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Research Article

The impact of testing and treatment on the dynamics of Hepatitis B virus

[version 1; peer review: 2 approved]
PUBLISHED 17 Sep 2021
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Abstract

Despite the intervention of WHO on vaccination for reducing the spread of Hepatitis B Virus (HBV), there are records of the high prevalence of HBV in some regions. In this paper, a mathematical model was formulated to analyze the acquisition and transmission process of the virus with the view of identifying the possible way of reducing the menace and mitigating the risk of the virus. The models' positivity and boundedness were demonstrated using well-known theorems. Equating the differential equations to zero demonstrates the equilibria of the solutions i.e., the disease-free and endemic equilibrium. The next Generation Matrix method was used to compute the basic reproduction number for the models. Local and global stabilities of the models were shown via linearization and Lyapunov function methods respectively. The importance of testing and treatment on the dynamics of HBV were fully discussed in this paper. It was discovered that testing at the acute stage of the virus and chronic unaware state helps in better management of the virus.

Keywords

: Positivity and boundedness of solutions, Equilibria of solutions, Next generation matrix, Linearization, Lyapunov functions, local and global stabilities.

1. Introduction

Hepatitis is an inflammation/scarring of the liver that contributes to various health complications, including death. It occurs due to an immune system attack by the virus in the liver and damages this vital organ of the body in the process (Ciupe et al., 2014). The hepatitis B virus (HBV) can survive outside the body for at least seven days. If the virus enters the body of someone who is not protected by vaccination during this time, it can still cause infection. The average incubation time for HBV is 75 days, but it can range from 30 to 180 days. Within 30 to 60 days of infection, the virus may be detected, persist, and grow into chronic hepatitis B (CDC, 2019). Hepatitis B is most common in the Western Pacific region with prevalence rate 6.2% and Africa with prevalence rate of 6.1%, with the Americas region (0.7%) having the lowest prevalence (WHO, 2019).

In highly endemic areas, the most common form of transmission of hepatitis B is from mother to child at birth (vertical transmission) or through horizontal route (contact with infected blood), particularly from infected children to uninfected children during the first five years of life. Chronic infection develops in infants infected by their mothers or before the age of five. It is often transmitted through transdermal or mucosal contact of infected persons to infected blood and different body fluids, such as spittle, catamenial, vaginal and spermatic fluids and, to a lesser degree, perspiration, breast milk, tears, and urine. In particular, hepatitis B can be transmitted through sexual contact in unvaccinated men who have sex with men (MSM) and heterosexual people who have multiple sexual partners or have contact with sex workers. However, adult infection contributes to chronic hepatitis in less than 5% of cases. This transmission may similarly ensue when needles and syringes are reused, whether in healthcare settings or among drug users. Furthermore, an infection can occur during medical, surgical, and dental procedures, such as tattooing or using razors and other similar objects contaminated with infected blood (Mpeshe and Nyerere, 2019).

2. Mathematical formulation

Some chronic carriers are unaware of their status and as such transmit the virus unknowingly and also at higher risk of cirrhosis and makes treatment less effective (Niederau, 2014, Mcpherson et al., 2013, Cohen et al., 2011, Piorkowsky, 2009, Lin et al., 2009, Meffre et al., 2004).

In view of this, this model is developed to factor the aforementioned set of people. In the model, the population is divided into the following different groups: the susceptible, the acute, the chronic unaware carriers, the chronic aware carriers, the treated chronic aware and the recovered individuals.

The total population at time t, denoted by Nt is divided into the six subgroups corresponding to different epidemiological status: susceptible individualsSt, acute At, unaware chronically infected Cut, aware chronically infected Cat, treated Tct, and removed/recovered class Rt. The model equation is subject to the initial conditions,

(1)
St0,At0,Cut0,Cat0,Tct0,Rt0

Figure 1 represents schematically the epidemiology of HBV infected model. The different disease stages are reproduced by the different circle and the arrows indicate the way individual progress from one stage to the other. It is assumed that at time, t, susceptible individuals, S, enter the population at a constant rate, Π. For all classes, individuals die at a constant natural mortality rate, μ.HBV chronically infected individuals (Cut, Cat)have an additional death rate due to HBV, c (Zhang and Zhang (2018)). It is assumed that HBV infected individuals on treatment, Tct do not transmit HBV infection. Susceptible individuals, St, may acquire HBV infection when in contact with individuals in A,Cu, and Ca,populace at a rate, λ (force of infection associated with HBV), where

(2)
λ=βA+α1Cu+α2CaN

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure1.gif

Figure 1. Compartmental flow diagram of HBV model.

