Fractals/Mathematics/sequences

Difference between sequences, orders and series types of sequences Integer sequences A137560 A137867 Fraction sequences Farey sequence thumb|right|The Stern-Brocot tree is a data structure showing how the sequence is built up from 0 (= 0 / 1 ) and 1 (= 1 / 1 ), by taking successive mediants. The Farey sequence of order n is the sequence of completely reduced vulgar fractions between 0 and 1 which when in lowest terms have denominators less than or equal to n, arranged in order of increasing size. Each Farey sequence starts with the value 0, denoted by the fraction 0⁄1, and ends with the value 1, denoted by the fraction 1⁄1 (although some authors omit these terms). Farey Addition = the mediant of two fractions : Terms next term = child Previous terms = parentsFinding parents in the Farey tree by Claude Heiland-Allen Farey tree = Farey sequence as a tree Sorted F1 = {0/1, 1/1} F2 = {0/1, 1/2, 1/1} F3 = {0/1, 1/3, 1/2, 2/3, 1/1} F4 = {0/1, 1/4, 1/3, 1/2, 2/3, 3/4, 1/1} F5 = {0/1, 1/5, 1/4, 1/3, 2/5, 1/2, 3/5, 2/3, 3/4, 4/5, 1/1} F6 = {0/1, 1/6, 1/5, 1/4, 1/3, 2/5, 1/2, 3/5, 2/3, 3/4, 4/5, 5/6, 1/1} F7 = {0/1, 1/7, 1/6, 1/5, 1/4, 2/7, 1/3, 2/5, 3/7, 1/2, 4/7, 3/5, 2/3, 5/7, 3/4, 4/5, 5/6, 6/7, 1/1} F8 = {0/1, 1/8, 1/7, 1/6, 1/5, 1/4, 2/7, 1/3, 3/8, 2/5, 3/7, 1/2, 4/7, 3/5, 5/8, 2/3, 5/7, 3/4, 4/5, 5/6, 6/7, 7/8, 1/1} See also Fibonacci Numbers hidden in the Mandelbrot Set - Numberphile Sequences and orders on the parameter plane Sequences of Misiurewicz points external ray for angle 1/(4*2^n) land on the tip of the first branch: 1/4, 1/8, 1/16, 1/32, 1/64, ... 1/(6*2^n) - land on the second branch principal Misiurewicz point of wake p/q How to compute external angles of principal Misiurewicz point of wake p/q using Devaney's algorithm ? program Mandel by Wolf Jung primary_separators degree take the Misiurewicz point for and increase n ( proposed by Owen Maresh) The constant (parameter c) for the quadratic (n=2) , cubic ( n=3), and quartic (n=4) polynomials are: (-0.7432918908524301520519705530861564778806 ,0.1312405523087976002753516038253522297699); -0.0649150006787816892861875745218343125883 , 0.76821968591243610206311097043854440463 ); (-0.593611822136354943067129147813253628530 ,0.5405019391915187246754930586066158919613 ); Point c is a Misiurewicz point tip of the longest branch ( ftip ) The angle 8388607/25165824 or 01010101010101010101010p01 has preperiod = 23 and period = 2 from wake 12/25 , with center c = -0.739829393511579 +0.125072144080321 i and period = 25 root point c = -0.738203140939397 +0.124839088573366 i m-describe 53 30 500 -0.7432918908524301 0.1312405523087976 4 the input point was -7.4329189085243008e-01 + 1.3124055230879761e-01 i nearby hyperbolic components to the input point: - a period 1 cardioid with nucleus at 0.00000e+00 + 0.00000e+00 i the component has size 1.00000e+00 and is pointing west the atom domain has size 0.00000e+00 the atom domain coordinates of the input point are -nan + -nan i the atom domain coordinates in polar form are -nan to the east the atom coordinates of the input point are -0.74329 + 0.13124 i the atom coordinates in polar form are 0.75479 to the west the nucleus is 7.54789e-01 to the east of the input point - a period 2 circle with nucleus at -1.00000e+00 + 0.00000e+00 i the component has size 5.00000e-01 and is pointing west the atom domain has size 1.00000e+00 the atom domain coordinates of the input point are 0.25671 + 0.13124 i the atom domain coordinates in polar form are 0.28831 to the east-north-east the atom coordinates of the input point are 0.51342 + 0.26248 i the atom coordinates in polar form are 0.57662 to the east-north-east the nucleus is 2.88311e-01 to the west-south-west of the input point external angles of this component are: .(01) .