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Bull Math Biol (2015) 77:1237–1255 DOI 10.1007/s11538-015-0084-6 ORIGINAL ARTICLE An Epidemic Patchy Model with Entry–Exit Screening Xinxin Wang 1 · Shengqiang Liu 1 · Lin Wang 2 · Weiwei Zhang 1 Received: 25 April 2014 / Accepted: 30 April 2015 / Published online: 15 May 2015 © Society for Mathematical Biology 2015 Abstract A multi-patch SEIQR epidemic model is formulated to investigate the long- term impact of entry–exit screening measures on the spread and control of infectious diseases. A threshold dynamics determined by the basic reproduction number 0 is established: The disease can be eradicated if 0 < 1, while the disease persists if 0 > 1. As an application, six different screening strategies are explored to examine the impacts of screening on the control of the 2009 influenza A (H1N1) pandemic. We find that it is crucial to screen travelers from and to high-risk patches, and it is not necessary to implement screening in all connected patches, and both the dispersal rates and the successful detection rate of screening play an important role on determining an effective and practical screening strategy. Keywords Epidemic model · Patchy environment · Threshold dynamics · Dispersal · Entry–exit screening 1 Introduction With the rapidly growing travel among cities and countries, newly emerging infectious diseases and many re-emerging once-controlled infectious diseases have the trend to spread regionally and globally much faster than ever before (Jones et al. 2008). Interna- tional travel has been a major factor causing the SARS outbreak in 2003 (Lipsitch et al. B Shengqiang Liu [email protected] 1 Academy of Fundamental and Interdisciplinary Sciences, Harbin Institute of Technology, 3041#, 2 Yi-Kuang Street, Nan-Gang District, Harbin 150080, China 2 Department of Mathematics and Statistics, University of New Brunswick, Fredericton, NB E3B 5A3, Canada 123

An Epidemic Patchy Model with Entry–Exit Screening · 2017. 8. 26. · Takeuchi (2006) do not include a latent compartment, while many infectious diseases do undergo latent stages

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  • Bull Math Biol (2015) 77:1237–1255DOI 10.1007/s11538-015-0084-6

    ORIGINAL ARTICLE

    An Epidemic Patchy Model with Entry–Exit Screening

    Xinxin Wang1 · Shengqiang Liu1 · Lin Wang2 ·Weiwei Zhang1

    Received: 25 April 2014 / Accepted: 30 April 2015 / Published online: 15 May 2015© Society for Mathematical Biology 2015

    Abstract Amulti-patch SEIQR epidemicmodel is formulated to investigate the long-term impact of entry–exit screening measures on the spread and control of infectiousdiseases. A threshold dynamics determined by the basic reproduction number �0 isestablished: The disease can be eradicated if �0 < 1, while the disease persists if�0 > 1. As an application, six different screening strategies are explored to examinethe impacts of screening on the control of the 2009 influenza A (H1N1) pandemic.We find that it is crucial to screen travelers from and to high-risk patches, and it is notnecessary to implement screening in all connected patches, and both the dispersal ratesand the successful detection rate of screening play an important role on determiningan effective and practical screening strategy.

    Keywords Epidemicmodel · Patchy environment ·Threshold dynamics ·Dispersal ·Entry–exit screening

    1 Introduction

    With the rapidly growing travel among cities and countries, newly emerging infectiousdiseases and many re-emerging once-controlled infectious diseases have the trend tospread regionally and globallymuch faster than ever before (Jones et al. 2008). Interna-tional travel has been amajor factor causing the SARS outbreak in 2003 (Lipsitch et al.

    B Shengqiang [email protected]

    1 Academy of Fundamental and Interdisciplinary Sciences, Harbin Institute of Technology, 3041#,2 Yi-Kuang Street, Nan-Gang District, Harbin 150080, China

    2 Department of Mathematics and Statistics, University of New Brunswick, Fredericton,NB E3B 5A3, Canada

    123

    http://crossmark.crossref.org/dialog/?doi=10.1007/s11538-015-0084-6&domain=pdfhttp://orcid.org/0000-0001-7919-0801

  • 1238 X. Wang et al.

    2003; Ruan et al. 2006), the A (H1N1) influenza pandemic in 2009 (Tang et al. 2010,2012; Yu et al. 2012), and the outbreak of a novel avian-origin influenza A(H7N9)(Gao et al. 2013). To better understand how travel among patches (a patch could be assmall as a community village, or as large as a country or even a continent) influencesthe spread of infectious diseases, many deterministic models involving the interactionand dispersal of meta-populations in two or multiple patches have been proposed andinvestigated. See for example, Allen et al. (2007), Alonso and McKane (2002), Arinoet al. (2005), Arino and van denDriessche (2003a, b, 2006), Bolker (1999), Brauer andvan den Driessche (2001), Brauer et al. (2008), Brown and Bolker (2004), Eisenberget al. (2013), Gao and Ruan (2013), Hethcote (1976), Hsieh et al. (2007), Sattenspieland Herring (2003) and references therein.

    Being aware that travel can quickly bring infectious diseases from one patch toanother, it is natural for the authorities to implement traveler health screeningmeasuresat borders for exit and entry when an outbreak occurs. For example, the World HealthOrganization (WHO) declared the influenza A (H1N1) outbreak a pandemic in Juneof 2009. As a response, many countries implemented the entry–exit health screeningmeasures for travelers (Ainseba and Iannelli 2012; Cowling et al. 2010). In China, anational surveillance was established which includes the border entry screening: Anyone entering China was required to undergo screening at the border. Moreover, allpatients with suspected A (H1N1) pdm09 virus infection were admitted to designatedhospitals for containment (Yu et al. 2010). Exit screening was also conducted by thescreening of travelers at Mexican airports before they boarded flights out of Mexico(Khan et al. 2013). There are several broad approaches to border screening, includingscan of travelers by thermal scanners for elevated body temperature, observation oftravelers by alert staff for influenza symptoms (e.g., cough) as well as collection ofhealth declaration forms (Cowling et al. 2010; Li et al. 2013). During the 2009 A(H1N1) pandemic, it was shown that about one-third of confirmed imported H1N1cases were identified through entry screening to Hong Kong and Singapore (Cowlinget al. 2010), while for China, the detection rate of entry screening was about 45.56%(1027 detected cases over the total 2254 imported cases) (Li et al. 2013).

    Practically, the screening process is very complicated, and many questions shouldbe considered. For example, should ‘exit screening’, or ‘targeted entry screening’ or‘indiscriminate entry screening’ (Khan et al. 2013) be implemented? When to initiateand when to discontinue the measures? As screening measures may have tremendousimpacts on travel and trade and hence result in huge consequences in public healthand economy, it is of great importance to assess the effectiveness and impact of theentry–exit screening measures on the spread and control of infectious diseases. In thisregard, a recent study analyzed the effectiveness of border entry screening in Chinaduring this pandemic (Yu et al. 2012), and another paper performed a retrospectiveevaluation for the entry and exit screening of travelers flying out of Mexico during theA (H1N1) 2009 pandemic (Khan et al. 2013).

