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Physics And Chemistry Basis Of Biotechnology - De Cuyper - tiera.ru

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Radiation-induced bioradicals: technologies and research<br />

determined with a (near) experimental accuracy, erroneous results can be produced in<br />

those cases where the incorporation of electron correlation, the instantaneous<br />

interaction of the electrons, is quintessential. This is particularly t<strong>ru</strong>e for the calculation<br />

of magnetic properties of radicals such as hyperfine coupling constants. The electron<br />

correlation can be accounted for by so-called post-Hartree-Fock approaches that are<br />

however characterised by a dramatic increase of the computational work involved.<br />

Consequently, their use is limited to small molecular systems, even with the formidable<br />

computer power currently available. Therefore, resort has to be sought to other methods<br />

if one is interested in routinely calculating properties to a high degree of accuracy in<br />

systems that are of t<strong>ru</strong>e interest to a biologist or chemist such as radicals derived from<br />

biomolecules.<br />

<strong>De</strong>nsity functional calculations have proved valuable in this respect over the last<br />

few years. The basis for density functional theory (DFT) is the proof by Hohenberg and<br />

Kohn (1964) that the ground state electronic energy of an atomic or molecular species<br />

is completely determined by the electron density r. This means that there exists a oneto-one<br />

correspondence between the electron density of the system and the energy. The<br />

problem is that although it has been proven that each different density yields a different<br />

ground-state energy, the functional 2 connecting these two quantities is unknown. The<br />

goals of DFT methods is to design functionals that connect the electron density with the<br />

energy.<br />

In analogy with the wave function approach, the energy functional can be divided<br />

into three parts, kinetic energy, T[ρ ], attraction between the nuclei and electrons,<br />

E ne[ρ], and electron-electron repulsion, E ee[r]. The E ee[ρ] term may be hrther divided<br />

into a Coulomb and exchange part, J [r] and K[r], respectively. The exchange energy is<br />

a correction that should be made to the Coulomb energy to take into account the effect<br />

of spin correlation . 3 Thus the energy functional is written as<br />

E[r] = T[r] +Ene[r]+ J[r] +K[r]*<br />

The key for the practical use of DFT methods in computational chemistry lies in the<br />

Kohn-Sham theory. Central in this theory is the calculation of the kinetic energy Ts[r]<br />

assuming that the electrons are not interacting (in the same way as non-interacting<br />

electrons are described in wave mechanics by the HF method). In reality, the electrons<br />

are interacting, so the Kohn-Sham kinetic energy does not provide the total kinetic<br />

energy. However, the difference between the exact kinetic energy and that calculated<br />

2 A functional is a prescription for producing a number from a function which in turn<br />

depends on variables. The electron density p is a function (of spatial and spin coordinates)<br />

whereas an energy dependirig on the density is a functional, denoted with<br />

brackets, E[ρ].<br />

3 Spin correlation refers to the quantum mechanical effect that gives electrons of<br />

opposite spin an increased probability of being found near to each other, whereas those<br />

of the same spin are preferentially kept apart.<br />

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