Parameter β represents the probability that a contact will result in an HBV infection while α1,α2>1 respectively account for modification parameter of chronic HBV-infected individuals.

A proportion of the acute HBV-infected individuals, σ, spontaneously clear the virus, then return to being susceptible. The HBV acutely infected individuals develop to chronic without been aware if no testing at a rate, γ. The acutely infected and chronic unaware individual progress to chronic aware stage with a testing ν1,ν2 respectively and moved to treatment stage after testing at the rateδ. ω is the recovery rate of treated infected individual with full immunity.

These assumptions lead to the system of equations in (3)

(3)
dSdt=ΠλS+σAμSdAdt=λS(σ+γ+ν1)AdCudt=γA(ν2+μ+dc)CudCadt=ν2Cu+ν1A(δ+μ+dc)CadTcdt=δCa(ω+μ)TcdRdt=ωTcμR

where λ=βA+α1Cu+α2CaN

2.1 Positivity and boundedness of solutions

For the system of equations (3) to be epidemiologically meaningful, it is important to prove that all solution with non-negative initial conditions will remain non-negative.

Lemma 1: The initial values of the parameters are

S00A00Cu00Ca00Tc00R00andN00Φ

Then the solution of the model StAtCutCatTctRtNt is positive for all t0.

Proof

Considering the first equation in (3),

dSdt=ΠλS+σAμS
dSdtλ+μS1SdSλ+μdt
SS0eλ+μt0

Hence, S0

with respect to the second equation in (3);

dAdt=λSσ+γ+ν1A
dAdtσ+γ+ν1A
1AdAσ+γ+ν1dt
AA0eσ+γ+ν1t0

Hence, A0. Same goes for the other compartments

Clearly, the above state variables are positive on bounding plane +6.

For the boundedness the following calculation follows:

Nt=St+At+Cut+Cat+Tct+Rt
N=S+A+Cu+Ca+Tc+R
(4)
N=ΠλS+σAμS+λSσ+γ+ν1A+γAν2+μ+dcCu+ν2Cu+ν1Aδ+μ+dcCa+δCaω+μTc+ωTc-μR

Simplifying:

(5)
N+μN=ΠdcCu
(6)
N+μNΠ

Integrating gives:

NΠμ+keμt
maxlimnNlimnΠμ+keμtΠμ

It follows that the solutions of the model system (3) are positive and bounded in the region

T=S+A+Cu+Ca+Tc+R+6:S+A+Cu+Ca+Tc+RΠμ

It follows from Lemma 1 that it is sufficient to consider the dynamics of system (3) and the model can be considered to be epidemiologically well-posed.

2.2 Equilibrium points

The disease-free equilibrium of the equation (3) exists and is given by:

(7)
E0=Πμ00000

The endemic steady states are calculated here which is done by setting system of equation in (3.3.3) to zero and setting S=S,A=A,Cu=Cu,Ca=Ca,Tc=Tc,R=R so that

(8)
S=Π(μ3+δ+γ+2dc+υ1+υ2μ2+(dc2+υ1+υ2+δ+γdc+υ2+δγ+υ2+δυ1+δυ2)μ)+δυ1dc+υ2υ1+γυ1+σ+γL
(9)
A=υ1β+γ+σdc2+2υ12β+2γ+2σμ+υ2+δβα1γ+υ2+δβα2υ1βσυ2+δdc+υ1β+γ+σμ2+υ2+δβα1γ+υ2+δβα2υ1βσυ2+δμ+δα1α2υ2βΠL
(10)
Cu=Aγ
(11)
Ca=Cu((υ1+υ1μ)+υ2υ1+γ)γ
(12)
Tc=Caμ2dc2+μdc+υ2μ2+1υ1+υ2δ
(13)
R=ωTc

where

L=υ2+μ+dcυ1+γ+σμ3+2υ1+2γ+2σdc+υ1+γ+συ2+β+δγ+β+δυ1+δσμ2+υ1+γ+σdc2+υ1+γ+συ2γ2+2β+δσ2υ1γυ12+2β+δσυ1+δσdc+β+δγ+β+δυ1+δσυ2+βυ1+γγα1+α2υ1+δμυ1+γυ1β+γ+σdc2+υ1+γυ1β+γ+συ2+βα1δγ2+δ+α1+α2βυ1+δβσγ+δ+α2υ1βυ1dc+βγα1+α2υ1+δυ2+δγα1)υ1+γδ+μ+dcμ+ω

