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Synthesis, structural characterization and thermal stability of a 2D layered Cd(II) coordination polymer constructed from squarate (C4O42) and 2,2’-bis(2-pyridyl)ethylene (2,2’-bpe) ligands

  • A mixed-ligands Cd(II) coordination polymer, [Cd(2,2’-bpe)(C4O4)(H2O)2] (1) (2,2’-bpe = 1,2-bis(2-pyridyl)ethylene; C4O42− = dianion of squaric acid), has been synthesized and structurally characterized by single-crystal X-ray diffraction method. The coordination environment of Cd(II) ions in compound 1 is six-coordinate bonded to four oxygen atoms from two μ1,3-squarate (C4O42−) and two water molecules, and two nitrogen atoms from two 2,2’-bpe ligands. The squarate and 2,2’-bpe both act as bridging ligands with bis-monodentate coordination modes, connecting the Cd(II) ions to form a two-dimensional (2D) layered metal-organic framework (MOF). Adjacent 2D layers are then arranged in an ABAB parallel non-interpenetrating manner to construct its three dimensional (3D) supramolecular network. Intra- and inter-layers hydrogen bonding interactions between the C4O42− and water molecules in 1 provide an extra-stabilization energy on the construction of its 3D supramolecular network. The thermal stability of 1 is studied and discussed in details by TG analysis and in-situ PXRD measurement.

    Citation: Chih-Chieh Wang, Yu-Fan Wang, Szu-Yu Ke, Yanbin Xiu, Gene-Hsiang Lee, Bo-Hao Chen, Yu-Chun Chuang. Synthesis, structural characterization and thermal stability of a 2D layered Cd(II) coordination polymer constructed from squarate (C4O42−) and 2,2’-bis(2-pyridyl)ethylene (2,2’-bpe) ligands[J]. AIMS Materials Science, 2018, 5(1): 145-155. doi: 10.3934/matersci.2018.1.145

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  • A mixed-ligands Cd(II) coordination polymer, [Cd(2,2’-bpe)(C4O4)(H2O)2] (1) (2,2’-bpe = 1,2-bis(2-pyridyl)ethylene; C4O42− = dianion of squaric acid), has been synthesized and structurally characterized by single-crystal X-ray diffraction method. The coordination environment of Cd(II) ions in compound 1 is six-coordinate bonded to four oxygen atoms from two μ1,3-squarate (C4O42−) and two water molecules, and two nitrogen atoms from two 2,2’-bpe ligands. The squarate and 2,2’-bpe both act as bridging ligands with bis-monodentate coordination modes, connecting the Cd(II) ions to form a two-dimensional (2D) layered metal-organic framework (MOF). Adjacent 2D layers are then arranged in an ABAB parallel non-interpenetrating manner to construct its three dimensional (3D) supramolecular network. Intra- and inter-layers hydrogen bonding interactions between the C4O42− and water molecules in 1 provide an extra-stabilization energy on the construction of its 3D supramolecular network. The thermal stability of 1 is studied and discussed in details by TG analysis and in-situ PXRD measurement.


    Corona Virus Disease 2019 (COVID-19), caused by SARS-CoV-2, has been seriously impacting the world since the end of 2019 [1]. As of April 13, 2022, there have been over 499 million confirmed cases of COVID-19, including over 6 million deaths all over the world [2].

    Since the outbreak of COVID-19, many scholars have used different methods to study its transmission [3], such as neural network [4], time series analysis [5] and kinetic modeling [6].

    Dynamics models have played a key role in studying the development of things and assessing the impact of different intervention strategies [7,8]. In particular, during the COVID-19 outbreak, multiple dynamics models have been developed to investigate its spread and control.

    Before the availability of effective vaccines, non-pharmaceutical interventions strategies (NPIs) were taken into account controlling the pandemic transmission, such as lockdowns, the use of face-masks in public, quarantine of close contacts, isolation of confirmed cases, among others [9]. Ngonghala et al. [10] proposed a detailed mathematical model of COVID-19 that combined quarantine and isolation to assess the impact of NPIs on combating and mitigating the burden of COVID-19. Their results indicated that the early implementation (and enhancement of effectiveness) of these intervention measures is obviously critically-important to curtail COVID-19 transmission. NPIs could mitigate the spread of the virus, but it is not the permanent solution to the problem [11].

    Since January 2021, more than ten types of vaccines against SARS-CoV-2 have been fully or limitedly approved and used clinically [12]. And many countries are starting vaccination campaigns, which has improved the global epidemic to some extent [13]. Iboi et al. [14] developed a mathematical model for assessing the impact of an anti-COVID-19 vaccine on the spread of COVID-19 in the United States. This study showed that the prospect of eliminating COVID-19 in the US using the imperfect hypothetical vaccine is promising. Moreover, the integration of vaccination and physical distancing interventions, can result in better pandemic prevention [15]. Zou et al. [16] established a multiple patch coupled model to explore the impact of vaccination and NPIs on the control of COVID-19 and the results indicated that effective vaccination has positive impact on prevention of pandemic transmission and the joint implementation of vaccination and quarantine ensures the controllability of the epidemic.

    However, new variants of COVID-19 with high transmission rates are spreading around the world and vaccines are less effective in preventing infection than they were for earlier virus variants, which have brought new challenges to the elimination of pandemic [17,18]. Recently, Li et al. [19] developed a mathematical model of COVID-19 transmission with imperfect vaccination to explore effective and reasonable plans to prevent the spread of Delta variant. Their results found that the optimal control measure is to dynamically adjust three control measures, namely, vaccination, isolation and nucleic acid testing, to achieve the lowest number of infections at the lowest cost. Truszkowska et al. [20] developed an extremely detailed mathematical model, to study the combined effect of booster shot administration and testing practices in this stage of the pandemic.

    Motivated by the implement of NPIs, the promotion of vaccination strategy and the emerging of variants of COVID-19, we consider a mathematical model for mutated COVID-19 with quarantine, isolation and vaccination, make some theoretical analysis of the model, verify the applicability of the model by the COVID-19 pandemic mainly caused by Delta variant in South Korea, and finally, assess the impact of quarantine and vaccination on eliminating mutated COVID-19 transmission.

    The organization of this paper is as follows. In Section 2, the basic model formulation is discussed. In Section 3 we derive the disease free equilibrium and basic reproduction number R0. The local asymptotic stability and global asymptotic stability of the model at the disease free equilibrium are proved. In Section 4, the numerical simulation is carried out to verify the correctness of the proof. In Section 5, according to the epidemic data of COVID-19 in South Korea from August 22 to October 20, 2021, unknown parameters are obtained by two-stage fitting, and then the epidemic is predicted, which is compared with the real data to verify the applicability of the model. In Section 6, the impact of quarantine and vaccination on the control of COVID-19 are assessed by numerical simulation. Finally, in Section 7, we give some discussions.

