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Ion Implantation and Synthesis of Materials - Studium

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12 2 Particle InteractionsThe restriction to r-dependence is usually a good approximation. Throughoutthis text, the variable r will define the separation distance between two interactingparticles. The pairs might be atom–atom, electron–atom, electron–electron, ion–atom, etc.The potential energy, or binding energy, <strong>of</strong> a single atom is the work done inbringing all components <strong>of</strong> the atom from infinity to their equilibrium positions inthe atom. The simplest example is the semiclassical picture <strong>of</strong> the hydrogen atom.Thus, if an electron or charge, e, is brought from infinity to a distance r from thecenter <strong>of</strong> a proton under the attractive Coulomb field, the (negative) potentialenergy would ber ⎛∫ ∞ ⎜⎝⎞⎟⎠2e2a( ) = d = −( / ).2V r r e rr(2.3)2.3 Short- <strong>and</strong> Long-Range Interatomic ForcesThere are different types <strong>of</strong> forces that make up the interaction between two atomsover a large range <strong>of</strong> separation. Both experimental phenomena <strong>and</strong> theoreticalconsiderations suggest that the forces can be categorized as short- <strong>and</strong> long-rangeforces.The nature <strong>of</strong> the long-range force depends on whether the system consists <strong>of</strong>neutral atoms, charged ions, or a combination <strong>of</strong> the two. The force <strong>of</strong> greatestmagnitude at large separations is the Coulomb electrostatic interaction betweentwo charged ions, assumed to be point charges. The Coulomb potential is obtainedby applying (2.2) to (2.1) to give21 2c ( ) =−⎛ ZZeV r ⎜⎞⎟⎝ r ⎠.(2.4)where Z 1 e <strong>and</strong> Z 2 e are the charges <strong>of</strong> the ions. From (2.2) we see that the forceF(r) for a given central force field is expressed in terms <strong>of</strong> the interaction potentialbyc ( )∞V r = ∫rF ( r )d. r(2.5)If one or both <strong>of</strong> the particles are neutral, this Coulomb force is zero in the twobodyapproximation, <strong>and</strong> the long-range interaction is greatly reduced.As two atoms approach each other, some degree <strong>of</strong> merging <strong>of</strong> the particlesoccurs. As the particles merge, the electron orbits from the electrons <strong>of</strong> eachatom begin to overlap, <strong>and</strong> a limitation in the occupation <strong>of</strong> available electronstates arises due to the Pauli Exclusion Principle. Under such circumstances, the

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