2.3 Basic reproduction number

The basic reproduction number (Ro) which is the number of secondary infections caused by an infectious individual is determined by the next generation matrix which is given by ρFV1

where:

F=ββα1βα2000000
V=σ+γ+υ100γdc+μ+υ20υ1υ2dc+μ+δ
V1=1σ+γ+υ100γσ+γ+υ1dc+μ+υ21dc+μ+υ20γυ2+υ1μ+υ1dc+υ1υ2σ+γ+υ1dc+μ+υ2dc+μ+δυ2dc+μ+υ2dc+μ+δ1dc+μ+δ
(14)
Ro=βσ+γ+υ1+βα1γσ+γ+υ1dc+μ+υ2+βα2γυ2+υ1μ+υ1dc+υ1υ2σ+γ+υ1dc+μ+υ2dc+μ+δ

2.4 Local stability analysis of the disease-free equilibrium E0

Theorem 1: E0 is locally asymptotically stable if R0 < 1 and unstable if R0 > 1.

Proof: The resulting matrix from the linearized model is dXdt=AX

X=x1x2x3x4x5,x6T,x1x2x3x4x5,x6R+6,and

The resulting Jacobian matrix at E0 is

(15)
JE0=μλβ+σβα1βα2000βσγν1λβα1βα2000γdcμν2λ0000ν1ν2dcμδλ00000δωμλ00000ωμλ

From (15), λ1=μ,λ2=ωμ,λ3=μ

and the resulting quadratic equation is:

(16)
βσγν1λdcμν2λdcμδλβα1dcμδλγ+βα2dcμν2λν1γν2
(17)
fλ=λ3+2μ+ν1+ν2β+δ+γ+σ+2dcλ2+βα2ν1βδ2βμ2βdcβν2+δγ+δμ+δσ+δdc+δν1+δν2+2γμ+2γdc+γν2+μ2+2μσ+2μdc+2μν1+μν2+2σdc+σν2+dc2+2dcν1+dcν2+ν1ν2γβα1λ+γμ2+γdc2+μ2σ+μ2ν1+σdc2+dc2ν1+μσν2+2μdcν1+μν1ν2+σdcν2+dcν1ν2βδμβδdcβδν22βμdcβμν2βdcν2βμ2βdc2+δγμ+δγdc+δγν2+δμσ+δμν1+δσdc+δσν2+δdcν1+δν1ν2+2γμdc+γμν2+γdcν2+2μσdcβδγα1βγμα1βγα1dc+ν2γβα2+ν1βα2dc+ν1βα2μ+ν1βα2ν2

Now, λ1, λ2,λ3 < 0 since the values are assumed positive. If R0 < 1, E0 is stable and unstable when R0 < 1.

2.5 Global stability of the disease-free equilibrium

The global behavior of the equilibrium system (3) is analyzed here in this section.

Theorem 2: For system (3), the disease-free equilibrium E0 is asymptotically stable globally if R0<1.

Proof: Considering the Lyapunov function defined as:

(18)
GACuCa=1B0A+βα1B0B1+βα2υ2B0B1B2Cu+βα2B0B2Ca
(19)
GACuCa=1B0A+βα1B0B1+βα2υ2B0B1B2Cu+βα2B0B2Ca
(20)
GACuCa=1B0βA+α1Cu+α2CaNSσ+γ+ν1A+βα1B0B1+βα2υ2B0B1B2γAν2+μ+dcCu+βα2B0B2ν2Cu+ν1Aδ+μ+dcCa

At DFE, S=N so that (20) becomes:

(21)
GACuCa=1B0βA+α1Cu+α2Caσ+γ+ν1A+βα1B0B1+βα2υ2B0B1B2γAν2+μ+dcCu+βα2B0B2ν2Cu+ν1Aδ+μ+dcCa

Expanding and simplifying (21) gives:

(22)
G=βB0+βα1γB0B1+βα2υ2γB0B1B2+βα2ν1B0B21A+βα1B0βα1B1B0B1βα2υ2B1B0B1B2+βα2ν2B0B2Cu+βα2B0βα2B2B0B2Ca
(23)
G=R01A0

From Equation (23), it can be deduced that the DFE is globally stable since R0 < 1.