    We develop an epidemic model, which incorporates the main interventions being implemented to curtail COVID-19 transmission (such as quarantine, isolation and vaccination). We stratify the population as susceptible (Su), vaccinated (Vu), exposed (Eu), asymptomatically-infectious (Ia), symptomatically-infectious (Iu) and recovered (R) compartments, and further stratify the population to include quarantined susceptible (Sq), quarantined vaccinated (Vq), quarantined exposed (Eq) and hospitalized (Ih) compartments, so that the total population of the model N(t) is divided into 10 compartments, namely

    N(t)=Su(t)+Sq(t)+Vu(t)+Vq(t)+Eu(t)+Eq(t)+Iu(t)+Ih(t)+Ia(t)+R(t).

    For developing the mathematical model, the basic assumptions are as follows:

    (ⅰ) The recruitment rate (either by birth or by immigration) of the population is given by a constant rate Λ and they are all susceptible.

    (ⅱ) Susceptible individuals move to exposed compartment by effective contacts with exposed, symptomatically-infectious or asymptomatically-infectious individuals and after latency period, they become infectious and move to infectious compartment.

    (ⅲ) After recovery the individuals have immunity to COVID-19 in a short time.

    (ⅳ) A part of vaccinated individuals will lose their immunity and rejoin the susceptible compartment.

    (ⅴ) After the immunity period, the vaccinated individuals become susceptible again.

    (ⅵ) Hospitalization is completely effective.

    (ⅶ) The exposed individuals and the asymptomatically-infectious individuals are also infectious, but the infectivity is weaker than that of symptomatically-infectious individuals, measuring by coefficients ηu and ηa respectively(0<ηu,ηa<1).

    (ⅷ) The contact rate c is the same for the individuals in symptomatically-infectious Iu, non-quarantined exposed Eu and the asymptomatically-infectious Ia compartments.

    (ⅸ) The latency period is defined as the days from exposure to the onset of illness.

    (ⅹ) The asymptomatically-infectious compartment Ia includes those with mild symptoms or no clinical symptoms of the COVID-19 at the end of the latency period.

    (ⅹⅰ) Considering that the number of people that an infected person can contact per unit time is finite, a more realistic standard incidence is used in the model.

    (ⅹⅱ) The vaccinated individuals will not lose immunity during the quarantine period.

    (ⅹⅲ) If the quarantine individuals have symptoms, they will be sent to the hospital.

    The assumptions above lead to the flow diagram of the model depicted in Figure 1.

    Figure 1.  Flow diagram of the model.

    It is worth noting that hospitalization indicates isolation at the hospital in this study. With contact tracing, a proportion, q, of individuals exposed to the virus is quarantined. The quarantined individuals, if infected, move to the compartment Eq and and the remaining individuals can either stay in compartment Vq or Sq, depending on whether they are vaccinated or not. For those individuals who are missed from contact tracing, the situation is similar.

    The model is given by the following deterministic system of nonlinear differential equations.

    dSudt=Λ[β(1q)λ+βqλ+(1β)qλ+ξv+d]Su+ωSq+ηvVu,dSqdt=(ω+θβλ+d)Sq+(1β)qλSu,dVudt=[ηv+εvβ(1q)λ+εvβqλ+p2(1β)qλ+d]Vu+ξvSu+p1ωVq,dVqdt=(p1ω+εvθβλ+d)Vq+p2(1β)qλVu,dEudt=[αu+f1σu+f2σu+(1f1f2)σu+d]Eu+β(1q)λSu+εvβ(1q)λVu,dEqdt=[rσq+(1r)σq+d]Eq+βqλSu+θβλSq+εvβqλVu+εvθβλVq+αuEu,dIudt=(ϕu+δu+γu+d)Iu+f1σuEu,dIhdt=(δh+γh+d)Ih+f2σuEu+rσqEq+ϕuIu+σaIa,dIadt=(σa+δa+γa+d)Ia+(1f1f2)σuEu+(1r)σqEq,dRdt=γuIu+γhIh+γaIadR. (2.1)

    where λ(t)=c(Iu+ηuEu+θηuEq+ηaIa)Su+Vu+Eu+Iu+Ia+R+θ(Sq+Eq+Vq).

    The initial conditions for system (2.1) are as follows:

    Su(0)=Su00,Sq(0)=Sq00,Vu(0)=Vu00,Vq(0)=Vq00,Eu(0)=Eu00,Eq(0)=Eq00,Iu(0)=Iu00,Ih(0)=Ih00,Ia(0)=Ia00,R(0)=R00. (2.2)

    The state variables and parameters of the model are described in Tables 1 and 2, respectively.

    Table 1.  Description of state variables of the model (2.1).
    State variable Description
    Su Population of non-quarantined susceptible individuals
    Sq Population of quarantined susceptible individuals
    Vu Population of non-quarantined vaccinated individuals
    Vq Population of quarantined vaccinated individuals
    Eu Population of non-quarantined exposed individuals
    Eq Population of quarantined exposed individuals
    Iu Population of non-hospitalized symptomatically-infectious individuals
    Ih Population of hospitalized symptomatically-infectious individuals
    Ia Population of asymptomatically-infectious individuals with mild or no clinical symptoms of the disease
    R Population of recovered individuals

     | Show Table
    DownLoad: CSV
    Table 2.  Description of the parameters of the model (2.1).
    Parameter Description Values
    c Effective contact rate 0.1
    β Probability of infection per contact 0.5
    q Proportion of infectious individuals quarantined at time of exposure 0.05
    ξv Vaccination rate (the reciprocal of the time during which everyone has completed vaccination) 0.8
    ηv Rate of immunity loss after vaccination (1/ηv is the mean duration of vaccine immunity) 0.56
    εv Ineffectiveness of vaccine against COVID-19 variants 0.14
    ηu Modification parameter accounting for the relative infectiousness of individuals in the Eu compartment in relation to individuals in the Iu compartment (0<ηu<1) 0.1
    ηa Modification parameter accounting for the relative infectiousness of individuals in the Ia compartment in relation to individuals in the Iu compartment (0<ηa<1) 0.1
    θ Ineffectiveness of quarantine 0.5
    ω Rate at which individuals in the Sq compartment revert to the Su compartment (1/ω is the duration of quarantine) 0.5
    αu Rate at which individuals in the Eu compartment are detected and placed in quarantine 0.116
    1σu(1σq) Latency period for non-quarantined (quarantined) exposed individuals 5.1
    σa Rate at which individuals in the Ia compartment are detected and hospitalized 0.309
    f1 Proportion of individuals in the Eu compartment who progress to the Iu compartment at the end of the incubation period (f1+f2<1) 0.4
    f2 Proportion of individuals in the Eu compartment who progress to the Ih compartment at the end of the incubation period (f1+f2<1) 0.2
    1f1f2 Proportion of individuals in the Eu compartment who progress to the Ia compartment 0.4
    r(1r) Proportion of individuals in the Eq compartment who move to the Ih (Ia) compartment 0.7
    ϕu Hospitalization rate of individuals in the Iu compartment 0.2
    p1 Modification parameter accounting for the relative release rate of individuals in the Vu compartment in relation to individuals in the Su compartment 0.5
    p2 Modification parameter accounting for the relative quarantine rate of individuals in the Vu compartment in relation to individuals in the Su compartment 1
    γu Recovery rate for individuals in the Iu compartment 0.1
    γh Recovery rate for individuals in the Ih compartment 0.125
    γa Recovery rate for individuals in the Ia compartment 0.13978
    δu Disease-induced mortality rate for individuals in the Iu compartment 0.015
    δh Disease-induced mortality rate for individuals in the Ih compartment 0.015
    δa Disease-induced mortality rate for individuals in the Ia compartment 0.075
    Λ Recruitment rate 20
    d Natural death rate 0.2

