—In this paper, we investigate the relationship between migration and species distribution in multizone environment. We present a discrete model for migration of three competing species over three zones. We prove that the migration tactics of species leads to the fact that the system exponentially converges to one of two typical configurations: the first one is a case where each zone contains only one species, the second one is a case where one species is of density 1 in one zone, another species stays and dominates in the two other zones, and the last species is evenly split into the 3 zones with a density one third in each. We also show a characterization of the initial conditions under which the system converges to one of the two configurations.
Trang 1Effects of Migration of Three Competing
Species on Their Distributions in
Multizone Environment
Phan Thi Ha Duong
Institute of Mathematics,
Vietnam Academy of Science
and Technology,
Hanoi, Vietnam
Email: phanhaduong@math.ac.vn
Doanh Nguyen-Ngoc School of Applied Mathematics, and Informatics, Hanoi University of Science and Technology, Hanoi, Vietnam
Email: doanh.nguyenngoc@hust.vn
K´evin Perrot LIP (UMR 5668 CNRS-ENS de Lyon-UCBL1),
46 alle dItalie 69364 Lyon Cedex 07 - France Email: kevin.perrot@ens-lyon.fr
Abstract—In this paper, we investigate the
rela-tionship between migration and species distribution
in multizone environment We present a discrete
model for migration of three competing species over
three zones We prove that the migration tactics of
species leads to the fact that the system exponentially
converges to one of two typical configurations: the
first one is a case where each zone contains only one
species, the second one is a case where one species is
of density 1 in one zone, another species stays and
dominates in the two other zones, and the last species
is evenly split into the 3 zones with a density one third
in each We also show a characterization of the initial
conditions under which the system converges to one
of the two configurations
An important issue in ecology is to understand
the effects of the tactics that individuals may adopt
at the population and community levels
Individu-als migrate because the food is limited, they
com-pete with others, environmental conditions are not
good for them (weather, natural calamity, ) and so
on This leads to various portraits of distribution of
species in environment
There was also a lot of interest in the
rela-tionship between migration of species individuals
among multizone environment and species
distribu-tion One of the most common and simple
theoreti-cal explanation for effects of individuals’ migration
on the species distribution is ideal free distribution (IFD) theory The theory states that the number
of individuals that will aggregate (or else clump)
in various zones is proportional to the amount of resources available in each For example, if zone
1 contains twice as many resources as zone 2, there will be twice as many individuals foraging
in zone 1 as in zone 2 The IFD theory predicts that the distribution of individuals among zones will minimize resource competition and maximize fitness ( [4], [5], [6], [10], [7])
Some recent investigations studied another fac-tor leading to individuals’ migration and also showed the link between the migration and the species distribution over multizone environment (see for examples in [2], [8], [2], [9] The authors showed that interaction between species leads to migration of individuals and therefore to species distribution These investigations, however, take into account only two species and two zones The main reason is that a model with more than two species and two zones is much more complex and less tractable The aim of this work is to follow this approach by taking into account three competing species for territory among three zones The raised question is “what is the stable distribution of the three species among three zones?” There is
no simple answer to this question We show in this paper that it depends on migration tactics of
Trang 2individuals as well as the initial distribution of
species
The paper is organized as follows Section
II is dedicated to the presentation of the model
Section III shows simulations of the model: typical
examples and remarks Thereafter, in section IV,
we present the main results Finally, section V is
about discussion and conclusion
n C1
n B1
n A1
zone 1
n C2
n B2
n A2
zone 2
n C3
n B3
n A3
zone 3
S, i ∈ Z In the figure: density of species A in black, density
of species B in grey while density of species C in white over
three zones.
The system evolves in discrete time and
con-tinuous space We consider the case of 3 species
S = {A, B, C} and 3 zones Z = {1, 2, 3} (see
Fig 1) We call configuration at time t a
distribu-tion of the individuals of each species into the 3
zones, composed of a density nXi(t) of individuals
of species X in zone i at time t, for example
nA1(t) is the density of individuals of species A
is zone 1 at time t, such that for every species
X : P
i∈ZnXi(t) = 1 Formally, a configuration
is determined by its density matrix:
n(t) =
nA1 nA2 nA3
nB1 nB2 nB3
nC1 nC2 nC3
!
