Hyperbolicity in a class of one-dimensional maps
Abstract
In this paper we provide a direct proof of hyperbolicity for a class of onedimensional maps on the unit interval. The maps studied are degenerate forms of the standard quadratic map on the interval. These maps are important in understanding the Newhouse theory of infinitely many sinks due to homoclinic tangencies in two dimensions.
Full text
Publicacions Matemátiques, Vol 34 (1990, 93-105 . Abstract HYPERBOLICITY IN A CLASS OF ONE-DIMENSIONAL MAPS GREGORY J . DAVIs In this paper we provide a direct proof of hyperbolicity for a class of onedimensional maps on the unit interval . The maps studied are degenerate forms of the standard quadratic map on the interval . These maps are important in understanding the Newhouse theory of infinitely many sinks due to homoclinic tangencies in two dimensions . Introduction In the theory of infinitely many sinks, two-dimensional invariant sets are formed when homoclinic tangencies between stable and unstable manifolds of a hyperbolic periodic point are formed . In order to show that infinitely many sinks occur in this situation, we must show that these invariant sets are hyperbolic ([1], [4], or [6]), which is a major undertaking . When the homoclinic tangency is quadratic in nature, the two-dimensional problem has been thought of as a perturbation of the one-dimensional map ([3], [5]) . In [5], a more complete and elegant proof was obtained by conjucating the hyperbolic invariant set for the quadratic map fb(x) = bx(1 - x) to the twodimensional invariant set in the two-dimensional infinitely many sinks problem . In the case where the homoclinic tangency is degenerate (Le ., of order r, r = 4,6 . . . . ), the present proof is very long and involved [1] . If a conjucacy between the one and two-dimensional degenerate problems can be determined, then it may be possible to treat the higher order tangencies in two dimensions using the same type of ideas as presented in [5] . With the above motivation, we will examine the hyperbolicity of the following family of one-dimensional maps on the unit interval . The one-dimensional maps that we are concerned with are of the form r fb(x) = b[2 r - Cx - 2) 1, b>2r, r=4,6,8, ... where b is a real parameter and r is a fixed positive even integer . By studying these one-dimensional maps we will gain insight as to how the hyperbolicity of an invariant set near a degenerate homoclinic tangency in two-dimensions is justified . We will restrict our attention to the cases where r > 2, due to the fact that when r = 2 we obtain the well known and studied quadratic map fb(x) = bx(1 - x) ; see [2], [3] or [5] for more information about this map .
94 G .J . DAvis Statements of results It is easily seen that fb(x) = 0 for x = 0,1 and that fb(x) achieves its maximum value of b/2'r when x = 1/2 . In order for I = [0,1] to be covered by itself under the map fb(x), bmust be larger than 2' . We are interested in the set A contained in I that is invariant for fb(x) ; Le ., fb(A) =A . Explicitly, the invariant set which we are interested in for this máp is given by A = (1°_ ° o fb 2 (I) . (The set A is the analogue of A (t) in the two-dimensional problem [1]) . It is our goal to show that A is a hyperbolic set for fb(x) . A hyperbolic set for fb is a closed, bounded, invariant set A for which there exists an K > 0 such that for all x E A we have j(fb)'(x)j > 1 for all k > K . If b is large enough, the hyperbolicity of A is relatively easy to establish . Set fb 1(I) = I 1 U 12, where I 1 = [0, c], c E [0,1/2], and 12 = [d, l], dE [1/2,1], so that fb(Ii) = I, i = 1, 2 . Then we have Proposition 1 . Leí fb(x)=b[2 -(x-2)rJ, b>2 r , r=4,6,8, ... thenforb>_2''(3), f b '(x)1 > 1 for al' x E fn 1 (I) . The proof of proposition 1 and the remaining propositions in this section will be deferred to the next section . Continuing with our discussion of the hyperbolicity of fb(x), if 2 r <b<2 r C 3r+2 1 3r ' then not all points in the pre-image of I, fn 1(I), have 1 fb(x) 1 > 1 . Fortunately, the absolute value of fb(p) is greater than one where p is the fixed point of fb which is an element of 1 2 . (See Figure 1) . Figure 1
Proposition 2 . HYPERBOLICITY IN ONE-DIMENSIONAL MAPS 95 The fixed point p of fb(x) which líes in ¡he interval 12 is a repellor, that is l fb(P)1 > 1 . Let xi be the poinis such that jfb(ij j = 1 ; 2i E Ii, i = 1,2 . Define J I = [0,¡,) and J 2 = (i2,1] . Clearly all xEJ I U J 2have ¡he property lfb(x)1 > 1 . Proposition 3 . If x o E A(1[(h UI 2 )-(J I UJ 2 )], then there is a positive integer k = k(xo) > 1 such that j(fti y(x o )j > 1 . The idea behind Proposition 3 is that the values of x o that do not Nave j(fb)'(xo)j > 1 are mapped close to one and then near zero . When a point is mapped near zero, the point stays in the interval J l , where the derivative is greater than one, for its next few iterates . The accumulative result is that the iterates for which the derivative is greater than one overcome the initial contraction of the point xo . We now have, by Propositions 1-3, the following result : Main result . Let fb(x) = b [2 - (x - 2)1- , b > 2 1- , r = 4, 6, 8 . . . . fixed . The invariant set A = fl°_= o fn '(I) is a hyperbolic set for fb(x) . Proof of Proposition 1 : Set a=331-2, and b 1 =2 1- ( 3 ) =2 1- « . It is sufFicient to show Jfb,(x)j > 1 since Jfb(x)j > Jfb,(x)j for b > b l . Consider the function Differentiating fb,(x) with respect to x, we obtain fb, (x) = -2ra(2x - 1)1--1 . Therefore, Jfb l (x)j = I2ra(2x - 1)''-1 . Let xi E I, where i = 1, 2, be the points such that fb,(xi) = 1 ; Le ., a[1 - (2xi - 1) 1- ] = 1 . Solving for xi we obtain, Proofs of results fb,(x) - b [2 1- - (x - 2/ 1-J = a[1 - (2x - 1)1-] . 1_(2xi_1)r1 a (2xi _ 1) 1- = 1 - 1 a
96 G .J . DAvis or and For all x E f~,i(I), xi = 2[± .(l1) +ll . 1fbi(x)1 ~ 1fbi(xi)1, l fb,(xi)l = I2ra Define the function lab(z) to be = 2r = 2r 2rf (112 ) -11 __ IL 3r 2 3r - 3r 4 +2 (3r+2~ - Therefore Jfb l ( x)j > 3r+2 ( 3 )' > 1 . Thus Jfb l (x)1 > 1 for all xE f¿l l (I), and Proposition 1 is proven . . " Proof of Proposition 2 : The idea of this proof is to show that l a < p < 1 which implies jb(p)j > 1 . Consider gb(x) = fb(x) - x, and note that gb(p) = 0 . Set z = (x - 1/2), then 96(x) _ .fb Cz + ~) - ( z + 2/ = b (2 r - z r ) - (z + 2/ r i _ -b (Zr + b + 2 2rb b l . ri hb(z) = zr + b + 2 2rb b .
and Evaluating hb(z) at z = (p - 1/2) and z = 0 yields the following : since b > 2r . Because hb(y) has only one variation in sign, Descartes's rule of signs implies that hb(y) has at most one positive real root ; however, we already know that z = (p - 1/2) is a positive root of hb(z) . Therefore, to prove that x2 < p, that is p E J 2 , it is sufficient to show that hb(z) < 0 where z = (xl - 1/2) . First it is necessary to calculate z . Recall that and The point x2 satisfies the relation fb(-¡2) = -1 ; that is 1)r-1 _ -1 . Replacing (i 2 - 1/2) with z we obtain We now proceed to show that hb(z) < 0 . hb(z) = zr + z/b -f- (2b) -1 - 2-r _ (rb) 11 + b-1(rb) 11 -}- (2b) -1 - 2-r < (r2r) r-1 + 2r (r2r) r-1 + 2 12r - 2-r' - (r2 r ) r-1 + 2r (r2 r ) r-1 2 +1 2r [(rr22r) r11 + (r2r) r11 - 2 HYPERBOLICITY IN ONE-DIMENSIONAL MAPS 97 hb(p - 1/2) = 0, 2r-1 - b hb(0) = 2rb < 0 fb(x) = b (1- (x - 1)r1 2r 2 ' r-1 fb(x) = -rb (x - 2) -rbzr -1 = -1, or z = (rb) r=1 . 1+ r -2 -1 1 r -1 2r(2r )=1 since b > 2r
9 8 G .J . DAvis Set A= <0 . then hb(2) < A (1 -}- r - r(2r) r 11 < A (1 -Ir - r [1 -fr 1 l ln(2r) J = A (1 - rr 1 ln(2r)1 - =A (1 - (1 + r 1 1 ) ln(2r) I ln(2r) 1 < A - , since 1n(2r) > 1 for r >_ 2 r-1 Thus, we will have shown that hb(z) < 0 as soon as equation (*) is verified ; however, equation (*) is true due to the fact that (2r)~'r = e7'r ln(2r) Proof of Proposition 3 : where (higher order terms) > 0 since rl il ln(2r) > 0 for r > 2 . Therefore, hb(2) < 0, which implies pE J2 or Jfb(p)j > 1, and the proof of Proposition 2 is complete . Let 1 + gbe the maximum value obtained by fb(x) where x EI ; i .e ., let 1+g = fb(1/2) . Choose any x o E Afl[I l UI2)-(J, UJ2)] . Define 6 = S(xo) > 0 so that the distance between fb(xo) and 1 -fg is b6', and define y = -y(X0) > 0 to be the distance between fb(xo) and 1 . Then fb(xo) = rb6r -i , and y < bbr . = 1 + 1 ln(2r) + (higher order terms) r-1 < 1 + 1 r-1 ln(2r)
(See Figure 2) . but HYPERBOLICITY IN ONE-DIMENSIONAL MAPS 99 Let ~max be the maximum value of f¿(x) where x E I ; that is, let Define k = k(x o ) >2 to be the integer such that for j < k - 1 . We now have that Then Figure 2 Amax = fb(O) = rb(1/2)r-1 . ,xk-1 Y 1 max 21 ~maxy 1 2 , \max - > 2bbr' y _ Define 0, where 0 < A < 1/2, to be the value of ó for which bAr = 2 + 9 bA r =2+9=fb(1/2)=2 -2 . Solving for Qr we find that O r ___ __ 1 b 1 _ 1 b-2 r 1 b (2r 2) b2 r (
10 0 Therefore, r amex From this relation we have that Therefore, for which y = y(x o ) has the property G .J . DAvis Let a,nin be the minimum value of fb(x) for x E [0,12 - 0l, = f b (112 -,á) = rbár-1 . Using our formula for Ar we see that Or -1 is given by Qr-1 = (Or) r - i = ,~ b2r (b - 2r-1)1 - Amin = rb (b2r (b_ 2r Combining the formulas for An,ax and Amin we obtain the following ratio : Amin i 2-1-r -1 - (b - 2r-1)--r r b-2- > 1 . '/ r i \ k-1 ,\ min 1 in r ax (b-2 r r~b Z r r 2 l ~ r We will now show that (fñ),(xo) > 1 (f6 )i(xo) i rbór-lñmin (fb),(xo) ~ : (_\max)rrl(b-2r-1)_rrirrb2- .2ir_ r > rbór -1 -1 1 1 (b-2r - 1)rr l r :b rr2 l rr 2rr b= ar-1 2-2r 1+, 3 - r -, >2 -r b-(b-2 r -1 )= 2-2r +i «b-2r-1)r-1 \ =2 -r br_3 - r C (b - 2r - 1 )r-1 \ r-1 br-3 4- >1 . It should be noted that the above argument is valid only for the values of x o , \max?' > 2, but ñm ax y < 2
Retan that that is, xi satisfies HYPERBOLICITY IN ONE-DIMENSIONAL MAPS 101 where j < k - 1 and k = k(x o) >_ 2 . In addition, the above argument is only legitimate in the case when a < 11/2 - fb 1 (1 - yma .)I, where -%,,,a>, is the value of y for which ñmaxymax = 1/2 . In Lemma 4 we will prove the existente of certain parameter values b for which there exist values of x o that do not satisfy the above condition . These values of b are shown to also have the property of J(fb)'(x o )j > 1, where k = 2, but an argument different from the one above is required to show this fact . This argument will be presented in Lemma 5 . However, before we prove Lemma 4 and Lemma 5, it will be necessary to provide additional notation . Set ama . = 1 1 /2 - fb 1(1 - ymax)j and define the intervals L l and L 2 to be L l = I l r1 [1/2 - amax, 1 /2] ; L2 = 12 n [1/2, 1/2 + bmax] . Lemma 4 . There exist intervals of parameter values M(r) C ( 2r , u2 r ] such that L ; U Ji I i, i = 1, 2, where a= (3r±2\ . 3Jr Proof .. Define xi, where i = 1, 2, to be the values of x for which fb(~i) = 1 - ymax, and define ii, where i = 1, 2, to be the values of x for which jfb( .¡ i )1 = 1 . To prove Lemma 4 it is sufficient to show that there is an interval M(r) of parameter values b for which 11/2 - x i l < 11/2 - .¡¡l . Solving ñmaxymax = 1/2 for ymax we obtain ymax = 2 Amax rb Amax = 2r-1' Therefore, ymax = b, and hence, - ymax 4rb' The above equation implies that the value xi satisfies _ 2r fb(xé) = 1 4rb' 1)r1 2 . . 77z