1. Introduction
There is no doubt that a study on scattering theory is one of the most interesting topics of the Schrödinger equation. Recently, it has been revealed that the scatterings of some fundamental stationary Schrödinger equations on the real line with not only delta potentials [
1,
2,
3] but also continuous potential [
4] can be recovered by discrete-time quantum walks. These induced quantum walks are given by the following setting: the non-trivial quantum coins are assigned to some vertices in a finite region on the one-dimensional lattice as the impurities and the free-quantum coins are assigned at the other vertices. The initial state is given so that a quantum walker inflows into the perturbed region at every time step. It is shown that the scattering matrix of the quantum walk on the one-dimensional lattice can be explicitly described by using a path counting in [
5] and this path counting method can be described by a discrete analogue of the Feynmann path integral [
4]. There are some studies for the scattering theory of quantum walks under slightly general settings and related topics [
6,
7,
8,
9,
10,
11,
12].
Such a setting is the special setting of [
13,
14] in that the regions where a quantum walker moves freely coincide with tails in [
13,
14], and the perturbed region can be regarded as a finite and connected graph in [
13,
14]. The properties of not only the scattering on the surface of the internal graph but also the stationary state in the internal graph for the Szegedy walk are characterized by [
15] with a constant inflow from the tails.
By [
14], this quantum walk converges to a stationary state. Therefore, let
be the stationary state of the quantum walk on
. The perturbed region is
and we assign the quantum coin
to each vertex in
. The inflow into the perturbed region at time
n is expressed by
. In this paper, we compute (1) the scattering on the surface of the perturbed region
in the one-dimensional lattice; (2) the energy of the quantum walk. Here, the energy of quantum walk is defined by
This is the quantity that quantum walkers accumulate to the perturbed region
in the long time limit. We obtain a necessary and sufficient condition for the perfect transmitting, and also obtain the energy. As a consequence of our result on the energy, we observe a discontinuity of the energy with respect to the frequency of the inflow. Moreover, our result implies that the condition for
is equivalent to the condition for the perfect transmitting. Then, we obtain that the situation of the perfect transmitting not only releases quantum walker to the opposite outside but also accumulates quantum walkers in the perturbed region. Note that since this quantum walk can be converted to a quantum walk with absorption walls, the problem is reduced to analysis on a finite matrix
, which is obtained by picking up from the total unitary time evolution operator with respect to the perturbed region
. See [
16] for a precise spectral results on
.
This paper is organized as follows. In
Section 2, we explain the setting of this model and give some related works. In
Section 3, an explicit expression for the stationary state is computed using the Chebyshev polynomials. From this expression, we obtain the transmitting and reflecting rates and a necessary and sufficient condition for the perfect transmitting. We also give the energy in the perturbed region. In
Section 4, we estimate the asymptotics of the energy to see the discontinuity with respect to the incident inflow.
2. The Setting of our Quantum Walk
The total Hilbert space is denoted by
. Here
A is the set of arcs of one-dimensional lattice whose elements are labeled by
, where
and
represents the arcs “from
to
x“, and “from
to
x”, respectively. We assign a
unitary matrix to each
so-called local quantum coin
Putting
,
and
,
, we define the following matrix valued weights associated with the motion from
x to left and right by
respectively. Then, the time evolution operator on
is described by
for any
. Its equivalent expression on
is described by
for any
. We call
and
the transmitting amplitudes, and
and
the reflection amplitudes at
x, respectively. If we put
and
, then the primitive form of QW in [
17] is reproduced. Remark that
U and
are unitarily equivalent such that letting
be
then we have
. The free quantum walk is the quantum walk where all local quantum coins are described by the identity matrix, i.e.,
Then, the walker runs through one-dimensional lattices without any reflections in the free case.
In this paper, we set “impurities” on
in the free quantum walk on one-dimensional lattice; that is,
We consider the initial state
as follows.
where
. Note that this initial state belongs to no longer
category. The region
is obtained a time dependent inflow
from the negative outside. On the other hand, if a quantum walker goes out side of
, it never come back again to
. We can regard such a quantum walker as an outflow from
. Roughly speaking, in the long time limit, the inflow and outflow are balanced and obtain the stationary state with some modification. Indeed, the following statement holds.
Proposition 1 - 1.
This quantum walk converges to a stationary state in the following meaning: - 2.
This stationary state is a generalized eigenfunction satisfying
Relation to an absorption problem
Let the reflection amplitude at time
n be
with
. We can see that
is rewritten by using
as follows:
The first term is the amplitude that the inflow at time n cannot penetrate into ; the m-th term is the amplitude that the inflow at time penetrates into and escapes from 0 side at time n. Therefore, each term corresponds to the “absorption” amplitude to with the absorption walls and M with the initial state . Then
Remark 1. The reflection amplitude coincides with the generating function of the absorption amplitude to with respect to time n while the transmitting amplitude coincides with the generating function of the absorption amplitude to M with respect to time n.
Put
and
which are the absorption/ first hitting probabilities at positions
and
M, respectively, starting from
. From the above observation, for example, we can express the
m-th moments of the absorption/hitting times to
and
M as follows:
Relation to Scattering of quantum walk
The stationary state
is a generalized eigenfunction of
U in
. The scattering matrix naturally appears in
(see [
5]). In the time independent scattering theory, the inflow can be considered as the incident “plane wave“, and the impurity causes the scattered wave by transmissions and reflections. Thus, we can see the transmission coefficient and the reflection coefficient in
for
. For studies of a general theory of scattering, we also mention the recent work by Tiedra de Aldecoa [
12].