    Mathematical models have been developed by many researchers over the pastdecades to evaluate the effectiveness of screening. For example, Gumel et al. (2004)formulated a model to investigate the long-term control strategies of SARS, where itwas suggested that the eradication of SARS would require the implementation of areliable and rapid screening test at the entry points in conjunction with optimal isola-

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1239

    tion. Hyman et al. (2003) formulated models with random screening to estimate theeffectiveness of control measures on the spread of HIV and other sexually transmit-ted diseases. In Nyabadza and Mukandavire (2011), screening strategy through HIVcounseling was incorporated into the model to qualify its impact on prevention ofHIV/AIDS epidemic in South Africa. For other epidemic models with screening, werefer to Ainseba and Iannelli (2012), Hove-Musekwa and Nyabadza (2009), Liu et al.(2011), Liu and Takeuchi (2006), Liu and Stechlinski (2013). Most of these studiesfocus on evaluations of screening in a single patch, but little attention has been paidto the effectiveness of screening on the travelers among patches (Liu et al. 2011; Liuand Takeuchi 2006).

    In Liu et al. (2011) and Liu and Takeuchi (2006), the entry–exit screening processis incorporated into an SIS model between two cities with transport-related infection.It is shown that the entry–exit screening measures have the potential to eradicatethe disease induced by the transport-related infection when the disease is otherwiseendemicwhen both cities are isolated. Note that themodels in Liu et al. (2011), Liu andTakeuchi (2006) do not include a latent compartment, while many infectious diseasesdo undergo latent stages before they show obvious symptoms and become activelyinfectious. In this paper, we will incorporate the entry–exit screening measures intoa compartmental deterministic model with multiple patches and study the impacts ofthe entry–exit screening measures on the spread and control of the 2009 influenza A(H1N1).

    The rest of this paper is organized as follows. In Sect. 2, based on the models ofGerberry and Milner (2009) (also Feng 2007; Hethcote et al. 2002; Hsu and Hsieh2005; Safi and Gumel 2010; Tang et al. 2010), we formulate a multi-patch modelto examine how entry–exit screening measures impact the spread and control of pan-demic infectious diseases among patches. In Sect. 3, we identify the basic reproductionnumber and establish a global threshold dynamics for our model. In Sect. 4, we applythe results in Sect. 3 to the case study of 2009 influenza A (H1N1) pandemic: Weshow the sensitivities of the basic reproduction number upon the variation of otherparameters before we discuss the impacts of various screening strategies on the con-trol of influenza A (H1N1). We conclude this paper in Sect. 5 with a summary anddiscussion.

    2 The n-Patch SEIQR Model with Entry–Exit Screenings

    In this section, we model the transmission dynamics of a disease in a population withn patches by taking into consideration entry–exit screening among patches. Within asingle patch, ourmodel is based on that ofGerberry andMilner (2009) (also Feng 2007;Hethcote et al. 2002; Hsu and Hsieh 2005; Safi and Gumel 2010) with a susceptible–exposed–infectious–isolation–recovered structure. Hereafter, the subscript i refers topatch i . Our patchy model is motivated by that of Tang et al. (2010).

    For patch i (i = 1, 2, . . . , n), the population is divided into five disjoint com-partments, namely, compartments of susceptible, exposed (infected but not infectiousand have not yet developed clinical symptoms), infective, isolated, and recovered.We use Si , Ei , Ii , Qi and Ri to denote the corresponding population sizes, respec-

    123

  • 1240 X. Wang et al.

    Fig. 1 Flow chart of the disease transmission process between patch i and patch j

    tively. Let μSi > 0, μEi > 0, μ

    Ii > 0, μ

    Qi > 0, μ

    Ri > 0 denote the death rates of

    the individuals in the five classes, respectively. Throughout the paper, we alwaysassume that μSi ≤ min{μEi , μQi , μIi , μRi }. The total population of patch i is givenby Ni = Si + Ei + Ii + Qi + Ri . It is assumed that all newly born individuals aresusceptible, and the birth rate Bi (Ni ) satisfies the following assumptions (see Tangand Chen 2002)

    (A1) Bi (Ni ) > 0 for Ni > 0;(A2) Bi (Ni ) is continuously differentiable and B ′i (Ni ) < 0;(A3) μSi > Bi (∞).

    Let γ Ii > 0 and γQ

    i > 0 denote the recovery rates of infectious individuals incompartments Ii and Qi , respectively.Weused Ai j ≥ 0, i �= j to denote the dispersal (ortravel) rate from patch j to patch i (thus d Aii = 0) for A = S, E, I, Q, R. We define thedispersal matrix by D A = (˜d Ai j )n×n , with ˜d Ai j = d Ai j , i �= j and ˜d Aii = −

    ∑nj=1, j �=i d Aji .

    It is assumed that DE and DI are irreducible. We denote by βi > 0 the diseasetransmission rate and assume the standard incidence rate of infection. Let θei j ∈ [0, 1)denote the probability that an infectious individual in patch j traveling to patch i issuccessfully detected by the entry screening in patch i . This individual is then isolatedin patch i . Similarly, we use θoi j ∈ [0, 1) to denote the probability that an infectiousindividual in patch j leaving for patch i is detected by the exit screening in patch jand is then put into isolation in patch j . We assume that a susceptible individual entersthe exposed class after being infected by an infectious individual and after 1

    αi> 0

    time units of latent period, the individual becomes infectious and thus can infect othersusceptible individuals. A flow chart of the transmission process between patches iand j is sketched in Fig. 1, where δoi j = 1 − θoi j and δei j = 1 − θei j .

    As shown in Fig. 1, we neglect the transport-related infection and assume thatindividuals do not change their disease states when they travel from one patch to

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1241

    another; moreover, for the sake of focusing our study on the entry–exit screening, weignore the contact tracing. Based on the above assumptions, our model can then bedescribed by the following system

    Ṡi = Bi (Ni )Ni − βi Si IiNi − μSi Si −n∑

    j=1d Sji Si +

    n∑

    j=1d Si j S j ,

    Ėi = βi Si IiNi − αi Ei − μEi Ei −n∑

    j=1d Eji Ei +

    n∑

    j=1d Ei j E j ,

    İi = αi Ei − γ Ii Ii − μIi Ii −n∑

    j=1d Iji Ii +

    n∑

    j=1δei jδ

    oi j d

    Ii j I j ,

    Q̇i = −γ Qi Qi − μQi Qi +n∑

    j=1θoji d

    Iji Ii +

    n∑

    j=1θei jδ

    oi j d

    Ii j I j ,

    Ṙi = γ Ii Ii + γ Qi Qi − μRi Ri −n∑

    j=1d Rji Ri +

    n∑

    j=1d Ri j R j ,

    i = 1, 2, . . . , n.

    (1)

    Throughout this paper, we use the following notation. For a vector x ∈ Rn, weuse diag(x) to denote the n × n diagonal matrix, whose diagonal elements are thecomponents of x. We use the ordering in Rn generated by the cone Rn+, and that is,x ≤ y if y − x ∈ Rn+, x < y if x ≤ y and x �= y and finally x y means xi < yi forany index i . We use (S(t), E(t), I (t), Q(t), R(t)) to denote the vector

    (S1(t), . . . , Sn(t), E1(t), . . . , En(t), I1(t), . . . , In(t),

    Q1(t), . . . , Qn(t), R1(t), . . . , Rn(t))T ∈ R5n+ ,

    and we denote A0 =(S(0), E(0), I (0), Q(0), R(0)), then for any nonnegative ini-tial condition A0, it follows from the standard existence and uniqueness theorem forordinary differential equations (Perko 2001) that system (1) admits a unique solution(S(t), E(t), I (t), Q(t), R(t)).

