Dynamical Systems, Textbooks in mathematical sciences Springer, 1996, Template:Isbn
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External links

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