4. Asymptotics of Energy
If
, then by Corollary 3, it is immediately obtained that
Let us consider the case of
as follows. Note that
where
(
), while
(
) such that
and
. To observe the asymptotics of
for
, we rewrite
as follows: -4.6cm0cm
From now on, let us consider the asymptotics of
for large
M. We summarize our results on the asymptotics of
in
Table 1. In the following, we regard
as a function of
,
M; that is
because
can be expressed by
and consider the asymptotics for large
M.
4.1.
Let us see that
Note that
. Then by (
21), we have
By (
22), if
, then
. To connect it to the limit for the case of
described by (
20) continuously, we consider
and
simultaneously, so that
. Let us see that
Noting that
, for
and
, we have
Therefore, if we design the parameter
so that
then the energy of
continuously closes to that of
in the sufficient large system size
M.
4.2.
In this paper, since we determine satisfying , we set . Remark that for any because is invariant under this deformation.
By (
21), if
, we have
for sufficiently large
M, which implies that
if
is fixed. Then, we conclude that
if
is fixed for
. On the other hand, if we design
so that the condition of the perfect transmitting is satisfied;
,
(see Corollary 1) and choose
ℓ which is very close to 0 or
M, then
. Note that if
, which means
, then the coefficient of the upper bound in (
26) diverges.
Then, from now on, let us consider the following three cases having a magnitude relation between and M;
(i) ; (ii) ; (iii) .
Case (i):
Let us start to evaluate RHS of (
21). Since
the “
“ part in RHS of (
21) can be evaluated by
. The denominator of (
21) is evaluated by
. Combining them, we have
This is consistent with (
20).
Case (ii):
Under this condition, the parameter
lives around 0 or
if
M is large. Since we consider
, we can evaluate
by
, or
for large
M. We define
if
and
if
. Because
by the assumption, we have
. Therefore, we put
with
and
. Then up to the value
, let us see
Note that if
, then
and
,
and so on. Inserting them into (
21), we have
On the other hand, if
, since
and
, by (
21), we have
Case (iii):
The “
” part in (
21) is estimated by
because
. Then, we have
for sufficiently large
M which is the same as (
25). Let us consider the following case study:
- (a)
Let us see
in this case. If
, then the coefficient of
M in (
29) is a finite value, then we have (
26). On the other hand, if each of
or
, then (
29) implies
- (b)
Since
, we evaluate
by
Then, there exists a natural number
m such that
. Note that
is also sufficiently small. Then, the natural number
m must be
if
and
if
. Putting
, we have
Therefore,
holds. Then, (
29) implies
We summarize the above statements in the following theorem by setting , as a special but natural design of the parameters.
Theorem 2. Let us set so thatwith the parameters and . If or with fixed M, then . On the other hand, if we take and fix , then we have 5. Conclusions
We considered the quantum walk on the line with the perturbed region
; that is, an non-trivial quantum coin is assigned at the perturbed region and the free quantum coin is assigned at the other region. We set an
initial state so that free quantum walkers are inputted at each time step to the perturbed region. A closed form of the stationary state of this dynamical system was obtained and we computed the energy of the quantum walk in the perturbed region. This energy represents how quantum walker feels “comfortable“ in the perturbed region. We showed that the “feeling” of quantum walk depends on the frequency of the initial state. We can divide the region of the frequency into three parts to classify the asymptotics of the energy for large
M;
,
,
. The region
coincides with the continuous spectrum of the quantum walk with
[
5]. We showed that quantum walkers prefer to the initial state whose frequency corresponds to the continuous spectrum in the infinite system. More precisely, the energy of the quantum walk in the perturbed region is estimated by
if
, while one is estimated by
if
and
almost all pseudo momentum
gives
-energy, but some momentum gives
if
(Theorem 2). Such an initial state exactly exists but it is quite rare from the view point of the Lebesgue measure. The most comfortable initial state for quantum walkers has the frequency whose pseudo momentum
lives in some neighborhood of the boundary
and accomplishes the perfect transmitting. If the momentum of the initial state exceeds the boundary
from the internal region
, then the energy is immediately reduced to
. It suggests that the control of the frequency of the initial state to give the maximal energy in the perturbed region is quite sensitive from the view point of an implementation.
The spectrum of the boundary
for
produces the two singular points of the density function of the Konno limit distribution and is characterized by the Airy functions. In [
16], details of the spectrum behavior around
is discussed. Indeed, a kind of “speciality“ also appears as the non-diagonalizability of
T when
in our work (Lemma 2). Note that the infinite system does not have any
edges, which means every node is “impurity”, while our quantum walker feels the
edges of the impurities; nodes 0 and
M. Therefore, to see the effect of such a finiteness on the behavior of the quantum walker comparing with the infinite system, computing how a quantum walker is distributed in the perturbed region is interesting which may be possible from the explicit expression of the stationary state in Theorem 1. Moreover, to consider the escaping time from the perturbed region seems to be useful to estimate the finesse as the interferometer motivated by quantum walk and it would be possible to extract some information from (
3) and (
4). This remains one of the interesting problems for the future.