    To show the existence of the disease-free equilibrium (DFE), we let Ei = Ii =Qi = Ri = 0, i = 1, 2, . . . , n in (1) to get

    Ṡi = Bi (Si )Si −n

    j=1d Sji Si +

    n∑

    j=1d Si j S j − μSi Si , Si (0) > 0, i = 1, 2, . . . , n. (2)

    In order for system (2) to have a positive equilibrium, we assume that

    (A4) s(diag(Bi (0) − μSi ) + DS) > 0, where s(·) represents the stability modulus ofan n ×n matrix and is defined by s(M) := max{Reλ, λ is an eigenvalue of M}.

    Biologically,Assumption (A4) guarantees that the number of susceptible populationis positive when there is no infective individual.

    Following similar arguments as those in Wang and Zhao (2004), Zhao and Jing(1996), we have

    123

  • 1242 X. Wang et al.

    Lemma 1 Under the assumptions (A1)–(A4), system (2) admits a unique positiveequilibrium (S0)T = (S01 , S02 , . . . , S0n ), which is globally asymptotically stable forR

    n+\{0}.Our preliminary results are the following two lemmas, whose proofs are similar to

    those given in Wang and Zhao (2004) and thus are omitted.

    Lemma 2 Under the assumptions (A1)–(A4), system (1) admits a unique DFE P0 =(S0, 0, . . . , 0) with (S0)T = (S01 , S01 , . . . , S0n ) ∈ Rn+ and 0T = (0, . . . , 0) ∈ Rn+.

    Lemma 3 If (A1)–(A4) hold, then system (1) is dissipative, that is, there exists anN∗ > 0 such that every forward orbit (S(t), E(t), I (t), Q(t), R(t)) eventually entersthe set G := {(S(t), E(t), I (t), Q(t), R(t)) ∈ R5n+ :

    ∑ni=1(Si (t) + Ei (t) + Ii (t) +

    Qi (t) + Ri (t)) ≤ N∗} and G is positively invariant with respect to system (1).

    3 Model Analysis

    3.1 The Basic Reproduction Number

    In this section, we identify the basic reproduction number, �0 for system (1).Following the procedure introduced in van den Driessche and Watmough (2002),�0 = ρ(FV −1), where ρ represents the spectral radius of a matrix. Here F = F3n×3nand V = V3n×3n represent new infections and transition terms, respectively. They aregiven by

    F3n×3n =⎛

    0 F12 00 0 00 0 0

    ⎠ , V3n×3n =⎛

    V11 0 0V21 V22 00 V32 V33

    with

    F12 =

    β1 0 . . . 00 β2 . . . 0...

    .... . .

    ...

    0 0 . . . βn

    V11 =

    α1 + μE1 +n∑

    j=1d Ej1 − d E12 . . . − d E1n

    − d E21 α2 + μE2 +n∑

    j=1d Ej2 . . . − d E2n

    ......

    . . ....

    − d En1 − d En2 . . . αn + μEn +n∑

    j=1d Ejn

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1243

    V21 =

    −α1 0 . . . 00 −α2 . . . 0...

    .... . .

    ...

    0 0 . . . −αn

    V22 =

    γ I1 + μI1 +n∑

    j=1d Ij1 − δe12δo12d I12 . . . −δe1nδo1nd I1n

    −δe21δo21d I21 γ I2 + μI2 +n∑

    j=1d Ij2 . . . −δe2nδo2nd I2n

    ......

    . . ....

    −δen1δon1d In1 − δen2δon2d In2 . . . γ In + μIn +n∑

    j=1d Ijn

    V32 =

    −n∑

    j=1θoj1d

    Ij1 − θe12δo12d I12 . . . −θe1nδo1nd I1n

    −θe21δo21d I21 −n∑

    j=1θoj2d

    Ij2 . . . −θe2nδo2nd I2n

    ......

    . . ....

    −θen1δon1d In1 − θen2δon2d In2 . . . −n∑

    j=1θojnd

    Ijn

    and

    V33 =

    γQ1 + μQ1 0 . . . 00 γ Q2 + μQ2 . . . 0...

    .... . .

    ...

    0 0 . . . γ Qn + μQn

    Both V −111 and V−122 are nonsingular M-matrices, which shows their inverses are

    nonnegative. This allows us to simplify the basic reproduction number as follows:

    �0 = ρ(F3n×3n · V −13n×3n) = ρ(−F12V −122 V21V −111 ). (3)

    Under some special circumstances, we have the following result.

    Proposition 1 If αi = α, γ Ii = γ I , μEi = μE , μIi = μI , d Ai j = d for A = E, I ,θoi j = θei j = θ ∈ [0, 1], for ∀ i, j = 1, 2, . . . , n with i �= j , then

    limd→0+

    �0 = maxi

    αβi

    (α + μE )(γ I + μI ) . (4)

    123

  • 1244 X. Wang et al.

    Proof Note that in this special case,

    V11 =

    α + μE + (n − 1)d − d . . . − d− d α + μE + (n − 1)d . . . − d...

    .... . .

    ...

    − d − d . . . α + μE + (n − 1)d

    and

    V22 =

    γ I + μI + (n − 1)d − (1 − θ)2d . . . − (1 − θ)2d− (1 − θ)2d γ I + μI + (n − 1) . . . − (1 − θ)2d...

    .... . .

    ...

    − (1 − θ)2d − (1 − θ)2d . . . γ I + μI + (n − 1)d

    Thus, limd→0 V −111 = 1α+μE Id and limd→0 V −122 = 1γ I +μI Id, where Id denotes then×n identitymatrix.Therefore, using (3),weobtain limd→0+ �0=max

    i

    αβi(α+μE )(γ+μI ) .

    3.2 Global Stability of the DFE

    It follows from van den Driessche and Watmough (2002, Theorem 2) that the DFE islocally asymptotical stable if �0 < 1 and is unstable if �0 > 1.Theorem 1 Assume that (A1)–(A4) are satisfied. If �0 < 1, then the solution(S(t), E(t), I (t), Q(t), R(t)) of (1) satisfies

    limt→∞(S(t), E(t), I (t), Q(t), R(t)) = P

    0.

    Proof By Lemma 3, there exists a T ′ > 0 and when t > T ′:⎧

    Ėi ≤ βi Ii − αi Ei − μEi Ei −n∑

    j=1d Eji Ei +

    n∑

    j=1d Ei j E j ,

    İi = αi Ei − γ Ii Ii − μIi Ii −n∑

    j=1d Iji Ii +

    n∑

    j=1δei jδ

    oi j d

    Ii j I j ,

    Q̇i = −γ Qi Qi − μQi Qi +n∑

    j=1θoji d

    Iji Ii +

    n∑

    j=1θei jδ

    oi j d

    Ii j I j .