If there is no ambiguity, we will usually omit the
dependence on the time t and simply refer to a
no-tation n instead of n(t) The set of configurations
is denoted by C
To describe the dynamics of the system, we are
going to introduce some definitions as follows:
Definition 1 In a configuration, a species
domi-nates a zone if its density is strictly greater than
the densities of the two other species in this zone Definition 2 The evolution rule is that if a species dominates a zone at time t then those individuals stay into this zone in the next time step (t + ∆t), and if a species does not dominate a zone then in the next time step half of them move into each of the two other zones
For a configuration c(t) at time t, we denote
by c(t + k∆t) the configuration obtained from c(t) after k time steps
Definition 3 A stable configuration is a configu-ration such that its density matrix does not change over the time
A lot of simulations were done We present here three of them showing the typical stable configurations that appear Top of Fig 2 shows the
Initial configuration ⇒ Stable configuration
A
(0.8)
B (0.2)
C
(0.5) zone 1
A (0.1)
B
(0.6)
C (0.1) zone 2
A (0.1)
B (0.45)
C
(0.4) zone 3 zone 1
A
(1)
zone 2
B
(1)
zone 3
C
(1)
A
(0.5)
B (0.1)
C
(0.4) zone 1
A
(0.3)
B (0.2)
C
(0.3) zone 2
A (0.2)
B
(0.8)
C
(0.3) zone 3
A
(0.6)
C
(1/3) zone 1
A
(0.4)
C
(1/3) zone 2
B
(1)
C
(1/3) zone 3
A
(0.6)
B (0.1)
C
(0.3) zone 1
A
(0.3)
B
(0.5)
C
(0.4) zone 2
A (0.1)
B
(0.4)
C
(0.3) zone 3
A
(1)
C
(1/3) zone 1
B
(0.55)
C
(1/3) zone 2
B
(0.45)
C
(1/3) zone 3
Fig 2 Three typical stable configurations Left panel is about initial configurations Right panel is about the corresponding stable configurations.
case where densities of each species are equal to 1
in one zone and are equal to 0 in the others zones
In the middle of Fig 2, species A is in two zones and dominates both, species B is only in one zone where it dominates, while species C is evenly split into the three zones At bottom of Fig 2, species
A is only in one zone where it dominates, species
B is in the two others zones and dominates both, while species C is in evenly split into the three
Trang 3zones We have the following remarks from the
above simulations:
Remark 1 There are three remarks as follows:
(1) there are two typical stable configurations: in
the first stable configuration each zone contains
only one species (top of Fig 2), in the second
one species is of density 1 in one zone, another
species stays and dominates in the two other zones,
and the last species is evenly split into the 3
zones with a density 1/3 in each (bottom of Fig
2); (2) the system converges rapidly to the stable
configurations;(3) it is not easy to figure out under
which conditions the system converges to one of the
two above typical configurations
The next section is a formal analysis of these
remarks
We begin in subsection IV-A by explaining that
we can discard the cases of equality in our study,
without changing the results we obtain about the
dynamic of the system, by proving that cases of
equality almost never happen Then we describe the
two typical dynamics of the system in subsection
IV-B Finally, subsection IV-C is devoted to the
study of the dynamics of the system according to
the initial configuration
Firstly, we introduce some definitions as
fol-lows:
Definition 4 Let c and c0 be two configurations
with density matrices n and n0, respectively The
distance between the two configurations is defined
by
d(c, c0) = max
X∈S
i∈Z
{|nXi− n0Xi|}
Definition 5 Starting from a configuration c(t0),
we say that the system converges to a stable
configurations if
∀ > 0, ∃ k(), ∀ k > k() : d(c(t0+k∆t), s) <
Moreover, ifk() in O log2 1 we say that the
systems exponentially converges tos
Definition 6 We call a one-each configuration,
denoted by cOE, a configuration such that each
zone contains only one species
Definition 7 We call a one-two configuration, denoted by cOT, a configuration such that one species is of density 1 in one zone, another species stays and dominates in the two other zones, and the last species is evenly split into the 3 zones with a density 1/3 in each
A Ignoring cases of equality
We denote C∗the set of configurations such that there is a case of equality between the densities of two species competing for dominancy in a zone Formally,
C∗= {c ∈ C | ∃ X, Y, i : nXi= nY i} where n is the density matrix of c