     | Show Table
    DownLoad: CSV

    Let H(t)=(Su(t),Sq(t),Vu(t),Vq(t),Eu(t),Eq(t),Iu(t),Ih(t),Ia(t) ,R(t)).

    Lemma 1. Consider the initial data Hi(0)0,i=1,2,...,10. Then, for any t>0, we have the non-negative solution for the system (2.1).

    Proof. Consider t1=sup{t>0:Hi(t)>0,i=1,2,...,10}. So, t1>0. The following result is given using the first equation of the model (2.1),

    dSudt=Λ+ωSq+ηvVu(d+ξv)Su[βλ+(1β)qλ]SuΛ(d+ξv)Su[βλ+(1β)qλ]Su.

    Then, it can be written as,

    ddt{Su(t)exp[(d+ξv)t+t0[βλ(ρ)+(1β)qλ(ρ)]dρ]}Λexp[(d+ξv)t+t0[βλ(ρ)+(1β)qλ(ρ)]dρ].

    Thus,

    Su(t1)exp[(d+ξv)t1+t10[βλ(ρ)+(1β)qλ(ρ)]dρ]Su(0)t10Λexp[(d+ξv)x+x0[βλ(ζ)+(1β)qλ(ζ)]dζ]dx,

    so that

    Su(t1)(Su(0)+t10Λexp[(d+ξv)x+x0[βλ(ζ)+(1β)qλ(ζ)]dζ]dx)×exp[(d+ξv)t1t10[βλ(ρ)+(1β)qλ(ρ)]dρ]>0.

    For the remaining equations, we take the same steps to show Hi(t)>0 (i=2,3,...,10) for every t>0.

    Let the closed and biologically feasible region be Ω, shown by Ω={(Su,Sq,Vu,Vq,Eu,Eq,Iu,Ih,Ia,R)R10+,0Su,Sq,Vu,Vq,Eu,Eq,Iu,Ih,Ia,R,NΛd}.

    Next, we present the following results for this feasible region.

    Lemma 2. The region Ω is a positively invariant and attracting region for system (2.1) with the non-negative initial conditions (2.2).

    Proof. Summing up the ten equations in system (2.1) and considering that all parameters of the model are non-negative, we get

    dN(t)dt=ΛdNδaIaδuIuδhIhΛdN.

    Now integrating both sides of the above inequality and using the comparison theorem [21], we obtain

    0<N(t)Λd+(N(0)Λd)edt.

    Clearly, 0<N(t)Λd, as t. If N(0)Λd, then N(t)Λd. Thus, the region Ω is positive invariant and attracts all the possible solutions of the model (2.1). We will consider the dynamic behavior of model (2.1) on Ω.

    Obviously, the model (2.1) always has a disease free equilibrium (DFE) P0(S0,0,V0,0,0,0,0,0,0,0), where

    S0=Λ(ηv+d)d(ηv+d+ξv),V0=Λξvd(ηv+d+ξv).

    The basic reproduction number R0 will be calculated using the next generation matrix method [22,23]. It follows that the next generation operator matrices, F and V for the new infection terms and the transition terms, are given, respectively,

    F=(ηuM1θηuM1M10ηaM1ηuM2θηuM2M20ηaM2000000000000000),andV=(K10000αuK2000f1σu0K300f2σurσqϕuK40(1f1f2)σu(1r)σq00K5),

    where, M1=cβ(1q)S0+εvV0Λ/d, M2=cβqS0+εvV0Λ/d, K1=σu+αu+d, K2=σq+d, K3=ϕu+γu+δu+d, K4=γh+δh+d, K5=σa+γa+δa+d. By the definition of the basic reproduction number R0, we get

    R0=ρ(FV1)=REu+REq+RIu+RIa, (3.1)

    where,

    REu=ηuK1M1,REq=θηu(αuK1K2M1+1K2M2),RIu=f1σuK1K3M1,RIa=ηa[((1f1f2)σuK1K5+αu(1r)σqK1K2K5)M1+(1r)σqK2K5M2].

    The quantity R0 is the basic reproduction number of the model (2.1). It measures the average number of the new COVID-19 infections generated by a typical infective individual introduced into a population where basic public health interventions (quarantine, isolation, vaccination, etc.) are implemented.

    In this section, we analyse the stability of the model (2.1) at the DFE. First, we show the local stability of system (2.1) at the DFE.

    Theorem 1. The DFE of the model (2.1) is locally asymptoticallystable if R0<1, and unstable if R0>1.

    Proof. Let ˉH=(Eu(t),Eq(t),Iu(t),Ia(t),Su(t),Sq(t),Vu(t),Vq(t),Ih(t),R(t)), we can obtain the Jacobian matrix of the system corresponding to ˉH at P0, and partition the matrix.

    It is given by

    J(P0)=(K1+ηuM1θηuM1M1ηaM1000000αu+ηuM2K2+θηuM2M2ηaM2000000f1σu0K30000000(1f1f2)σu(1r)σq0K5000000(ξv+d)ωηv0000(ω+d)0000ξv0(ηv+d)p1ω00000(p1ω+d)000000(δh+γh+d)00000γhd)=(J1J2J3J4)

    Using the Laplace theorem, it's easy to find that the eigenvalues of J(P0) are determined by the eigenvalues of J1 and J4.

    Consider the eigenvalues of J4 first.

    It is obvious that J4 has always four negative eigenvalues λ1=d, λ2=(δh+γh+d), λ3=(p1ω+d) and λ4=(ω+d), and the other eigenvalues of J4 are determined by the equation

    λ2+(ξv+ηv+2d)λ+ξvd+ηvd+d2=0.

    Clearly, λ5+λ6=(ξv+ηv+2d)<0, λ5λ6=ξvd+ηvd+d2>0, so λ5 and λ6 are both negative.