2.6 Local stability of endemic equilibrium

Theorem 3: If R0>1, then the endemic equilibrium is locally asymptotically stable.

Proof:

The endemic equilibria of system (3), denoted by SACuCaTcR, can be rewritten as:

LetS=x+S,A=y+A,Cu=z+Cu,Ca=h+Ca,Tc=p+Tc,R=j+R
(25)
J=B0μλB1+σB2B3B4B5B6B7σγν1λB8B9B11B120γdcμν2λ0000ν1ν2dcμδλ00000δωμλ00000ωμλ

From (25), λ1=μ,λ2=ω+μ,λ3=dc+μ+ν2, then;

(26)
J=B0μλB1+σB2B6B7σγν1λB80γdcμν2λ

from (26);

λ3+γ+2μ+σB0B4+dc+ν1+ν2λ2+2γμB0γ+γdc+γν2+μ2+2μσμB02μB4+μdc+2μν1+μν2σB0+σB3+σdc+σν2+B0B4B0dcB0ν1B0ν2B3B1B4dcB4ν2+dcν1+ν1ν2λ+B5γ+γμν2+μσν2+μν1ν2+B3B2γ+γμ2+μ2σ+μ2ν1+μdcν1+γμdc+μσdcμ2B4γμB0γB0dcγB0ν2μσB0+μσB3+μB0B4μB0ν1μB3B1μB4dcμB4ν2σB0dcσB0ν2+σB3dc+σB3ν2+B0B4dc+B0B4ν2B0dcν1B0ν1ν2B3B1dcB3B1ν2

The result of the determinant of the Jacobian matrix is of the form:

(27)
a0λ3+a1λ2+a2λ+a3

where

a0=1
a1=γ+2μ+σB0B4+dc+ν1+ν2
a2=2γμB0γ+γdc+γν2+μ2+2μσμB02μB4+μdc+2μν1+μν2σB0+σB3+σdc+σν2+B0B4B0dcB0ν1B0ν2B3B1B4dcB4ν2+dcν1+ν1ν2
a3=B5γ+γμν2+μσν2+μν1ν2+B3B2γ+γμ2+μ2σ+μ2ν1+μdcν1+γμdc+μσdcμ2B4γμB0γB0dcγB0ν2μσB0+μσB3+μB0B4μB0ν1μB3B1μB4dcμB4ν2σB0dcσB0ν2+σB3dc+σB3ν2+B0B4dc+B0B4ν2B0dcν1B0ν1ν2B3B1dcB3B1ν2

By the Routh–Hurwitz criterion governing the polynomials of order 3, we have the following:

  • 1. a2.a3 are positive

  • 2. a1a2>a3

From equation (27), 1 and 2 are satisfied.

Therefore, endemic equilibrium is locally asymptotically stable.

2.7 Global stability of the endemic equilibrium

Theorem 4: The equations of the model have a positive distinctive endemic equilibrium whenever R0 > 1, which is said to be globally asymptotically stable.

Proof: Considering the Lyapunov function defined as:

(28)
LSACuCaTcR=SSlnSS+AAlnAA+CuCulnCuCu+CaCalnCaCa+TcTclnTcTc+RRlnRR

where L takes it derivative along the system directly as:

(29)
dLdt=1SSdSdt+1AAdAdt+1CuCudCudt+1CaCadCadt+1TcTcdTcdt+1RRdRdt
(30)
dLdt=1SSΠβA+α1Cu+α2CaNS+σAμS+1AAβA+α1Cu+α2CaNSσ+γ+ν1A+1CuCuγAν2+μ+dcCu+1CaCaν2Cu+ν1Aδ+μ+dcCa+1TcTcδCaω+μTc+1RRωTcμR

