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Ion Implantation and Synthesis of Materials - Studium

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4.3 Energy-Transfer Cross-Section 43From the above analysis <strong>of</strong> Fig. 4.5, we can define the probability <strong>of</strong> a projectilewith energy E undergoing a scattering event or a collision with a target nucleuswhile traversing a thickness ∆x asPE ( ) = Nσ( E) ∆ x.(4.10)Equation (4.10) defines the total collision cross-section, σ (E), between an energeticparticle <strong>of</strong> energy E <strong>and</strong> the target atoms. The total cross-section gives ameasure <strong>of</strong> the probability for any type <strong>of</strong> collision to occur where energytransfersare possible, for energies up to <strong>and</strong> including the maximum valueT M = 4M 1 M 2 E 0 /(M 1 + M 2 ) 2 .In addition to the total cross-section, we also wish to consider the more restrictivetypes <strong>of</strong> interactions that can occur between target nuclei <strong>and</strong> particles withenergy E. Consider the condition where we wish to know the probability that aprojectile with energy E will transfer an amount <strong>of</strong> energy between T <strong>and</strong> T + dTto a target atom. Such a probability function defines the differential energytransfercross-section, dσ (E)/dT, <strong>and</strong> is obtained by differentiating (4.10)d PE ( ) d σ( E) 1 d σ( E)PET ( , )dT≡ dT= N∆xdT=d T,dT d T σ ( E) dT(4.11)where P(E, T) is the probability that an ion with energy E will undergo a collisionproducing an energy-transfer in the range T <strong>and</strong> T + dT while traversing a distance∆x, <strong>and</strong> is simply defined as the ratio <strong>of</strong> the differential cross-section to the totalenergy-transfer cross-section.Probability functions can be constructed based on the scattering processes describedby Figs. 4.2 <strong>and</strong> 4.3. The probability <strong>of</strong> a collision producing a deflectionθ c in the incident projectile’s trajectory is given byP( θ ) = σ( θ ) Nd x,cc(4.12a)<strong>and</strong> the probability <strong>of</strong> scattering the projectile into the angular range between θ c<strong>and</strong> θ c + dθ c while it travels a distance dx is given byd P( θc) d σ( θc) 1 d σ( θc)P( θc, b)db ≡ = N dbdx =d b,db d b σθ ( ) dbc(4.12b)where σ (θ c ) is the total angular scattering cross-section given in (4.3), <strong>and</strong> dσ (θ c )is the differential angular scattering cross-section given in (4.4). An expression

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