    Then consider the eigenvalues of J1. Through calculation and integration, we have

    det(λEJ1)=a0λ4+a1λ3+a2λ2+a3λ+a4=0,

    where,

    a0=1,a1=K1+K2+K3+K5ηuM1θηuM2,a2=K5(K2θηuM2)(1r)σqηaM2+(K1ηuM1)(K2+K5θηuM2)+K3(K1+K2+K5ηuM1θηuM2)ηa(1f1f2)σuM1+θηuM1(αuηuM2)f1σuM1,a3=K3[K5(K2θηuM2)(1r)σqηaM2+(K1ηuM1)(K2+K5θηuM2)ηa(1f1f2)σuM1+θηuM1(αuηuM2)]+K1[K5(K2θηuM2)(1r)σqηaM2]ηuK2K5M1αuθηuK5M1ηaαu(1r)σqM1ηa(1f1f2)σuK2M1f1σu(K2+K5)M1,a4=K3{K1[K5(K2θηuM2)(1r)σqηaM2]ηuK2K5M1αuθηuK5M1ηaαu(1r)σqM1ηa(1f1f2)σuK2M1f1σuK2K5M1}.

    If R0<1, we have ηuK1M1<1 and θηuK2M2<1, so it can be observed that a1>0.

    Because of a4K1K2K3K5=1R0, we obtain a4>0 if R0<1.

    Due to

    a3K1K2K3K5=1K1[1θηuK2M2ηa(1r)σqK2K5M2]+1K5(1ηuK1M1αuθηuK1K2M1θηuK2M2f1σuK1K3M1)+1K2[1ηuK1M1f1σuK1K3M1ηa(1f1f2)σuK1K5M1]+1K3{1ηuK1M1αuθηuK1K2M1θηuK2M2ηa[(1f1f2)σuK1K5+αu(1r)σqK1K2K5]M1ηa(1r)σqK2K5M2}>1K1(1REqRIa)+1K5(1REuREqRIu)+1K2(1REuRIuRIa)+1K3(1REuREqRIa)>0,

    then a3>0.

    Meanwhile, we can also obtain that

    a1a2a3=(K1+K2+K5ηuM1θηuM2)[K5(K2θηuM2)(1r)σqηaM2+K1K5ηuK5M1ηa(1f1f2)σuM1]+(K1+K2+K3+K5ηuM1θηuM2)[K3(K1+K2+K5ηuM1θηuM2)f1σuM1]+(K1+K2+K5ηuM1θηuM2)[K1(K2θηuM2)ηuK2M1αuθηuM1]K1K5(K2θηuM2)+ηuK2K5M1+αuθηuK5M1+(1r)σqηaM2ηaαu(1r)σqM1ηa(1f1f2)σuK2M1+f1σu(K2+K5)M1>(K1+K2+K5ηuM1θηuM2)[K5(K2θηuM2)(1r)σqηaM2+K1K5ηuK5M1ηa(1f1f2)σuM1]+(K1+K2+K3+K5ηuM1θηuM2)K3(K2+K5θηuM2)+(K1+K2ηuM1θηuM2)[K1(K2θηuM2)ηuK2M1αuθηuM1]+K5K1(K2θηuM2)K5ηuK2M1K5αuθηuM1K1K5(K2θηuM2)+ηuK2K5M1+αuθηuK5M1=(K1+K2+K5ηuM1θηuM2)[K5(K2θηuM2)(1r)σqηaM2+K1K5ηuK5M1ηa(1f1f2)σuM1]+(K1+K2+K3+K5ηuM1θηuM2)K3(K2+K5θηuM2)+(K1+K2ηuM1θηuM2)[K1(K2θηuM2)ηuK2M1αuθηuM1]>0.

    The first inequality is established due to (ηuK1+f1σuK1K3)M1<1, if R0<1. It is apparent from the above analysis that it satisfies the Routh-Hurwitz stability criterion. Thus, it follows that the DFE P0 is locally asymptotically stable if R0<1. On the other hand, we have a4K1K2K3K5=1R0<0 if R0>1, then a4<0, which shows that at least one of the eigenvalues of J1 is positive. Therefore, the DFE P0 is unstable if R0>1. This completes the proof.

    Theorem 2. The DFE of the model (2.1) is globallyasymptotically stable in Ω if R0<1.

    Proof. Let X=(Eu,Eq,Iu,Ih,Ia)T. It can be stated that

    dXdt(FV)X,

    with F and V are matrices on calculating R0. Let u=(ηu,θηu,1,0,ηa). It then follows from the fact R0=ρ(FV1)=ρ(V1F) and direct calculation that u is a left eigenvector of the matrix V1F, i.e., uV1F=R0u.

    Consider a Liapunov function

    L0=uV1X.

    Differentiating the above equation, we have

    dL0dt=uV1dXdtuV1(FV)X=u(R01)X.

    If R0<1, the equality dL0dt=0 implies that uX=0. This leads to Eu=Eq=Iu=Ia=0 by noting that all components of u except for the fourth element are positive.

    Clearly, let

    E={(Su,Sq,Vu,Vq,Eu,Eq,Iu,Ih,Ia,R)ΩdL0dt=0}={Eu=Eq=Iu=Ia=0},

    then the largest invariant set of the system in E is M={Eu=Eq=Iu=Ia=0}. By LaSalle's Invariant Principle [24], we get limtEu(t)=limtEq(t)=limtIu(t)=limtIa(t)=0. Then, it is easy to solve the 8th equation of the model (2.1), and we have

    Ih(t)=[Ih0+t0(f2σuEu(τ)+rσqEq(τ)+ϕuIu(τ)+σaIa(τ))eK4τdτ]eK4t.

    Using L'Hospital's rule,

    limtIh(t)=limtf2σuEu(t)+rσqEq(t)+ϕuIu(t)+σaIa(t)K4=0.

    In a similar way, for the 2nd, 4th and 10th equation of the model (2.1), we have limtSq(t)=limtVq(t)=limtR(t)=0. Hence, we can obtain the limit system of (2.1) as follows.

    dSudt=Λ(ξv+d)Su+ηvVu,dVudt=ξvSu(ηv+d)Vu. (3.2)

    It is easy to solve that

    Su(t)=S0+(Su(0)Λ(ηv+d)d(ηv+d+ξv))e(ηv+d+ξv)t,Vu(t)=V0+(Vu(0)Λξvd(ηv+d+ξv))e(ηv+d+ξv)t.

    Clearly, we can get limtSu(t)=S0, limtVu(t)=V0, so (S0,V0) is globally attractive for the limit system (3.2). By discussion of linearization systems for (3.2), it can be known that (S0,V0) is locally asymptotically stable if R0<1. Combining global attraction of (S0,V0), we can obtain that (S0,V0) is globally asymptotically stable for the limit systems (3.2). It follows that P0(S0,0,V0,0,0,0,0,0,0,0) is globally attractive for the original system (2.1). In addition, combining Theorem 1, we eventually concluded that P0 is globally asymptotically stable if R0<1.

    In this section, we present the numerical solution of the system (2.1).