At equilibrium,

(31)
Π=(β(A+α1Cu+α2Ca)N)SσA+μS(σ+γ+ν1)=(β(A+α1Cu+α2Ca)AN)S(ν2+μ+dc)=γACu(δ+μ+dc)=ν2CuCa+ν1ACa(ω+μ)=δCaTcω=μRTc
(32)
dLdt=1SSβA+α1Cu+α2CaNSσA+μSβA+α1Cu+α2CaNS+σAμS+1AAβA+α1Cu+α2CaNSβA+α1Cu+α2CaANSA+1CuCuγAγACuCu+1CaCaν2Cu+ν1Aν2CuCa+ν1ACaCa+1TcTcδCaδCaTcTc+1RRμRTcTcμR=1SSβASN+βα1CuSN+βα2CaSNσA+μSβASNβα1CuSNβα2CaSN+σAμS+1AAβASNβASN+βα1CuSNβα1CuSAAN+βα2CaSNβα2CaSAAN+1CuCuγA1ACuACu+1CaCaν2Cu1CuCaCuCa+ν1A1ACaACa+δCa1TcTc1CaTcCaTcμR1RR1RTcRTc
(33)
=1SSβASN1ASNASNβα1CuSN1CuSNCuSN+βα2CaSN1CaSNCaSNσA1AAμS1SS+1AAβASN1ASNASNβα1CuSN1CuSANCuSAN+βα2CaSN1CaSANCaSAN+1CuCuγA1ACuACu+1CaCaν2Cu1CuCaCuCa+ν1A1ACaACa+δCa1TcTc1CaTcCaTcμR1RR1RTcRTc
=μS1SS2βASN1SS1ASNASNβα1CuSN1SS1CuSNCuSNβα2CaSN1SS1CaSNCaSNσA1SS1AA+βASN1AA1SNSN+βα1CuSN1AA1CuSANCuSAN+βα2CaSN1AA1CaSANCaSAN+σA1CuCu1ACuACu+ν2Cu1CaCa1CuCaCuCa+ν1A1CaCa1ACaACa+δCa1TcTc1CaTcCaTcμR1RR1RTcRTc
(34)
=μS1SS2+P1SACaCuTcR+P2SACaCuTcR

where,

P1SACaCuTcR=βASN1SS1ASNASNβα1CuSN1SS1CuSNCuSNβα2CaSN1SS1CaSNCaSNσA1SS1AAμR1RR1RTcRTc
P2SACaCuTcR=βASN1AA1SNSN+βα1CuSN1AA1CuSANCuSAN+βα2CaSN1AA1CaSANCaSAN+σA1CuCu1ACuACu+ν2Cu1CaCa1CuCaCuCa+ν1A1CaCa1ACaACa+δCa1TcTc1CaTcCaTc

P10 whenever

(35)
ASNASN,CuSNCuSN,CaSNCaSN,RTcRTc

and P20 whenever

(36)
SNSN,CuSANCuSAN,CaSANCaSAN,ACuACu,CuCaCuCa,ACaACa,CaTcCaTc

Thus, dLdt0 if the condition in (35) and (36) holds.

therefore, by LaSalle asymptotic stability theorem (LaSalle, 1976), and Oke et al. (2020) the positive equilibrium state dLdt is globally asymptotically stable in the positive regionR+6.

3. Numerical computation

The numerical study is carried out using maple software embedded code for the Runge-Kutta of fourth order. Here, the subsequent default values are assumed for the embedded parameters taken from theoretical studies in literatures γ=0.9,β=0.008,σ=0.59,dc=0.00693,μ=0.00693,ω=0.1,ν1=0.002,ν2=0.002,α1=0.0016,α2=0.0016,δ=0.0085,Π=0.07. The values remain unchanged throughout* the computations except otherwise indicated.