    (5)

    Set M1 = F − V and �0 < 1, it follows that s(M1) < 0. Let vT = (v1, . . . , vn) bea positive eigenvector associated with s(M1). Choose k > 0 small enough such thatkv ξ . Since kv is a positive eigenvector associated with s(M1), the solution of thecomparison system (5) is given by kves(M1)(t−T ′). According to the comparison prin-ciple (Smith 1995, 2008), (E(t), I (t), Q(t)) ≤ kves(M1)(t−T ′), for t > T ′. Therefore,

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1245

    we get (E(t), I (t), Q(t)) → (0, 0, 0) as t → ∞. Further using the equations for Riof model (1), we can prove that limt→∞ R(t) = 0.

    Next we prove that limt→∞ S(t) = S

    0. Let Φ(t) : Rn+ → Rn+ be the solution semi-flow of (1), that is, Φ(t)(S0, E0, I0, Q0, R0) = (S(t), E(t), I (t), Q(t), R(t)) withthe nonnegative initial value (S0, E0, I0, Q0, R0).

    Given (S0, E0, I0, Q0, R0) ∈ G with Si0 �= 0, it easily follows that S(t) ∈ Int(Rn+),∀t > 0. Let ω = ω(S0, E0, I0, Q0, R0) be the omega limit set of Φ(t). Since(E(t), I (t), Q(t), R(t)) → (0, 0, 0, 0) as t → ∞, there holds ω = ω̃×{(0, 0, 0, 0)}.We claim that there must be ω̃ �= {0}. Otherwise, if this is not true, i.e., ω̃ = {0},then we must have lim

    t→∞(S(t), E(t), I (t), Q(t), R(t)) = (0, 0, 0, 0, 0). By Assump-tion (A4), we can choose a small η > 0, such that s(diag(Bi (0) − μSi ) + DS −ηdiag(1)) > 0, where 1 = (1, . . . , 1). It follows that there exists a t1 > 0such that Bi (Ni (t)) − βi Ii (t)Ni (t) ≥ Bi (0+) − η for ∀t ≥ t1, i = 1, . . . , n. ThenS(t)T = (S1(t), S2(t), . . . , Sn(t)) satisfies

    Ṡi (t) > (Bi (0+) − ηi )Si (t) −n∑

    j=1d Sji Si (t) +

    n∑

    j=1d Si j S j (t) − μSi Si (t). (6)

    Let ωT = (ω1, . . . , ωn) be a positive eigenvector of the matrix diag(Bi (0) − μSi ) +DS −ηdiag(1) associated with the eigenvalue s(diag(Bi (0)−μSi )+ DS −ηdiag(1)).Choose a small number α > 0 such that S(t1) > αω. Then the comparison principle(Smith 1995, 2008) implies that

    S(t) ≥ αωes(diag(Bi (0) − μSi ) + DS − ηdiag(1))(t − t1), ∀t ≥ t1

    and then Si (t) → ∞, i = 1, 2 . . . n, a contradiction. It is easy to see thatΦ1(t)|ω(S(t),0, 0, 0, 0) = (Φ1(t)S(t), 0, 0, 0, 0), where Φ1(t) is the solution semi-flow of system(2). By Hirsch et al. (2001, Lemma 2.10), ω is an internal chain transitive set forΦ(t), and hence, ω1 is an internal chain transitive set for Φ1(t). Since ω1 �= 0 andS0 is globally asymptotically stable for (1) in Rn+\{0}, we have ω1 ∩ W s(S0) �= ∅.By (Hirsch et al. 2001, Theorem 3.1 and Remark 4.6), we then get ω1 = S0, provingω = {P0}. This proves Theorem 1. �

    3.3 Disease Persistence and Existence of the Endemic Equilibrium

    It follows from van den Driessche and Watmough (2002, Theorem 2) that the DFEP0 is unstable if �0 > 1. The following result shows that �0 > 1 actually impliesthat model (1) admits at least one endemic equilibrium (EE) and the disease persistsuniformly.

    Define X = {(S, E, I, Q, R) : Si ≥ 0, Ei ≥ 0, Ii ≥ 0, Qi ≥ 0, Ri ≥ 0, i =1, 2, . . . , n}, X0 = {(S, E, I, Q, R) : Ei > 0, Ii > 0, i = 1, 2, . . . , n}, ∂ X0 =X\X0.

    123

  • 1246 X. Wang et al.

    Theorem 2 Suppose the assumptions (A1)–(A4) hold and the basic reproductionnumber �0 > 1. Then system (1) is uniformly persistent, that is, there exists a positiveconstant � > 0 such that every solution A(t) of (1) with

    A0 ∈ Rn+ × (Rn+\{0}) × (Rn+\{0}) × Rn+ × Rn+satisfies

    limt→∞ inf(Ei (t), Ii (t)) ≥ (�, �), i = 1, . . . , n.

    Moreover, there exists at least one EE.

    Proof Let Φ(t) : X → X be the solution flow associated with system (1), that is,Φ(t)(A0) = A(t).

    It follows from Lemma 3 that X is positively invariant and system (1) is pointdissipative. By the comparison principle for cooperative systems (Smith 1995, 2008),it follows that (E, I ) � (0, 0). This implies that X0 is positively invariant, thus ∂ X0is relatively closed in X .

    Set M∂ = {A0 ∈ X : A(t) ∈ ∂ X0, ∀t ≥ 0}. We claim that

    M∂ = {(E(t), I (t)) = (0, 0), ∀t ≥ 0}.

    Suppose on the contrary, i.e., there exists a t0 ≥ 0 such that E(t0) > 0, or I (t0) > 0.Without loss of generality, we assume that E(t0) > 0. We partition {1, 2, . . . , n} intotwo sets, Z1 and Z2, such that

    Ei (t0) = 0,∀i ∈ Z1, and Ei (t0) > 0,∀i ∈ Z2.

    Next we claim that Ei (t) > 0 for t0 < t < t0 + �0, ∀i = 1, · · · , n for �0 > 0small enough, which could be easily verified provided that Z1 = ∅. Assume Z1 �= ∅,since Z2 �= ∅ as E(t0) > 0. Then for ∀i ∈ Z1,

    Ėi (t0) = βi Si (t0)Ii (t0)Ni (t0) − αi Ei (t0) −n∑

    j=1d Eji Ei (t0) +

    n∑

    j=1d Ei j E j (t0) − μEi Ei (t0)

    = βi Si (t0)Ii (t0)Ni (t0) +∑

    j∈Z2d Ei j E j (t0).

    According to the irreducibility of DE , there is always a chain j1, j2, . . . , jn withj1 = j, jn = i , which ensures that ∑ j∈Z2 d Ei j E j (t0) > 0 ⇒ Ėi (t0) > 0, and hence,there exists an �0 > 0 such that Ei (t) > 0 for t0 < t < t0+�0. Clearly, we can restrict�0 > 0 small enough such that Ei (t) > 0, t0 < t < t0 + �0 for ∀i ∈ Z1∪Z2. Thisproves Ei (t) > 0, i = 1, . . . , n, t0 < t < t0 + �0.