    We can get R0=0.0147<1 and P0=(48.7179,0,51.2821,0,0,0,0,0,0,0,0,0) by using the parameter values given in Table 2. The dynamical behavior for different initial conditions of model (2.1) is presented in Figure 2. It's easy to find that, Su tends to 48.7179, Sq tends to 0, Vu tends to 51.2821, Vq tends to 0, Eu tends to 0, Eq tends to 0, Iu tends to 0, Ih tends to 0, Ia tends to 0, and R tends to 0. It shows that system (2.1) has a DFE and it is globally asymptotically stable with different initial values when R0<1. The numerical simulation results support the case stated in Theorem 2.

    Figure 2.  The dynamical behavior for different initial conditions of non-quarantined susceptible individuals Su, quarantined susceptible individuals Sq, non-quarantined vaccinated individuals Vu, quarantined vaccinated individuals Vq, non-quarantined exposed individuals Eu, quarantined exposed individuals Eq, non-hospitalized symptomatically-infectious individuals Iu, hospitalized infectious individuals Ih, asymptomatically-infectious individuals Ia and recovered individuals R, subfigures (a)–(j) represent them, respectively.

    In order to show that the model is practical, the COVID-19 pandemic mainly caused by Delta variant in South Korea is analysed and verified in this section. The experimental data come from the Central Disaster Management Headquarters of Korea [25]. About 97% of confirmed cases were infected by the Delta variant on August 22, 2021 [26], so August 22, 2021 is chosen as the starting date of the data set. The data in this paper is the official data of COVID-19 in Korea from August 22, 2021 to October 20, 2021.

    In order to verify the training effect, the data set is divided into training set (from August 22 to October 14, 2021, 54 days in total) and verification set (from October 15 to 20, 2021, 6 days in total) according to the ratio of 9:1. The unknown parameters of the model are obtained by fitting the real data of the training set, and the prediction effect of the model is tested by using the real data of the verification set. According to the Korea Disease Control and Prevention Agency (KDCA) [27], since September 24, 2021, the vaccinated individuals can be exempted from quarantine if they show no symptoms after close contact with the confirmed individuals. Therefore, this paper considers the training set in two stages. The first stage is from August 22, 2021 to September 23, 2021, and the second stage is from September 24, 2021 to October 14, 2021.

    Before fitting the parameters, we fix some parameters from previous literatures and studies to reduce the complexity.

    Since the recommended duration in quarantine for people suspected of being exposed to COVID-19 in South Korea was 14 days [28], we set ω = 1/14 per day. Further, Zhang et al. estimated that the mean incubation period of Delta variant was 4.4 days [29], which was shorter than that of the original strain reported by Yin et al. (4.4 vs. 6.8) [30]. Thus, we consider σu = σq = 1/4.4 per day. Some studies have suggested that most COVID-19 infections (over 95.6%) show moderate, mild, or asymptomatic infections, about 3.08% show severe symptoms (but without requiring ICU admission), and 1.32% show critically-severe symptoms requiring ICU admission [31,32]. Consequently, we set f2 = 0.044. According to [33], the proportion of asymptomatically-infectious individuals is 16%. Hence, we get f1 = 0.80304 and 1f1f2 = 0.15296 respectively. The modification parameter for the relative infectiousness of asymptomatically-infectious individuals (ηa) was estimated from [31,34] to be 0.5, so we set ηa=0.5. Due to the strict quarantine policy in South Korea [28], we assume that the ineffectiveness of quarantine θ=0. The average lifespan of Korean is 83.3 years [35]. Therefore, we have the natural death rate d=1/(83.3×365) per day. The latest total population of South Korea is about N(0) = 51,821,669 [36], hence, the recruitment rate Λ is obtained from Λ/d = N(0), so Λ=1704.41 per day. The World Health Organization (WHO) explicitly wrote in the document [37] that the critical characteristic or the minimal requirement is to confer protection for at least six months. Therefore, we assume that the average duration of vaccine immunity is 180 days, then ηv=1/180 per day. It can be seen from [38] that COVID-19 vaccine was on average 86.6% effective in preventing infections, so we select εv = 0.134. According to [39], the maximum and minimum values of disease-induced mortality rate from August 22 to October 14 were 0.93% and 0.82%, respectively, and we take the average value as 0.875%. Thus we set δu=δh=0.00875 per day. To obtain estimation for δa, we assume that δa=0.5δu (so that δa=0.004375 per day). According to [39] and calculation, vaccination rate ξv is about 7.6×103 per day. As can be seen from [27], the vaccinated individuals, like the unvaccinated individuals, needed to be quarantined, so p1=p2=1 in the first stage. However, since the vaccinated individuals did not need to be quarantined since September 24 [27], p1=p2=0 in the second stage. In addition, we fix the initial hospitalized population Ih(0) and total population N(0) as 27,959 and 51,821,669 respectively according to the data information. From [40], it can be known the number of newly confirmed cases per day confirmed by temporary screening. Let the vaccination proportion on August 22 be ξ. According to [41], ξ = 22.5%. The default parameter values and the initial values of state variables are given in Tables 3 and 4, respectively.

    Table 3.  Parameter values from the literatures (and those assumed).
    Parameter Default values Reference Parameter Default values Reference
    Λ 1704.41 [35,36] 1f1f2 0.15296 [31,32,33]
    d 1/(83.3×365) [35] r 0.7 [10]
    ξv 7.6×103 [39] σa 0.2435 [10]
    ηv 1/180 [37] ϕu 1/5 [10,31]
    εv 0.134 [38] p1 1   0 [27]
    ηu 0.5 Assumed p2 1   0 [27]
    ηa 0.5 [31,34] γu 1/10 [10,31]
    θ 0 [28] γh 1/8 [10,31]
    ω 1/14 [28] γa 0.13978 [42]
    σu(σq) 1/4.4 [29] δu 0.00875 [39]
    f1 0.80304 [31,32,33] δh 0.00875 [39]
    f2 0.044 [31,32] δa 0.004375 [39]

     | Show Table
    DownLoad: CSV
    Table 4.  Initial value of state variables.
    Variable Initial value Reference
    Su 39,465,104 (1ξ)(N(0)Sq(0)Vq(0)Eu(0)Eq(0)Ih(0)Iu(0)Ia(0)R(0))
    Sq 478,691 Derived from the number of newly confirmed cases per day confirmed by temporary screening, ω and ξ
    Vu 11,457,611 ξ(N(0)Sq(0)Vq(0)Eu(0)Eq(0)Ih(0)Iu(0)Ia(0)R(0))
    Vq 138,975 Derived from the number of newly confirmed cases per day confirmed by temporary screening, ω and ξ
    Eu 1664 Derived from Iu(0), Ia(0) and σu
    Eq 4852 Derived from the number of newly confirmed cases per day confirmed by temporary screening and σq
    Iu 1751 Derived from the proportion of symptomatically-infectious individuals, Ih(0) and ϕu
    Ih 27,959 Official data
    Ia 333 Derived from the proportion of asymptomatically-infectious individuals, Ih(0) and σa
    R 244,729 Derived from official data and the proportion of newly confirmed cases per day confirmed by temporary screening

     | Show Table
    DownLoad: CSV

    The remaining parameters are obtained by fitting the data in the training set. The model is solved by using lsqcurvefit function in Matlab, which utilizes a nonlinear least squares method to estimate parameters. The fitting parameters in two stages are given in Table 5.

