Abstract
Abstract
We consider a multichannel wire with a disordered region of length L and a reflecting boundary. The reflection of a wave of frequency ω is described by the scattering matrix
S
(
ω
)
, encoding the probability amplitudes to be scattered from one channel to another. The Wigner–Smith time delay matrix
Q
=
−
i
S
†
∂
ω
S
is another important matrix, which encodes temporal aspects of the scattering process. In order to study its statistical properties, we split the scattering matrix in terms of two unitary matrices,
S
=
e
2
i
k
L
U
L
U
R
(with
U
L
=
U
R
T
in the presence of time reversal symmetry), and introduce a novel symmetrisation procedure for the Wigner–Smith matrix:
Q
̃
=
U
R
Q
U
R
†
=
(
2
L
/
v
)
1
N
−
i
U
L
†
∂
ω
U
L
U
R
U
R
†
, where k is the wave vector and v the group velocity. We demonstrate that
Q
̃
can be expressed under the form of an exponential functional of a matrix Brownian motion. For semi-infinite wires, L → ∞, using a matricial extension of the Dufresne identity, we recover straightforwardly the joint distribution for
Q
’s eigenvalues of Brouwer and Beenakker (2001 Physica E 9 463). For finite length L, the exponential functional representation is used to calculate the first moments
⟨
t
r
(
Q
)
⟩
,
⟨
t
r
(
Q
2
)
⟩
and
⟨
t
r
(
Q
)
2
⟩
. Finally we derive a partial differential equation for the resolvent
g
(
z
;
L
)
=
lim
N
→
∞
(
1
/
N
)
t
r
z
1
N
−
N
Q
−
1
in the large N limit.
Funder
European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme
Netherlands Organization for Scientific Research
Subject
General Physics and Astronomy,Mathematical Physics,Modeling and Simulation,Statistics and Probability,Statistical and Nonlinear Physics
Cited by
1 articles.
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