Intuitively, if we consider the set C which
is uncountable (continuous space) then a case of equality in C∗somehow corresponds to the restric-tion of an uncountably large degree of liberty to a countable one, hence the following result holds Theorem 1 |C|C|∗| = 0
We will apply this result without explicit refer-ence: when comparing densities of two competing species it allows to convert an inequality into a strict inequality
B Two typical behaviors Now, we are going to show the two lemmas about cOE and cOT
Lemma 1 (One each) From a configuration c = c(t0) such that each species X dominates exactly one zone i, the system exponentially converges
to the stable configuration where the density of species X in zone i is 1
Proof: Without loss of generality, let us con-sider a configuration such that A dominates zone
1, B dominates zone 2 and C dominates zone 3 First of all, we can notice that the repartition of dominancy will never change since nXi(t + ∆t) ≥
1
2 if and only if species X dominates zone i at time
t (recall Theorem 1)
We now prove that the system exponentially converges to the stable configuration s of density
Trang 4matrix m such that
mXi=1 for Xi ∈ {A1, B2, C3}
0 otherwise
We can notice that
d(c(t0+k∆t), s) = 1− min
Xi∈{A1,B2,C3}nXi(t0+ k∆t) since the difference is at least as important for
species A (resp B, C) in zone 1 (resp 2, 3) than
in other zones According to the repartition of
dominancy, we have
d(c(t0+ (k + 1)∆t), s) = d(c(t0+ k∆t), s)
2 because half of the individuals in a zone where
they are not dominant move to their dominant zone
Consequently, for all > 0, we have
d(c(t0+ k∆t), s) < ⇐⇒ k > log2 d(c, s)
which concludes the proof
Lemma 2 (One-two) If, during two
consecu-tive configurations c = c(t0) and c(t0 + ∆t), a
species X dominates zone i and another species
Y dominates the two other zones, then the system
exponentially converges to the stable configuration
s of density matrix m, defined as follows:
mXi= 1, and mXj = 0,j 6= i
mY i= 0, and mY j= nY j+nY i
2 ,j 6= i
mZj= 13 forZ /∈ {X, Y }, ∀j
wheren is the density matrix of c
Proof:Without loss of generality, we consider
that A dominates zone 1 and B dominates zone 2
and zone 3 and that nB2> nB3 (let us denote this
property by (*)) We first prove that the property
(*) keeps satisfied during the evolution For that,
it is sufficient to prove that at time t0+ 2∆t, (*)
is still satisfied, which means that if (*) is true for
two consecutive steps then it is true for the third
step, so it is true for all steps
• Consider zone 1, after two steps we have:
nA1(t0+ 2∆t) = nA1(t0+ ∆t)
+1−nA1 (t 0 +∆t)
2
nB1(t0+ 2∆t) = 0
nC1(t0+ 2∆t) = 1−nC1 (t o +∆t)
≤1
so A dominates zone 1
• Consider zone 2, after two steps we have:
nA2(t0+ 2∆t) = nA3 (t 0 +∆t)
2
nB2(t0+ 2∆t) = nB2(t0+ ∆t)
+nB1 (t 0 +∆t)
2
nC2(t0+ 2∆t) = 1−nC2 (t 0 +∆t)
2
so B dominates zone 2
• Consider zone 3, after one step, the density
of the three species are the following:
nA3(t0+ ∆t) = nA2 (t 0 )
2
nB3(t0+ ∆t) = nB3(t0) +nB1 (t 0 )
2
nC3(t0+ ∆t) = 1−nC3 (t 0 )
By hypothesis, we know that B dom-inates zone 3 after one step, then
nB3(t0) + nB1 (t 0 )
2 is greater that nA2 (t 0 )
2
and 1−nC3 (t 0 )
Let us consider now the situation after two steps:
nA3(t0+ 2∆t) = nA2 (t 0 +∆t)
2
= nA3 (t 0 )
4 < nB3(t0)
nB3(t0+ 2∆t) = nB3(t0+ ∆t)
= nB3(t0) +nB1 (t 0 )
2
nC3(t0+ 2∆t) = 1−nC3 (t 0 +∆t)
2
= 1+nC3 (t 0 )
We will now prove that B still dominates zone 3 at this step, that means nB3(t0+ 2∆t) > nC3(t0+ 2∆t) In fact, from the hypothesis that B dominates zone 3 at time
t0and t0+ ∆t, we have:
nB3(t0) > nC3(t0)
nB3(t0) +nB1 (t 0 )
2 >1−nC3 (t 0 )
this implies that 4nB3(t0) + nB1(t0) >
1 + nC3(t0), then nB3(t0 + 2∆t) =
nB3(t0) +nB1 (t 0 )
2 > nB3(t0) +nB1 (t 0 )
4 >
1+n C3 (t 0 )
4 = nC3(t0+ 2∆t)
We can conclude that after two steps, B dominates zone 3
We now prove that the system exponentially converges to the stable configuration s
For the species B, after one step, their
Trang 5individ-uals do not move any more For the species A, we
can apply the same argument as in Lemma 1 to
prove the exponential convergence
We will now prove that the density of species
C in each zone exponentially converges to 13 Let
us denote by di(t) the different nCi(t) − 1
3 for
i ∈ {1, 2, 3} The density of C in zone 1 after one
step is:
nC1(t0+ ∆t) = nC2(t0) + nC3(t0)
2
= 1
3 +
d2(t0) + d3(t0) 2
= 1
3 −d1(t0)
2 .
