Eigenvectors of the 1-dimensional critical random Schrödinger operator
The purpose of this paper is to understand in more detail the shape of the eigenvectors of the random Schrödinger operator H = Δ + V on ℓ 2 ( Z ) . Here Δ is the discrete Laplacian and V is a random potential. It is well known that under certain assumptions on V the spectrum of this operator is pure...
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Published in | Geometric and functional analysis Vol. 28; no. 5; pp. 1394 - 1419 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Cham
Springer International Publishing
01.10.2018
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | The purpose of this paper is to understand in more detail the shape of the eigenvectors of the random Schrödinger operator
H
=
Δ
+
V
on
ℓ
2
(
Z
)
. Here
Δ
is the discrete Laplacian and
V
is a random potential. It is well known that under certain assumptions on
V
the spectrum of this operator is pure point and its eigenvectors are exponentially localized; a phenomenon known as Anderson Localization. We restrict the operator to
Z
n
and consider the critical model,
(
H
n
ψ
)
ℓ
=
ψ
ℓ
-
1
,
n
+
ψ
ℓ
+
1
,
n
+
v
ℓ
,
n
ψ
ℓ
,
ψ
0
=
ψ
n
+
1
=
0
,
with
v
k
are independent random variables with mean 0 and variance
σ
2
/
n
. We show that the scaling limit of the shape of a uniformly chosen eigenvector of
H
n
is
exp
-
|
t
-
U
|
4
+
Z
t
-
U
2
,
where
U
is uniform on [0,1] and
Z
is an independent two sided Brownian motion started from 0. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 1016-443X 1420-8970 |
DOI: | 10.1007/s00039-018-0460-0 |