The effects of varying the testing rate of the acute individuals υ1, testing rate of chronic individuals (υ2) and treatment rate of chronic individuals (δ) on the population dynamics are shown in Figures 2 to 7. From Figures 2 and 3, an increase in the parameters values reduces susceptible and acute populations thereby reducing the spread HBV due to low interaction between the host immune system and the virus. Therefore, the appearance of HBV and the pathogenesis reduces, which in so doing, lessens the potential injury on the liver. Hence, the liver is shielded from hepatocellular carcinoma over time. The rate of chronic unaware and chronically aware individuals is examined in Figures 4 and 5. The parameter variations show a significant decrease in the chronic unaware population which implies that testing at that stage is a great tool for reducing the disease transmission. The transmission process dies down as the time progresses; this discourages liver inflammation as a result of lowering the infected individuals. Meanwhile, the chronic population in Figure 5, depicts a high significant influence of the acutely infected and chronically unaware infected individuals over time. A chronic infection phase is found at the time range 10<t<20, as such, the individuals are exposed to liver carcinoma or cirrhosis. Hence, the chronic population diminishes as the parameters are increased.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure2.gif

Figure 2.

Behavioral dynamics of susceptible population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure3.gif

Figure 3.

Behavioral dynamics of acute population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure4.gif

Figure 4.

Behavioral dynamics of chronic unaware population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure5.gif

Figure 5.

Behavioral dynamics of chronic aware population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure6.gif

Figure 6.

Behavioral dynamics of treated population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

2ce6cd63-4244-4853-ad3d-6bf40f0e4e5c_figure7.gif

Figure 7.

Behavioral dynamics of recovered population when varying testing rate for acute and chronic individuals and treatment for chronic individuals.

In Figures 6 and 7, the impact of varying the testing rate of the acute individuals υ1, testing rate of chronic individuals (υ2) and treatment rate of chronic individuals (δ) on the treated and the recovered population are presented. The treated population increases with parameters variation along the rising time (t) as a result of long time effect of parameter values. The recovery rate is enhanced as observed in Figure 7 due to significant simulation of surface antibodies of Hepatitis B. This is in conformity with the works of Pang et al. (2010) and Ullah et al. (2019). This result implies that an intensification in testing at all infectious states and rise in treatment of chronic individual will bring about a reduction in the HBV transmission process which is a response to the WHO goal for 2030 that concentrating efforts on awareness program and campaign will sure bring about a decrease or eradication in the transmission process of the virus (WHO, 2020).

4. Conclusion

A deterministic model of hepatitis B testing was developed and investigated, which included testing in the chronic unaware state as well as testing in all infectious states. The model has disease-free and endemic equilibria. The basic reproduction number was calculated using the next generation matrix method. The equilibria's local and global stability were discussed and shown to be asymptotically stable. The testing and treatment rate effects were thoroughly discussed.

Data availability

No data are associated with this article.

Grant information

None declared.

Competing interests

None declared.

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Oludoun O, Adebimpe O, Ndako J et al. The impact of testing and treatment on the dynamics of Hepatitis B virus [version 1; peer review: 2 approved]. F1000Research 2021, 10:936 (https://doi.org/10.12688/f1000research.72865.1)
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Reviewer Report 17 Dec 2021
Segun oke, Department of Mathematical and Applied Mathematics, University of Pretoria, Pretoria, South Africa 
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The authors worked on the impact of testing and treatment on the dynamics of Hepatitis B virus. Although the manuscript is well presented and gives new insight into the Hepatitis B virus, especially for unvaccinated men who have sex with ... Continue reading
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oke S. Reviewer Report For: The impact of testing and treatment on the dynamics of Hepatitis B virus [version 1; peer review: 2 approved]. F1000Research 2021, 10:936 (https://doi.org/10.5256/f1000research.76473.r94650)
NOTE: it is important to ensure the information in square brackets after the title is included in all citations of this article.
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Reviewer Report 06 Oct 2021
Sulyman Olakunle Salawu, Department of Mathematics, Landmark University, Omu-aran, Nigeria 
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Reviewer Reports on the impact of testing and treatment on the dynamics of Hepatitis B virus.
The impacts of different parameters were examined. The manuscript is well written and presented logically. The abstract captures accurately the whole work and ... Continue reading
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Salawu SO. Reviewer Report For: The impact of testing and treatment on the dynamics of Hepatitis B virus [version 1; peer review: 2 approved]. F1000Research 2021, 10:936 (https://doi.org/10.5256/f1000research.76473.r94651)
NOTE: it is important to ensure the information in square brackets after the title is included in all citations of this article.

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