    Using the equation of system (1) for Ii , we obtain that either Ii (t0) > 0, or Ii (t0) = 0and İi (t0) > 0 holds true, for both cases, we have Ii (t) > 0, t0 < t < t0 + �1, ∀i =1, · · · , n for �1 > 0 sufficiently small. This results in A(t) /∈ ∂ X0 for t0 < t < t0 +min{�0, �1}, which contradicts the assumption of M∂ , this proves E(t) = 0, ∀t ≥ 0.

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1247

    Repeating the same way on I (t), we can show that I (t) = 0∀t ≥ 0, and thus we verifythe above claim on M∂ .

    Next we show that the solution A(t) through A0 ∈ X0 satisfies

    lim supt→∞

    max1≤i≤n{Ei (t), Ii (t)} > �2.

    for some positive constant �2.Suppose this is not true, there must exist a T1 > 0 such that

    0 < max1≤i≤n{Ei (t), Ii (t)} ≤ �2, for all t ≥ T1,

    then it follows from the equations of Qi , Ri , i = 1, . . . , n of system (1) that ∃k0 > 0,such that (Qi (t), Ri (t)) < (k0�2, k0�2). As the boundedness of S, we can restrictβi Si Ii

    Ni≤ ξ(�2). Then we have

    Ṡi = Bi (Ni )Ni − βi Si IiNi

    −n

    j=1d Sji Si +

    n∑

    j=1d Si j S j − μSi Si

    ≥ Bi (Si + (2k0 + 2)�2)Si − (μSi + ξ(�2))Si −n

    j=1d ji Si +

    n∑

    j=1di j S j

    Consider the following auxiliary equation

    Ṡi = Bi (Si + (2k0 + 2)�2)Si − (μSi + ξ(�2))Si −n

    j=1d Sji Si +

    n∑

    j=1d Si j S j ,

    (S1(T1), . . . , Sn(T1)) = (S1(T1), . . . , Sn(T1)), i = 1, . . . , n . (7)

    By the comparison principle Smith (1995), Smith (2008), we have S(t) ≥S(t),∀t ≥ T1, here ST (t) = (S1(t), . . . , Sn(t)). By (7), there exists a constant vec-tor S0(�2) > 0 such that (S0)T (�2) is globally asymptotically stable for (7) and thatS0(0) = S0. Then there exists a sufficiently small ηwith ηT = (η1, . . . , ηn) ∈ Rn+ anda sufficiently large T > 0, such that S0(�2) > S0−η, and that S(t) ≥ S0(�2) ≥ S0−ηfor all t ≥ T + T1. As a consequence, SiNi = 1 −

    Ei +Ii +Qi +RiNi

    ≥ 1 − (2k0+2)�2S0i −ηi

    ,∀t ≥T + T1, hence we have

    Ėi = βi Si IiNi

    − αi Ei −n

    j=1d Eji Ei +

    n∑

    j=1d Ei j E j − μEi Ei

    ≥ βi Ii (1 − (2k0 + 2)�2S0i − ηi

    ) − (αi + μEi )Ei −n

    j=1d Eji Ei +

    n∑

    j=1d Ei j E j .

    123

  • 1248 X. Wang et al.

    Consider the following auxiliary system:

    ˙̃Ei = βi˜Ii (1 − (2k0+2)�2S0i −ηi ) − αi˜Ei − μEi ˜Ei −

    n∑

    j=1d Eji ˜Ei +

    n∑

    j=1d Ei j ˜E j ,

    ˙̃Ii = αi ˜Ei − γi˜Ii − μIi ˜Ii −n∑

    j=1d Iji˜Ii +

    n∑

    j=1δei jδ

    oi j d

    Ii j

    ˜I j ,

    ˙̃Qi = −γi ˜Qi − μIi ˜Qi +n∑

    j=1θoji d

    Qji˜Ii +

    n∑

    j=1θei jδ

    oi j d

    Qi j

    ˜I j .

    (8)

    Since �0 > 1, we know that the matrix (1 − (2k0+2)�2S0i −ηi )M1 has a positive eigenvalues((1− (2k0+2)�2

    S0i −ηi)M1) with a positive eigenvector. Let ṽT = (v1, . . . , vn) be a positive

    eigenvector associated with s((1− (2k0+2)�2S0i −ηi

    )M1), then the solution of Eq. (8) is given

    by k1ṽes((1− (2k0+2)�2

    S0i −ηi)M1)

    . Again, by the comparison principle (Smith 1995, 2008), wehave

    (E(t), I (t), Q(t)) ≥ k1ṽes((1− (2k0+2)�2

    S0i −ηi)M1)t

    , ∀t ≥ T .

    Then (Ei (t), Ii (t), Qi (t)) → (∞,∞,∞), i = 1, 2, . . . , n, for t → ∞, which leadsto a contradiction.

    Note that (S0)T is globally asymptotically stable in Rn+\{0} for system (2). By theafore-mentioned claim, it then follows that (0, 0, 0, 0, 0) and P0 are isolated invariantsets in X , W s((0, 0, 0, 0, 0)) ∩ X0 = ∅, and W s(P0) ∩ X0 = ∅. Clearly, every orbitin M∂ converges to either (0, 0, 0, 0, 0) or P0, and (0, 0, 0, 0, 0) and P0 are acyclic inM∂ . By Hirsch et al. (2001, Theorem 4.3 and Remark 4.3), we conclude that system(1) is uniformly persistent with respect to (X0, ∂ X0). By Zhao (1995, Theorem 2.4),system (1) has at least one equilibrium (S∗, E∗, I ∗, Q∗, R∗) ∈ X0, with E∗ � 0 andI ∗ � 0. We further show that S∗ ∈ Rn+\{0}. Suppose S∗ = 0, by the sum of equationsof Ei in (1), we get 0 =

    n∑

    i=1(αi + μi )E∗i , and hence E∗ = 0, a contradiction. Thus

    the proof is complete. 2. �

    4 Case Study for the 2009 Influenza A (H1N1)

    In this section, we use numerical simulations to explore the impacts of various screen-ing strategies on the control of 2009 influenza A (H1N1) pandemic.

    4.1 Sensitivity Analysis of �0 on Parameters for a Two-Patch Model

    We consider a special case of system (1) with n = 2 as follows:

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1249

    Ṡ1 = B1(N1)N1 − β1S1 I1N1

    − μS1 S1 − d S21S1 + d S12S2,Ė1 = β1S1 I1

    N1− α1E1 − μE1 E1 − d E21E1 + d E12E2,

    İ1 = α1E1 − γ I1 I1 − μI1 I1 − d I21 I1 + δe12δo12d I12 I2,Q̇1 = −γ Q1 Q1 − μQ1 Q1 + θo21d I21 I1 + θe12δo12d I12 I2,Ṙ1 = γ I1 I1 + γ Q1 Q1 − μR1 R1 − d R21R1 + d R12R2,Ṡ2 = B2(N2)N2 − β2S2 I2

    N2− μS2 S2 − d S12S2 + d S21S1,

    Ė2 = β2S2 I2N2

    − α2E2 − μE2 E2 − d E12E2 + d E21E1,İ2 = α2E2 − γ I2 I2 − μI2 I2 − d I22 I2 + δe21δo21d I21 I1,Q̇2 = −γ Q2 Q2 − μI2Q2 + θo12d I12 I2 + θe21δo21d I21 I1,Ṙ2 = γ I2 I2 + γ Q2 Q2 − μR2 R2 − d R12R2 + d R21R1.