    Table 5.  Fitted parameters.
    Parameter Fitted value of the first stage Fitted value of the second stage
    c 10.7392 24.6129
    β 0.1037 0.1216
    q 0.7727 1
    αu 0.0714 0.3156

     | Show Table
    DownLoad: CSV

    In order to evaluate the fitting and prediction effect, the mean absolute percentage error (MAPE) is used in this paper. MAPE between the cumulative number of confirmed cases obtained by model fitting and the actual data in the training set is used to evaluate the fitting effect of the model. Similarly, MAPE between the cumulative number of confirmed cases obtained by model prediction and actual data in the verification set is used to evaluate the prediction effect of the model. MAPE is expressed as:

    MAPE=1nnt=1|ˆCtCtCt|×100% (5.1)

    where, Ct is the actual cumulative number of confirmed cases on the t th day.

    The best fits to the reported data of the two stages via our model are depicted in Figure 3. Further, using the above parameters, we make a prediction on the verification set, and the prediction result is shown in Figure 4. As can be seen, there is a good agreement between the prediction result and the real data. The fitting and prediction effect of the model are shown in Table 6.

    Figure 3.  Data fitting of the model (2.1) in the first and second stages using COVID-19 cumulative number of confirmed cases in South Korea, subfigures (a) and (b) represent them, respectively.
    Figure 4.  Prediction of the model (2.1) (using the estimated parameters).
    Table 6.  Evaluation of fitting and prediction effect.
    Fitting effect of the first stage Fitting effect of the second stage Prediction effect
    MAPE 0.23% 0.22% 0.047%

     | Show Table
    DownLoad: CSV

    For simplicity of presentation, we make θ1=1θ and ε=1εv, i.e., θ1 is quarantine effectiveness and ε is vaccine efficacy.

    First of all, we simulate the impact of the quarantine rate (q) on the spread of COVID-19. As shown in the Figure 5(a), if the quarantine rate decreases, the cumulative number of deaths will sharply increase, which negatively affects prevention and control of COVID-19.

    Figure 5.  The cumulative number of deaths for various values of q and θ1, subfigures (a) and (b) represent them, respectively.

    Next, we consider the impact of quarantine effectiveness (θ1) on COVID-19 transmission. The results are shown in Figure 5(b), which imply that implementing strict quarantine measures is an effective means to prevent the development of the COVID-19 pandemic.

    We firstly assess the impact of the vaccination rate (ξv) on the prevention of COVID-19 transmission. The simulation results are presented in Figure 6(a), which show that a significantly large increasement in vaccination rate is necessarily needed for the control of COVID-19.

    Figure 6.  The cumulative number of deaths for various values of ξv, ε and ηv, subfigures (a), (b) and (c) represent them, respectively.

    As can be seen from the comparison results in Figure 6(b), when we increase vaccine efficacy (ε), the cumulative number of deaths markedly decreases. Meanwhile, it is easy to find that the stronger the effectiveness of vaccine, the faster the elimination of pandemic.

    Finally, we simulate the impact of rate of immunity loss (ηv) on dynamic transmission of the COVID-19. Depicted in Figure 6(c), the longer duration of vaccine immunity can have a better suppression effect on the spread of pandemic.

    A mathematical model for mutated COVID-19 combining quarantine, isolation and vaccination is established in this paper, and it is proved that the model is globally asymptotically stable at the DFE if R0<1, and the correctness of this result is verified by numerical simulation. The unknown parameters are obtained by fitting the COVID-19 epidemic data in South Korea from August 22 to October 14, 2021 in stages, and MAPE in two stages are 0.23 and 0.22%, respectively. The fitting effect of the model is satisfying. In the prediction of the data set from October 15 to October 20, 2021, MAPE is 0.047%, and the prediction effect is satisfactory, which also shows that the model is feasible. Numerical simulations indicate that it is essential to implement strict quarantine measures and strengthen contact tracing for combating the spread of COVID-19. Meanwhile, increasing vaccination rate and getting the vaccines with more effective and the longer duration of vaccine immunity have positive impact on the prevention of pandemic transmission.

    However, there are still many issues worthy of further study. For instance, most parameters (such as quarantine rate and vaccination rate) are dynamically changing during the development of COVID-19, but these characteristics are not taken into account in the current model. Thus, dynamic model with stochastic parameters deserves further study. Besides, the severity of infection is different in reality, so we can consider further the confirmed individuals with common and severe symptoms. These problems are of great interest which can be left for studying in the near further.

    The authors are grateful to the editors and the reviewers for their valuable comments and suggestions. This work was supported by the Fundamental Research Funds for the Central Universities (NO.2572018BC20).

    The authors declare there is no conflict of interest.