(10) the point escaped with dwell 472.09881 nearby Misiurewicz points to the input point: - 24p4 with center at -7.43291890852430202931624325972515e-01 + 1.31240552308797604770845906581477e-01 i the Misiurewicz domain has size 1.07586e-03 the Misiurewicz domain coordinate radius is 1.1395e-13 the center is 1.21387e-16 to the west of the input point the multiplier has radius 1.329970173958942893e+00 and angle 0.150434052944417735 (in turns) The angle 8388607/25165824 or 01010101010101010101010p01 has preperiod = 23 and period = 2. The corresponding parameter ray lands at a Misiurewicz point of preperiod 23 and period dividing 2. Do you want to draw the ray and to shift c to the landing point? c = -0.743291890852430 +0.131240552308798 i period = 0 Myrberg-Feigenbaum point Examples: sequence of root points for periods ( period doubling cascade) and the limit point of the sequence is the Myrberg-Feigenbaum point sequence of root points for periods and the limit point of the sequence is the Myrberg-Feigenbaum point Sharkovsky ordering It is the infinite sequence of positive integers ( natural numbers) It starts from 3 and ends in 1 It contains infinitely many subsequences.Sharkovskii's theorem in wikipedia the number is a period of the miget ( main pseudocardioid of the midget) that appear the first time in that order "The Sharkovski ordering : begins with the odd numbers >= 3 in increasing order ( n is increasing from left to right ), then twice these numbers, then 4 times them, then 8 times them, etc., ending with the powers of 2 in decreasing order, ending with 2^0 = 1." The On-Line Encyclopedia of Integer Sequences : A005408 = The odd numbers: a(n) = 2n+1 It is related with structure of the real slice of the Mandelbrot set ( along real exis): chaotic region, which consist of chaotic bands : MF = Myrberg-Feigenbaum point periodic region P with period doubling cascade = 2^n Period doubling scenario 1/2 family sequence of fraction in the elephant valley In the elephant valley muency : elephant valleyVisual Guide To Patterns In The Mandelbrot Set by Miqel ( from parameter plane ) there is a sequence of componts with period p : from 1/2 to 1/p Note that : internal ray 0/1 = 1/1 internal angle 1/p means that ray goes from period 1 component ( parent period = 1) to period p component ( child period = p) as child period grows computations are harder exponential growthinteger number in wikipedia of . One can easly create a numeric value that is too large to be represented within the available storage space ( integer overflowInteger overflow in wikipedia ). For example is to big for short ( 16 bit ) and long ( 32 bit) integer. The upper principal sequence of rotational number around the main cardioid of Mandelbrot setMandel Set Combinatorics : Principal Series n rotation number = 1/n parameter c2 1/2 -0.75 3 1/3 0.64951905283833*i-0.125 4 1/4 0.5*i+0.25 5 1/5 0.32858194507446*i+0.35676274578121 6 1/6 0.21650635094611*i+0.375 7 1/7 0.14718376318856*i+0.36737513441845 8 1/8 0.10355339059327*i+0.35355339059327 9 1/9 0.075191866590218*i+0.33961017714276 10 1/10 0.056128497072448*i+0.32725424859374 See : Slide show of rescaled limbs converging to the Lavaurs elephant - video by Wolf Jung made with Mandel sequence of parabolic points on the boundary of main cardioid Here: t = internal angle ( or rotation number) of main cardioid q = number of the critical orbit (star) arms. It means that one have to do q iterations around fixed point to move one point toward fixed point along arm. c is a root point between hyperbolic components of period 1 ( = main cardioid) and period q. This point is at the end ( radius = 1) of internal ray for angle t k = log10(q) (double) t 1 3/10 0.3 +0.047745751406263+0.622474571220695 i 2 33/100 0.33 -0.106920138306109 +0.649235321397436 i3 333/1000 0.333 -0.123186752260805 +0.649516204880454 i4 3333/10000 0.3333 -0.124818625550005 +0.649519024348384 i5 33333/100000 0.33333 -0.124981862061192 +0.649519052553419 i6 333333/1000000 0.333333 -0.124998186201184 +0.649519052835480 i 7 3333333/10000000 0.3333333 -0.124999818620069 +0.649519052838300 i8 33333333/100000000 0.33333333 -0.124999981862006 +0.649519052838329 i 9 333333333/1000000000 0.333333333 -0.124999998186201 +0.649519052838329 i10 3333333333/10000000000 0.3333333333 -0.124999999818620 +0.649519052838329 i sequence from Siegel disk to Leau-Fatou flower plain Siegel disk digitated Siegel diskscholarpedia : Siegel_disks , Quadratic_Siegel_disks, Digitation virtual Siegel disk ? Leau-Fatou flower ? 