    (9)

    The basic reproduction number of system (9) is given by

    �0∣

    (9) = ρ(

    −F̃12Ṽ −122 Ṽ21Ṽ −111)

    (10)

    where

    F̃12 =⎛

    β1 0

    0 β2

    ⎠ ; Ṽ21 =⎛

    γ I1 + μI1 + d I21 − δe12δo12d I12−δe21δo21d I21 γ I2 + μI2 + d I12

    ⎠ ;

    Ṽ21 =(−α1 0

    0 −α2

    )

    ; Ṽ11 =(

    α1 + μE1 + d E21 − d E12− d E21 α2 + μE2 + d E12

    )

    .

    Note that the basic reproduction number �0 defined in (10) involves a group ofparameters. To identify to which parameters �0 is sensitive, we carry out a sensitivityanalysis by evaluating the partial rank correlation coefficients (PRCCs) for all inputparameters against the output variable �0 (Blower and Dowlatabadi 1994; Wu et al.2013). We take parameter values as in Table 1. Moreover, we denote β = β1 =β2, α = α1 = α2, μK = μK1 = μK2 ; d K = d K12 = d K21, (K = S, I, E, R), and we setγ = 1/6.56 = γ I1 = γ I2 , d I = 0.5× d S, d E = 0.9× d S , where d S = 0.135; we alsoassume θe = 0.37 = θe21 = θe12, θo = θo21 = θo12 with θo = 0.3 × θe.

    We show that the infection rateβ is themost sensitive parameter of�0 of system (9).For other coefficients, Fig. 2 shows that the six parameters with most impacts on �0are the rate of progression to latent (α), the recovery rate (γ ), the entry screening rate(θe), the exit screening rate (θo), the susceptible dispersal rate (d S), and the infecteddispersal rate (d I ).

    123

  • 1250 X. Wang et al.

    Table 1 The parameter estimates for the 2009 influenza A (H1N1) pandemic

    Parametersi, j = 1, 2 i �= j

    Definitions Values References

    βi The infection rate (days−1) in

    patch i0.3936

    Tang et al. (2012)

    αi Rate of progression to latent(days−1) in patch i

    0.55Tang et al. (2012)

    γ Ii Recovery rate (days−1) in

    patch i1/7.48–1/6

    Tang et al. (2012),Xiao et al. (2015)

    μSi The natural death rate(days−1) in patch i

    3.805 × 10−5Wang and Wang(2012)

    μIi , (μEi ) Infectious (Exposed) death

    rate (days−1) in patch i5.307 × 10−5

    Xu et al. (2011)

    θei j Entry screening rate oftravelers from patch j to i

    0.33–0.4556Cowling et al. (2010),Li et al. (2013)

    θoi j Exit screening rate oftravelers from patch j to i

    0.165–0.2228 Estimated

    d Si j , (dRi j ) Dispersal rate (days

    −1) of thesusceptible (recovered)from patch j to i

    0.0135–0.135Tang et al. (2010)

    d Ii j , (dEi j ) Dispersal rate (days

    −1) of theinfectious (exposed) frompatch j to i

    0.0122–0.122 Estimated

    Fig. 2 Partial rank correlation coefficients illustrating the dependence of �0 on each parameter

    4.2 Impacts of Various Screening Strategies

    For the model (1), if patch i is not connected to any other patch, then the patch-specificbasic reproduction number is given by

    �0i = βiαi(αi + μEi )(γ Ii + μIi )

    .

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1251

    If �0i < 1, then we call patch i a low-risk patch, while if �0i > 1, then we call it ahigh-risk patch (Allen et al. 2007). Therefore, the disease persists in isolated high-riskpatches and dies out in isolated low-risk patches. During the 2009 H1N1 pandemic,Mexico could be regarded as a high-risk patch, and it is believed that the pandemic wascaused by the global connection with Mexico (Khan et al. 2013; Smith et al. 2009).

    To examine the impacts of various screening strategies on the control of diseases,we assume there are one high-risk patch, labeled as patch 1, and 4 low-risk patches,labeled as patches 2, 3, 4, and 5, and the overall basic reproduction number�0 is largerthan 1.

    For simulation purpose, we take parameter values as in Table 1: μSi = μRi =3.805 × 10−5, μEi = μIi = 5.307 × 10−5, αi = 0.55 for i = 1, . . . , 5, and β1 =0.3936 � βi = 0.15, γ I1 = 1/7.48 < γ Ii = 1/6 for i = 2, . . . , 5. For this set ofparameter values, �01 = 2.772 � 1, �02 = �03 = �04 = �05 = 0.900 < 1.That is, patch 1 is a high-risk patch, and the remaining 4 patches are low-risk patches.Considering reduced dispersal rates for exposed and infectious individuals, we taked Ei j = 0.9 × d Si j , d Ii j = 0.5 × d Si j , i �= j. Further we assume that patch 5 has lesscommunication with patch 1. For simplicity, we assume d S15 = d S51 = 0.1 × d S ,d S1 j = d Sj1 = d S for j = 2, 3, 4 and d Si j = d Sji = d S for i, j = 2, 3, 4, 5 and i �= j .

    The question we want to address is: what types of screening strategies are capableof preventing the endemic disease? To answer this question, we explore the outcomesof several possible screening strategies.

    We first consider Strategy I, “indiscriminate entry–exit screening” strategy: regard-less of the risk level and dispersal rates, same strength of entry and exit screeningsare implemented to each patch. That is, θoi j = θei j = θ for i, j = 1, . . . , 5. Forthe parameter values taken, we find numerically that this strategy is the most effec-tive of the six strategies considered. Moreover, the detection rate needs to be higheras the dispersal rates decrease, and when the dispersal rate d S < dc1 = 0.090,the screening strategy cannot control the disease even when the detection is perfect(see Fig. 3a).

    Strategy II is called the “indiscriminate entry screening” strategy: only entry screen-ing of each patch is implemented. That is, θei j = θ for i, j = 1, ..., 5. By comparingFig. 3a with Fig. 3b, we find that Strategy II can control the disease if Strategy I can,but Strategy II requires higher successful detection rate of infectious travelers.

    Strategy III in consideration is called the “targeted entry screening”: only applyentry screening for travel from and to the high-risk patch, patch 1. That is, θej1 =θe1 j = θ for j = 2, 3, 4, 5. As shown in Fig. 3c, the disease will die out if the dispersalrate d S is higher than a critical value dc2 (in our simulation, dc2 = 0.095).

    In practice, a natural question to be asked is: do we need to implement screeningin all patches? To answer this question, we examine Strategy IV, “selective entryscreening”: only apply entry screening to the high-risk patch and patches that arehighly connected to the high-risk patch (i.e., those patches with larger dispersal rates).In our simulation, we assume θej1 = θe1 j = θ, j = 2, 3, 4. Figure 3d indicates thatthis strategy can also eliminate the disease if the dispersal rate d S is higher than thecritical value dc3 = 0.097. This implies that there is no need to implement screeningat all patches.

    123

  • 1252 X. Wang et al.