    [1] Chen B, Xiang S, Qian G (2010) Metal–Organic Frameworks with Functional Pores for Recognition of Small Molecules. Accounts Chem Res 43: 1115–1124. doi: 10.1021/ar100023y
    [2] Liu FL, Kozlevčar B, Strauch P, et al. (2015) Robust Cluster Building Unit: Icosanuclear Heteropolyoxocopperate Templated by Carbonate. Chem Eur J 21: 18847–18854. doi: 10.1002/chem.201502834
    [3] Wang XP, Chen WM, Qi H, et al. (2017) Solvent-Controlled Phase Transition of a CoII-Organic Framework: From Achiral to Chiral and Two to Three Dimensions. Chem Eur J 23: 7990–7996. doi: 10.1002/chem.201700474
    [4] Wang Z, Li XY, Liu LW, et al. (2016) Beyond Clusters: Supramolecular Networks Self-Assembled from Nanosized Silver Clusters and Inorganic Anions. Chem Eur J 22: 6830–6836. doi: 10.1002/chem.201504728
    [5] Yuan S, Deng YK, Sun D (2014) Unprecedented Second-Timescale Blue/Green Emissions and Iodine-Uptake-Induced Single-Crystal-to-Single-Crystal Transformation in ZnII/CdII Metal–Organic Frameworks. Chem Eur J 20: 10093–10098. doi: 10.1002/chem.201402211
    [6] Khan MI, Chang YD, Chen Q, et al. (1994) Synthesis and Characterization of Binuclear Oxo–Vanadium Complexes of Carbon Oxoanion Ligands. Crystal Structures of the Binuclear Vanadium(IV) Complex (NH4)[V2O2(OH)(C4O4)2(H2O)3]·H2O, of the Mixed-Valence Vanadium(V)/Vanadium(IV)–Squarate Species [(n-C4H9)4N][V2O3(C4O4)2(H2O)3]·3H2O and [(C4H9)4N]4[V4O6(C4O4)5(H2O)4]·6H2O, and of the Binuclear Vanadium(IV)–Oxalate Species [V2O2Cl2(C2O4)(CH3OH)4]·2Ph4PCl. Inorg Chem 33: 6340–6350.
    [7] Chen Q, Liu S, Zubieta J (1990) Coordination Chemistry of Polyoxomolybdates: The Structure of a Dodecanuclear Molybdate Cage Incorporating Hydrogen Squarate Ligands, [(C4H9)4N]4[Mo12O36(C4O4H)4]·10Et2O. Angew Chem Int Edit 29: 70–72. doi: 10.1002/anie.199000701
    [8] Lee CR, Wang CC, Wang Y (1996) Structural relationship of various squarates. Acta Crystallogr B 52: 966–975. doi: 10.1107/S0108768196009639
    [9] Bouayad A, Brouca-Cabarrecq C, Trombe JC, et al. (1992) Lanthanide(III)-copper(II) squarates: synthesis, crystal structure, magnetism and thermal behaviour of [La2Cu(C4O4)4(H2O)16]·2H2O and [Gd2Cu(C4O4)4(H2O)12]2H2O. Inorg Chim Acta 195: 193–201. doi: 10.1016/S0020-1693(00)85312-8
    [10] Petit JF, Gleizes A, Trombe JC (1990) Lanthanide(III) squarates 1. Five families of compounds obtained from aqueous solutions in an open system. Crystal structure and thermal behaviour. Inorg Chim Acta 167: 51–68.
    [11] Trombe JC, Petit JF, Gleizes A (1990) Lanthanide(III) squarates 2. High diversity of rare coordination modes of the squarate anion in a series of weakly hydrated cerium(III) squarates prepared by pseudo-hydrothermal methods. Inorg Chim Acta 167: 69–81.
    [12] Bouayad A, Trombe JC, Gleizes A (1995) Barium-copper(II) oxocarbon compounds: synthesis, crystal structures and thermal behaviours of [Ba(H2O)5][Cu(C2O4)2(H2O)] and [Ba(C4O4)0.5(H2O)2]2[Cu(C4O4)2(H2O)2]. Inorg Chim Acta 230: 1–7.
    [13] Trombe JC, Sabadie L, Millet P (2002) Synthesis and crystal structure of La(H2O)(C2O4)2·(CN3H6) and of [Nd(H2O)]2(C2O4)4·(NH4)(CN3H6). Solid State Sci 4: 1199–1028. doi: 10.1016/S1293-2558(02)01378-X
    [14] Trombe JC, Sabadie L, Millet P (2002) Hydrothermal synthesis and structural characterization of Fe(II)-squarate Fe2(OH)2(C4O4). Solid State Sci 4: 1209–1212.
    [15] Soules R, Dahan F, Laurent JP, et al. (1988) A novel coordination mode for the squarate ligand [dihydroxycyclobutenedionate(2–)]: synthesis, crystal structure, and magnetic properties of catena-diaqua(2,2'-bipyridyl)-µ-(squarato-O1,O2)-nickel(II) dehydrate. J Chem Soc Dalton Trans 587–590.
    [16] Beneto M, Soto L, Garcia-Lozano J, et al. (1991) Crystal and molecular structure and properties of the first characterized copper(II) one-dimensional polymer containing mepirizole [4-methoxy-2-(5-methoxy-3-methyl-1H-pyrazol-1-yl)-6-methylpyrimidine]. J Chem Soc Dalton Trans 1057–1061.
    [17] Hall LA, Williams DJ, Menzer S, et al. (1997) The Complexing Properties of 1-Aminosquarate Derivatives with Lead. Inorg Chem 36: 3096–3101. doi: 10.1021/ic961341+
    [18] Alleyne BD, Hall LA, Hosein HA, et al. (1998) Hydrogen-bonding interactions in the series of complexes [M(C4O4)(OH2)2(dmf)2] and [M(C4O4)(OH2)4] (M = Mn, Co, Ni, Cu, Zn). J Chem Soc Dalton Trans 3845–3850.
    [19] Crispini A, Pucci D, Aiello I, et al. (2000) Synthesis and crystal structure of dinuclear cyclopalladated 1,2- and 1,3-bridged squarato complexes. Inorg Chim Acta 304: 219–223. doi: 10.1016/S0020-1693(00)00091-8
    [20] Lin KJ , Lii KH (1997) Halozeotypes: a New Generation of Zeolite-Type Materials. Angew Chem Int Edit 36: 2076–2077.
    [21] Lai SF, Cheng CY, Lin KJ (2001) Hydrothermal synthesis of a thermally stable poroussupramolecular π–π framework: [{Co2(C12H8N2)4(μ-C4O4)(OH2)2}C4O4]·8H2O. Chem Commun 1082–1083.
    [22] Grove H, Sletten J, Julve M, et al. (2001) Syntheses, crystal structures and magnetic properties of one- and two-dimensional pap-containing copper(II) complexes (pap = pyrazino[2,3- f][4,7]phenanthroline). J Chem Soc Dalton Trans 259–265.
    [23] Nather C, Greve J, Jeβ I (2002) New Coordination Polymer Changing Its Color upon Reversible Deintercalation and Reintercalation of Water:  Synthesis, Structure, and Properties of Poly[Diaqua-(μ2-Squarato-O,O')-(μ2-4,4'-Bipyridine-N,N')- Manganese(II)] Trihydrate. Chem Mater 14: 4536–4542.
    [24] Piggott PMT, Hall LA, White AJP, et al. (2003) Attempted Syntheses of Lanthanide(III) Complexes of the Anisole- and Anilinosquarate Ligands. Inorg Chem 42: 8344–8352. doi: 10.1021/ic034922p
    [25] Yang BP, Mao JG (2005) New Types of Metal Squarato-phosphonates:  Condensation of Aminodiphosphonate with Squaric Acid under Hydrothermal Conditions. Inorg Chem 44: 566–571. doi: 10.1021/ic048685h
    [26] Maji TK, Mostafa G, Sain S, et al. (2001) Construction of a 3D array of cadmium(II) using squarate as a building block. CrystEngComm 3: 155–158. doi: 10.1039/b105080j