It means that di(t0+ ∆t) = −12 di(t0), and more
generally di(t0+ k∆t) = (−1)2kkdi(t0) This fact
implies the exponential convergence for species C
The proof of this Lemma is then completed
C Dynamics of the system
The following theorem is about the portrait of
the dynamics The theorem proves the first and
second remark of the previous section
Theorem 2 Beginning from any configuration, the
system always converges exponentially to acOEor
acOT
Proof: Let c = c(t0) be any configuration
We show that after k steps with k ≥ 2, the
con-figuration c(t0+ k∆t) will satisfies the condition
of Lemma 1 or Lemma 2, then applying those
Lemmas, one can deduce the statement of this
theorem
To do that, we will check every possible case,
in many cases the proofs are similar We perform a
case disjunction according to the dominant species
in each zone The density of one species in a zone
has to be greater than any other one Furthermore,
no species can dominate all of the three zones
Without loss of generality, we consider that
nA1= max
X∈S
i∈Z
{nXi} and nB3= max
X∈S{nX3}
The initial picture, where dominant densities are
boxed, is pictured below
zone 1 zone 2 zone 3 The first disjunction goes according to the dominant species in zone 2:
(case 1) (case 2) (case 3) max
X∈S{nX2(t0)} = nA2 nB2 nC2 (case 1) We know all the dominancies, therefore we can perform one time step We picture c(t0+ ∆t) below
nA1+nA3
n A3
n B2
2
n B1
2 nB3+nB1 +n B2
2
n C2 +n C3
2
n C1 +n C3
2
n C1 +n C2
2
Species A dominates zone 1 because nA1 is the maximal density, and nA1 is greater than nA2 which dominated over nB2at time t0 The compar-ison with C uses similar arguments Analogously, species B dominates zone 3
At this stage, we perform again a case disjunc-tion, according to the dominant species in zone 2: (case 1.1) If A dominates zone 2, i.e max
X∈S{nX2(t0+ ∆t)} = nA2+ nA3/2 Then we apply Lemma 2 and deduce that the system con-verges exponentially to a cOT
(case 1.2) If B dominate zone 2, i.e max
X∈S{nX2(t0+∆t)} = nB1/2 This case is impos-sible At time t0, nC2 < nA2 and at time t0+ ∆t,
n C1 +n C3
2 < nB1
2 , then 1 = nC1+ nC2+ nC3 <
nB1 + nA2 which implies that nB1 > nA1, a contradiction with the maximality of nA1 (case 1.3) If C dominates zone 3, i.e max
X∈S{nX2(t0+ ∆t)} = (nC1+ nC3)/2We apply Lemma 1 and deduce that the system exponentially converges to a cOE
(case 2) Analogously, in this case, the system always converges exponentially to either a cOE or
a cOT
Trang 6(case 3) We apply Lemma 1 and deduce
that the system exponentially converges to a cOE
The following theorem shows characterization
of the cases when the system converges to a cOE
(resp cOT)
Theorem 3 Let c be a configuration Without loss
of generality, one can suppose that
nA1= max
X∈S
i∈Z
{nXi} and nB3= max
X∈S{nX3}
Then the system exponentially converges to acOT
if c satisfies one of the following conditions,
other-wise the system exponentially converges to acOE
1) nB2 = max
X∈S{nX2} and nB2+nB1
2 >nC1 +n C3
2
and nB3+nB1
2 >nC1 +n C2
2
2) nA2= max
X∈S{nX2} and nA2+nA3
2 >nC1 +n C3
2
We have presented a discrete model for
mi-gration of individuals of three competing species
for territory over three zones As a first results,
from a mathematical point of view, we have
distin-guished two typical stable configurations: cOE and
cOT From an ecological point of view, we could
take into account two possibilities concerning the
species distribution: clumped distribution and
uni-form distribution depending on initial conditions
Top of Fig 2 shows a typical stable
configura-tion where species individuals form a clumped
dis-tribution Below, species A and B form a clumped
distribution while species C forms an uniform
dis-tribution However, there are differences between
the two cases In the middle of Fig 2, species A
forms a clumped distribution over two zones while
species B forms a clumped distribution only in
the other At bottom of Fig 2, species A forms
a clumped distribution only in one zone while
species B forms a clumped distribution over the
two other zones
The main conclusion that emerges from this
study is the existence of a relationship between
(density dependent) migration tactics and distribu-tion of species over the three zones In this study,
we just consider three species and three zones It would also be very interesting to take into account
of four (or in general n) species and four (or in general n) zones (n > 4) This would lead to
a more complicated model and less tractable that would be interesting to investigate in future work
This work was done while the authors were
at Vietnam Institute of Advanced Study in Math-ematics (VIASM) This work was also partially supported by the project VAST.DLT.01/12-13
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