With advances in computing power, DFT calculations
have expanded fromthe calculation of static properties to dynamical
and temperature-dependent simulations. For example,we have
recently validated our DFT simulations of the electrical conductivity
of aluminum in warm dense matter [22] and the EOS and conductivity
of high energy densitywater [23]. Furthermore, as the power
of high performance computers, such as Sandia’s Red Storm [24],
continues to increase, it appears feasible that quantum calculations
can be performed on numbers of atoms that are relevant to the
mesoscale.
With advances in computing power, DFT calculationshave expanded fromthe calculation of static properties to dynamicaland temperature-dependent simulations. For example,we haverecently validated our DFT simulations of the electrical conductivityof aluminum in warm dense matter [22] and the EOS and conductivityof high energy densitywater [23]. Furthermore, as the powerof high performance computers, such as Sandia’s Red Storm [24],continues to increase, it appears feasible that quantum calculationscan be performed on numbers of atoms that are relevant to themesoscale.
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