ROUTE TO CHAOS IN THREE-DIMENSIONAL MAPS OF LOGISTIC TYPE. 1 Abstract : A route to chaos is studied in 3-dimensional maps of logistic type. Mechanisms of period doubling for invariant closed curves (ICC) are found for specific 3-dimensional maps. These bifurcations cannot be observed for ICC in the 2-dimensional case. When the parameter of the system is modified, localized oscillations occur on the ICC that give rise to weakly chaotic rings, then to chaotic attractors, which finally disappear by contact bifurcations. These maps can be considered as models for the symbiotic interaction of three species. I INTRODUCTION ! " & # # % " $% ' $ % & "& λ # '# & 3 + =λ 0 + − + =λ 0 + − + =λ 0 + − + =λ + + + − + =λ + + + − + =λ + + + − & ' # 2 0 ( )$ & $& & " 0 4 $ 1 21 "& λ & % , $ ( ) (*) (+), - & $ ( ) (*), . '# " & , %2 & & % & " ' ' ' 0 & # & / % % % & & $ # & # & % # & λ & % $ , , II PERIOD DOUBLING OF INVARIANT CLOSED CURVES $ & , 4 0 $4 *λ − 0 + λ λ 5 % ' (6,78 6,9:8) '# # ' ' $ $ & ' % ,& / $ & 4 2 & λ<6,::98 .@@ @ & $& % * $ , '# "1 0 ;% λ<6,9:8 ' = >& / ? $ # .@@ @ ' ,@ ' / $ * & % λ<6,:768 ' .@@ # (7)(9) $ 0 & & , , ' % ' , % .@@ @2 ' 0 1 &' !"#$$ % ( ) ' '* & 8666: D ' - , )' $@ & - A. . @ B $ A C # D ' 2 @0 @2 @ ' 8 4 $ ' 8 $ @0 , ' & 2 & & # ' & ' # $ 2 " lambda = 0.895 .@@ ' ' 0 7 $ , lambda = 0.975 z z y ' x 1 # y x ' # .@@ @ $& 1 ' $.@@ @ , la m b d a = 0 .9 9 9 5 la m b d a = 0 .9 7 5 y y x x ' 1 E $.@@ @ , ' 1 E $ .@@ @ $ ', la m b d a = 1 .0 0 0 4 3 6 7 5 lambda = 0.9995 y z y ' x 1 .@@ @ $ ', x ' 2 1 F " / ' .@@ @ , 0 la m b d a = 1 .0 0 1 la m b d a = 1 .0 0 0 4 3 6 7 5 y y x x ' 2 1B '& $ ' 2 , ' 2 1 .@@ @ la m b d a = 1 .0 0 1 & % /" ' 5@ , lambda = 0.986 y z y ' x ' 2 1B '& $ ' x 0 1- .@@ @2 $& , 2 , l a m b d a = 0 .9 8 6 5 la m b d a = 0 .9 8 6 y y x x ' 0 1 E $.@@ @2 , ' 0 1 E $.@@ @2 ', $ + lambda = 1.15 lambda = 1.17 z z ' x x y y 9 1 % , " .@@ $ ' 7 & " ' 9 1 $ $ ' $ 9 % & " ' , III FROM WEAKLY CHAOTIC RINGS TO CHAOS $ & ' $ @ ' + 5@ $ '$ $$ .@@ $ % & $ 2 ' 2 & # , F " / ' ' 2 $% /" ' 5 @ (8) ' 2 $ .@@ @ ' * $ .@@ @2 $ .@@ @0 $& ,-& G / H $ # ' 2 I* # $ 2 & (*), ' ' + $ .@@ @0 $ 9 $ 2 " .@@ $ 2 , IV MULTISTABILITY . $& 0 " # 2 % @2 .@@ @0 ' , .@@ @2 % 2 " .@@ 4 # ' ' 7 I & ' ' 2 .@@ @ : ' 4 & # $ 6 % 2 % & 4 % ' " , .@@ ' : % & (*), & ' 6 , @0 # 4 , $ & '% 9 , " 9 , & .@@ @ 4 & 0 5@ % # ' .@@ @2 .@@ @ 2 " $ $ " lambda = 0.95332 lambda = 0.95 z z y ' : 1! 0 " .@@, y x 4 $.@@ @ $ ' : 1 ! 5@ , x 0 " .@@ & 7 la m b d a = 0 .9 5 3 3 3 7 lambda = 0.986 y z y ' x ' : 1 E $.@@ $ ' : 6 1! 4 $.@@ @ @2, , lambda = 1.004 lambda = 0.9876 z z y ' x y x 6 1! @2, 4 $.@@ @ x ' 1! 5 @ @2, 4 $ @ V DISAPPEARANCE OF ATTRACTORS 2 # % / " & $ $ 0 $ $ , & 2, $ % " lambda = 1.0040009 3 $ & , lambda = 0.98762 z z y ' & $ 21 ! $ $ y x @0 ,3 $ E ' $ @, ' 01 ! $ $ x @2 ,3 $ E ' $ @, 9 lambda = 1.18 lambda = 1.02 z z y ' $ y x *1 ! @ $ ' 8 1 ! $ , $ @0 @2 ; '# $ $ '# $ λ< ,626 ' ' $ 2 % % @ ' E " & & ' λ< , 968 ' 2 ' $ $@2 ' " $ ' x ' & ";$ 2 @0 0, " & % * 8 (8), VI CONCLUSION % 0 & , # , & ' $.@@, ' & & $ ' % ' 5 @ '# ' , % / 2 " % & , & & 2 # # # ' & 0 & ' % & # " # $ & $& & & # ' & ' ' 2 & 0 & # % $& & $ " # # # # $ & # " $ 0 % " " $ & ' , 4 4, REFERENCES () , ' # , K2 266* (2) , $$ " & $ ' " J , &' 2* 2668 98 6 , (0) , , J@ & 4 1 $$ " % & & 'J ' . ' - ' , # , 0 K8 (*) , , JA A$ 2 & ' & ' %, ' B@. B# ' M ! & A (8)@, ! ,M , A ' N,@, @ O@ " & % & $ Q , 26 +0+ ' N ::+, (+) ,M , & , , LO ' & - ' , ' # ,* K ::* *8 7+, (7) , M , @,! & ! ,M,! OA $ / Q & P, + .) )+ ,)# , *7 K0 :97 *88 *92, (9) , ' , G &F " 1 # H, .)+/ %,/ ') , K R :9* 2* 299, $% J+ , , J@ & , G. 4 # ' & $ 067 L02*, "& " $ $ 2660 297 0 , J ' ' 2662 , # & P5 P, ' . ' & ' $ $
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