    [27] Konar S, Corbella M, Zangrando E, et al. (2003) The first unequivocally ferromagnetically coupled squarato complex: origin of the ferromagnetism in an interlocked 3D Fe(II) system. Chem Commun 1424–1425.
    [28] Manna SC, Zangrando E, Ribas J, et al. (2005) Squarato-bridged polymeric networks of iron(II) with N-donor coligands: Syntheses, crystal structures and magnetic properties. Inorg Chim Acta 358: 4497–4504. doi: 10.1016/j.ica.2005.07.014
    [29] Ghosh AK, Ghoshal D, Zangrando E, et al. (2006) Structural diversity in manganese squarate frameworks using N,N-donor chelating/bridging ligands: syntheses, crystal structures and magnetic properties. Dalton Trans 1554–1563.
    [30] Heinl U, Hinse P, Mattes RZ (2001) Oxalato- und Quadratato-Komplexe hochkoordinierter Metallionen: Die Raumnetzstrukturen von La2(C2O4)(C4O4)2(H2O)8 . 2,5 H2O und K[Bi(C2O4)2] ·5 H2O. Anorg Allg Chem 627: 2173–2177.
    [31] Habenschuss M, Gerstein BC (1974) An x-ray, spectroscopic, and magnetic study of the structure of nickel squarate dihydrate, NiC4O4.2H2O. J Chem Phys 61: 852–860.
    [32] Hosein HA, Hall LA, Lough AJ, et al. (1998) Attempted Syntheses of Transition Metal and Lanthanide (Dialkylamino)squarates. The Hydrolysis Problem. Inorg Chem 37: 4184–4189. doi: 10.1021/ic9801490
    [33] Hosein HA, Jaggernauth H, Alleyne BD, et al. (1999) First-Row Transition-Metal Complexes of the 1-Methoxycyclobutenedionate(1−) Ion. Inorg Chem 38: 3716–3720. doi: 10.1021/ic990199k
    [34] Spandl J, Brüdgam I, Hartl H (2001) Solvothermal Synthesis of a 24-Nuclear, Cube-Shaped Squarato-oxovanadium(IV) Framework: [N(nBu)4]8[V24O24(C4O4)12(OCH3)32]. Angew Chem Int Edit 40: 4018–4020. doi: 10.1002/1521-3773(20011105)40:21<4018::AID-ANIE4018>3.0.CO;2-7
    [35] Mukherjee PS, Konar S, Zangrando E, et al. (2002) Synthesis, crystal structure and magneto-structural correlation of two bi-bridging 1D copper(II) chains. J Chem Soc Dalton Trans 3471–3476.
    [36] Neeraj S, Noy ML, Rao CNR, et al. (2002) Sodalite networks formed by metal squarates. Solid State Sci 4: 1231–1236.
    [37] Dan M, Rao CNR (2003) An open-framework cobalt oxalato-squarate containing a ligated amine. Solid State Sci 5: 615–620. doi: 10.1016/S1293-2558(03)00047-5
    [38] Kurmoo M, Kumagai H, Chapman KW, et al. (2005) Reversible ferromagnetic–antiferromagnetic transformation upon dehydration–hydration of the nanoporous coordination framework, [Co3(OH)2(C4O4)2]·3H2O. Chem Commun 3012–3014.
    [39] Gandara F, Gomez-Lor B, Iglesias M, et al. (2009) A new scandium metal organic framework built up from octadecasil zeolitic cages as heterogeneous catalyst. Chem Commun 2393–2395.
    [40] Gutschke SOH, Molinier M, Powell AK, et al. (1997) Hydrothermal Synthesis of Microporous Transition Metal Squarates: Preparation and Structure of [CO33-OH)2(C4O4)2]·3H2O. Angew Chem Int Edit 36: 991–992. doi: 10.1002/anie.199709911
    [41] Yufit DS, Price DJ, Howard JAK, et al. (1999) New type of metal squarates. Magnetic and multi-temperature X-ray study of di-hydroxy(µ6-squarato)manganese. Chem Commun 1561–1562.
    [42] Robl C, Weiss AZ (1987) Darstellung und Struktur von Ag2C4O4. Anorg Allg Chem 546: 161–168. doi: 10.1002/zaac.19875460317
    [43] Yang CH, Chou CM, Lee GH, et al. (2003) Self-assembly of two mixed-ligands metal-organic coordination polymers, [MII2(DPA)2(C4O4)(C2O4)] (M = Cu, Zn). Inorg Chem Commun 6: 135–140. doi: 10.1016/S1387-7003(02)00705-0
    [44] Wang CC, Yang CH, Tseng SM, et al. (2004) A new moisture-sensitive metal-coordination solids {[Cd(C4O4)(bipy)(H2O)2]·3H2O} (bipy = 4,4'-bipyridine). Inorg Chim Acta 357: 3759–3764. doi: 10.1016/j.ica.2004.05.016
    [45] Wang CC, Yang CH, Lee GH, et al. (2005) Syntheses, Structures, and Magnetic Properties of Two 1D, Mixed-Ligand, Metal Coordination Polymers, [M(C4O4)(dpa)(OH2)] (M = CoII, NiII, and ZnII; dpa = 2,2'-dipyridylamine) and [Cu(C4O4)(dpa)(H2O)]2·(H2O). Eur J Inorg Chem 1334–1342.
    [46] Wang CC, Yang CH, Lee GH (2006) Hydrothermal Synthesis and Structural Characterization of Two pH-Controlled Cd–Squarate Coordination Frameworks, [Cd2(C4O4)2.5(H2O)4]·(dpaH)·1.5(H2O) and [Cd(C4O4)(dpa)(OH2)] (dpa = 2,2'-dipyridylamine). Eur J Inorg Chem 820–826.
    [47] Wang CC, Tseng SM, Lin SY, et al. (2007) Assemblies of Two Mixed-Ligand Coordination Polymers with Two-Dimensional Metal−Organic Frameworks Constructed from M(II) Ions with Croconate and 1,2-Bis-(4-pyridyl)ethylene (M = Cd and Zn). Cryst Growth Des 7: 1783–1790.
    [48] Smart V (1995) 4.043 Software for CCD Detector System, Siemens Analytical Instruments Division, Madison, WI, USA.
    [49] Saint V (1995) 4.035 Software for CCD Detector System, Siemens Analytical Instruments Division, Madison, WI, USA.
    [50] Sheldrick GM (1993) Program for the Refinement of Crystal Structures, University of Göttingen, Göttingen, Germany.
    [51] Sheldrick GM (1995) SHELXTL 5.03 (PC-Version), Program Liberary for Structure Solution and Molecular Graphics, Siemens Analytical Instruments Division, Madison, WI, USA.
    [52] Toby BH, Von Dreele RB (2013) GSAS-II: the genesis of a modern open-source all purpose crystallography software package. J Appl Crystallogr 46: 544–549. doi: 10.1107/S0021889813003531
    [53] Ito M, Weiss RJ (1963) New Aromatic Anions. IV. Vibrational Spectra and Force Constants for C4O4−2 and C5O5−2. J Am Chem Soc 85: 2580–2584.
    [54] Blatov VA, Shevchenko AP, Serezhkin VN (2000) TOPOS3.2: A new version of the program package for multipurpose crystal-chemical analysis. J Appl Crystallogr 33: 1193–1193.
    [55] Blatov VA, Carlucci L, Ciani G, et al. (2004) Interpenetrating metal–organic and inorganic 3D networks: A computer-aided systematic investigation. Part I. Analysis of the Cambridge structural database. CrystEngComm 6: 377–395.
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