    (a)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θoij = θeij = θ, i, j = 1, · · · , 5

    R0

    (b)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θeij = θ, i, j = 1, · · · , 5

    R0

    (c)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θe1j = θej1 = θ, j = 2, · · · , 5

    R0

    (d)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θe1j = θej1 = θ, j = 1, · · · , 4

    R0

    (e)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θej1 = θ, j = 2, · · · , 5

    R0

    (f)

    0 0.2 0.4 0.6 0.8 10.7

    0.8

    0.9

    1

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    θe1j = θ, j = 1, · · · , 5

    R0

    Fig. 3 Plots of �0 under screening Strategies I–VI. Parameters: γ I1 = 1/7.48; γ I2 = γ I3 = γ I4 = γ4 =1/6, β1 = 0.3936;β2 = β3 = β4 = β5 = 0.15.The black solid line: d S = 0.09; The pink solid linewith ∗:d S = 0.095; the blue dotted line: d S = 0.097; the red dot-and-dash line d S = 0.107; the green dashedline: d S = 0.135 (Color figure online)

    It is worth mentioning Strategy V, “one-way entry screening”: applying entryscreening at low-risk patches to individuals traveling from the high-risk patch only.In our simulations, we take θej1 = θ for j = 2, 3, 4, 5, and all other screening ratesare set to be zero. Then for our chosen parameter values, the dispersal rate d S must besufficiently large, larger than dc4 = 0.135 in our simulations (See Fig. 3e). However,another “one-way entry screening”, Strategy VI: applying entry screening at the high-risk patch to travelers from all low-risk patches is capable of eradicating the disease.

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1253

    In our simulation, we choose θe1 j = θ for j = 2, 3, 4, 5, and we can lower �0 to beless than 1 provided that d S > dc5 = 0.107 (see Fig. 3f).

    5 Summary and Discussion

    In this paper, we have investigated a general multi-patch SEIQRmodel with entry–exitscreenings. Our theoretical results, Theorems 1 and 2, were established by appealingto the comparison principle and uniform persistence principle. Our results show thatthe disease dies out when �0 < 1 and persists when �0 > 1. Thus the basic repro-duction number is a vital index to measure the level of the disease (Bauch and Rand2000; Clancy and Pearce 2013). Our Proposition 1 provides a theoretical confirmationfor the simulation results obtained in Sattenspiel and Herring’s (2003): When the dis-persal rates are very low, screening must be highly effective to alter disease patternssignificantly.

    We have also explored six different screening strategies to examine how the screen-ing impacts the control of influenza A (H1N1). Our numerical results show that itis crucial to screen travelers from and to high-risk patches, and it is not necessaryto implement screening in all connected patches, though the minimum number ofpatches that should implement screening depends critically on the dispersal rates andthe accuracy of screening process.

    During the 2009 influenza A (H1N1) pandemic in mainland China, besides theisolation of those detected infected individuals from the border screening, the indi-viduals who had been exposed to those who had been detected and isolated infectedwas traced and received medical observations (Yu et al. 2012), it is interesting to studythe combined effects of contact tracing and border screening, which we leave as ourfuture work.

    Acknowledgments The authors would like to extend their thanks to Professor Mark Lewis and the threeanonymous referees for their valuable comments and suggestions which led to a significant improvementin this work. The authors thank Professor Sanyi Tang for his very kind help in the sensitivity analysis andthank Professor Philip Maini and Dr. Jinzhi Lei for their helpful advice on the revision of this manuscript.The revision of this work was partially completed during XW’s visit to Wolfson Centre for MathematicalBiology, the University of Oxford, and she would like to acknowledge the hospitality received there. S. L.is supported by the National Natural Science Foundation of China (No. 11471089) and the FundamentalResearch Funds for the Central Universities (Grant No. HIT. IBRSEM. A. 201401) and LW is partiallysupported by NSERC of Canada.

    References

    Ainseba B, Iannelli M (2012) Optimal screening in structured SIR epidemics. Math Model Nat Phenom7(03):12–27

    Allen L, Bolker B, Lou Y, Nevai A (2007) Asymptotic profiles of the steady states for an sis epidemic patchmodel. SIAM J Appl Math 67(5):1283–1309

    Alonso D, McKane A (2002) Extinction dynamics in mainland-island metapopulations: an N-patch sto-chastic model. Bull Math Biol 64(5):913–958

    Arino J, Davis JR, Hartley D, Jordan R, Miller JM, van den Driessche P (2005) A multi-species epidemicmodel with spatial dynamics. Math Med Biol 22(2):129–142

    Arino J, van den Driessche P (2003a) A multi-city epidemic model. Math Popul Stud 10(3):175–193

    123

  • 1254 X. Wang et al.

    Arino J, van denDriesscheP (2003b)The basic reproduction number in amulti-city compartmental epidemicmodel. In: Benvenuti L, De Santis A, Farina L (eds) Positive systems, Springer, Berlin, Heidelberg,pp 135–142

    Arino J, van den Driessche P (2006) Disease spread in metapopulations. Nonlinear Dyn Evol Equ FieldsInst Commun 48:1–13

    Bauch C, Rand D (2000) A moment closure model for sexually transmitted disease transmission through aconcurrent partnership network. Proc R Soc Lond Ser B Biol Sci 267(1456):2019–2027

    Blower SM, Dowlatabadi H (1994) Sensitivity and uncertainty analysis of complexmodels of disease trans-mission: an HIV model as an example. Int Stat Rev 62:229–243

    Bolker BM (1999) Analytic models for the patchy spread of plant disease. Bul Math Biol 615:849–874Brauer F, van den Driessche P (2001) Models for transmission of disease with immigration of infectives.

    Math Biosci 171(2):143–154Brauer F, van den Driessche P, Wang L (2008) Oscillations in a patchy environment disease model. Math

    Biosci 215(1):1–10BrownDH, Bolker BM (2004) The effects of disease dispersal and host clustering on the epidemic threshold

    in plants. Bull Math Biol 66(2):341–371Clancy D, Pearce CJ (2013) The effect of population heterogeneities upon spread of infection. J Math Biol

    67(4):963–987Cowling B et al (2010) Entry screening to delay local transmission of 2009 pandemic influenza A (H1N1).

    BMC Infect Dis 10:82Eisenberg MC, Shuai Z, Tien JH, van den Driessche P (2013) A cholera model in a patchy environment

    with water and human movement. Math Biosci 246(1):105–112Feng Z (2007) Final and peak epidemic sizes for SEIR models with quarantine and isolation. Math Biosci

    Eng 4(4):675–686Gao D, Ruan S (2013)Modeling the spatial spread of Rift Valley fever in Egypt. Bull Math Biol 75:523–542Gao R, Cao B, Hu Y, Feng Z, Wang D, Hu W, Chen J, Jie Z, Qiu H, Xu K et al (2013) Human infection

    with a novel avian-origin influenza A(H7N9) virus. N Engl J Med 368(20):1888–1897Gerberry D, Milner F (2009) An SEIQR model for childhood diseases. J Math Biol 59:535–561Gumel AB, Ruan SG, Day T et al (2004) Modelling strategies for controlling SARS outbreaks. Proc R Soc

    Lond B 271:2223–2232Hethcote HW (1976) Qualitative analyses of communicable disease models. Math Biosci 28(3):335–356Hethcote HW, Ma Z, Liao S (2002) Effects of quarantine in six endemic models for infectious diseases.