1 over 2 1 over 3 n t 0 0.2763932022500210 +0.1538380639536641 + 0.5745454151066985 i 1 0.3231874668087892 -0.0703924965263780 + 0.6469145331346999 i2 0.3322326933513446 -0.1190170769366243 + 0.6494880316361160 i3 0.3332223278292314 -0.1243960357918422 + 0.6495187369145560 i4 0.3333222232791965 -0.1249395463818515 + 0.6495190496732967 i5 0.3333322222327929 -0.1249939540657307 + 0.6495190528066729 i 6 0.3333332222223279 -0.1249993954008480 + 0.6495190528380124 i7 0.3333333222222233 -0.1249999395400276 + 0.6495190528383258 i 8 0.3333333322222222 -0.1249999939540022 + 0.6495190528383290 i9 0.3333333332222223 -0.1249999993954002 + 0.6495190528383290 i 10 0.3333333333222222 -0.1249999999395400 + 0.6495190528383290 i 11 0.3333333333322222 -0.1249999999939540 + 0.6495190528383290 i sequence of fractions tending to the golden mean ( Golden Ratio Conjugate ) thumb|right|Approximations to the reciprocal golden ratio by finite continued fractions, or ratios of Fibonacci numbers thumb|right|Golden Mean Quadratic Siegel Disc n = 1 ; p_n/q_n = 1.0000000000000000000 = 1 / 1 n = 2 ; p_n/q_n = 0.5000000000000000000 = 1 / 2 n = 3 ; p_n/q_n = 0.6666666666666666667 = 2 / 3 n = 4 ; p_n/q_n = 0.6000000000000000000 = 3 / 5 n = 5 ; p_n/q_n = 0.6250000000000000000 = 5 / 8 n = 6 ; p_n/q_n = 0.6153846153846153846 = 8 / 13 n = 7 ; p_n/q_n = 0.6190476190476190476 = 13 / 21 n = 8 ; p_n/q_n = 0.6176470588235294118 = 21 / 34 n = 9 ; p_n/q_n = 0.6181818181818181818 = 34 / 55 n = 10 ; p_n/q_n = 0.6179775280898876404 = 55 / 89 n = 11 ; p_n/q_n = 0.6180555555555555556 = 89 / 144 n = 12 ; p_n/q_n = 0.6180257510729613734 = 144 / 233 n = 13 ; p_n/q_n = 0.6180371352785145888 = 233 / 377 n = 14 ; p_n/q_n = 0.6180327868852459016 = 377 / 610 n = 15 ; p_n/q_n = 0.6180344478216818642 = 610 / 987 n = 16 ; p_n/q_n = 0.6180338134001252348 = 987 / 1597 n = 17 ; p_n/q_n = 0.6180340557275541796 = 1597 / 2584 n = 18 ; p_n/q_n = 0.6180339631667065295 = 2584 / 4181 n = 19 ; p_n/q_n = 0.6180339985218033999 = 4181 / 6765 n = 20 ; p_n/q_n = 0.6180339850173579390 = 6765 / 10946 n = 21 ; p_n/q_n = 0.6180339901755970865 = 10946 / 17711 n = 22 ; p_n/q_n = 0.6180339882053250515 = 17711 / 28657 n = 23 ; p_n/q_n = 0.6180339889579020014 = 28657 / 46368 n = 24 ; p_n/q_n = 0.6180339886704431856 = 46368 / 75025 n = 25 ; p_n/q_n = 0.6180339887802426829 = 75025 / 121393 n = 26 ; p_n/q_n = 0.6180339887383030068 = 121393 / 196418 n = 27 ; p_n/q_n = 0.6180339887543225376 = 196418 / 317811 n = 28 ; p_n/q_n = 0.6180339887482036214 = 317811 / 514229 n = 29 ; p_n/q_n = 0.6180339887505408394 = 514229 / 832040 n = 30 ; p_n/q_n = 0.6180339887496481015 = 832040 / 1346269 n = 31 ; p_n/q_n = 0.6180339887499890970 = 1346269 / 2178309 n = 32 ; p_n/q_n = 0.6180339887498588484 = 2178309 / 3524578 n = 33 ; p_n/q_n = 0.6180339887499085989 = 3524578 / 5702887 n = 34 ; p_n/q_n = 0.6180339887498895959 = 5702887 / 9227465 n = 35 ; p_n/q_n = 0.6180339887498968544 = 9227465 / 14930352 n = 36 ; p_n/q_n = 0.6180339887498940819 = 14930352 / 24157817 n = 37 ; p_n/q_n = 0.6180339887498951409 = 24157817 / 39088169 n = 38 ; p_n/q_n = 0.6180339887498947364 = 39088169 / 63245986 n = 39 ; p_n/q_n = 0.6180339887498948909 = 63245986 / 102334155 n = 40 ; p_n/q_n = 0.6180339887498948319 = 102334155 / 165580141 n = 41 ; p_n/q_n = 0.6180339887498948544 = 165580141 / 267914296 n = 42 ; p_n/q_n = 0.6180339887498948458 = 267914296 / 433494437 n = 43 ; p_n/q_n = 0.6180339887498948491 = 433494437 / 701408733 n = 44 ; p_n/q_n = 0.6180339887498948479 = 701408733 / 1134903170 n = 45 ; p_n/q_n = 0.6180339887498948483 = 1134903170 / 1836311903 This is a sequence of rational numbers ( Julia sets are parabolic). It's limit is an irrational number ( Julia set has a Siegel disk). Sequence on the dynamic plane More orbit period of the orbit References Hardy-DivergentSeries Mandelbrot Buds and Branches by Timothy Chase: