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On the Behaviour of the spectral characteristic of Feigenbaum’s map
Let T g : [−1, 1] → [−1, 1] be the Feigenbaum map. It is well known that T g has a Cantor-type attractor F and a unique invariant measure µ 0 supported on F . The corresponding unitary operator ( U g φ )( x ) = φ ( g ( x )) has pure point spectrum consisting of eigenvalues λ n,r , n ≥ 1, 0 ≤ r ≤ 2 n...
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Published in: | P-adic numbers, ultrametric analysis, and applications ultrametric analysis, and applications, 2012-10, Vol.4 (4), p.259-270 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Let
T
g
: [−1, 1] → [−1, 1] be the Feigenbaum map. It is well known that
T
g
has a Cantor-type attractor
F
and a unique invariant measure µ
0
supported on
F
. The corresponding unitary operator (
U
g
φ
)(
x
) =
φ
(
g
(
x
)) has pure point spectrum consisting of eigenvalues
λ
n,r
,
n
≥ 1, 0 ≤
r
≤ 2
n
−1
− 1 with eigenfunctions
e
r
(
n
)
(
x
). Suppose that
f
∈
C
1
([−1, 1]),
f
′ is absolutely continuous on [−1, 1] and
f
″ ∈
L
p
([−1, 1],
d
µ
0
),
p
> 1. Consider the sum of the amplitudes of the spectral measure of
f
:
Using the thermodynamic formalism for
T
g
we prove that
S
n
(
f
) ∼ 2
−
n
q
n
, as
n
→ ∞, where the constant
q
∈ (0, 1) does not depend on
f
. |
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ISSN: | 2070-0466 2070-0474 |
DOI: | 10.1134/S2070046612040024 |