    Math Biosci 180:141–160Hirsch MW, Smith HL, Zhao XQ (2001) Chain transitivity, attractivity, and strong repellors for semidy-

    namical systems. J Dyn Differ Equ 13(1):107–131Hsieh YH, van den Driessche P, Wang L (2007) Impact of travel between patches for spatial spread of

    disease. Bull Math Biol 69(4):1355–1375Hsu SB, Hsieh YH (2005) Modeling intervention measures and severity-dependent public response during

    severe acute respiratory syndrome outbreak. SIAM J Appl Math 66(2):627–647Hove-Musekwa SD, Nyabadza F (2009) The dynamics of an HIV/AIDS model with screened disease

    carriers. Comput Math Methods Med 10(4):287–305Hyman JM, Li J, Stanley E (2003)Modeling the impact of random screening and contact tracing in reducing

    the spread of HIV. Math Biosci 181(1):17–54Jones KE, Patel NG, Levy MA, Storeygard A, Balk D, Gittleman JL, Daszak P (2008) Global trends in

    emerging infectious diseases. Nature 451(7181):990–993Khan K, Eckhardt R, Brownstein JS, Naqvi R, Hu W, Kossowsky D, Scales D, Arino J, MacDonald M,

    Wang J et al (2013) Entry and exit screening of airline travellers during the A(H1N1) 2009 pandemic:a retrospective evaluation. Bull World Health Organ 91(5):368–376

    Li JY, Cui B, Wang L, Chen CT, Ci Y, Guo WJ (2013) The effect of strengthening the frontier healthquarantine to prevent and control the epidemic of influenza A (H1N1) from abroad. J Insp Quar (Chin)23(2):56–58

    Lipsitch M, Cohen T, Cooper B, Robins JM, Ma S, James L, Gopalakrishna G, Chew SK, Tan CC, SamoreMH et al (2003) Transmission dynamics and control of severe acute respiratory syndrome. Science300(5627):1966–1970

    Liu XN, Chen X, Takeuchi Y (2011) Dynamics of an SIQS epidemic model with transport-related infectionand exit–entry screenings. J Theor Biol 285(1):25–35

    123

  • An Epidemic Patchy Model with Entry–Exit Screening 1255

    Liu XN, Takeuchi Y (2006) Spread of disease with transport-related infection and entry screening. J TheorBiol 242(2):517–528

    Liu XZ, Stechlinski P (2013) Transmission dynamics of a switched multi-city model with transport-relatedinfections. Nonlinear Anal Real World Appl 14(1):264–279

    Nyabadza F, Mukandavire Z (2011) Modelling HIV/AIDS in the presence of an A(H1N1) testing andscreening campaign. J Theor Biol 280(1):167–179

    Perko L (2001) Differential equations and dynamical systems. Springer, New YorkRuan S, Wang W, Levin SA et al (2006) The effect of global travel on the spread of SARS. Math Biosci

    Eng 3(1):205–218Safi M, Gumel A (2010) Global asymptotic dynamics of a model for quarantine and isolation. Discrete

    Contin Dyn Syst Ser B 14:209–231Sattenspiel L, Herring DA (2003) Simulating the effect of quarantine on the spread of the 1918–19 flu in

    central Canada. Bull Math Biol 65(1):1–26Smith GJ, Vijaykrishna D, Bahl J, Lycett SJ, Worobey M, Pybus OG, Ma SK, Cheung CL, Raghwani J,

    Bhatt S et al (2009) Origins and evolutionary genomics of the 2009 swine-origin H1N1 influenza aepidemic. Nature 459(7250):1122–1125

    Smith HL (1995) The theory of the chemostat: dynamics of microbial competition, vol 13. CambridgeUniversity Press, Cambridge

    SmithHL (2008)Monotone dynamical systems: an introduction to the theory of competitive and cooperativesystems, vol 41. American Mathematical Society, Providence

    Tang S, Chen L (2002) Density-dependent birth rate, birth pulses and their population dynamic conse-quences. J Math Biol 44(2):185–199

    Tang S, Xiao Y, Yang Y, Zhou Y, Wu J, Ma Z et al (2010) Community-based measures for mitigating the2009 H1N1 pandemic in China. PLoS One 5(6):e10911

    Tang SY, Xiao YN, Yuan L, Cheke RA,Wu JH (2012) Campus quarantine (Fengxiao) for curbing emergentinfectious diseases: lessons from mitigating A/H1N1 in Xi’an, China. J Theor Biol 295(4):47–58

    van den Driessche P, Watmough J (2002) Reproduction numbers and sub-threshold endemic equilibria forcompartmental models of disease transmission. Math Biosci 180(1):29–48

    Wang L, Wang X (2012) Influence of temporary migration on the transmission of infectious diseases in amigrants’ home village. J Theor Biol 300:100–109

    Wang W, Zhao XQ (2004) An epidemic model in a patchy environment. Math Biosci 190(1):97–112Wu J, Dhingra R, GambhirM, Remais JV (2013) Sensitivity analysis of infectious disease models: methods,

    advances and their application. J R Soc Interface 10:20121018Xiao YN, Tang SY, Wu JH (2015) Media impact switching surface during an infectious disease outbreak.

    Sci Rep 5:7838. doi:10.1038/srep07838Xu CL, Sun SH et al (2011) Epidemiological characteristics of confirmed cases of pandemic influenza A

    (H1N1) 2009 in mainland China, 2009–2010. Dis Surveill 26:780–784Yu H, Cauchemez S, Donnelly CA, Zhou L, Feng L, Xiang N, Zheng J, Ye M, Huai Y, Liao Q et al (2012)

    Transmission dynamics, border entry screening, and school holidays during the 2009 influenza A(H1N1) pandemic, China. Emerg Infect Dis 18(5):758

    Yu H, Liao Q, Yuan Y, Zhou L, Xiang N, Huai Y, Guo X, Zheng Y, van Doorn HR, Farrar J et al (2010)Effectiveness of oseltamivir on disease progression and viral rna shedding in patients with mild pan-demic 2009 influenza A H1N1: opportunistic retrospective study of medical charts in China. Br MedJ 341:c4779. doi:10.1136/bmj.c4779

    Zhao XQ (1995) Uniform persistence and periodic coexistence states in infinite-dimensional periodic semi-flows with applications. Can Appl Math Q 3:473–495

    Zhao XQ, Jing ZJ (1996) Global asymptotic behavior in some cooperative systems of functional differentialequations. Can Appl Math Q 4(4):421–444

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    http://dx.doi.org/10.1038/srep07838http://dx.doi.org/10.1136/bmj.c4779

    An Epidemic Patchy Model with Entry--Exit ScreeningAbstract1 Introduction2 The n-Patch SEIQR Model with Entry--Exit Screenings3 Model Analysis3.1 The Basic Reproduction Number3.2 Global Stability of the DFE3.3 Disease Persistence and Existence of the Endemic Equilibrium

    4 Case Study for the 2009 Influenza A (H1N1)4.1 Sensitivity Analysis of 0 on Parameters for a Two-Patch Model4.2 Impacts of Various Screening Strategies

    5 Summary and DiscussionAcknowledgmentsReferences