• Matter and Radiation at Extremes
  • Vol. 6, Issue 1, 015902 (2021)
Sergio Davis1、2, Felipe González-Cataldo3、4, Gonzalo Gutiérrez4, Gonzalo Avaria1、2, Biswajit Bora1、2, Jalaj Jain1, José Moreno1、2, Cristian Pavez1、2, and Leopoldo Soto1、2
Author Affiliations
  • 1Comisión Chilena de Energía Nuclear, Casilla 188-D, Santiago, Chile
  • 2Departamento de Física, Facultad de Ciencias Exactas, Universidad Andres Bello, Sazié 2212, piso 7, Santiago 8370136, Chile
  • 3Department of Earth and Planetary Science, University of California, Berkeley, California 94720, USA
  • 4Grupo de Nanomateriales, Departamento de Física, Facultad de Ciencias, Universidad de Chile, Casilla 653, Santiago, Chile
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    DOI: 10.1063/5.0030158 Cite this Article
    Sergio Davis, Felipe González-Cataldo, Gonzalo Gutiérrez, Gonzalo Avaria, Biswajit Bora, Jalaj Jain, José Moreno, Cristian Pavez, Leopoldo Soto. A model for defect formation in materials exposed to radiation[J]. Matter and Radiation at Extremes, 2021, 6(1): 015902 Copy Citation Text show less

    Abstract

    A simple model for the stochastic evolution of defects in a material under irradiation is presented. Using the master-equation formalism, we derive an expression for the average number of defects in terms of the power flux and the exposure time. The model reproduces the qualitative behavior of self-healing due to defect recombination, reaching a steady-state concentration of defects that depends on the power flux of the incident radiation and the material temperature, while also suggesting a particular time scale on which the incident energy is most efficient for producing defects, in good agreement with experimental results. Given this model, we discuss the integral damage factor, a descriptor that combines the power flux and the square of the irradiation time. In recent years, the scientific community involved in plasma-facing materials for nuclear fusion reactors has used this parameter to measure the equivalent material damage produced in experiments of various types with different types of radiation and wide ranges of power flux and irradiation time. The integral damage factor is useful in practice but lacks formal theoretical justification. In this simple model, we find that it is directly proportional to the maximum concentration of defects.
    F=Q×t=EA×t12,(1)

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    P(n|t)t=P(n|t)mnW(n,m)+mnP(m|t)W(m,n),(1)

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    W(n,m)=ω+(n)δm,n+1+ω(n)δm,n1,(2)

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    P(n|t)t=P(n|t)ω+(n)+ω(n)+P(n+1|t)ω(n+1)+P(n1|t)ω+(n1).(3)

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    ω+(n)=ωT(β,Ev)+ωQ(Q,Ev)NnN,(4)

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    QAEvΔt=QNσEvΔt.(1)

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    ω+(n)=ωT(β,Ev)+ηQσEvNnN,(5)

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    ω(n)=ωR(β)nN.(6)

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    P(x|t)t+xμ(x)P(x|t)=0,(7)

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    μ(x)=ωT+ηQσEv(1x)ωRx.(8)

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    txt=ωT+ηQσEv1xtωRxt,(9)

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    xQ,t,β=exp(t/τ)xeq(β)Aτ+Aτ,(10)

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    A=ωT+ηQσEv,τ=1A+ωR.(11)

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    xeq(β)AτQ=0=0(1)

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    xeq(β)=exp(βEv)=ωTωT+ωR.(1)

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    ωTτ0=xeq(β),ωRτ0=1xeq(β),(12)

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    xt,Q,β=ηQτ(Q)σEv(1exp(t/τ(Q)))+xeq(β),(13)

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    τ0τ(Q)=1+ηQτ0σEv=1+QQ0,(14)

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    xt,Q,β=Q1+Q1exp(t(1+Q))+xeq(β),(15)

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    Q1+Q1xeq(β)(16)

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    Ev=3.6 eV,(17a)

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    σ=1(3.1652Å)20.1Å2.(17b)

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    η=104,(18a)

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    τ0=300 ps,(18b)

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    Q0=σEvητ0=1.93×1010 W/cm2.(18c)

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    xmax=Q1+Q+xeq(β)(19)

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    F=Qt(20)

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    xQ,t=f(Qt),(21)

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    F0=Q0τ0=333486Ws12/cm2.(22)

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    Q(t,F)=F/t.(23)

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    ddFx*(F)F=0=2u01+2u02=α,(24)

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    xmax(F)αFF0(25)

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    xmax(F)=exp(Ev/kBTeffmax(F)),(26)

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    Teffmax(F)=EvkBln(xmax(F))EvkBlnF0/(αF).(27)

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    Sergio Davis, Felipe González-Cataldo, Gonzalo Gutiérrez, Gonzalo Avaria, Biswajit Bora, Jalaj Jain, José Moreno, Cristian Pavez, Leopoldo Soto. A model for defect formation in materials exposed to radiation[J]. Matter and Radiation at Extremes, 2021, 6(1): 015902
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